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Energy field-assisted high-speed dry milling green machining technology for difficult-to-machine metal materials

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Energy field-assisted machining technology has the potential to overcome the limitations of machining difficult-to-machine metal materials, such as poor machinability, low cutting efficiency, and high energy consumption. High-speed dry milling has emerged as a typical green processing technology due to its high processing efficiency and avoidance of cutting fluids. However, the lack of necessary cooling and lubrication in high-speed dry milling makes it difficult to meet the continuous milling requirements for difficult-to-machine metal materials. The introduction of advanced energy-field-assisted green processing technology can improve the machinability of such metallic materials and achieve efficient precision manufacturing, making it a focus of academic and industrial research. In this review, the characteristics and limitations of high-speed dry milling of difficult-to-machine metal materials, including titanium alloys, nickel-based alloys, and high-strength steel, are systematically explored. The laser energy field, ultrasonic energy field, and cryogenic minimum quantity lubrication energy fields are introduced. By analyzing the effects of changing the energy field and cutting parameters on tool wear, chip morphology, cutting force, temperature, and surface quality of the workpiece during milling, the superiority of energy-field-assisted milling of difficult-to-machine metal materials is demonstrated. Finally, the shortcomings and technical challenges of energy-field-assisted milling are summarized in detail, providing feasible ideas for realizing multi-energy field collaborative green machining of difficult-to-machine metal materials in the future.
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Energy field-assisted high-speed dry milling green
machining technology for difficult-to-machine
metal materials
Jin ZHANGa,b, Xuefeng HUANGa,b, Xinzhen KANGa,b, Hao YIa,b, Qianyue WANGa,b, Huajun CAO ()a,b
aCollegeofMechanicalandVehicleEngineering,ChongqingUniversity,Chongqing400044,China
bStateKeyLaboratoryofMechanicalTransmissions,ChongqingUniversity,Chongqing400044,China
Correspondingauthor.E-mail:hjcao@cqu.edu.cn(HuajunCAO)
©TheAuthor(s)2023.Thisarticleispublishedwithopenaccessatlink.springer.comandjournal.hep.com.cn
ABSTRACT Energyfield-assistedmachiningtechnologyhasthepotentialtoovercomethelimitationsofmachining
difficult-to-machinemetalmaterials,suchas poor machinability, low cutting efficiency,andhighenergyconsumption.
High-speeddrymillinghas emerged asatypicalgreenprocessingtechnologydueto its highprocessingefficiencyand
avoidanceofcuttingfluids.However,thelackofnecessarycooling and lubrication in high-speed dry milling makes it
difficult to meet the continuous milling requirements for difficult-to-machine metal materials. The introduction of
advancedenergy-field-assistedgreenprocessingtechnologycanimprovethemachinabilityofsuchmetallicmaterialsand
achieve efficient precision manufacturing, making it a focus of academic and industrial research. In this review, the
characteristics and limitations of high-speed dry milling of difficult-to-machine metal materials, including titanium
alloys,nickel-basedalloys,andhigh-strengthsteel,aresystematicallyexplored.Thelaserenergyfield,ultrasonicenergy
field,andcryogenicminimumquantitylubricationenergyfieldsareintroduced.Byanalyzingtheeffectsofchangingthe
energyfieldandcuttingparametersontoolwear,chipmorphology,cuttingforce,temperature,andsurfacequalityofthe
workpiece during milling, the superiority of energy-field-assisted milling of difficult-to-machine metal materials is
demonstrated. Finally, the shortcomings and technical challenges of energy-field-assisted milling are summarized in
detail, providing feasible ideas for realizing multi-energy field collaborative green machining of difficult-to-machine
metalmaterialsinthefuture.
KEYWORDS difficult-to-machine metal material, green machining, high-speed dry milling, laser energy field-
assistedmilling,ultrasonicenergyfield-assistedmilling,cryogenicminimumquantitylubricationenergyfield-assisted
milling
1Introduction
With continuous improvements in advanced manufac-
turing fields such as aerospace, rail transit, and clean
energy equipment production, various high-performance
alloys (e.g., nickel-based alloys, titanium alloys, and
high-strengthsteels)are widely used.However, they are
regarded as typical difficult-to-machine metal materials
because of their good toughness, high strength, and
excellentwearresistance,whichposeaseriouschallenge
to the high-performance manufacturing process of high-
efficiencyandprecisionmachining[13].
The poor machinability of difficult-to-machine metal
materialsisreflectedinthefollowing:
Chemicallevel
For titanium alloys containing Ti, Mo, Cr, and V,
highly chemically active metal elements can reduce
machinability[4].Furthermore,theαphaseformedinthe
organization of the alloy structure is a hexagonal lattice
structure,whichincreasescuttingdifficulty.
Fornickel-basedalloys,whichexhibitasingleaustenite
structureorganization, Al, Ti,and other oxygen-friendly
elements promote the oxidation of materials at high
temperatures,resulting in tool adhesion. In addition, the
strengthening phases (intermetallic compounds, borides,
and carbides) in the alloy materials form hard particles,
resultinginincreasedtoolwear[5].
ReceivedJuly13,2022;acceptedNovember29,2022
Front.Mech.Eng.2023,18(2):28
https://doi.org/10.1007/s11465-022-0744-9
REVIEWARTICLE
ThecontentsofCr,Mn,Si,Ni, andotherelementsare
high in high-strength steel, which has a tempered
martensite structure. Different vc (cutting speed) values
correspond to different chip morphologies and play a
leading role in improving performance. The addition of
Cr can change the hardness, strength, and toughness of
steel; the presence of Mn can influence its hot
machinability, and the addition of Si can improve its
tensile and yield strength. The addition of Ni can
simultaneously improve the strength and hardness of
metal materials and increase the cutting force and
processingenergyconsumption[6].
Thermalconductivity
Compared with 45 steel, the thermal conductivity of
titaniumalloysisreducedby80%,whichcaneasilylead
to plastic deformation in the shear zone and at high
temperatures, thus aggravating tool wear and causing
workhardening[7].
Thethermalconductivityofnickel-basedalloysislow,
andheataggregationduringtheprocessingofsuchalloys
can easily occur, resulting in high local temperatures,
which causes surface stress, a considerable temperature
gradientintheworkpiece,andawork-hardeningproblem
[8].
The thermal conductivity of high-strength steel is low
(only 40% of that of 45 steel), which hinders the
transmission of the cutting heat, resulting in the
phenomenon that the temperature of the tool-workpiece
contactsurfacecanbetoohigh,thusleadingtothework-
hardeningproblemoftheworkpiecesurface[9].
Cuttingmachinability
Titanium alloy cutting, which is a typical shear
machining process, is inclined to produce large shear
angles [10] and the ‘negative shrinkage’ phenomenon,
which has a negative impact on the machining process.
Compared with 45 steel, the machinability of titanium
alloysisintherangeof0.15–0.5[11].
Becauseoftheincreaseinheataccumulation,cracksor
burns on the surface of the workpiece can easily occur,
whichmakesitdifficulttoensurethequalityandintegrity
of the machined surface during the cutting process of
nickel-basedalloys. Compared to 45 steel, the machina-
bilityofnickel-basedalloysislessthan0.15[12].
Theplasticdeformationofhigh-strengthsteelmaterials
is large, and because of the severe friction during the
machining process, it is easy to produce chip tumors.
Furthermore,theunevenstressdistributioncausessevere
tooltipwear,which leads toinstabilityinthemachining
process and reduces the cutting efficiency. Compared
with45steel,themachinabilityofhigh-strengthsteelisin
therangeof0.5–0.65[13].
High-speed cutting has the advantages of improving
machining efficiency and reducing production costs and
is also used in the field of difficult-to-machine metal
materials [1417]. Because the deformation zone of
materials subjected to high-speed cutting is usually
accompaniedbystrongstrain,ahighstrainrate,andhigh
temperatures[1820], traditional coolingand lubrication
ofthe cutting deformation zoneby pouring cuttingfluid
isnecessaryduringthecuttingprocess[21,22].Compared
withconventionalmilling (CM),thefrictionbetweenthe
workpieceandthe tool ismoreintenseinthehigh-speed
milling process, and the time at which the deformation
zone remains in a high-temperature state is longer. The
heatofthecuttingfluidisuneven,andlocaldropletscan
start boiling [23]. A large number of microbubbles are
blockedbyanoilfilm,resultinginanincreaseintheheat
transfer resistance and a decrease in the heat exchange
efficiency [24]. In addition, the extensive use of cutting
fluidnotonly endangers thehealth of operators (cancer,
asthma,andskin diseases)butalsoseriouslypollutesthe
environment (air, soil, and water) and increases the
economiccost ofprocessing wasteliquid andchips; the
costofcuttingfluidfrompurchasetoprocessingaccounts
for 16% to 30% of the total cost of manufacturing
difficult-to-machine metal materials, which is much
higherthanthetoolcostofonly7%[2529].Therefore,
new green and low-carbon processing technologies that
canreplacepouringandcuttingshouldbeexplored.
High-speed dry milling (HSDM) is regarded as a
typicalgreenandefficientmachiningtechnologybecause
it not only improves the machining efficiency but also
eliminates the use of cutting fluids [3033]. The
developmentoftoolcoatings and high-speed dry cutting
machine tools has enabled the use of HSDM for
machining [3436]. Lu et al. [37] used coated tools for
the HSDM of hardened steel and found that the cutting
force decreased and the tool life increased. The
ChongqingMachineToolGroup,jointlywithChongqing
University, pioneered high-speed dry cutting machine
tools such as YS3116CNC7 and Y3120CNC7, which
improvedtheproduction efficiency ofmachinetoolsand
reduced the manufacturing cost of workpieces [38].
Considering the inherent characteristics of difficult-to-
machine metal materials, coupled with the high cutting
speedandlackofcuttingfluidnecessaryfor coolingand
lubrication in the HSDM manufacturing process, the
frictionbetweenthe tool andtheworkpieceandbetween
thetool andthechipisextremelyintense,resulting inan
increase in the temperature of both the tool and
workpiece, which affects the machining accuracy of the
workpiece[39,40].Consequently,theHSDMofdifficult-
to-machinemetalmaterialscanachievethedesiredeffect
only in a specific process-feasible regime, and it is
difficult to achieve full-condition adaptation [22].
Therefore, research on innovative HSDM processes is
crucial.
Thermal-assisted machining (TAM) was proposed in
the 1950s [41]. Its advantage is that preheating can not
only reduce the ultimate strength of materials but also
promote plastic deformation of hard materials during
processing. The advantages of TAM also include
improved manufacturing performance, machining
2Front.Mech.Eng.2023,18(2):28
efficiency, and quality of difficult-to-machine metal
materials by increasing the temperature of the cutting
zone through an external heat source. Under ideal
conditions,theshearbandofthematerialinstantaneously
reaches the ideal temperature, and most of the heat is
removedbythechip,therebyavoidingheatgenerationin
theshearzone[42].ForthepositivecontributionofTAM
technologytothecutting process, theheatsourceshould
be local, fast, and controllable. Lasers, induction coils,
plasma,andoxyacetylene torcheshavebeenwidelyused
[4345].Becauseimproperselectionofaheatsourcewill
lead to adverse changes in the microstructure after
machining [46,47], researchers have mainly focused on
thetwo commonly used heating methods of plasma and
laser in machining. Considering that the laser has the
advantages of a precise and controllable local area, no
need for protective gas, and high spatial accessibility, it
hasemergedas the mostpromisingauxiliaryheatsource
fortheprocessingofdifficult-to-machinemetalmaterials,
and subsequent research has mainly focused on laser-
assistedprocessingtechnology[42].
The implementation process of laser energy field-
assisted milling (LAM) uses a laser to preheat the
workpiece locally in advance to achieve material
softeningandchange the materialpropertiesoftheshear
zonethat isreadytoberemoved,whichcan improvethe
manufacturingperformanceof difficult-to-machinemetal
materials under temperature-assisted conditions [48]. At
present,laserswidelyusedfordifficult-to-machinemetal
materials mainly include carbon dioxide (CO2) lasers,
high-power semiconductor lasers (HPDL), and neody-
mium-doped yttrium aluminum garnet (Nd:YAG) lasers
[42].Aseachofthethreelasershasitsownmerits,itis
necessary to make reasonable choices according to the
properties of the materials to be processed. After the
materialareatoberemovedisheatedbylaserassistance,
thesubsequentmachiningprocesscanreduce the cutting
force,prolongthetoollife,improvethematerialremoval
rate, reduce cutting energy consumption, reduce
manufacturingcosts, and optimize the surface quality of
theworkpiece [4951]. However,the difficulty ofLAM
machining is the precise control of the preheating
temperature of the workpiece. Studies have shown that
the laser power, heat source size, laser scanning speed,
and heating position have a significant influence on the
preheatingtemperatureofthematerial[52,53].Therefore,
toobtain ideal resultsin the shearregion of difficult-to-
machine metal materials, laser energy field-assisted
machiningparametersshouldbereasonablyselected[54].
The introduction of a laser energy field in CM
machining prolongs the entire machining cycle, and
ultrasonic vibration energy field-assisted milling
(UVAM) with intermittent cutting characteristics can
improvethematerialremovalrate,whichcancompensate
for the disadvantage of the long machining cycle of
LAM. Therefore, UVAM is important. In the UVAM
process, electrical signals are converted into ultrasonic
frequencyvibrations,which act along acertaindirection
ontheworkpieceortool[55,56]torealizetool-workpiece
separationsothatthecutting area is periodically opened
to ensure that the traditional cutting fluid enters the
cutting area and provides rapid cooling at high
temperatures[57].Furthermore,duringtheprocessing of
difficult-to-machine metal materials, the chip removes
most of the heat, and ultrasonic separation can ensure
rapid chip breaking [5860], thereby avoiding the
accumulationofheatonthetoolandworkpiece.UVAM
alsoexhibitsanacousticsofteningeffect[61].Inaddition
to the above advantages, UVAM can also reduce the
cutting force [62,63], improve the material removal rate
[64], optimize the surface quality of the workpiece
[65,66], extend the tool life [67,68], reduce the
manufacturing costs, and achieve green and low-carbon
machining [69] by regularly changing the contact state
between the workpiece and tool [70,71]. However, the
vibration frequency and amplitude of UVAM signifi-
cantly influence the machining process. Therefore, to
maintain the advantages of UVAM, it is necessary to
controlthevibrationfrequencyandamplitudereasonably.
The minimum quantity lubrication (MQL) technology
can effectively solve the heat transfer problem of
difficult-to-machine metal materials in HSDM. In 1997,
KlockeandEisenblätter[72]proposedaneconomicaland
environmentally friendly MQL technology. In this
process, a very small amount of atomized droplets is
sprayed into the cutting area with high-pressure gas for
lubrication[73],andanycuttingheatpositionisreached
withthehelpofthetrachea,whichcaneffectivelyreduce
the cutting force and cutting heat, prolong the tool life,
andoptimizethesurfacequalityoftheworkpiece[74,75].
However, under some specific conditions, micro-
lubrication technology has some shortcomings: When
usingMQLtoassistinthehigh-speedcuttingofdifficult-
to-machine metal materials, excessive heat production
leadstotheruptureofthelubricatingoilfilm,resultingin
insufficient cooling in the cutting area and lubrication
failure [76,77]. In addition, the cooling performance of
micro-lubricationtechnologywithhigh-pressureatomiza-
tion airflow is limited, and a performance gap remains
between this technology and traditional pouring cutting
[78,79].Therefore, further researchon MQL technology
isneeded.
Nanofluid minimum quantity lubrication (NMQL)
technologyisanenhancementofMQLtechnologythatis
realized by adding nanoparticles in proportion to the
MQL fluid. Compared with ordinary MQL, the thermal
conductivityofnanofluids is higher, whichisdue to the
addition of nanoparticles with excellent antifriction and
antiwear properties [80], thereby reducing the heat
transfer resistance and improving the heat exchange
efficiency and material removal rate. In addition,
nanoparticles with small volumes undergo Brownian
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 3
motionin the base fluid, which can improve lubrication
[81]. Compared to MQL, the lubrication advantages of
NMQL have been confirmed in many studies [8286].
However, when the cutting temperature is high (600–
1000°C),theheattransferefficiencyofthenanoparticles
is still limited [87]. Although the cutting temperature is
reducedfortitaniumalloys[88],nickel-basedalloys[89],
high-strength steel [90], and other difficult-to-machine
metal materials, the range of the cooling amplitude is
small, and defects such as burns and adhesion on the
surfaceoftheworkpiecestill occur. Therefore, the heat-
exchangeproblemintheNMQL-assistedcutting process
ofdifficult-to-cutmaterialsremains.
Cryogenic technology is generally used to solve the
problem of heat transfer in the cutting process by
injecting a liquid/gaseous medium into the shear
deformation zone [91]. Currently, the main cryogenic
media used for difficult-to-machine metal materials
includeliquidnitrogen(LN2)[92],liquidcarbon dioxide
(LCO2)[93],supercritical carbon dioxide (SCCO2)[94],
and cold air (CA) [95]. Cryogenic processing can not
only improve the material removal rate but also
effectively prolong tool life [96]; thus, the cryogenic
manufacturing cost is far lower than the traditional
pouring processing cost [97,98]. Different temperature
thresholds can be realized using different liquid/gaseous
mediato avoid insufficient cooling or excessive cooling
hardening. However, the lubrication performance of
cryogenic technology is insufficient, and its friction
reduction and wear resistance characteristics must be
improved[99].
Inviewofthehigh-performancemanufacturingprocess
ofdifficult-to-machinemetalmaterials,thecurrentlybest-
recognized method is the combination of the cryogenic
cold medium, MQL (NMQL), and milling, which is
referred to as cryogenic minimum quantity lubrication
energy field-assisted milling (CMQLAM). CMQLAM
not only reduces the temperature of the shear zone but
also retains the lubrication ability of MQL (NMQL).
Apart from being a green low-carbon technology, its
advantages include adequate cooling, reducing cutting
force, optimizing the surface quality of the workpiece,
extending tool life, and reducing manufacturing costs
[100102].Consideringthatthecryogenicmediumtype,
gaspressure,andMQL flow rate affecttheperformance
ofCMQLAM,itisnecessarytoreasonablyregulatethese
three parameters to obtain the optimal effect of
CMQLAM. Figure1 shows the overall structure of this
review.
It has been widely reported that the processing
performance of HSDM can be improved using LAM,
UVAM, or CMQLAM alone. However, it is difficult to
select an appropriate auxiliary process from multiple
energy fields and to realize machining under various
harsh conditions. Based on this, this paper reviews the
latest research progress of energy-field-assisted green
machining technology for difficult-to-machine metal
materials;summarizestheoperatingmechanisms,techni-
cal difficulties, and application status of HSDM, LAM,
UVAM, and CMQLAM for difficult-to-machine metal
materials; and compares and analyzes the effects on
cutting force, heat, chip morphology, tool life, specific
cuttingenergy,materialremovalrate,andsurfacequality
of titanium alloy, nickel-based alloy, and high-strength
steel compared with traditional milling under energy-
field-assisted conditions. The development direction of
energy-field-assisted green machining technology is
reported in this paper to provide a reference for multi-
energy-fieldcomposite-assistedgreenmachining techno-
logy.
2HSDM of difficult-to-machine metal
materials
Compared with CM pouring cutting, HSDM is a near-
zero-emission green processing technology that elimi-
natestheenvironmentalpollutionandoccupationalhealth
hazards caused by cutting oil and avoids the cleaning
process of cutting oil adhering to the surface of the
workpiece and some iron chips. Under appropriate
process conditions with high-performance coated tools,
HSDMcanreducethecuttingforce,temperature,surface
roughness,andtoolwear.Accordingtothecuttingspeed
rangesoftheHSDM,difficult-to-machinemetalmaterials
can be divided into three parts. The logical structure of
theclassificationisshowninFig.2.
For HSDM of titanium alloys, after finding that the
effectofcuttingparameteroptimizationontoolwearwas
notclear, chemicalvapordeposition(CVD)andphysical
vapor deposition (PVD) tool coatings were utilized to
compare the cutting effect of HSDM. The PVD coating
was more suitable for HSDM. In addition, the effect of
the AlTiN and TiAlSiN multi-nanocomposite structure
coatings were analyzed. The results showed that the
quaternaryTiAlSiNcoatingnotonlyresultedinuniform
chipsbutalsohadhighoxidationresistance,significantly
prolongingtoollife.
To analyze the HSDM of high-strength steel, first,
frictionandwearexperimentsshowedthatHSDMcould
reduce the wear of the machined surface to a greater
extent than CM. Second, the optimal cutting parameters
were obtained when using the CVD coating of Al2O3 +
TiC.Subsequently,threeotheroptimalTiN/TiCN/TiAlN
coatings and their cutting parameters were obtained.
Finally, using the TiCN-NbC coating, the influence of
cuttingparameters onthe surface roughness, microhard-
ness,andresidualstressoftheworkpiecewasanalyzed.
For the HSDM of nickel-based alloys, first, the
influenceof cutting parameters on thecutting force was
investigatedbasedon(Al,Ti)N-coatedtools.Second,the
effect of cutting parameters on tool wear was studied
4Front.Mech.Eng.2023,18(2):28
using TiN/TiAlN-coated tools. Third, the influence of
cuttingparametersonthecuttingforceandtoolwearwas
analyzed using polycrystalline cubic boron nitride
(PCBN) tools. Furthermore, the influences of cutting
Fig. 1Overall structure of this review. HSDM: high-speed dry milling, LAM: laser-assisted milling, UVAM: ultrasonic vibration-
assistedmilling,CMQLAM:cryogenicminimumquantitylubricationenergyfield-assistedmilling.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 5
parameters on the surface roughness when using
TiAlN/TiN PVD nano-multilayer coated tools were
analyzed.Inaddition,theeffectsofcuttingparameterson
thematerialremovalrate,cuttingtemperature,microhard-
ness, and residual stress were briefly described for the
application of the SiAlON ceramic tool. The effects of
thistool andthePVDnano-multilayercoatedtoolonthe
surfaceroughnesswerecompared, and it was foundthat
the SiAlON ceramic tool could obtain better surface
roughness. The effects of cutting parameters on the
surfaceroughness,cuttingtemperature,cuttingforce,and
microhardnesswereanalyzedindetailbasedontheuseof
SiAlON ceramic tools. Finally, to gain a real-time
perceptionofthecuttingforceandcuttingtemperature,a
detailed calculation formula for the cutting force and
cutting temperature was established based on SiAlON
ceramictools,anditsaccuracywasverified.
2.1HSDMoftitaniumalloy
The cutting parameters have a significant impact on the
entire machining process. Krishnaraj et al. [104]
conducted an HSDM experiment on Ti–6Al–4V (TC4).
Basedon theTaguchiexperimentaldesign, theeffectsof
vc, vf (feed speed), and αp (axial cutting depth) on the
cutting force, temperature, and surface roughness were
analyzed.Theexperimental resultsshowthatfz(feedper
tooth) and αp have the greatest impact on the cutting
force, whereas vc has a significant influence on the
cutting temperature and surface roughness. Within the
selected range of these cutting parameters, when vc, vf,
and αp were 150 m/min, 0.075 mm/r, and 0.75 mm,
respectively (for cutting titanium alloy, the high-speed
cuttingrangewasreachedwhenvcwas100m/min[103]),
the cutting effect was the best, and the machining
efficiencywasthehighest[104].However, the influence
of cutting parameters on the tool life and tool wear has
notbeenstudied.
Basedontheaboveresearch,GintingandNouari[105]
studiedtheprocesscapabilityof the HSDM of Ti-6242S
with ordinary uncoated cemented carbide tools. The
impact of vc and fz on tool wear was investigated. By
observingFig.3(a) [105], theauthor found that when vc
and fz were 150 m/min and 0.1 mm/z, respectively, the
tool could work for 22.4 min. When fz increased to
0.15 mm/z, the tool life decreased by a factor of two,
indicating that fz had a great influence on the tool life.
Irrespectiveofwhether fzwas0.1or0.15mm/z, the tool
wearincreasedwith increasingvc,whichsuggeststhat vc
wasanotherimportantfactoraffectingtoollife.Thetool
wearandchipmorphologywereanalyzedusingthefinite
elementmethod(FEM)andscanningelectronmicroscopy
(SEM). It was observed that the tool-wear mechanism
would be transformed from abrasive wear to adhesive
wear if the value of vc increased. The chip gradually
obtained a large serrated curvature when fz was
0.15 mm/z and vc ranged from 60–150 m/min, also
indicating that the radius of the chip curvature was
directly affected by the vc value [105]. Based on the
above studies, the optimal machining effect can be
Fig. 2Logicalstructureofhigh-speeddrymillingdifficult-to-machinemetalmaterials.CVD:chemicalvapordeposition,PVD:physical
vapordeposition,HSDM:high-speeddrymilling.
6Front.Mech.Eng.2023,18(2):28
obtained by appropriately adjusting the process parame-
ters. The influence of changing the parameters on tool
wearwasnotobvious.Therefore,itisnecessarytofurther
explore the influence of other methods (such as tool
coating)ontoolwear.
The influence of cutting force and temperature on the
surface quality of TC4 during the HSDM process at
differentvc values was systematically investigated by Li
et al. [106]. They used CVD-coated tools (Ti(C, N)-
Al2O3)forHSDMofTC4.Theresultsshowed that with
the increase in vc and fz, tool wear aggravated, and tool
life decreased sharply. The reason for the tool injury
would transform from cutting load into thermal damage
with increasing vc value. With the development of the
Fig. 3Influenceofcuttingparametersontoolwear,cutting forceandtemperature:(a)effectofvcandfzontoolwear[105],(b)cutting
forceunderdifferentvc [106], and (c) cutting temperature underdifferentvc[106].Reproducedwithpermissions from Refs. [105,106]
fromElsevierandSpringerNature.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 7
machining process, it was found that the cutting force
(Fig.3(b) [106]) and temperature (Fig.3(c) [106]) were
the main factors affecting the tool wear [106].
Furthermore, the authors found that the average cutting
force decreased significantly with increasing vc, and the
reason for the observed reduction was attributed to the
thermalsofteningoftheworkpiececausedbytheincrease
in cutting temperature. Based on the SEM results, the
surfacemicrostructureandgrainorientationchangedwith
differentfeeddirections,asshowninFig.4(a)[107].The
authorsalsoobservedchipmorphologyduringtheHSDM
processing of TC4 and found that chip morphology
corresponded to different vc values. At the same SEM
doublingrate,thenumberoflamellaealsochanged.With
anincrease in vc, the number of lamellae decreased,but
the lamellar structure became clearer, as shown in
Fig.4(b) [108]. By observing the serrated chip
morphology in Fig.4(c) [108], it was found that the
degreeofserrationincreasedwithincreasingvc,whichis
more conducive to chip breaking [108]. Although these
Fig. 4Influence of cutting parameters on microstructure and chip morphology: (a) workpiece microstructure and deformation zone
underdifferentvc[107],(b)effectofvconchipmorphology[108],and(c)majorsection ofchips atdifferent vc[108]. Reproducedwith
permissionsfromRefs.[107,108]fromTransTechPublicationsLtd.andSpringerNature.
8Front.Mech.Eng.2023,18(2):28
findingsindicatethatCVD-coatedtoolscouldshowgreat
cuttingeffectswithsuitablevcvalues,theauthorsdidnot
studythemillingofTC4withPVD-coatedtools.
Evenwhenusingcoatedtools,thecuttingparametersof
HSDMshouldbereasonablyselected.Safarietal.[109]
tested the surface roughness and microhardness of a
workpiecesurfaceunderdifferentcuttingconditionswith
aPVD-coatedtool(TiAlN/TiN)whenvcrangedfrom100
to 300 m/min and fz from 0.03 to 0.06 mm/z. As vc
increasedfrom100to300m/min,thesurfaceroughness
decreased by 55%. The surface roughness decreased by
40%atavcvalueof100m/minasfzincreasedfrom0.03
to 0.06 mm/z. Tool wear and work-hardening problems
were also observed when vc and fz increased simultane-
ously[109]. Furthermore, the researchers used the same
PVD tool for the HSDM processing of TC4-ELI. The
resultsshowedthatthemachinedsurfaceimprovedas vc
increasedfrom200to300m/min.Whenfzwassmall,the
cuttingforceintheHSDMprocesswaslowerthanthatin
the CM process. Compared to the uncoated tool, the
PVD-coatedtooldidnotsignificantlyimprovethesurface
roughness because of the adverse effect of the large vc
value[110].Theresultsindicatedthat,evenifthecoated
tool was selected, it was difficult to improve the
machining effect if the selection of cutting parameters
wasnotsuitable.
The above studies did not compare the cutting effects
of CVD-coated and PVD-coated tools under the same
conditions. Niu et al. [111] used PVD coating
(TiN/TiAlN) and CVD coating (TiN/Al2O3/TiCN) as
tools for HSDM processing of TC6 titanium alloy.
Relevant research on the HSDM of TC6 regarding the
cuttingforceandsurfaceroughnesswassummarized,and
the difference between the PVD and CVD tool coating
performance was demonstrated from the aspects of the
tool wear evolution and failure mechanism. The milling
forceandsurfaceroughnessofTC6were high when the
vcvaluewashigherthan80m/min.Thisindicatedthatthe
two coated tools were not suitable for the HSDM
processing of the TC6 titanium alloy. However, it is
apparent that the tool wear resistance of PVD-coated
tools is much better than that of CVD-coated tools
becausethe thermalconductivityofAl2O3decreasedand
that of TiAlN increased with increasing cutting
temperature [111]. Considering the influence of tool
coating on HSDM processing, Liu et al. [112] assumed
that the regressive development of tool coating was the
main factor restricting the promotion and application of
HSDM in the industry. Based on this, they reported the
influence of AlTiN-coated tools and TiAlSiN-coated
tools on HSDM processing of TC4. The XRD (X-ray
diffraction) diffraction patterns of the two differently
coated tools, shown in Fig.5(a) [112], were compared.
ComparedtotheAlTiNtool,thetoollifeoftheTiAlSiN-
Fig. 5XRD, flank wear and tool wear images of AlTiN- and TiAlSiN-coated tools: (a) XRD diffraction patterns, (b) flank wear of
cuttinglengthunderdifferent vc,and(c)toolflankwearimages underdifferent cuttinglengths[112].Reproducedwithpermissionfrom
Ref.[112]fromSpringerNature.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 9
coatedtoolincreasedby32%and66%atvcvaluesof150
and200m/min,respectively,asshowninFig.5(b)[112].
The tool-wear image in Fig.5(c) [112] reveals that the
TiAlSiNcoatingcansignificantlyprolongthetoollifeof
the cutting edge. Furthermore, the TiAlSiN-coated tool
exhibits better oxidation resistance and more uniform
chips[112].
2.2HSDMofhigh-strengthsteel
The wear resistance of the workpieces determines their
service performance. Huang et al. [114] focused on the
influence of HSDM of AISI D2 (when milling high-
strengthsteel,thehigh-speedcuttingrangeisreachedata
vcof 300m/min[113])onthesurfaceintegrityandwear
resistance. After the HSDM, the wear resistance of the
machined surface was evaluated through friction and
wear tests without lubrication. The results showed that
the surface morphology, microhardness, and yield
strengthoftheworkpieceexhibitedanisotropiccharacter-
istics after friction and wear experiments. Because of
anisotropy,the wear resistance of the workpiece surface
mainlydependsontheslidingdirection.Furthermore,the
surfaceoftheworkpiecehardens.Duringtheinitialphase
ofwear(thefirst10min),thesurfacewearofHSDMwas
62%lessthanthatofCMmilling[114].
The surface quality indices include the surface
roughness, hardness, and residual stress. Zheng et al.
[115] used a CVD-coated tool (Al2O3 + TiC) for the
HSDM of AISI 4340 steel. The relationships between
cutting parameters, cutting force, and surface roughness
were discovered, and the effects of tool wear on the
cuttingforceandsurface roughness were studied. Itwas
found that the cutting force was most influenced by αp,
whereas fz had the greatest effect on the surface
roughness.Basedontheempiricalmodel,optimalcutting
parametersforsmallcuttingforceand surface roughness
were obtained when αp ranged from 0.2 to 0.4 mm, fz
rangedfrom0.03 to 0.06mm/z,vcwasselectedbetween
350–450m/min,andαerangedfrom3to4mm.Basedon
theSEMresults,thewearrateofthecoatedtoolwaslow.
By observing the effects of friction and wear, it was
found that the increase in the cutting force and surface
roughnesswassmallintheinitialandstablewearstages.
However, when the wear value exceeded 0.25 mm, the
increaseincuttingforcesuddenlyincreasedsignificantly.
The experimental results also indicated that the wear of
coated tools was mainly caused by adhesion, oxidation,
anddiffusion,accompaniedbyasmallamountofspalling
and chipping [115]. In addition, the authors studied the
influence of tool coating (TiAlN + TiN, AlTiN, and
TiN/TiCN/TiAlN) and cutting parameters on the cutting
force and surface roughness. Among these three coated
tools, the TiN/TiCN/TiAlN-coated tools were the most
suitableforthe HSDM processing ofAISI 4340. Owing
to the resultant force, the flank wear width and surface
roughness values were minimal. As the optimal cutting
parameters,valuesforαpof0.4mm, fzof0.02mm/z,αe
of2mm,andvcintherangefrom280–440m/min were
obtained [116]. In addition to the above investigations,
researchersused aTiCN-NbCcompositecoatingtoolfor
HSDM of AISI 4340 steel and found that when the
cutting parameters were within HSDM conditions, the
surfaceroughness valuechanged from0.25 to0.45 µm,
and the surface roughness was minimal at a vc of 350
m/min.Furthermore, applying the TiCN-NbC composite
coatingtoolresultedinworkhardeningof theworkpiece
surface.Theresultsshowedthatthehardnessvalueafter
processingwas1.1–1.2timesthatofthe workpiecebody
material,andthehardeninglayerdepthwas60to80µm,
as shown in Fig.6(a) [117]. The residual stresses in the
cuttingdirectionrangedfrom‒490to‒320MPa,whereas
the residual stresses in the feed direction ranged from
−600 to ‒370 MPa, as shown in Fig.6(b) [117].
Furthermore, higher fz, vc, and αe and smaller αp values
canprovidea workpiece withhigh residual compressive
stress[117].
2.3HSDMofnickel-basedalloy
Thecuttingparameterscansignificantlyaffectthecutting
force and generate tool wear. Li et al. [118] conducted
HSDM experiments on Inconel 718 workpieces with an
(Al, Ti)N-coated milling cutter (for nickel-based alloy
cutting,thehigh-speedcuttingrangewasreachedatavcof
100 m/min) [119]. The change in cutting forces was
investigatedasαp,vc,and fzvaluesincreasedfrom0.5to
2 mm, from 140 to 240 m/min, and from 0.1 to 0.18
mm/z, respectively. According to the results, the radial,
tangential,andaxialforcesincreasedwithanincreasein
fz. With increasing vc, the axial force fluctuated
significantlyandthendecreased,butthechangeinvchad
little effect on radial and tangential forces. With the
increaseinαp,irrespectiveofthechangesinfzandvc,the
values of the radial, tangential, and axial forces always
increased [118]. The above investigations demonstrate
that only an increase in vc can appropriately reduce the
cuttingforce.However,theeffectsofcuttingparameters
ontoolwear havenotbeenstudied.Thetool wearunder
differentvcisshown in Fig.7 [120,121]. Kamdanietal.
[120] used PVD-coated tools (TiN/TiAlN) to study the
influenceof vcandαe(radialcutwidth)on thetoolwear
of Inconel 718 processed by HSDM and observed that
whenvcwasintherangeof80–120m/min,thetoolwear
increasedwithanincreaseinαeandreacheditsmaximum
whenvc increased to 120 m/min. According to Fig.7(a)
[120],tool wear wasmore severe with an increasein vc
andαe.
As the above studies did not simultaneously consider
both the cutting force and tool wear mechanism in the
HSDM processing of nickel-based alloys, Zhang et al.
[122]appliedPCBNtools to the HSDM ofGH4169and
10 Front.Mech.Eng.2023,18(2):28
observed the influence of vc, fz, and αp on cutting force
and tool wear. The cutting force increased with an
increaseinαp,whereasitdecreasedwithanincreaseinvc.
Furthermore,withanincreaseinvcandfzoradecreasein
αp, flank wear gradually decreased. When vc, fz, and αp
were1065m/min, 0.12 mm/z,and0.5mm,respectively,
the corresponding cutting parameters were optimal. The
tool-wear values of the rake and flank surfaces became
moreuniformwhen vc was1065m/min.BecauseTi,Al,
and O elements were concentrated on the bond layer at
Fig. 6Microhardnessandresidualstressunderdifferentcuttingparameters:(a)microhardnessofdepthfromthemachinedsurfaceunder
different cutting parameters and (b) variation of machining surface residual stress with cutting parameters [117]. Reproduced with
permissionfromRef.[117]fromElsevier.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 11
thecuttingedge,themainwearmechanismwasadhesive
wear[122].
The above studies demonstrated the influence of
milling parameters on the cutting force and tool wear
during HSDM. However, the influence of the cutting
parameterson thesurface roughnessof coatedtools has
not been studied. Therefore, Qiao et al. [123] used a
PVD-coated (TiAlN/TiN) tool to conduct HSDM of
nickel-basedFGH97alloy.Thesurfaceroughnessof the
workpiece surface was explored within the specified
limitswhenαpchangedfrom0.1to0.3mm,vcfrom30to
210 m/min, and fz from 0.08 to 0.12 mm/z. The results
showed that the surface roughness increased with an
increasein αp and fz, but with increasing vc, the surface
roughness first increased and then decreased. The
minimumsurfaceroughnesswasobtainedforvcvaluesin
therangeof170–190m/min[123].
The cutting parameters not only affect the surface
roughness but also influence the tool wear and cutting
temperature. In addition to the cutting parameters, the
coating type also affects the surface roughness.
Molaiekiyaetal.[124]studiedthecuttingperformanceof
aSiAlON ceramictoolinthe HSDMofInconel718 and
measuredthetoollife,toolwear,andcuttingforceduring
machining. When the same volume of material was
removed, tool wear first decreased and then increased
withanincrease invc.Whenvcremainedin therangeof
900–1100m/min,the tool lifewasthelongest,asshown
in Fig.7(b) [121]. The change rule of the tool surface
temperature gradient was also explored using the FEM
under different vc conditions. During HSDM, a large
amount of cutting heat was generated on the contact
surface of the tool and chip, and the temperature was
mainly concentrated in the narrow strip of the second
deformation zone, as shown in Fig.8(a) [121]. This is
becauseoftheextremelylowthermalconductivityofthe
SiAlONceramictoolandtheshortcuttingtimewithinthe
setrangeofvc.Furthermore,whenvcwas900m/min,the
thermal softening effect was prominent, leading to a
relatively low cutting force. Based on the experimental
dataforthecuttingforce,cuttingheat,andtoolwear,the
optimal vc value was 900 m/min. By analyzing the tool
Fig. 7Toolwearunderdifferentvc:(a)toolwearunderdifferentmachiningconditions[120]and(b)experimentaftercutting21.75cm3
andflankwearoffiniteelementmethod[121].ReproducedwithpermissionsfromRefs.[120,121]fromMalaysianTribologySocietyand
SpringerNature.
12 Front.Mech.Eng.2023,18(2):28
wear under different cutting parameters of FEM, it was
found that at the same tool wear rate, compared with
ordinary cemented carbide tools, the SiAlON ceramic
toolcouldimprovethematerialremovalratefour tofive
times, as shown in Fig.8(b) [121]. In addition, the
authors used a SiAlON ceramic tool and a PVD-coated
(WC-Co)tool forHSDMprocessing.Comparedwiththe
PVD-coated tool, the SiAlON ceramic tool exhibited a
better surface roughness, as shown in Fig.9 [124].
However,theceramictoolformedaveryhardwhitelayer
withdepthsrangingfrom1to2µmonthesurfaceofthe
workpiece during HSDM. After corrosion, it remained
whiteunderametallographicmicroscope.Themaximum
residualtensilestressinHSDMprocessedwiththePVD-
Fig. 8Cuttingtemperatureandtoolwearunderdifferent cutting conditions: (a) temperature distribution under different vc conditions
and(b)toolwearwithdifferentcuttingvolumes[121].ReproducedwithpermissionfromRef.[121]fromSpringerNature.
Fig. 9Surfaceroughness corresponding todifferentcoated tools: (a)SiAlONtool and (b)physicalvapor deposition tool[124].PVD:
physicalvapordeposition.ReproducedwithpermissionfromRef.[124]fromSpringerNature.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 13
coatedtoolwas2.5times higher than that obtainedwith
CMpouringcutting,which was caused by rapidcooling
at high temperatures. Therefore, CMQL technology is
necessarytoreducethethermaldamagecausedbytoolor
workpiecesurfacesduringHSDMprocessing[124].
AlthoughMolaiekiyaetal.[124]systematicallystudied
the HSDM process of SiAlON ceramic tools, the
hardnessofthehardwhitelayerand cutting forces were
not explored under HSDM and CM conditions. To
determinethechangeinhardness,Şirinetal.[125]used
HSDM and SiAlON ceramic tools to process nickel-
based X-750 alloys. The surface roughness, cutting
temperature, cutting force, and microhardness of the
workpiece were measured in the vc range of 500–
700m/min,andthevfrangeof0.025–0.075mm/r.Itwas
found that the surface roughness increased with
increasing vc and vf. Under all cutting conditions, the
surfaceroughnesscorrespondingtoHSDMwasrelatively
large. The cutting force and temperature were 565.7 N
and 450 °C, respectively. The tool wear was small
because the tool coating provided anti-wear properties
during processing. Compared with CM pouring cutting,
HSDM can increase the hardness of the workpiece by
16.94%[125].
The above studies systematically revealed the cutting
effectoftheHSDMofnickel-basedalloyswithSiAlON
ceramic tools, but a formula for the cutting force and
cutting temperature in the cutting process has not been
established. Thus, Zha et al. [126] investigated the
HSDM process of Inconel 718 with a SiAlON ceramic
toolbasedon FEM andderivedformulas for thecutting
force and cutting temperature. Subsequently, an HSDM
experiment was performed using the specific cutting
temperaturetoverifythecuttingforceformula.Whenαp,
αe, fz, and vc reached 0.3 mm, 6 mm, 0.03 mm/z, and
527.52 m/min, respectively, the cutting force began to
decrease,indicatingthatthecuttingtemperatureexceeded
the softening temperature of Inconel 718. The experi-
ments showed that when vc was higher than 527.52
m/min, the HSDM process for Inconel 718 was easier.
The accuracy of the formula for the cutting force and
temperature was verified based on experimental results
[126].
2.4SummaryofHSDMofdifficult-to-machinemetal
materials
Based on the above investigations, the cutting speed
ranges of difficult-to-machine metal materials are
different in the HSDM process owing to the different
properties of these materials. The suitable cutting speed
range is 100–300 m/min for titanium alloy, 300–
450m/min for high-strength steel,and 500–1100 m/min
for nickel-based alloys. Titanium alloys are commonly
usedfor aircraft fuselages, while nickel-based alloys are
primarilyused for aircraftengines. However, the engine
servicelife is typically shorter thanthat of the fuselage.
Toincrease thecuttingspeedofnickel-basedalloys,itis
necessary to introduce high-performance SiAlON cera-
mic tools. In terms of the entire aircraft, the content of
titanium alloy is much higher in structural parts than in
high-strength steel landing gears. This means that
increasing the cutting speed of titanium alloy has a
greaterimpactthanincreasingthecuttingspeedofhigh-
strength steel. Based on Fig.10 and the above research
results, the cutting force and surface roughness in the
HSDMprocessaredifficultto reduce with uncoated and
ordinarycoatedtools(TiN/TiAlN,TiN/Al2O3/TiCN,and
AlTiN), and the tool wear is also severe. High-perfor-
mance tools (SiAlON ceramic tools) and composite-
coated tools (TiN/TiCN/TiAlN, TiCN-NbC) can reduce
thecuttingforce,temperature,andsurfaceroughnessand
minimize tool wear during the machining process.
However,comparedwith CM pouringcutting,the depth
of the surface-hardening layer and the residual stress of
HSDMmachiningarehigher,whichlimitstheapplication
and promotion of the HSDM machining process.
ConsideringthatthedeficiencyofHSDMprocessingcan
be eliminated by LAM, UVAM, and CMQL technolo-
gies, which have been sufficiently researched, the
subsequent work of HSDM mainly focuses on energy
field-assistedmillingtechnology.
3LAM of difficult-to-machine metal
materials
LAM is a new auxiliary processing mode for the local
softeningofworkpieces using a laserheatsource before
processing.BecauseLAMtechnology can reduceenergy
consumptionbyreducing thecuttingforce,itisa typical
greenandlow-carbon processing technology [127].This
principleisshowninFig.11(a)[128].Theincidentangle
of the laser beam (feeding simultaneously with the
milling cutter) is set to ensure that the heat source
radiated into the shear zone of the workpiece surface.
Subsequently,the optimal laserparameters (PL, dL, etc.)
and milling parameters (vc, αp, etc.) are combined to
reduce the strength and hardness of difficult-to-cut
materials.Therefore, LAM can reduce the cutting force,
prolongthe tool life, improve thematerial removal rate,
reduce the cutting energy consumption, reduce the
manufacturing cost, and optimize the workpiece surface
quality [128]. The LAM of difficult-to-machine metal
materials is divided into three classes according to the
LAM preheating temperature range, and the logical
structureisshowninFig.11(b).
For studies on LAM of high-strength steel, first, the
laserparametersandcuttingparameterswerechanged to
reduce the cutting force and improve tool rigidity.
Second,the influenceofthelaser preheatingtemperature
on the cutting force and specific cutting energy was
14 Front.Mech.Eng.2023,18(2):28
studied.Third,itwasverifiedthatLAMcouldreducethe
cuttingforcewiththehelpofFEM.CombiningtheFEM
methodandexperiments,theresearchersfoundthatLAM
couldreducethecuttingforceandsurfaceroughnessand
that the most influential parameter on the surface
roughness was the cutting speed. A comparison of the
tool wear under high and low feed conditions revealed
that LAM can significantly improve material removal
under high feed conditions. Subsequently, after the
optimization of the laser and cutting parameters, it was
verified based on slot milling experiments that LAM
couldgreatlyreducesurfaceroughnessandtoolwear.To
reducetheexperimentalworkload,aphysical-basedLAM
cuttingforcemodelisproposed,andtheaccuracyofthe
modelisverified. Furthermore, toattainanoptimallaser
preheatingeffect,atwo-stageLAMprocesswasproposed
to match the laser softening depth with the cutting
manufacturing depth. Finally, to effectively control the
range of the heat-affected zone (HAZ), the influence of
the laser preheating parameters on the HAZ size was
exploredindetail.
To study the LAM of titanium alloys, the preheating
temperature was first set to 618 °C to explore the
influence of cutting parameters on the cutting force and
microstructure of the planar workpiece. Second, the
optimal laser power for surface machining was
determinedby combining FEM with the tool inclination
angle, and its accuracy was experimentally verified.
Third, a laser-assisted fillet milling strategy was
developed, and it was found that the cutting force,
specificenergy,and surface roughness couldbereduced
ata preheating temperature of 600 °C. Furthermore, the
surface LAM strategy of the tool inclination and fillet
was integrated to reduce the cutting force and cutting
specific energy. Subsequently, the cost of single-piece
manufacturingunderLAM conditionscanbereducedby
adjusting the laser parameters to obtain a preheating
temperature of 500 °C. Finally, the laser and milling
parameters were adjusted simultaneously to reduce the
annualproductioncostsoftheenterprise.
When investigating the LAM of nickel-based alloys,
thepreheating temperature wasfirst set to800 °C using
external laser-assisted equipment, and the effects of
increasingtheLAMplaneoftheworkpieceonthecutting
force, surface roughness, and tool wear were compared.
Second, the influence of the laser power parameters on
the tool wear in plane milling was studied. Third, the
influenceofsimultaneouschangesinthelaserandcutting
parametersonthecuttingforce and surface roughness in
plane milling was explored. It was found that adjusting
onlythelaserandcuttingparametersledtoanincreasein
thesurfaceroughness.Subsequently,anewlaser-assisted
reciprocatingpreheatingprocesswasproposed,andLAM
backandforth(B&F)preheatingwasfoundtoreducethe
surfaceroughnessvalueduringplanemilling.Subsequen-
tly,contour LAM and slope LAM were proposed based
on the results of the parameter optimization and a new
process of plane milling. When comparing the cutting
Fig. 10Summaryofhigh-speeddrymillingmachinability.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 15
force,surfaceroughness, andspecificcuttingenergy,the
contourLAM had better effectsthan the slopeLAM. In
addition,theactual temperatureoftheworkpiecesurface
significantlyinfluencestheLAM manufacturing process.
The constant laser energy used in the experiment could
notprovide a stable preheating temperature. A tempera-
ture feedback control method is proposed to establish a
tool life prediction model, and its accuracy is verified.
Finally,itwasestablishedthattheheatingareawaslarger
thantheheatsourcesizeunderactualworkingconditions,
and a new space- and time-controlled laser-heating
method was proposed. The chip morphologies and
microstructuresobtained by LAM, CM, and single laser
scanning (LS) were compared in detail. Based on the
hollow tool-holder fiber system, the effect of LAM on
reducingthecuttingforceandtoolwear was verified by
changingthelaserparameters.
3.1LAMofhigh-strengthsteel
The laser parameters (PL, laser position) and cutting
parameters(vc,αp,andαe)significantlyaffectthecutting
forceand dimensional accuracy of the workpiece. Singh
andMelkote[129]conductedLAMexperimentsonH-13
steel using an ytterbium fiber laser (wavelength of
1064 nm) and a preheating temperature of 890 °C. The
results showed that under the given cutting conditions,
the laser parameters had a significant influence on the
machining process. By properly controlling the PL, dL,
andlaser position,thestrengthof theworkpiecematerial
would be reduced, which can minimize the risk of tool
failure,reduce thecuttingforce,andimprovetherigidity
ofthetool.By observing the LAM hardnessdata,itwas
found that there was a measurable HAZ on the laser-
heatedsurfaces.TheHAZareadecreasedwithincreasing
VL[129].Inaddition,itwasobservedthatαpandPLhad
a significant influence on the cutting force during the
LAMprocessandthatthesurfaceroughnesswasaffected
byPL[130].ConsideringthatPLcouldaffecttheheating
temperature, Jeon and Pfefferkorn [131] used a 200-W
(continuous wave) Nd:YAG laser (wavelength of
1064nm)forLAMprocessingexperimentson1018steel
withvariable laserheatingtemperatures.When thelaser-
assisted temperature increased from 27 to 867 °C, the
Fig. 11Laser-assistedmilling(LAM)principleandlogic:(a)LAMschematicdiagram[128]and(b)logicalstructureofLAMdifficult-
to-machine metal materials. FEM: finite element method; B&F: back and forth. Reproduced with permission from Ref. [128] from
SpringerNature.
16 Front.Mech.Eng.2023,18(2):28
averagefeedandcuttingforceswerereducedby56%and
32%,respectively.Thespecificcuttingenergydecreased
by32%[131].BecauseFEMcanreducetheexperimental
cost and support the analysis of the temperature field
distribution in the machining process, Özel and
Pfefferkorn[132]conductedLAMresearchonAISI4340
steelbasedonFEMandexperiments.AnNd:YAGlaser
(wavelengthof1064nm)wasusedintheheatingprocess.
The FEM results were analyzed using DEFORM-2D
software.Athigh vf, the cutting forceofLAM (400 °C)
wassmallerthanthatofCM[132].Caoetal.[133]found
thebestLAM process conditions for13-8stainless steel
using a 1-kW HPDL laser (wavelength range of 940–
980nm)toobtainasurfacetemperatureof550°C.First,
the temperature field distribution of the laser-beam-
preheatedworkpiece was determined based on the FEM
method. Subsequently, the Taguchi experimental design
was applied by changing vc, vf, and αp. Finally, the
optimal process parameters of LAM were established
using variance analyses. Compared with the CM, the
cutting force and surface roughness of the LAM were
reducedby20.1%and34.4%,respectively.Theresultsof
variance analyses showed that under the appropriate
LAM conditions, the cutting force was affected by αp,
whereas vc had the greatest influence on the surface
roughness[133].
Theabovestudies showed that,inadditiontothelaser
parameters, cutting parameters also have a significant
influenceontheLAMprocess. Bermingham et al. [134]
used a 2.2-kW HPDL laser (wavelength range of
940–980nm)andapreheatingtemperatureof300°Cand
conducted comparative processing experiments with or
without LAM of high-feed milling (H.F) or low-feed
milling(L.F).Basedontheaboveexperimentalvariables
in Fig.12(a) [134], they established the relationship
betweenthematerialremovalvolume and tool wear and
observed no difference in tool wear between LAM and
CM at 100 m/min H.F. However, under L.F conditions,
the tool wear of LAM and CM was quite different. For
thesametool wear,vfwas117and150 m/minforLAM
andCM, respectively,andthematerialremovalbyLAM
wasmorethandoublethatofCM.However,whenvfwas
78m/min,theremovalrateofLAMwasonly50%higher
than that of CM. Based on the mechanism of adhesive
wear and abrasive wear, it was proven that LAM
technology could effectively prolong tool life. In
addition,compared to CM, LAM canreduce the cutting
forceby33%[134].
Afteroptimizingthecuttingparameters,itis necessary
to design a variety of experiments (such as groove
milling) to reduce surface roughness and tool wear.
Meikote et al. [135] used an ytterbium fiber laser
(wavelengthof1060nm)toconductlaser-assistedgroove
millingexperiments onA2toolsteel. Theymeasuredthe
dimensional accuracy, surface roughness, and tool wear
oftheequipment.Theauthorsfoundthatthedimensional
precisionoftheworkpiecegrooveoftheLAMwascloser
tothedrawingsettingprecisionthan that of the CM. As
shown in Fig.12(b) [135], the surface roughness of the
LAM (7.5 W) was smaller than that of the CM at
different cutting lengths, and the tool wear rate of the
LAMwaslower[135].
The cutting-force prediction model can reduce the
workload of cutting experiments and accurately deter-
minethecutting force intheLAMprocess.Kumaretal.
[136] proposed a physical-based cutting force model to
predict the cutting force during the LAM process, as
shown in Fig.13(a) [136]. The contents of the model
included the thermal model of laser heating, thermal
modeloftemperature rise causedby plastic deformation
(shear) in the process of chip formation, material
strength-relatedshearanglemodel,materialflowstrength
model,millingmodel,andtooljumpmodel.Basedonthe
newmodel,thecuttingforceduringLAMprocessingwas
Fig. 12Cutting forces and grain deformation distribution: (a) tool wear under different cutting conditions [134] and (b) surface
roughnessatdifferentvc [135]. CM: conventional milling; LAM: laser-assisted milling; H.F: high-feed milling; L.F: low-feed milling.
ReproducedwithpermissionsfromRefs.[134,135]fromElsevier.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 17
predictedand verified. The PLand VL parameters ofthe
52100 bearing steel were changed using an ytterbium
fiber laser (wavelength of 1060 nm). The experimental
resultsshowedthatthecuttingforceofLAM(18W)was
smallerthan that of CM.Both the materialremoval rate
andtoollifeofLAMwerehigher[136].
The HAZ on the machined surface affects the dimen-
sionalaccuracyandserviceperformanceoftheworkpiece
afterheatingusingthelasersystem. Kadivar et al. [137]
proposedatwo-stageLAMprocesstosolvetheproblems
in which a continuous wave or short-pulse laser may
producean HAZ that may be retained on the surface of
thefinishedproduct,andtheuseofcoolantwouldleadto
a decrease in laser heating efficiency. The first stage is
basedonanultrashortpulselasertosoftentheshearzone
on the workpiece surface. In the second stage, a micro-
milling cutter is used to change the softened surface
constructed in the first stage to the final size. The
advantage of using an ultrashort pulse laser was that it
achieved control of the HAZ range in real time. The
workpiececouldbe machined to acertain softening size
bycontrollingthelaserparameters.Theworkpieceisthen
processed under different cutting conditions. Therefore,
theprocessing parameters were independent of the laser
parameters. However, the two-stage coordination can
match the laser softening depth with the cutting
manufacturing depth. The LAM of X5CrNi18-10 steel
was conducted using a Yb:YAG picosecond laser. The
laser heat parameters included PL and the distance
betweenthe laser spotand tool. Thecutting transforma-
tionparameters were vc, fz, and αe. Itwas observed that
the cutting force is affected by vc. Compared with CM,
LAMsignificantlyreducedtheaxialandtangentialforces
by70%and 50%, respectively.Regardingchip morpho-
logy,theLAMchipwassmallandthin,asshowninFig.
13(b)[137], whichalsoledtoasmallermilling forcefor
LAM. In addition, appropriate laser parameters are
essentialforachievingefficientLAMmachining.Setting
PLto10Wreducedthemachiningtemperatureby50%.
Therefore,foroptimalLAMperformanceparameters,the
laser power should be set to 10 W, and the distance
betweenthespotandthetoolshouldbe250µm[137].
Controlling the HAZ is crucial for machining
processes.Zeng etal.[138]foundthatLAMmayinduce
aworkpiecetoproduceaharmfulHAZ. Accordingly,an
HAZanalysismodelwasestablished to predict the HAZ
generated by laser heating in the LAM of AerMet100
steel.A 1-kW HPDL laser(wavelength of 915nm) was
used to verify the proposed analysis model by
transforming PL and vf. According to Fig.14 [138], the
HAZ size increased significantly with an increase in PL
(from200to 1000 W)anddecreasedwithanincreasein
vf. The temperature change in the HAZ ranged from
138.8 to 574.7 °C. The HAZ width increased with dL,
while the HAZ depth decreased because of the inverse
correlation of the dL energy concentration. Therefore,
Fig. 13Force prediction and cutting morphology: (a) laser-assisted milling (LAM) force prediction methodology [136] and
(b)comparisonofchipmorphology[137].CM:conventionalmilling.ReproducedwithpermissionsfromRefs.[136,137]fromASMEand
Elsevier.
18 Front.Mech.Eng.2023,18(2):28
consideringthat the side millingae value wassmall and
theapvaluewaslarge,itwasrecommendedtousealaser
witha smaller dL value, whereas the opposite applies to
face milling, for which a laser with a larger dL value
should be utilized. Compared with the other laser
parameters, the influence of the laser incident angle on
theHAZwas small.Furthermore,asshowninFig.14(a)
[138], the HAZ could be caused by a critical PL value
becausethePLvaluewaslessthan the critical PL value.
The absorption temperature of the workpiece did not
reach the austenite transformation temperature of the
material[138].
3.2LAMoftitaniumalloy
LAM can aid in optimizing the cutting force and
improvingthemicrostructure of planarworkpieces.Kim
and Lee [139] used a 1-kW HPDL laser (wavelength
rangeof 940–980nm)andsetthesurfacetemperatureof
theLAMworkpieceto618°C(laserpower of 80 W) to
perform comparative cutting experiments on TC4
workpieces with and without LAM processing. The
purposeofthisstudywastoassesstheinfluenceofvc,fz,
andαponcuttingforce,toolwear,andsurfaceroughness.
TheresultsshowedthatthecuttingforceoftheLAMwas
reduced by 13%–46% compared with that of the CM.
Adhesion of cracks and chips was not observed on the
tool wear surface under the SEM conditions. In all
experiments, the surface roughness and microstructure
wereimproved,asshowninFig.15[139].
In actual machining processes, titanium alloy parts
mostly possess curved surfaces, such as compressor
blades and casings of aeroengines. The optimal laser
powerfor machining curvedsurfaces can be determined
based on the tool-inclination angle. Sim and Lee [140]
workedonthe preheating andmachiningoptimizationof
thetool-pathinclinationangleintheLAMprocess.First,
FEMwasappliedforthethermalanalysisofTC4.Based
onthis, the optimalPL was determined according to the
tool-path angle. TC4 milling experiments were then
conductedusing a 1-kW HPDL laser (wavelength range
of808‒980nm,laserpowerof80W).Accordingto the
results, the preheating temperature decreased with
increasing tool-path inclination, as shown in Fig.16(a)
[140].However,whenthetoolinclinationangleexceeded
75°, the preheating temperature began to increase. The
accuracy of the simulation process was verified by the
experimentalresults. The experiments also revealed that
thecutting force in the LAM process decreasedwith an
increaseinthetool-pathinclinationangle[140].
Consideringthereductioninthestressconcentrationof
fillets, the fillet can improve the service life of the
workpiece, and the fillet strategy is widely utilized in
actualtoolpathdesign.Therefore,itisnecessarytocreate
Fig. 14Effectof differentlaserparameters onheat-affectedzone:(a) PL,(b)dL, (c)vf,and (d)laserincident angle[138].HAZ: heat-
affectedzone.ReproducedwithpermissionfromRef.[138]fromSpringerNature.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 19
a detailed LAM strategy for the tool path of the fillets.
WooandLee[141]proposedalaserenergyfield-assisted
fillet milling strategy to solve the problem in which the
laserbeamcouldnotcontinuouslyirradiatethetopofthe
workpiecewhenlaserenergyfield-assistedcornermilling
wasconductedusinganadditionalaxislasermodule.The
laser-assistedfilletmillingpathandprocessingconditions
based on the linear difference are shown in Fig.16(b)
[141].The specific implementation scheme included the
following: First, the milling origin (0, 0), the expected
filletradius(R),thenumberofcoordinatepoints,andthe
tool radius angle (αi) were determined to calculate the
coordinate tool point (Pci). The calculation formula for
thetoolcoordinatepointcanbeexpressedas
x=r×cos(180 + α)+r,r=rc+R,(1)
y=r×sin(180 + α)+r,(2)
where r represents the radius of the cutting tool, and rc
representsthesumoftheradiusofthecuttingtool.
Second, the distance (xcl) between the tool center and
the laser heat source center as well as the heat source
radius were determined, and the distance (xi) between
theinitialcoordinatepoint(Pli)oftheheatsourceandthe
end coordinate point (PLi) of the laser heat source was
calculated. Finally, the calculated tool coordinates and
laserheatsourcecoordinatesweretransformedintoGand
Mcodesandwereinputintothemachinetool.
After the fillet LAM strategy was completed, the
effectivecuttingdepth wasobtainedbythermalanalysis,
asshownin Fig.17 [142]. Theresponse surface method
was used to design the experiments. Finally, the
experiment was conducted using a 1-kW HPDL laser
with wavelengths ranging from 940 to 980 nm and a
preheating temperature of 600 °C. A cutting-force
predictionmodelwasestablishedbasedontheregression
analysis. Optimal manufacturing conditions for milling
TC4 are provided. The results showed that, compared
with CM, the feed force, axial force, cutting ratio, and
surface roughness of LAM were reduced by 23.7%,
20.6%,24.2%,and47%,respectively[141,142].
The LAM of curved surfaces under real operating
conditions can be determined by combining the tool-
inclinationangle with the fillet LAM strategy. Oh et al.
[143] combined a curved surface milling method with
LAMtechnologyusing a1-kWHPDLlaser(wavelength
rangeof940–980nm)anddeterminedthatthepreheating
temperature for milling TC4 material was 980 °C. The
cuttingforceand specific energyofconventionalsurface
milling and curved-surface LAM technology under
differentprocessingconditionswere assessed. Compared
with conventional surface milling, the cutting force and
Fig. 15Conventionalmillingand laser-assisted milling (LAM) machinedsurface:(a)surfaceroughness and (b) microstructure [139].
CM:conventionalmilling.ReproducedwithpermissionfromRef.[139]fromMDPI.
20 Front.Mech.Eng.2023,18(2):28
specificcuttingenergyofcurvedsurfaceLAMdecreased
by33%andby28%to41%,respectively[143].
According to Taylor’s tool-life equation, the single-
piece manufacturing cost of LAM can be quickly
obtained.Hedberg et al. [144] conducted LAM research
onTC4usinga1-kWIPGPhotonicsytterbiumfiberlaser
(wavelength of 1071 nm). Based on the heat transfer
mechanismofTC4,a temperature distributionprediction
model for LAM was established. The appropriate laser
parameters were optimized using the prediction model.
The surface quality, unit cost, and annual cost are
presented in Fig.18 [144,145]. To ensure the surface
Fig. 16Rotationangleandroundangleoflaser-assistedmilling:(a)temperaturedistributionofrotationangle[140]and(b)round-angle
laser-assistedmillingpath[141].ReproducedwithpermissionfromRefs.[140,141]fromSpringerNature.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 21
integrity and service performance of the workpiece
manufactured by LAM, the cutting force, tool wear,
microstructure(Fig.18(a)[144]),XRDstructure,surface
hardness,residualstress (Fig.18(b)[144]),andeconomy
of LAM technology were determined. According to
Taylor’stoollifeequationobtainedfromtheresultsofthe
hypothesis and experimental tests, the total costs of a
singlepiece manufactured by CM and LAM technology
underdifferentvcvalueswerecalculated,andtheresults
are shown in Fig.18(c) [144]. Compared to CM, the
cutting force, residual stress, and manufacturing cost of
LAM (preheating temperature of 500 °C) were reduced
by20%, 10%, and33%, respectively. Inaddition, LAM
extendedthetool life by64%andimprovedthematerial
removalrateby35%[144,146].
After optimizing the LAM parameters, the annual
production cost of the enterprise can be significantly
reduced.Wiedenmannet al. [147]applied LAM techno-
logytoconductexperimentsonTC4titaniumalloys.The
experiment was set up based on the central composite
design (CCD) method using a 4-kW Nd:YAG laser
(wavelength of 1064 nm) as an experimental auxiliary
tool and PL, dL, xL, αp, αe, and fz as the parameter
variables. After studying the influence of simultaneous
changesinthelaserandmillingparametersonthecutting
force, the authors found that among the selected
parameters, PL had the greatest influence on the cutting
forceinalldirections,withanoveralldecreasingtrendin
the cutting force with increasing PL. The determined
theoretical optimal value of dL was 2.65 mm [147].
Furthermore,comparedwithCM,LAMtechnologycould
reduce the cutting force, improve the material removal
rateby33%,andprolongthetool life by 19% when the
preheating temperature was 800 °C [145]. As shown in
Fig.18(d) [145], taking the milling of titanium turbine
bladesas an example, the highest economic potential of
LAM is the production of 1200 parts per year, which
couldsaveup to 10.5%ofthe manufacturing costofall
products.
3.3LAMofnickel-basedalloys
Externallaserauxiliary equipment iswidely used owing
to its convenient installation. Kong et al. [148] used an
Nd:YAGlaser(wavelengthof1064nm)andapreheating
temperature of 800 °C to conduct LAM of a planar
workpiece made of K24 nickel-based alloy. The effec-
tiveness of the LAM was explored by measuring the
cutting force, surface roughness, and tool wear at
different material removal temperatures, which could
reducethe surfaceroughnessandcutting force.Fromthe
experimental results, they discovered that the cutting
force was reduced by 30%–70%, and the life of the
coated tools was extended by 46%. By comparing
different coated tools, the authors found that the main
wearmechanismsof the toolsin the LAM processwere
adhesivewearandabrasivewear,asshownin Fig.19(a)
[148]. The TiAlN-coated tools had the highest wear
resistance at a cutting speed of 30 m/min, whereas the
TiCNcoatinghad the poorest performance.Notchescan
beobservedafterprocessingforacertaintime,asshown
inFig.19(b)[148]. Becausethetooldamagewas caused
by the high temperature in the machining process, Tian
et al. [149] proposed a transient three-dimensional
thermalmodelforLAMtoaccuratelyobtainthetempera-
turedistribution. Theaccuracyofthe modelwasverified
by measuring the surface temperature using an infrared
thermalimagerandthermocouple. The LAMexperiment
on a planar workpiece made of Inconel 718 was
conducted using a 4-kW HPDL laser (wavelength of
808 nm). Tool wear was observed by SEM, indicating
that with increasing PL, abrasive wear became more
uniform. Excessive PL leads to an increase in the tool
wear, as shown in Fig.19(c) [149]. Therefore, the
following experimental conclusion was obtained. The
verification model could provide the transient tempera-
ture distribution of the workpiece when its geometrical
shape changed during the machining process. After
adjusting PL, the laser temperature was set to 520 °C.
Under this condition, compared with CM, LAM can
Fig. 17Thermalanalysisoflaser-assistedmilling[142].ReproducedwithpermissionfromRef.[142]fromSpringerNature.
22 Front.Mech.Eng.2023,18(2):28
Fig. 18Surfacequality,unitcostandannualcost:(a)microstructure,(b)residualstress,(c)costoftheunitunderdifferentvc[144],and
(d) annual costs of produced parts [145]. CM: conventional milling; LAM: laser-assisted milling. Reproduced with permissions from
Refs.[144,145]fromSpringerNatureandElsevier.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 23
reduce the cutting force, number of chips, and surface
roughness by 40% to 50%, 50%, and 50%, respectively
[149].
A systematic understanding of the comprehensive
mechanism of the processing technology and choice of
laserparametersiscrucialforadetailedunderstandingof
theLAMprocess.KinandLee[150]performedanLAM
experiment on a planar workpiece made of Inconel 718
witha1-kWHPDLlaser(wavelength range of 940–980
nm).First, material properties (thermal conductivity and
specific heat) were obtained. The appropriate PL and
rangeofthepredictedtemperatureweredeterminedbased
Fig. 19Flank face wear at different milling conditions: (a) scanning electron microscope of coated tool at 10s with laser-assisted
milling, (b) scanning electron microscope of coated tool at 16.6 min with laser-assisted milling [148], and (c) scanning electron
microscope of the coated tool at 20 mm with laser-assisted milling under different PL [149]. Reproduced with permissions from
Refs.[148,149]fromSpringerNatureandASME.
24 Front.Mech.Eng.2023,18(2):28
on the FEM. Subsequently, LAM experiments were
conducted with different PL and αp. According to the
results, the cutting force decreased with increasing PL
irrespective of the change in αp. Compared to CM, the
cutting force of LAM decreased by 55% when the
preheating temperature was set to 900 °C (180 W), but
thesurfaceroughnessincreasedby70%[150].Second,to
eliminatethe observed negative effect ofthe increase in
surfaceroughness,anewtechnology,B&F,wasproposed
with a preheating temperature of 900 °C. In the experi-
ments, different workpiece inclination angles were
applied. The results showed that the cutting force
decreased with increasing workpiece inclination. The
levelsoftooldamageandsurfacequalitywereimproved,
as shown in Fig.20 [151]. Finally, the cutting force of
LAM (B&F) was smaller than that of LAM and CM.
Compared with CM, the surface roughness of LAM
(B&F) and LAM decreased by 34.2% and 56.8%,
respectively [151]. Based on the parameter optimization
for planar LAM and the new technology, the LAM
experiments on contour and slope non-uniform rational
B-spline(NURBS)three-dimensionalsurfacesoutperfor-
med at a set preheating temperature of 940 °C. The
cuttingforcesofcontourLAMandslopeLAMdecreased
by39.6%and 33.7%, respectively,comparedwith those
of CM. The surface roughness and cutting ratio were
reduced by 38.59% and 49.91%, respectively. It was
demonstrated that contour LAM was better than slope
LAM[152].
Thetemperatureofthe workpiece surface significantly
influences the LAM process. Wu et al. [153,154] found
that the laser preheating temperature was the most
important parameter affecting the laser heating effect.
However, a constant laser energy could not provide a
stablepreheatingtemperatureduring the cutting process.
The temperature feedback and cutting temperature are
shown in Fig.21 [153,154]. A temperature feedback
controlmethodfortheLAMprocesswasproposedbased
on the results shown in Fig.21(a) [153]. The authors
established a composite simulation model including a
preheating temperature model, temperature feedback
model, temperature difference prediction model, and
cuttingprocessmodel. Furthermore,thecuttingtempera-
turefieldandcuttingprocessweresimulatedtodetermine
differences in temperature. Subsequently, the laser-
heatingtemperaturecan be controlledbymonitoringand
adjusting. The simulation and experimental results
showed that PL was the main factor affecting the
difference between the preheating, shear zone, and
monitoring temperatures, as shown in Figs.21(b) [154]
and21(c)[154].TheLAMofInconel718wasperformed
using a 1-kW HPDL laser (wavelength of 808 nm).
Compared with CM, the main cutting forces correspon-
dingtopreheatingtemperaturesof400and700°Cwere
reducedby23%and45%,respectively[154].Comparing
the tool life of the CVD-coated tools and PVD-coated
tools, it was found that the CVD coating was more
suitable for the LAM process. The error of the tool life
prediction model was less than 15% according to the
experimental results, which verified the accuracy of the
model[153].
An optimized process can effectively heat a region
whoseareaiswiderthandLandensuretheuniformityof
thetemperaturedistributionintheheating region. Shang
et al. [155] proposed a new spatially and temporally
controlled (S&T) laser heating method, which was
characterized by laser points with oscillations along
specific trajectories and the generation of HAZs. In
contrast to the oscillating heating method proposed by
Bermingham et al. [134], the S&T method not only
provides information about the configuration of laser
heating(suchasPL, VL, and thelaserscanningpath)but
also shows the heating effect. In their study, the
correctnessofthelaserconfigurationwas mainly proven
Fig. 20Theinfluenceofworkpieceinclinationanglesoncuttingforceandtooldamage:(a)workpieceinclinationandcuttingforceand
(b)workpieceinclinationandtooldamage[151]. CM: conventional milling; LAM: laser-assisted milling. Reproduced with permission
fromRef.[151]fromSpringerNature.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 25
by forward and inverse heat conduction. Forward heat
conductioncandeterminethetemperaturedistributionin
the workpiece with a given laser beam configuration.
Reverse heat conduction was used to determine the
optimal laser system parameters. The LAM of Inconel
718 was conducted using a 10-kW HPDL laser at a
preheatingtemperatureof800°C.Theaveragevalueand
peak of the cutting force in the LAM process were
calculatedbasedonthemeasuredcutting force shown in
Fig.22(a)[155].Thepeakandaveragevaluesofthemain
cutting force were reduced by 55% and 47.8%,
respectively, after the proposed S&T controlled laser
heatingmethodwas applied. Thepeak and average feed
forces decreased by 26.3% and 26.1%, respectively,
whichreduced the cutting power by 35.4%. In addition,
comparedwith dry milling, LAM with the laser heating
methodcontrolledbyS&Treducedthesurfaceroughness
by14%[155]. Theauthorsalsoconducteda comprehen-
sivestudyontheresidualstressesandmicrostructureofa
workpieceprocessedbyLAMtechnology(laserpowerin
therangeof 1300–1500 W)andfurther studied thechip
morphologyandmicrostructureformation.Bycomparing
LAM,CM,and LS,ameltinglayerwasobserved onthe
freesurfaceofthechipsgeneratedbyLAMbycomparing
LAM, CM, and single laser scanning. The bending
phenomenon of the LS workpiece was also compared.
Thisbending effectwas noteliminated afterremoval of
the softening layer by the LAM process. These results
indicate that LAM technology is more suitable for the
machining of cylindrical parts. In addition, to further
understand the plastic strain during processing, it is
necessary to measure the intragranular local misorienta-
tion (LMO) in the chip crystal, namely, the dislocation
accumulated in the crystal during grain deformation, as
showninFig.22(b)[156].Amongtheimages,aslipband
composed of several slip planes is present in the LAM
chip. However, the CM image showed a more obvious
directional dislocation, and the LS image showed no
obvious dislocation. The results indicated that LAM
combines the advantages of reducing the cutting force
andimprovingthematerialremovalrates[156].
Built-inlaserauxiliary equipment isdifficulttoinstall,
anditslarge-scaleimplementationhashighcosts.Brecher
etal.[157]developeda2.3-kW(wavelengthof1070nm)
fiberlasersystemmovedbyanHohl ShaftKegel(HSK)
hollow shank based on Fraunhofer Institute for Produc-
tion Technology (Fraunhofer IPT), which preheated the
surface of the shear zone of an Inconel 718 workpiece
before machining to 800 °C. During the experiment, it
was necessary to change PL and measure the cutting
force. Compared with the CM, the cutting force, axial
force,feedforce,andtoolwearoftheLAMwerereduced
by60%, 60%,40%,and57.14%, respectively.Finally,it
was observed that the tool wear was the smallest when
thePLvaluewas1.54kW[157].
3.4SummaryofLAMofdifficult-to-machinemetal
materials
Based on the above investigations, the preheating
temperature ranges during LAM of difficult-to-machine
metalmaterialsaredifferentbecauseoftheirinconsistent
basic properties. The tensile strength of high-strength
steeldecreaseswhenthepreheatingtemperatureexceeds
400 °C. Because material oxidation can easily occur at
temperaturesabove600°C,thepreheatingtemperatureof
high-strength steel for effective processing ranges from
400 to 550 °C [132,133,138]. The tensile strength of
Fig. 21Temperaturefeedback andcuttingtemperature:(a)effect ofPLon cuttingtemperature,(b)effectof VLoncuttingtemperature
[154], and (c) schematic diagram of the temperature feedback system [153]. Reproduced with permission from Refs. [153,154] from
SpringerNature.
26 Front.Mech.Eng.2023,18(2):28
titanium alloys is significantly reduced at temperatures
above 600 °C, and the preheating temperature range of
titaniumalloys isbetween 500and 620°C foreffective
processing [139,141,142]. The yield strength of nickel-
based alloys decreases sharply when the temperature
exceeds650°C,andthepreheatingtemperatureofnickel-
basedalloysfor effective processing rangesfrom650 to
950°C[148,150,151].Compared with CM, althoughthe
preheating temperature range of difficult-to-machine
metalmaterialsforeffectiveprocessingisdifferent,LAM
of high-strength steel, titanium alloy, and nickel-based
alloyhasadvantages,suchasasmall cutting force, high
materialremovalrate,longtoollife, low specific cutting
energy,lowmanufacturingcost,smallchipsize,andhigh
surface quality, as shown in Fig.23. However, the
superiorityofLAMforvariousdifficult-to-machinemetal
materialshas been verified experimentally.The research
mainly focuses on the influence of the laser parameters
Fig. 22Cuttingforces and graindeformationdistribution: (a) cuttingforcesof path-optimized laser-assistedmilling(LAM) [155] and
(b) grain deformation distribution in different machining processes [156]. CM: conventional milling; LS: single laser scanning.
ReproducedwithpermissionsfromRefs.[155,156]fromElsevier.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 27
(PL,VL, dL, laser incident angle, and laserposition) and
cutting parameters (vc, vf, αp, and αe) on the effect of
machining processes and the results of the experiments.
However, some research aspects of LAM machining
processes, including real-time temperature control and
HAZ, are still worth studying. LAM processing
technologies include laser-assisted cavity milling, spiral
milling, and cycloid milling. Real-time temperature
control is critical in LAM, and it involves various
algorithms,suchasfuzzy control, proportional−integral−
Fig. 23Summaryoflaser-assistedmillingmachinability.HAZ:heat-affectedzone.
28 Front.Mech.Eng.2023,18(2):28
derivative (PID) control, and generalized predictive
control. To avoid producing HAZ during LAM,
researchers use finite element transient thermal analysis
and consider emissivity and absorptivity in the HAZ
modeltodeterminethelaserparameters.Furtherresearch
in LAM should focus on the theory and mechanism of
material removal and chip breaking using FEM and
temperature field control technology. It is essential to
monitorthetemperatureandphasetransitionoftheshear
zoneunderdifferentprocessingconditionstounderstand
the variation law of LAM of difficult-to-machine metal
materials. A real-time sensing model of temperature
change and microstructure transformation in the shear
zone can help optimize the process parameters. To
prevent HAZ from remaining on the workpiece surface,
LAM processes should be optimized using FEM chip
breaking simulation models and HAZ range. This
optimization includes laser scanning path, laser incident
angle, and temperature control times. Moreover, by
consideringtheeffectsoflaserandcuttingparameterson
various factors like cutting force, material removal rate,
toollife,cuttingspecificenergy,manufacturingcost,chip
morphology, and surface quality, prediction models can
bedevelopedusing various intelligentalgorithms.These
models can help promote the industrialization and
applicationofLAMtechnology.
4Ultrasonic energy field-assisted milling
of difficult-to-machine metal materials
UVAM is a typical intermittent cutting process that can
periodically open a cutting area [158]. By applying a
micron-level ultrasonic frequency vibration to the
workpiece or tool, f, and controlling the vibration
direction,A,thehigh-frequencyperiodicseparationofthe
workpieceandtoolinthecuttingprocessisrealized,and
the milling vibration is effectively reduced, thereby
improvingthemachinabilityofdifficult-to-machinemetal
materials. The basic principle and device of UVAM are
shown in Fig.24(a) [159,160]. Compared with CM,
UVAM can reduce the cutting force and temperature,
prolong the tool life, and optimize the quality of the
workpiece surface. Periodic separation of the workpiece
and tool produces a cutting process with variable
thickness,whichplaysaneffectiveroleinchip breaking
[161,162]. The UVAM of difficult-to-machine metal
materials can be divided into three classes according to
the applied vibration amplitude ranges; the logical
structureisshowninFig.24(b).
Forstudieson UVAMofnickel-basedalloys,first,the
one-dimensional axial workpiece vibration method was
used to analyze the influence of cutting parameters on
cuttingforce, tool wear, and surface roughness. Second,
the one-dimensional feed workpiece vibration method
was used to analyze the influence of cutting parameter
changes on the surface roughness and the suppression
effectofAvaluesonburrs.Finally,theeffectsofUVAM
onthe microstructure, hardness, fatigue life, and surface
roughnessoftheworkpiecewereanalyzedusingtheone-
dimensionalaxialtoolvibrationmethod.
RegardingtheresearchonUVAMoftitaniumalloycut
by a one-dimensional tool with axial longitudinal
vibration, first, the influence of cutting parameters on
cuttingforceandsurfaceroughnesswasanalyzed,andthe
effect of UVAM on surface roughness was compared.
Second, the influence of A value on the cutting force,
cuttingtemperature,and surface roughnesswasassessed
by increasing the vibration amplitude. Third, the
influence of cutting parameters on the cutting force,
cutting temperature, residual stress, and surface rough-
ness was analyzed based on one-dimensional tool axial
longitudinal vibration. Working at the longitudinal
vibrationofa one-dimensional workpiecefeed, first, the
influence of A values on the surface scale structure and
the surface roughness of the workpieces was analyzed
based on the formation mechanism of the surface
microstructureandthetheoreticalmodeloftheformation
process of the surface microstructure. Second, by
combining the FEM with the tool tip trajectory, the
influence of A values on the cutting force and surface
roughness was assessed. Based on research on two-
dimensionalultrasonicvibration,acuttingedgegeometry
model of a ball-end milling cutter considering two-
dimensionallongitudinaltorsionaltoolvibrationandaxial
position angle was established to analyze the change in
the UVAM cutting force and build a model of cutting
forceunderdifferentflankwear.Second,theinfluenceof
the A value on the cutting force, tool wear, and surface
roughnesswas analyzed. Becausethe tool changein the
ultrasonic vibration machining process would lead to
burrsinthe connection areaduringtheactualproduction
process, a non-tool change machining method based on
UVAM of a flat surface and a free curved surface
connectionareawasdevelopedtoreducethecuttingforce
andsurfaceroughness.
For studies on UVAM of high-strength steel,
considering one-dimensional tool axial longitudinal
vibration,theeffectsofUVAMonthecuttingforce,chip
morphology,andsurfacequalitywerecompared.Second,
theinfluencesoff,A,andthetoolangleontoolwearand
surfaceroughnesswereanalyzed.Third,theinfluenceoff
onthesurface roughnessandresidualstresswas studied.
To identify how one-dimensional workpiece axial
vibration and one-dimensional workpiece feed vibration
influencethemachiningprocess,theinfluenceofUVAM
cuttingparametersonsurfaceroughnesswasfirststudied.
Second, a UVAM cutting force model was established,
and a new method for determining the relationship
between the critical cutting speed and undeformed chip
thickness was proposed. Third, the effects of cutting
parameters and milling methods on the cutting force,
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 29
surfaceroughness,and chip morphologywereinvestiga-
ted. Finally, based on the helical milling (HM) process,
theeffectsofUVAMoncuttingforce,machiningenergy
consumption, and surface roughness were compared.
Basedontwo-dimensionalplanevibration,theeffectsoff
andAon the toolwear,surfaceroughness,instantaneous
cutting thickness, and material removal rate were
analyzed.
4.1Ultrasonicenergyfield-assistedmillingofnickel-based
alloy
The one-dimensional axial vibration method (workpiece
vibration) can reduce milling temperature and tool wear
andimprovesurfacequality.Hsuetal.[163]conducteda
UVAMexperimentona nickel-based MAR-M247alloy.
Using Taguchi’s experimental design, they studied the
effects of different tool materials, workpiece tempera-
tures, cutting parameters, and f on the machining
characteristics.TheresultsindicatedthatUVAMreduced
themilling temperature. Minimizing αp can improve the
surfacequalityandreducetheprocessingtemperatureand
flankwear[163].
By applying one-dimensional feed longitudinal vibra-
tion (workpiece vibration), the influence of cutting
parametersonthesurfaceroughnesswasstudied,andthe
burrsuppressioneffectbychangingAwasexplored.Fang
et al. [164] used an ultrasonic energy field with f =
32 kHz and A = 3 µm for milling Inconel 718. The
influenceoffz(2–6µm/z)onthesurfacequalityandburr
ofthe workpiece under CM and UVAM conditions was
studied. The authors found that UVAM effectively
improved the surface quality. The number of surface
defectsdecreasedsignificantlywithincreasingfz.Whenfz
exceeded5µm/z,theinfluenceofUVAMonthesurface
qualitywassmall,as shown in Fig.25(a) [164], whereas
the CM of the workpiece resulted in a poor surface
quality within the given range of parameters. It is well
knownthat surfacequalitycangenerallybedescribedby
surface roughness, as shown in Fig.25(b) [164]. As
shown in Fig.25(b) [164], the surface roughness values
after UVAM were smaller than those after CM
Fig. 24Ultrasonicvibration-assistedmilling (UVAM) principle and logic: (a) UVAM principle and device [159,160] and (b)logical
structure of laser-assisted milling difficult-to-machine metal materials. CM: conventional milling. Reproduced with permissions from
Refs.[159,160]fromElsevier.
30 Front.Mech.Eng.2023,18(2):28
Fig. 25Changesinsurfacemorphology,burrsizeandsurfaceroughnessunderdifferentfz:(a)bottomsurfacemorphologyand(b)burr
widthandsurfaceroughness[164].UVAM:ultrasonicvibration-assistedmilling;CM:conventionalmilling.Reproducedwithpermission
fromRef.[164]fromSpringerNature.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 31
processing. Furthermore, the surface roughness of the
UVAM-processedworkpiece decreased with an increase
infzbut increased slightly whenfzwas6µm/z[164].At
the same f value, the team also studied the changes in
Inconel718burrsatdifferentvc,fz,andA, ranging from
18.84 to 75.36 m/min, 2 to 8 µm/z, and 0 to 9 µm,
respectively.TheyobservedthatwhentheratioofAtofz
wasgreaterthan0.5,thechipbreaking effect of UVAM
changedtheshapeofthechips.CombiningtheFEMand
experimentalresults,itwasestablishedthatUVAMcould
effectively reduce the size of chips and burrs. With
increasing A, the inhibitory impact of UVAM on burrs
significantly increased, as shown in Fig.25(b) [164].
Underconditionsofsmallvc,highfz,andhighAvalues,
UVAMhadthegreatestinhibitoryeffectonburrs[165].
One-dimensional axial longitudinal vibration (tool
vibration)isanauxiliarycuttingmethodthatcanprovide
good machining surface quality. Suárez et al. [166,167]
conductedUVAMofNialloy718,settingfto39.61kHz
and A to 1.5 µm. They focused on the influence of
UVAMonsurfaceintegrity,fatigueresistance,toolwear,
and cutting force. Compared to CM, UVAM reduced
cuttingforce,improvedsurfacemicrostructure(Fig.26(a)
[166]),and increasedsurfacehardnessand fatiguelifeof
the workpiece by 3.79% and 14.74%, respectively.
However,toolwearonthebacksurfaceincreasedby10%
[166]. After further study, the authors found that the
roughness of the workpiece surface treated by UVAM
decreasedby75%comparedtothatofCM,asshownin
Fig.26(b)[167].
4.2Ultrasonicenergyfield-assistedmillingoftitanium
alloy
Variations in cutting parameters and amplitude (A) can
impactthecuttingforce,cuttingtemperature,andsurface
roughness of materials processed by UVAM with one-
dimensional axial longitudinal vibration (tool vibration).
SuandLi[168]investigatedthecuttingperformanceand
mechanismofTC4titaniumalloyinacuttingexperiment
with f and A values of 30 kHz and 6 µm, respectively.
Compared to CM, an increase in fz and αp reduced the
correspondingcuttingforceofUVAMby0.8%–42%and
5.3%–65%, respectively. The surface roughness also
decreasedby10.82%to37.97%.[168].Basedonthis,the
team also compared the surface roughness of selective
laser melting (SLM) and conventional melting (CL) of
TC4 with and without UVAM processing. Compared
with CM, UVAM reduced the surface roughness values
ofthe(SLM)TC4and(CL)TC4workpiecematerialsby
23.3% and 19.1%, respectively. Furthermore, it was
observed that UVAM could effectively improve the
surfacemorphologyof (SLM)TC4and(CL)TC4 [169],
but the influence of UVAM on cutting temperature has
notbeenstudied. Gao etal.[170]studiedtheeffectof A
(from 0 to 6 µm) on the cutting force, cutting tempera-
ture,andsurfaceroughnessofTC4workpiecematerialat
an f value of 30 kHz, as shown in Fig.27(a) [170]. In
Fig.27(b)[170],theyobservedthatboththecuttingforce
andcutting temperature decreasedwith increasing A but
onlyslightlywithincreasingcuttingtemperature.WhenA
Fig. 26Microstructure and surface roughness of conventional milling (CM) and ultrasonic vibration-assisted milling (UVAM):
(a) microstructure of processed surface [166] and (b) three-dimensional surface roughness [167]. Reproduced with permissions from
Refs.[166,167]fromSpringerNatureandElsevier.
32 Front.Mech.Eng.2023,18(2):28
increased from 0 to 6 µm, the surface roughness Sa
(average roughness) and Sq (surface root mean square
roughness)decreasedby35.1%and34.0%, respectively,
and the surface morphology became more uniform,
provingthatthe cutting performanceand surface quality
ofTC4couldbesignificantlyimprovedbyUVAM[170].
The change in cutting parameters can also affect the
formation mechanism of the residual stress and surface
microstructure.Xieetal.[171]systematicallystudiedthe
UVAMofTC18andTC4cells.First,basedonthe one-
dimensional axial longitudinal vibration (tool vibration)
whenfwassetto33.9kHz,theeffectsofAandvconthe
machining performance of the TC18 titanium alloy
specimenswerestudied.The observation andanalysisof
these effects included the use of a dynamometer,
thermometer, scanning electron microscope, X-ray
diffractometer,andthree-dimensionalsurfacetopography
instrument. The authors found that vc had significant
effects on cutting force, surface morphology, cutting
temperature,and residualstress.ComparedwithCM,the
cutting force and cutting temperature of UVAM-
processed workpieces decreased by 34.1% and 19.5%,
respectively, whereas the residual stresses and surface
roughnessincreasedby50.9%and163.88%,respectively.
Furthermore, the UVAM-processed workpiece surface
exhibited a plastic deformation zone at a certain depth,
and the deformation zone increased with increasing A
[171]. Second, the basic formation mechanism of the
surfacemicrostructureduringUVAMwasanalyzedusing
atheoreticalkinematicmodel established by theauthors,
as shown in Fig.28(a) [172]. According to Fig.28(b)
[172], a regular-scale microstructure was generated by
UVAMalongthefeeddirection.Inaddition,vc,fz,andA
would affect the machining surface morphology and
accuracyoftheworkpiecesize.Thesingle-factorUVAM
experimenton TC4 titanium alloy with one-dimensional
feed longitudinal vibration was performed at f of
22.7kHzandvarious A values (0, 1, 2,3,and5 µm) to
verify the accuracy of the theoretical model. The team
also found that with an increase in A, the surface-scale
Fig. 27Testparameterflowanddatacomparison:(a)ultrasonicvibration-assisted millingoveralltestparameterflowand(b)Aimpact
onmeasurementdata[170].ReproducedwithpermissionfromRef.[170]fromElsevier.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 33
structure gradually became uniform. The surface
roughness value first decreased and then increased with
increasingA.Frictionandwearexperimentsrevealedthat
the friction coefficient of the UVAM-processed work-
piecesurfacewas60%lowerthanthatobtainedafterCM
[172].
The change in cutting parameters can also affect the
dimensionalaccuracyoftheworkpieceandtiptrajectory.
Xu et al. [173] used the UVAM of TC4 with one-
dimensional feed longitudinal vibration (workpiece
vibration)whenf was setto19.832 kHz. Theyexplored
the influence of UVAM on the cutting force, surface
quality,andworkpiece size accuracyfor different A and
vf.ComparedtoCM,UVAMreducedthecuttingforceby
17%. Therefore, the tool life is extended, and the
dimensional accuracy of the workpiece is improved.
Furthermore, according to the SEM observations of the
surface morphology, UVAM can effectively reduce
surface defects and machining tool marks. Thus, the
surfacequality isoptimizedafterUVAM [173].Thetool
tiptrajectoryalsoaffectedthemachiningeffect.Zhuetal.
[174] worked on the application of UVAM in the
machining process of a workpiece. The vibration
direction was along the feed direction, and the entire
system was fixed to the workbench by the flange. To
achieve an excellent vibration effect of the TC4
workpiece on the transducer, the resonant block was
optimizedusingFEM,asshowninFig.29(a)[174].
Consideringitsdirecteffectonthetextureandsurface
morphology of the workpiece, the tool path must be
analyzed. The UVAM tool path is composed of tool
rotation, table feed motion, and micron-scale ultrasonic
vibration along the feed direction. In the Cartesian
coordinatesystemoftheworkpiece,thetooltiptrajectory
equationis
x=xr+xf+xv,
y=yr,
z=0.
(3)
Because the ultrasonic generator can only output
ultrasonic sine or sine signals, the ultrasonic vibration
displacementfunctioncanbeexpressedas
xv=Asin ( f t +θ).(4)
Based on Eqs. (3) and (4), the tool path equation for
UVAMisobtainedas
{x=Rcosβ+vft+Asin ( ft +θ),
y=Rsinβ, (5)
β
ωr
vf
Nz
zi
Nz
β=ωrt2π(zi1)/Nz
xr=Rcos ωrt
yr=Rsin ωrt
xf=vft
wherex,y,andz representthetipdisplacements,fandA
aretheultrasonicfrequencyandamplitude,respectively,t
isthe cutting time, θis the initialphase of thevibration
signal, R is the radius of the end mill, is the tool
rotationangle, istheangularvelocityofthespindle,
represents the feed rate of the workpiece, is the
numberoftips,and isthecuttingedge number (i = 1,
2,…, ), , , ,
and .
Accordingto Eq. (5), the tiptrajectory in UVAM can
Fig. 28Theoreticalmodeland results:(a)theoreticalmodelofthemachinedsurfaceand(b)differentAvaluesofthemachinedsurface
[172].ReproducedwithpermissionfromRef.[172]fromJournalofVibroengineering.
34 Front.Mech.Eng.2023,18(2):28
be obtained, as shown in Fig.29(b) [174]. In Fig.29(b)
[174],thetrajectoryanddynamiccuttingthicknessofthe
UVAM tip are clearly more complex than those of the
CM process. In the local amplification diagram, the
characteristics of UVAM are a wave-shaped trajectory
andaphasedifference.Basedonthetoolpathanalysisof
UVAM, UVAM experiments with f = 19.8 kHz and A
ranging from 8 to 14 µm were performed. The results
showed that compared with CM, the milling force of
UVAM and the associated surface roughness were
reducedby30% to 34.4%and20%to45%,respectively
[174].
The mechanism of two-dimensional longitudinal-
torsional ultrasonic vibration is very complicated.
Therefore, a new technology for this vibration was
proposed. The design of the geometric model of the
cuttingedgeofthe ball-end milling cutterwiththe axial
positionangleasthe main parameterwaspresented.The
authors derived the cutting force model of a ball-end
milling cutter under the condition of longitudinal-
torsional composite vibration. When f was 35.476 kHz
and A was 10 µm, in the longitudinal-torsional UVAM
experimentonTC4 titanium alloy, theradial,tangential,
andaxialforcesofUVAMwerereducedby60%,27.7%,
and 33%, respectively, compared to CM [175].
Furthermore, under UVAM conditions, the relationship
between the tool flank and cutting force was not
established. Based on the above research, a new tool
flankwearmodelthatconsidersthechip flow angle and
discretization of the cutting edge was developed. This
modelcouldpredictthechangetrendofthecuttingforce
atdifferentflankwearvaluesandoptimizetheprocessing
parameters. The UVAM experiment on TC4 was
performed with an f value of 35 kHz, A values in the
range of 0–4 µm, and spiral angles between 35°–50°.
Accordingto the experimental results, when A was 2or
3µm, the tool wear became stable as the cutting length
increased.Figure30(a)[176] shows that the helixangle,
unit cutting-edge length, friction time, and cutting
temperatureincreased.Theinfluenceofthehelixangleon
toolflankwearchangedinasimilarmanner;thatis,when
the helix angle was 35°, the increase in the wear value
was more stable than at other helix angles, as shown in
Fig.30(b)[176]. Theerrorsbetweenthepredictedmodel
and experimental results in the feed (x) and normal (y)
directions of the coordinate tool system (o-xyz) were
19.1% and 12.9%, respectively. Compared to CM, the
feed and normal cutting forces of UVAM decreased by
21.7% and 5.4%, respectively. When the cutting length
exceeded 67.5 m, the tool wear value of UVAM
decreased by 38.7% [176]. The application of two-
dimensionallongitudinal torsional vibration can produce
Fig. 29Optimizationofresonantblockandanalysis of tool tip trajectory: (a) finite element method (FEM) structure optimization of
ultrasonicvibration-assistedmilling (UVAM) system andresonantblockand (b) tool-tip motiontrajectoryinUVAMand conventional
milling(CM)process[174].Unit:mm.ReproducedwithpermissionfromRef.[174]fromElsevier.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 35
bettermachining effects on the workpiece cutting force,
tool wear, and surface roughness. Rinck et al. [177]
studiedthecuttingforce,tool life, and surface qualityof
TC4 titanium alloy by changing A (4, 6, 8, 10, and 12
µm) based on two-dimensional longitudinal-torsional
vibration when f was 32 kHz. Compared with CM, the
cuttingforce,toolwear,andsurfaceroughnessofUVAM
were reduced by 57%, 20%, and 16.7%, respectively
[177].
The tool change in the machining process of straight
and free-curved surface cutting leads to burrs in the
connectionareaduringtheactualproductionprocess.Ren
et al. [178] proposed a machining method without tool
change based on UVAM for straight and free-curved
surfaceconnectionareas.Atf=25kHzandA=5.6µm,
the processing performance of UVAM and CM was
assessedbychangingparametersvc,vf,andαp.Compared
withCM,noobviousburrswereobservedattheinterface
between the planar and free-curved surfaces after using
UVAM, so there was no need to use a tilt spindle or
transform tool. In addition, the milling force of UVAM
decreased by 20%–40%, and the surface roughness
decreasedby 44.3%.AsshowninFig.31[178],whenvc
was less than 157 m/min, UVAM led to an increase in
surface roughness. However, when vc was greater than
157m/min,thesurfaceroughnessdecreased[178].
4.3Ultrasonicenergyfield-assistedmillingof
high-strengthsteel
One-dimensional axial longitudinal vibration of the
cuttingtoolcanaffectthecuttingforce,chipmorphology,
and surface quality. Ahmed et al. [179] established an
analysis model to calculate the cutting force during the
machiningprocess,and the results are shownin Fig.32.
An AISI H13 machining experiment was conducted at
f = 40 kHz and A = 2 µm. The machining process was
evaluatedbasedon cutting force,chipmorphology,wear
rate, and surface integrity. The results showed that
comparedwith CM, UVAM had a smaller cutting force
andcouldproducemoreuniform,thin,andsmoothchips.
The surface quality of the UVAM workpiece also
improved. By observing the friction and wear
experimentaldata,itwasfoundthatthetoolwearcaused
byCMor UVAM was similar. However,further studies
showedthatUVAMcouldprolongtool life by changing
thevibrationdirection[179].
Considering one-dimensional axial longitudinal
Fig. 30Principleand test results:(a)influence principleofdifferent helical angletoolson cuttingedgelengthand (b)effectof A and
helicalangleontoolwearvalueofdifferentcuttinglengths[176].ReproducedwithpermissionfromRef.[176]fromElsevier.
36 Front.Mech.Eng.2023,18(2):28
vibration(toolvibration),thevaluesoff, A, and the tool
angle can affect tool wear and surface roughness. Tsai
etal.[180]studiedtheeffectsoff(25and50kHz),A(0,
2.2,and3.68µm),toolrakeangles(6°and−6°),andtool
helix angles (25°, 35°, and 45°) on tool wear and
machined surface quality using AISI 420 processed by
UVAM.Theexperimentalresultsshowed that compared
withCM, the machined surfaceafter UVAM processing
was more uniform when f was 25 or 50 kHz. The
machining tool mark became shallow with increasing f.
WithincreasingA,theroughnessofthemachinedsurface
firstdecreasedandthenincreased.Thesurfaceroughness
afterUVAMwassmallest when the toolrakeangle was
6°. The surface quality was improved by increasing the
Fig. 31Three-dimensionalmorphologyofultrasonicvibration-assistedmilling(UVAM)andconventionalmilling(CM)machinedsurfaces:
(a) CM at vc = 125.6 m/min, (b) UVAM at vc = 125.6 m/min, (c) CM at vc = 157 m/min, and (d) UVAM at vc = 157 m/min [178].
ReproducedwithpermissionfromRef.[178]fromSpringerNature.
Fig. 32Ultrasonic vibration-assisted milling (UVAM) and conventional milling (CM) analysis model of cutting force [179].
ReproducedwithpermissionfromRef.[179]fromTaylor&Francis.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 37
UVAM helix angle, as shown in Fig.33(a) [180].
MaurottoandWickramarachchi[181]conductedUVAM
ofAISI316Lwhilevaryingthevalueoff(0,20,40,and
60kHz).Theyexploredtheinfluenceofdifferentfvalues
onthesurfaceroughnessandresidualstress.Accordingto
the results, the surface roughness increased slowly with
increasing f, and the surface quality worsened. In
addition, the residual stress was compressive when the
parametersremainedwithinagivenrange.Theminimum
compressivestress was obtainedwhen f was 40 kHz,as
showninFig.33(b)[181].
Scholars have already considered the simultaneous
influence of the axial vibration and feed vibration of
workpieces during the machining process. Razfar et al.
[182] studied the UVAM of high-strength steel. First, a
UVAM experiment was conducted on AISI 1020 steel
based on one-dimensional axial longitudinal vibration
(workpiecevibration) when f wasset to 20kHz and the
power was 250 W. Then, the effects of vc, fz, αp, and
ultrasonic treatment on the surface roughness were
investigated, and the results showed that the surface
roughness of CM and UVAM exhibited similar curves
andincreasedwithincreasingfzandvc.ComparedtoCM,
theaveragesurfaceroughnessafterUVAM increased by
12.9%[182].Second,basedonthesamevibrationmode,
apowerof220 W was usedtoconduct UVAM of AISI
304steel. Subsequently, the influence of UVAM on the
cuttingforceinthreedirectionswastested.Itwasfound
that under UVAM conditions, the cutting forces were
reducedin all three directions[183]. Finally, thecutting
forceinUVAMwas described inamathematicalmodel.
The authors proposed a new relationship between the
critical cutting speed and thickness of the undeformed
chips.Accordingtotheanalyticalrelationship,thecutting
force in the UVAM had different amplitudes. CM and
UVAM experiments based on longitudinal vibration
Fig. 33Ultrasonicvibration-assistedmilling(UVAM)andconventionalmilling(CM)surfacequality:(a)influenceoffandhelixangle
ontheprocessedsurface[180]and(b)effectoffzandfonsurfaceroughnessandresidualstress[181].Reproducedwithpermissionsfrom
Refs.[180,181]fromMDPIandElsevier.
38 Front.Mech.Eng.2023,18(2):28
(workpiecevibration)inaone-dimensionalfeeddirection
wereconductedatf=23kHzand A = 20 µm, and their
cutting force and workpiece surface roughness were
compared. UVAM of X20Cr13 stainless steel was first
performed,andtheeffectsofvc,vf,andmillingmethods
on chip formation and workpiece surface quality were
analyzed. The UVAM and CM chip morphologies and
tool wear are shown in Fig.34 [184,185]. The
experimental results showed that UVAM could produce
thinner and smaller chips, as shown in Fig.34(a) [184],
andthemachinedsurfacewassmoother.Comparedwith
CM, UVAM chips had larger curvatures and smaller
sizes.Withanincreaseinvf,thechipcurvaturedecreased
[184]. Furthermore, side milling of AISI 420 stainless
steel was performed. Subsequently, the effects of vc, vf,
and milling methods on the cutting force and surface
roughnesswere studied, indicating that the cutting force
in UVAM was smaller than that in CM. Moreover,
depending on the cutting conditions, the surface
roughnessof the workpiece in UVAM can be improved
Fig. 34Ultrasonic vibration-assisted milling (UVAM) and conventional milling (CM) chip morphology and tool wear: (a) chip
morphology under different vc [184] and (b) tool wear [185]. Reproduced with permissions from Refs. [184,185] from ASME and
Elsevier.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 39
compared with that obtained by CM. Further research
showedthatwhenvfwassmall,theinfluenceofUVAM
reverse milling on the cutting force was more obvious.
However, when vf was large, the influence of UVAM
forward milling was more pronounced. Under the
conditions of low vf, high vc, and the reverse milling
process, the effect of UVAM on the surface roughness
wasmoreevident[186].
Theone-dimensionalaxiallongitudinalvibration(work-
piecevibration)based on theHM process can affectthe
cuttingforce,machiningenergyconsumption,andsurface
roughness. Rao et al. [187] conducted UVAM of AISI
1020steelusinganfvalueof20 kHz and an A value of
5 µm. HM was used to improve the energy efficiency.
The energy consumption of the feed rate in three
directions, that is, the chip-size prediction model, was
theoreticallyestablished.Itwas found thatUVAMhada
significant intrinsic effect on chip morphology, cutting
force, and machining energy consumption. Compared
with the CM, the one-dimensional axial longitudinal
vibrationreducedtheaxialforce,radialforce,andcutting
energy consumption by 47%, 14%, and 34%, respec-
tively.Axiallongitudinalvibrationscanreducemanufac-
turingcosts.Theresultsof the prediction model werein
good agreement with the experimental results, with
average errors in cutting energy consumption, chip
length, and chip width of 4.36%, 2.51%, and 3.92%,
respectively [187]. This confirms the accuracy of the
model. Considering the difference between two-
dimensional plane vibration and one-dimensional axial
longitudinal vibration, Ding et al. [185] performed
UVAM of X46Cr13 stainless steel based on two-
dimensional plane vibration under different ultrasonic f
and A. Compared with CM, the surface roughness after
UVAM decreased by 28.3%. The tool wear of UVAM
decreasedby5%–20%,asshowninFig.34(b)[185].The
chipwasthinandsmall,andthetoollifewasprolonged
[185].TheauthorsalsoconductedanFEManalysisofthe
tool-tip trajectory using different vibration parameters
and proposed a calculation model of the chip thickness.
This model can accurately calculate the instantaneous
chipthickness.Researchersverifiedthecorrectnessofthe
model based on experimental process data [188] and
improvedthematerialremovalrate.
4.4Summaryofultrasonicenergyfield-assistedmillingof
difficult-to-machinemetalmaterials
Based on the above investigations, the ranges of
amplitudevaluesappliedinUVAMaredifferentbecause
oftheinconsistentbasicpropertiesofdifficult-to-machine
metalmaterials.Theamplituderangesofthenickel-based
alloy,titanium alloy,andhigh-strengthsteelare0–9µm,
0–14µm,and0–20µm,respectively.Theamplitudewas
consistent with the machinability of the three materials.
Combiningtheabovefindings,theoverallstructureofthe
UVAM machinability is summarized in Fig.35. By
controlling the vibration direction of UVAM, f, A, and
different processing parameters, the change rules of the
cutting force, surface morphology, surface roughness,
residualstress,chipmorphology,andtoolwearduringthe
workpiece machining process were explored. Based on
theexperimentaldata,itisconcludedthattheadvantages
of UVAM and LAM for difficult-to-machine materials
aresimilar.However,thetrajectoryoftheUVAMtooltip
anddynamiccuttingthickness were different from those
of the CM. Based on this, a calculation process for the
UVAM wave trajectory is developed. Furthermore,
consideringthe plastic deformation zone of UVAM, the
microstructure theory and the FEM model of the
machined surface were established. In addition, a new
tool flank wear model was developed based on the tool
angle to predict the surface roughness and tool wear of
UVAM-processed workpieces. Compared to CM, the
chipmorphologyandthickness of the UVAM-processed
materialschanged significantly. Toaccurately determine
the instantaneous chip morphology after UVAM, a chip
thickness model was developed using calculation and
FEM. The accuracy of each model was verified
experimentally. To improve the energy utilization rate,
UVAMandHM processes were used toconduct cutting
experiments on difficult-to-machine metal materials,
which effectively reduced the manufacturing cost.
Furthermore,basedon ultrasonicandcuttingparameters,
a prediction model showing the influence of the
instantaneous change in chip thickness on the cutting
force, surface morphology, surface roughness, residual
stress, chip morphology, and tool wear must be
established to promote the development of UVAM
technology.
5CMQLAM of difficult-to-machine metal
materials
CMQLAM is a new green machining technology that
combines the application of a cold medium, micro-
lubrication,andmilling.Inthisprocess,aliquid/gaseous
mediumissprayedintotheshearzoneinaccordancewith
the jet form, which can replace the traditional cutting
fluid to lubricate and cool the machining contact zone
[77]. The workflow and functions of the CMQLAM
systemareshownin Fig.36(a) [189].Theprincipleisto
combine a cold medium with atomizing oil mist and
water mist before reaching the nozzle, and then to cool
the shear zone through the nozzle. The water mist
vaporizesandabsorbsheat,whiletheoilmistispresentat
the contact surface between the workpiece and the tool,
reducingthe friction coefficientand heat generation due
tofriction.Thecoldmediumalsoreducestheviscosityof
the chips, which can achieve an excellent effect when
combined with micro-lubrication. Considering that
40 Front.Mech.Eng.2023,18(2):28
cuttingoil is usedin very small amounts inCMQLAM,
anoilfilmboundarylubricationisestablished,as shown
inFig.36(b)[189].
Duringnozzleoperation,theamountofoilattachedto
the machined surface increases, and the film thickness
graduallyincreases,asindicated by pointAinFig.36(b)
[189]. As CMQLAM continues, more lubricating oil is
gradually added to the low-lying surface of the shear
zone, as shown by point B. With increased amounts of
nozzleoilandprolongedinjectiontimes,thesurfacefilm
consistsofpeaksandvalleysduetofurtheradsorptionof
lubricating oil, as indicated by point C. When the oil
amount does not exceed point A, the amount of oil is
smallandtheoil film is thin, resultingindryfriction as
the tool directly contacts the peak of the workpiece.
WhentheoilamountisbetweenpointsAandC,onlythe
friction between the tool and the peak of the workpiece
occurs,resultinginaconstantfrictioncoefficient.Atthis
stage, the oil amount has little effect on the machined
surface. When the oil film at the top of the peak is
Fig. 35Summaryofultrasonicvibration-assistedmilling(UVAM)machinability.FEM:finiteelementmethod.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 41
damaged, the oil amount at point B can rapidly flow to
thetopofthepeakwithitsownfreeenergytorestorethe
original boundary lubrication state. However, when the
oil content exceeds point C, the stability of the friction
coefficient cannot be guaranteed [189]. Therefore, it is
important to control the CMQLAM lubrication parame-
ters carefully. CMQLAM of difficult-to-machine metal
materials is divided into three classes according to the
lubricationrangeofCMQLAM,asshowninFig.36(c).
Regarding the investigations on CMQLAM of nickel-
based alloys, based on a CO2 + MQL CMQL environ-
ment, first, different diameters of CO2 outlets were
compared, and numerical computational fluid dynamics
(CFD) simulations were performed to obtain the best
injection flow rate and nozzle diameter. Second, the
effectsofthefivecoolingandlubricationmethodsonthe
tool life were compared. Third, the effects of different
cooling and lubrication methods on machining tempera-
ture,cuttingspecificenergy,surfaceroughness,microhard-
ness,andresidualstresswereassessed.Then,theeffects
ofthefivecoolingandlubricationmethodsonthesurface
structure, surface morphology, and surface roughness
were compared. Based on an LN2 + MQL CMQL
environment, the effects of the three cooling and
lubrication methods on the surface roughness and tool
wearwere compared, and the effects of the toolcoating
and cooling lubrication conditions on the cutting force,
tool wear, surface roughness, and cutting temperature
were investigated. Based on a CA + MQL CMQL
environment,thecuttingforceandtoollifeunderdryand
CMQLconditionswerecompared.
TostudytheCMQLAMoftitaniumalloys,theeffects
of five micro-lubrication technologies and cutting speed
changesontoolwear,cuttingtemperature, cutting force,
andsurface roughness were analyzed based on a CO2 +
MQL CMQL environment. Under these conditions, the
cutting force was the lowest, the surface roughness was
the smallest, and optimal surface quality was obtained.
The cutting parameters and four green conditions were
varied to study their influence on cutting force, cutting
temperature,surface morphology,andsurfaceroughness.
SCCO2-OoWMQL had the best effect. Based on an
Fig. 36Cryogenicminimumquantitylubricationenergyfield-assistedmillingsystem(CMQLAM),lubricationmechanism and logic:
(a)CMQLAMsystem,(b)workpiecesurfaceboundarylubrication[189],and(c) logical structure of laser-assisted milling difficult-to-
machine metal materials. CA: cold air; MQL: minimum quantity lubrication. Reproducedwith permissionfromRef.[189]from
MechanicalScienceandTechnologyforAerospaceEngineering.
42 Front.Mech.Eng.2023,18(2):28
LN2 + MQL CMQL environment, the cutting force and
tool wear in a CMQLAM machining process were
analyzed,andtheeffectsofCMQLAMmachiningontool
life, surface roughness, cutting force, and productivity
were studied. In the CA + MQL CMQL environment,
CMQLAMsignificantlyreduced flankwear.Anewtype
of mixed nozzle capable of simultaneously injecting oil
mistandcryogenic gaswasdesigned.TheCoandaeffect
under different inlet flow rates, friction heat, and tool
wearusingconventionalandnewnozzleswerecompared.
The cutting force, tool wear, cutting temperature, and
manufacturing costs under CMQLAM conditions were
analyzed.
Regarding the studies on CMQLAM of high-strength
steel,theeffectsof four coolingandlubricationmethods
on the cutting force, cutting temperature, and tool wear
were compared in a CO2 + MQL CMQL environment.
Furthermore,theinfluenceofthenewCMQLmethodson
the cutting force, tool life, and surface roughness was
analyzed.Subsequently,the effects ofcuttingparameters
and cooling lubrication on tool life, material removal,
surface roughness, and residual stress were assessed.
Finally, the effects of the cutting speed and cooling
lubrication on the surface roughness, chip morphology,
flank wear, and cutting temperature were investigated.
Based on a CA + MQL CMQL environment, the
influence of cutting parameters on the cutting force and
temperaturewasanalyzedbysimulation,andaprediction
model was established. Experiments were conducted to
verifytheaccuracyoftheproposedmodel.Comparedto
dry milling, CMQL can reduce the cutting force and
cuttingtemperature. The influence of cuttingparameters
onthewhitelayerwasalsoanalyzed. Theeffectofthree
internalcooling channels on cutting forceand tool wear
wasinvestigatedwiththeresultthattheCMQLAMeffect
ofa double straight channel (DSC)internal cooling tool
wasthebest.
5.1CMQLAMofnickel-basedalloy
Theoptimalinjectionflowrate,nozzlediameter,andtool
life can be obtained in a CO2 + MQL CMQL environ-
ment. CMQLAM demonstrates good cooling and
lubrication effects. Pereira et al. [190] conducted
numericalandexperimentalanalyses of theCO2+MQL
CMQLAM. First, a CFD numerical simulation of CO2
outletswithdifferentdiameterswasconducted.Basedon
theCMQLenergyfieldwithaCO2pressureof14bar(1
bar=105Pa)andanMQLflowrateof100mL/h,Inconel
718 was processed via assisted milling, and the optimal
CO2injectionvelocityandoutletdiameterwere325m/s
and1.5mm,respectively.Theteamcomparedtheeffects
ofdrying,pouring,CO2,MQL,andCO2+MQLcooling
and lubrication methods on cutting. Different nozzle
diameters, cutting temperatures, and specific cutting
energiesareshowninFig.37[190,191].Comparedwith
CM pouring machining, the tool life of dry milling was
shortenedby53.3%. When only CO2or MQL was used
to assist milling, the tool life increased by 67.7% and
84.2%, respectively. CMQLAM could increase the tool
life to 93.5% and reduce the cutting oil by 90%, which
proved that CMQLAM could be applied in practical
engineering[190,192],asshowninFig.37(a)[190].
Theeffectsofdifferentcoolingandlubricationmethods
on the machining temperature, specific cutting energy,
surface roughness, microhardness, and residual stress
were compared in a CO2 + MQL CMQL environment.
Rossetal.[191]foundthatMQL and cryogenic cooling
can replace the CM cutting fluid; however, the cooling
andlubricationcharacteristicsofCO2+MQLCMQLAM
were not explored under high-speed cutting conditions.
They compared the processing effects of Nimonic 80A
underCO2,MQL, and CMQL conditionsandconducted
in-depth research on the processing temperature, energy
consumption,surface,andsubsurface.AtaCO2 pressure
of2.5barandMQLflowrateof60mL/h,theprocessing
temperature and specific cutting energy under CMQL
conditions ranged between 34%‒53% and between
17%‒19%,respectively,andwerereducedcomparedwith
MQL,as shown inFig.37(b) [191]. In addition, CMQL
decreased the grain size by reducing the friction at the
cutting point, thereby increasing the surface fatigue
strengthoftheworkpieceand providing the best cooling
effectduringprocessing,whichshowedthesuperiorityof
CMQL, as shown in Fig.38(a) [191]. The team also
conductedastudytoanalyzetheeffectsofCMpouring,
MQL, CO2, and CMQL on cutting temperature, surface
roughness,toolwear,microhardness,andresidualstress.
Theresultsshowedthat,comparedtoCMpouring,MQL,
and CO2, the processing temperature was reduced by
41%–53%, 29%–46%, and 17%–23%, respectively,
under CMQL conditions. The surface roughness also
decreased by 42%–54%, 34%–45%, and 19%–29%,
respectively. The tool wear was reduced by 48%–71%,
42%–56%,and22%–40%,respectively.Furthermore,the
surface microhardness increased by 9.57%, 9.13%, and
4.87%,respectively.WhencomparedtoCMpouring,the
residual compressive stress obtained by CMQL
processing increased by 25.18%. It was verified that
CMQLhastheadvantages of a lowcuttingtemperature,
high residual compressive stress, microhardness, and
goodsurfacequality,asshowninFig.38(b)[193].
Theeffectsoffive cooling and lubricationmethodson
the surface microstructure, morphology, and roughness
were compared in a CO2 + MQL CMQL environment.
Milling of Inconel 718 was conducted by Sterle et al.
[194]Theeffectsofdrying,CMpouring,LCO2,LCO2+
MQL (oil), and LCO2 + MQL (MoS2) cooling and
lubrication methods on the surface smoothness,
roughness,surfacemorphology,andmicrostructurewere
compared.The LCO2 pressure and MQL flow rate were
12 kg/h and 120 mL/h, respectively. The experimental
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 43
results showed that the surface finish under LCO2
treatment was close to that obtained with dry cutting.
Compared with LCO2 + MQL (oil), the surface
smoothness obtained by LCO2 + MQL (MoS2) was
improved,andtheMoS2 particles were easier to remove
after milling. Compared with CM casting milling, the
application of LCO2 + MQL (MoS2) resulted in lower
surfaceroughness,bettersurfacemorphology,andamore
uniformsurfacemicrostructure[194].
Inaddition toCO2+MQL,LN2+MQLalsocaused a
reduction in tool wear and surface roughness. Shokrani
etal.[195]foundthatMQL,LN2,andCMQLprocessing
were effective cooling lubrication technologies for
improvingthemachinabilityofdifficult-to-machinemetal
Fig. 37Different nozzle diameters, cutting temperatures, and specific cutting energies: (a) experimental results of different nozzle
diameteroutlets[190],and(b)effectsofgreenlubricationandcuttingparametersoncuttingtemperatureandspecificcuttingenergy[191].
MQL:minimumquantitylubrication.ReproducedwithpermissionsfromRefs.[190,191]fromSpringerNatureandElsevier.
44 Front.Mech.Eng.2023,18(2):28
Fig. 38Grain size distribution and scanning electron microscope: (a) effect of green lubrication on grain size distribution [191] and
(b) scanning electron microscope images of different green lubricants [193]. CM: conventional milling; MQL: minimum quantity
lubrication.ReproducedwithpermissionsfromRefs.[191,193]fromElsevier.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 45
materials. Therefore, groove milling experiments were
performed on Inconel 718 using the MQL, LN2, and
CMQL cooling and lubrication methods at an LN2
pressure of 1.2 bar and an MQL flow rate of 60 mL/h.
Compared with MQL, CMQL increased the tool life by
200% and reduced the surface roughness of the groove
bottom surface by 18% and that of the groove side
surface by 5% [195]. Based on the above experiments,
theteamchangedtheLN2pressureto1barandtheMQL
flow rate to 70 mL/h and conducted comparative
experiments under CM pouring cooling lubrication
conditions. The results showed that compared with CM
pouringcutting,CMQLcouldincrease tool life by 77%.
The surface roughness values of the side and bottom of
themachinedpartswerelessthan0.4µm.Bymonitoring
theenergyconsumptionofthemachinetool,itwasfound
that the energy consumption increased with tool wear.
Thesestudies clearly demonstrate thatthe application of
CMQLAMtoInconel718isfeasible[196].
Thecombination of toolcoating and greenlubrication
conditions will have a better effect on the machining
process. Şirin et al. [197] conducted an experimental
studyon theInconelX750alloyandexploredtheeffects
of tool coating (no coating, low-temperature treatment,
and TiAlN coating) and green lubrication conditions
(LN2, MQL, and CMQL) on tool wear, surface rough-
ness, surface morphology, cutting force, and cutting
temperature. Using an LN2 pressure of 15 bar and an
MQL flow rate of 50 mL/h, the authors showed that
althoughthehardnessofthetoolincreasedby7.36%after
low-temperaturetreatment, the tool life decreased in the
following order: TiAlN coating, low-temperature treat-
ment,andnocoating.ComparedwiththeuseofLN2,the
toolwearoftheuncoatedtoolwaslowerwhenapplying
MQL and CMQL; for the coated tool, the tool wear
decreasedby 63.8% and 70.1%, respectively. Compared
withtheuncoatedtool,thesurfaceroughnessofthetool
subjected to low-temperature treatment and the coated
tool was reduced by 2.72% and 6.22%, respectively,
whilethecuttingforcedecreasedby4.81%and7.11%,as
shown in Fig.39 [197]. Compared to the application of
LN2, the surface roughness values obtained with MQL
and CMQL decreased by 4.81% and 18.52%, respec-
tively. Under green lubrication conditions, compared to
LN2, the cutting forces using MQL and CMQL were
reducedby7.1%and10.76%,respectively,forthecoated
tool. Compared with the noncoated tools, the cutting
temperature of the coated tools decreased by 5.75%.
Fig. 39Differentgreen coolinglubricationandtool machiningsurfaces:(a) uncoatedtoolliquid nitrogen,(b)uncoated toolminimum
quantity lubrication (MQL), (c) uncoated tool cryogenic MQL (CMQL), (d) low-temperature treatment tool LN2, (e) low-temperature
treatmenttoolMQL,(f)low-temperaturetreatmenttoolCMQL,(g)TiAlN-coatedtool LN2,(h) TiAlN-coatedtoolMQL,and(i)TiAlN-
coatedtoolCMQL[197].ReproducedwithpermissionfromRef.[197]fromElsevier.
46 Front.Mech.Eng.2023,18(2):28
Compared to LN2, the cutting temperature decreased by
30.31%underCMQLcoolingand lubrication conditions
[197].
CA + MQL can prolong the tool life and reduce the
cuttingforce.Zhangetal.[198]studied the influence of
differentcuttingconditionsontoollifeandcuttingforce
changes during the machining of Inconel 718. In the
CMQLAMprocess,theCApressurewas1.5bar,andthe
MQL flow rate was 8 mL/h. Under dry milling and
CMQL conditions, flank wear and cutting edge fracture
werefoundtobethemainfactors leadingtotoolfailure.
Compared with dry milling, CMQL reduced the cutting
force, increased the tool life by a factor of 1.57, and
significantly improved the machinability of Inconel 718
[198].
5.2CMQLAMoftitaniumalloy
A minimal cutting force and surface roughness were
observed in the CO2 + MQL CMQLAM process.
Bagherzadeh et al. [199] studied the effects of MQL,
CO2,LN2,CO2 + MQL, andLN2+ MQL on toolwear,
cuttingtemperature,cuttingforce,andsurfaceroughness
in the machining process of TC4 at different cutting
speeds.The CO2andLN2pressuresandMQLflow rates
were set to 10.8 kg/h, 36, and 90 mL/h, respectively.
When comparing the tool wear under different cooling
lubricationconditionsatvc=60m/min,applyingCO2+
MQLresultedina31.8%lowertoolwearthanusingCO2
alone, while that under LN2 + MQL conditions was
59.6% lower than when using only LN2, and the
minimum tool wear could be obtained when applying
MQL only, as shown in Fig.40(a) [199]. When vc was
120m/min,thetoolwearobtainedusingCO2,LN2,CO2+
MQL, and LN2 + MQL decreased by 35.4%, 29.6%,
38.9%,and53.6%,respectively.Theminimumtoolwear
canbeachievedunderLN2+MQLconditions,asshown
inFig.40(b)[199]. The cutting force atvc = 120 m/min
undercoolingconditions (CO2 orLN2)alonewashigher
thanthatunderMQLconditions,whereasboththecutting
force and surface roughness were assumed to be the
lowest values when applying CMQLAM (CO2 + MQL)
[199].
Optimal surface quality can be obtained in a CO2 +
MQLCMQLenvironment.Hanenkampet al. [200] used
aCMQLenergyfield(CO2+MQL)withaCO2pressure
of 10 kg/h and an MQL flow rate of 60 mL/h for the
assisted milling of TC4. The research showed that
comparedwithCMgating cutting, thesurfaceroughness
values under CO2 and MQL conditions increased by
11.0% and 82.5%, respectively. When applying
CMQLAM,the surface roughness was the smallest, and
thesurfacequalitywasimproved[200].
The best results were obtained under SCCO2-
OoWMQLconditions.Caietal.[201]studiedthemilling
ofTC4infourgreenenvironments:drycutting,SCCO2,
SCCO2-WMQL, and SCCO2-OoWMQL. They analyzed
the effects of vc, fz, αe, and green lubrication on the
cutting force, temperature, surface morphology, and
surface roughness. In the experiments, the SCCO2
pressure and MQL flow rate were set to 7.5 bar and
50 mL/h, respectively. Irrespective of the green lubrica-
tion environment, when vc increased from 20 to
60m/min,theaveragecuttingforceincreasedby273.6%.
Under the SCCO2-OoWMQL condition, owing to its
excellent cooling lubrication, chip removal, and chip
breaking performance, the friction coefficient of the
contact surface between the tool and workpiece was
reduced,resulting in a lower cutting force. Furthermore,
owingtotheforcedconvectionheattransfer,vaporization
heat absorption, and promotion of chip removal and
lubricationofOoWMQLparticlesbySCCO2,thecutting
temperature and surface smoothness were optimal, as
shown in Fig.41(a) [201]. The cutting temperature
increased with an increase in vc, fz, and αe, whereas the
surfaceroughnessincreased with increasing vcandfz, as
shown in Fig.41(b) [201]. Under the action of SCCO2,
owing to the increase in material strength and hardness,
thefrictionatthetoolandworkpieceinterfacedecreased,
andthecuttingforceincreased,rangingfrom8%to64%.
Thiswouldresultinpoorprocessingperformance[201].
In an LN2 + MQL CMQL environment, the influence
of cutting parameters on the cutting force, tool wear,
surface roughness, and productivity was analyzed.
Suhaimietal.[202]appliedassistedmillingtoTC4with
aCMQLenergyfield (LN2 + MQL) using 2.5‒3barair
pressureandanMQLflowrateof180mL/h.Compared
to CM pouring cutting, the cutting force and tool wear
obtainedbyCMQLAM were reducedby54% and 90%,
respectively[202].Theteamalsoexploredtheprocessing
mechanismofCMQLAMandfoundthatusingonlyLN2
for processing led to strong adhesive wear of the tool.
Through the detection of the cutting force, it was
determined that the point where the cutting force
decreases to 0 N was the blade fracture point [203]. To
explore the influence of multiple parameters on
CMQLAMprocessing,Shokraniet al. [204], based ona
full-factor experimental design, combined the CMQL
energyfield (LN2+ MQL)with anLN2 pressureof 1.5
barandanMQLflowrateof70mL/hforassistedmilling
of TC4. It was found that compared with CM pouring,
CMQLAMincreasedthetoollifeby a factor of 30. The
effective cooling and lubrication characteristics of
CMQLAM control tool wear and adhesion rates. When
only LN2 was used to cool the workpiece surface, the
hardnessofthematerialandtheplasticdeformationofthe
cuttingedgeincreased,therebypromotingadhesivewear.
When vc was high, CMQLAM exhibited excellent
cooling and lubrication performance, which reduced the
frictionforceandtoolwear,asshowninFig.42(a)[204],
stabilizedthesurfaceroughnessat0.2µm,andincreased
productivity by 50%. To study the tool life under
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 47
Fig. 40Toolwearunderdifferentvcandlubrication/coolingmethods:(a)flankwearofalllubrication/coolingmethodsand(b)finaltool
wearofalllubrication/coolingmethods[199].ReproducedwithpermissionfromRef.[199]fromElsevier.
48 Front.Mech.Eng.2023,18(2):28
Fig. 41Effectofgreen lubricationandcuttingparameterson(a)cuttingtemperatureand(b)surfaceroughness[201].Reproducedwith
permissionfromRef.[201]fromSpringerNature.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 49
Fig. 42Toollifeandmicroscopicimagesunderdifferentcuttingconditions:(a)microscopicimagesofthecuttingedgeattheendoftool
lifeand(b)toollifemeasurementandpredictionresults[204].ReproducedwithpermissionfromRef.[204]fromElsevier.
50 Front.Mech.Eng.2023,18(2):28
different milling conditions, the tool life under multi-
parameter conditions was modeled and predicted, as
showninFig.42(b)[204].
Comparedwithothercryogenicmedia,theuseofCAis
relatedtoahighereconomicvalue, and CA + MQL can
significantlyreduceflankwear.Therefore,Suetal.[205]
employed TC4 in high-speed end milling experiments
andcomparedtheeffectsofdry,CA,andCMQLcooling
and lubrication methods on the cutting temperature and
toolwear.TheCApressureandMQL flowratewereset
to6bar and90mL/h,respectively.It wasfoundthatthe
measuredtemperaturevalues of theshearzoneincreased
in the order of CMQL, CA, and dry milling. The flank
wear when using CA was almost the same as that
obtained with dry milling, whereas the flank wear
observed when applying CMQL was significantly
reduced[205].
After the CMQL and milling parameters were deter-
mined, the atomizing nozzle structure of CMQL had a
directimpactonthemachiningprocess.Songetal.[206]
foundthatwhenMQLandcryogenicgaswereappliedon
bothsidesofthetool,theoilmistcouldnotpenetratethe
shear zone owing to the low injection pressure of the
cryogenic gas. Therefore, it is necessary to design a
hybridnozzlethatcansimultaneouslyinject oil mist and
cryogenic gases. Based on the Coanda effect and CFD
software analysis, the Coanda effect of the nozzle was
testedat differentinletflowrates,asshowninFig.43(a)
[206]. It can be observed by CFD that flow separation
occurs earlier at lower flow velocities. Therefore, the
flow parameters should be controlled to achieve ideal
cooling and lubrication effects after nozzle design. To
evaluate the performance of the nozzle, combined with
CA(pressureof 5 bar) and CO2gas (pressure of 8 bar),
TC4wasprocessedusingthedesignednozzle(MQLflow
rate of 19.8 mL/h) and conventional nozzle (MQL flow
rate of 54.9 mL/h). According to the results, low-tem-
perature micro-lubrication energy field-assisted milling
with the designed nozzle can reduce the friction heat in
the processing area, tool wear, and the minimum
Fig. 43Nozzlestructureandtoolwear:(a)nozzleCoandaeffect[206]and(b)influenceofgreenlubricationandcuttingvolumeontool
wear[207].ReproducedwithpermissionsfromRefs.[206,207]fromSpringerNature.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 51
temperatureofthecuttingzoneto310°C[206].Forthe
milling of TC4, the team also compared the cooling
lubrication performance of CMQL, dry conditions, CA,
andMQLwithaCO2pressureof4barandanMQLflow
rateof19.8mL/h.Theresultsshowedthatunderthesame
flow rate, CMQL reduced the cutting force, tool wear,
andcutting temperature by 23%, as shown inFig.43(b)
[207]. In addition, an economic analysis proved that
CMQLischeaperthanconventionalmethods[207].
5.3CMQLAMofhigh-strengthsteel
The new CMQL method can achieve better machining
effects. Mulyana et al. [94] conducted a milling
experimentonHTCSsteeland studied the effects ofdry
milling, MQL, SCCO2 and CMQL (SCCO2 + MQL)
conditions on the cutting force, temperature, and tool
wear. The pressure of SCCO2 was set to 4 bar, and the
flow rate of the MQL was 160 mL/h. Compared to dry
milling, the cutting force and cutting temperature under
CMQL conditions were reduced by 60% and 55%,
respectively. Compared with dry milling, MQL, and
SCCO2,thetoollife increased by 150%,87%,and22%,
respectively,whenusingCMQL.Overall,CMQLwasthe
best choice for reducing tool wear and prolonging tool
life, which could significantly improve the processing
efficiency [94]. In addition to the common CMQL
method (SCCO2 + MQL), Yuan et al. [208] proposed a
new CMQL (SCCO2-OoW) cooling and lubrication
system for milling 316L stainless steel. The effects of
SCCO2, OoW (oil-on-water), common CMQL, and new
CMQL on the cutting force, tool life, and surface
roughness were compared and analyzed. The SCCO2
pressure and MQL flow rate were set to 0.12 kg/h and
20 mL/h, respectively. The experimental results showed
thatcompared with common CMQL, SCCO2, and OoW
conditions, the application of the new CMQL method
maintainedalowercuttingforceand stable cutting force
variation throughout the cutting process. The tool life
decreasedinthe order ofthenewCMQLprocess,OoW,
ordinary CMQL, and SCCO2. When vc was 90 m/min,
comparedtoSCCO2andOoW,thesurfaceroughnessof
the new CMQL method decreased slightly. Compared
with SCCO2, the surface roughness of the workpieces
processed under OoW and CMQL conditions decreased
by25%and23%, respectively, when vc was120m/min.
Atavcof150m/min,thesurfaceroughnessofOoWand
CMQL was reduced by 39% and 32%, respectively,
compared with SCCO2, which proved that the new
CMQLmethodhadthebestmillingeffect[208].
The green lubrication parameters and cutting parame-
ters have a strong influence on machining. Wika et al.
[209] applied CM pouring and the CMQL (SCCO2 +
MQL) cooling lubrication mode at different vc and fz in
the milling of 304L stainless steel using an SCCO2
pressure of 6 bar and an MQL flow rate of 60 mL/h.
Compared with CM pouring cutting, the use of CMQL
resultedinthelongesttoollife,withanincreaseof324%
when vc and fz were 215 m/min and 0.5 mm/z, respec-
tively.TheCMQLmaterialremovalincreasedby158%.
Althoughthesurfaceroughnessdecreasedwithincreasing
fz,itincreasedwithincreasingvc.By using a high fz and
low vc, the surface roughness can be reduced by 30%.
UndertheconditionsofCMpouringandCMQL, tensile
residual stress was produced on the workpiece surface.
Whencombiningexperimentaldata,theauthors found fz
tobethemainfactoraffectingresidualstress,asshownin
Fig.44[209].
The above research shows that CMQLAM can
effectively prolong tool life when the vc value is high.
Basedonthis,ManimaranandNimelSwornaRoss[210]
studiedthe influence of vc inthe range of 45–75 m/min
on the cutting performance of AISI H13 steel at a
constantαp. Theeffectsofdrymilling,CMpouring,and
CMQL conditions on the surface roughness, chip
morphology, flank wear, and cutting temperature were
tested.TheCO2pressurewas2.5bar,andtheMQLflow
ratewas60 mL/h.Theresultsshowedthatunder CMQL
machining conditions, the cutting forces in the three
directions were reduced by 12%–16%, 11%–14%, and
12%–13% compared to dry milling. When compared to
the CM pouring process, the cutting forces were also
reduced by 6%–8%, 5%–7.5%, and 6.5%–8%,
respectively. Moreover, the application of CMQL
reducedthe cutting temperature by 52%–53% compared
to dry milling, and by 38%–41% compared to CM
pouring. Tool wear was also reduced by 50%–57%
comparedtodrymilling,andby14%–23%comparedto
CMpouring.Theaveragesurfaceroughnessdecreasedby
65%–71%and33%–41%,respectively. Additionally, the
machining hardness of CMQL was 6% and 2% higher
than those obtained by dry milling and CM pouring,
respectively. Compared with dry conditions and CM
pouringconditions,theuseofCMQLresultedinabetter
chip-breakingperformance,asshowninFig.45(a)[210].
Thecuttingforceandtemperatureaccompanytheentire
process. Zhang et al. [211] analyzed the influence of
CMQL on the cutting force and temperature during the
high-speedmillingof 300M steel. First,theinfluence of
cutting parameters on the cutting force and temperature
was investigated. The model was established using a
simulation and a prediction algorithm. Then, by single-
factorexperiments,withaCApressurerangeof6‒10bar
and an MQL flow rate of 265 mL/h, the variations in
cuttingforceandtemperaturewiththecuttingparameters
vc, fz, αp, and αe were studied under dry milling and
CMQL conditions, as shown in Fig.45(b) [211].
Comparedwith dry milling, the CMQLmethod resulted
in better lubrication and cooling effects, which could
effectivelyreducethecuttingforceandtemperatureinthe
shear zone. Based on this, the authors verified the
accuracy of the prediction model and provided a
52 Front.Mech.Eng.2023,18(2):28
theoretical and experimental basis for the subsequent
application of CMQL [211]. Furthermore, the team
performedmillingexperimentson300Msteelunderdry,
CA, water mist cooling, oil mist friction reduction, and
CMQLlubricationconditionsusingaCApressureof4.8
bar and an MQL flow rate of 150 mL/h. Through the
resultsofsingle-factorandorthogonalexperiments,itwas
foundthat, compared with other cooling and lubrication
conditions,CMQLcuttingconditionscouldobtainlower
cuttingforcesandbettersurfacesmoothness[212].
The white layer affects the service performance of
workpieces. Zhang et al. [213] studied the influence of
toolwearontheformationofawhitelayerindrymilling
andCMQLAMofH13steelat a CA pressure of 1.5bar
andMQLflowrate of 20mL/h.Theresultsshowedthat
CMQLAM could increase tool life by a factor of 1.78
comparedwithdrymilling.Furthermore,theformationof
thewhitelayerwasrelatedtotoolwear.Thethicknessof
the white layer increased with increasing tool wear.
According to the experimental results, the white layer
couldbepartiallyorcompletelyeliminatedunderCMQL
conditions by optimizing the parameters, as shown in
Fig.46(a)[213].This indicates that CMQL canimprove
the surface integrity [213]. The authors also conducted
side-milling experiments on H13 steel. Under CMQL
conditions using a CA pressure of 2 bar and an MQL
flowrateof 15 to 20 mL/h,the effects of three typesof
internal cooling tools, namely, double helix channel
(DHC), single straight channel (SSC), and DSC, on the
cutting force and tool wear were analyzed. Flank wear
andfracturewere found tobe the main factorsaffecting
toollife.The cutting force increasedwith an increase in
tool wear. Comparing the tool wear of three internal
coolingtools under CMQL conditions(Fig.46(b) [214])
revealed that the DSC tool achieved an effective
reduction in tool wear and a life 1.59 times longer than
that of the DHC tool, indicating that the DSC tool was
better than the DHC tool. From the perspective of
environmentalprotectionandeconomy,CMQLAMusing
a DSC internal cooling tool had the best effect on
machining[214].
5.4SummaryofCMQLAMofdifficult-to-machinemetal
materials
Based on the research presented above, the flow rate
range of MQL used in CM with CMQLAM varies
according to the basic properties of the difficult-to-
machinemetalmaterials beingused.TheMQLflowrate
ranges for nickel-based alloy, titanium alloy, and high-
strength steel are 8–120 mL/h, 19.8–180 mL/h, and
15–256 mL/h, respectively. These values are consistent
withthemachinabilityofthethreematerials.Insummary,
CMQLAM of difficult-to-machine metal materials is
depictedinFig.47.ComparedtoCMcastingcutting,the
types of low-temperature medium, gas pressure, MQL
flow rate, atomizing nozzle type, coating tool type, and
cutting parameters all affect the machining results. The
advantagesof CMQLAMincludelowcuttingforce,high
materialremovalrate,longtoollife, low cutting specific
energy, low cutting temperature, low manufacturing
costs,smallchipsize,andhighsurfacequality.However,
Fig. 44Average residual stresses corresponding to different fz and vc: (a) conventional milling 0° residual stresses, (b) conventional
milling 90° residual stresses, (c) cryogenic minimum quantity lubrication 0° residual stresses, and (d) cryogenic minimum quantity
lubrication90°residualstresses[209].ReproducedwithpermissionfromRef.[209]fromElsevier.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 53
Fig. 45Chipmorphology,cutting force, and cuttingtemperature:(a)chip morphology under differentlubricationenvironments[210]
and (b) influence of cutting parameters on cutting force and cutting temperature [211]. CM: conventional milling; CMQL: cryogenic
minimumquantitylubrication.ReproducedwithpermissionsfromRefs.[210,211]fromASTMandSpringerNature.
54 Front.Mech.Eng.2023,18(2):28
there is currently no model available to obtain optimal
parameters,andtheFEMmodelofthemachiningprocess
during cooling and lubrication and the predictive
optimization algorithm model still require further
research. Additionally, a normative guidance theory has
not been developed for the lubrication mechanism of
CMQLAM, and optimal processing parameters of
CMQLAM have not been defined. In the future, it is
necessary to design an intelligent matching system or
database to establish a quantitative correspondence
between the evaluation index level and the cooling
medium parameters, to realize the most effective
combinationof lubricatingoiltypesandprocessparame-
ters under different processing conditions. Moreover, an
intelligent nozzle and a multi-parameter coordinated
control system that can automatically adjust the space
attitude should be designed to guide the practical
production environment for the purpose of accurately
transportingtheCMQLfluidtothecuttingzone.
6Conclusions
The discussed shortcomings, such as the large removal
rate of titanium alloy, nickel-based alloy, high-strength
steel, and other difficult-to-machine metal materials, the
high energy consumption of machine tools, large tool
consumption, low processing efficiency, large emissions
of cutting oil mist and waste liquid, environmental
pollution and health hazards, and the dependence on
importedhigh-endtools andcuttingoil,seriouslyrestrict
the green low-carbon and independent and controllable
development of the manufacturing industry. With the
increasingdemandtoaddresstheissuesof‘carbonpeak’,
‘carbon neutralization’, and ‘manufacturing power’, the
concept of green manufacturing is becoming more
importantandwillhaveaprofoundimpactonthefuture
development of the global manufacturing industry. It is,
therefore, crucial to explore and address the limitations
and defects of energy-field-assisted green processing
technology for difficult-to-machine metal materials, and
toprovideinnovativeprocessingmethodsforglobalhigh-
endmanufacturing.
(1) Energy field-assisted machining mechanisms for
difficult-to-machinemetalmaterials
TheuseofLAM,UVAM,andCMQLAMtechnologies
toprocesstitanium alloys, nickel-basedalloys,andhigh-
strength steel can reduce the cutting force, improve the
material removal rate, prolong the tool life, reduce the
cutting specific energy, reduce manufacturing costs,
decrease chip size, and improve surface quality.
However, their processing mechanisms differ from one
another. LAM softens the shear zone using the laser
system before machining. UVAM applies ultrasonic
frequencyvibrationtotheworkpieceortool basedonan
ultrasonic system, which realizes a high-frequency
periodic separation of the workpiece and tool in the
cutting process. CMQLAM uses a jet device to spray a
liquid/gaseousmediuminto theshearzonedependingon
thejetform,which can replace theCMcutting fluid for
lubrication and cool the machining contact zone.
ComparedwiththeCM,theLAMhasagreaterinfluence
Fig. 46Subsurfaceandchannelstructures:(a)whitelayer[213]and(b)threechannelstructuresofinternalcoolingmillingtools[214].
ReproducedwithpermissionsfromRefs.[213,214]fromSAGEandSpringerNature.
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 55
onthecuttingforce,anditslimitvaluecanbereducedby
70%. UVAM has the greatest effect on chips, making
them thin and small. CMQLAM has the greatest
influenceonthetoollifeandcuttingtemperature,andits
limit values can be reduced by 157% and 60%,
respectively.
(2) Energy field-assisted machining methods for
difficult-to-machinemetalmaterials
Fig. 47Summaryofcryogenicminimumquantitylubricationenergyfield-assistedmilling(CMQLAM)machinability.
56 Front.Mech.Eng.2023,18(2):28
Currently, the use of titanium alloys, nickel-based
alloys, and high-strength steel is increasing. Traditional
processing methods cause severe tool wear, low proce-
ssing efficiency, and poor surface integrity. Therefore,
new processing methods are required for this purpose.
FortheLAMprocess,thispapersystematicallyillustrates
the influence of laser and cutting parameters on the
cutting force, material removal rate, tool life, cutting
specific energy, manufacturing cost, chip morphology,
and surface quality. To improve the data-driven proce-
ssingeffect,anintelligentalgorithmshouldbeestablished
topredicttheinfluenceofthelaserandcuttingparameters
onthecorrespondingparameters.FortheUVAMprocess,
inadditiontoexploringtheeffects of ultrasonic parame-
ters, cutting parameters, and vibration direction changes
oncuttingforce,surface morphology, surfaceroughness,
residual stress, chip morphology, and tool wear, a
predictionmodeloftheinfluenceofinstantaneouscutting
thicknesschange on the corresponding result parameters
should be developed based on ultrasonic and cutting
parameters. For the CMQLAM process, after exploring
the effects of air pressure, flow rate, and cutting para-
meters on cutting force, material removal rate, tool life,
cutting specific energy, cutting temperature, manufactu-
ringcost,chipsize,andsurfacequality,itisnecessaryto
establish a CMQLAM specification guidance theory to
definetheoptimalprocessingparameters.
(3) Difficulties in energy field-assisted machining of
difficult-to-machinemetalmaterials
A laser energy field can soften a material before
machining.Anultrasonicenergy field canimprovechip-
breaking ability. The CMQL energy field can reduce
cutting fluid emissions and realize green machining.
However, there are still difficulties restricting the
applicationanddevelopmentofenergyfields,suchasthe
longprocessingcycleofLAM,littleeffectofUVAMon
reducingthetemperature of theshear zone, and residual
oil on the surface of the CMQLAM-processed
workpieces. Therefore, the engineering application and
development of energy field-assisted HSDM green
machining technology requires combined global efforts.
This review provides feasible ideas for realizing multi-
energyfieldcollaborativegreenmachiningofdifficult-to-
machinemetalmaterialsinthefuture.
7Prospects
Difficult-to-machinemetalmaterialswillremainaglobal
research hotspot in the future. However, there are still
somelimitationstotheefficientandprecisemachiningof
difficult-to-machine metal materials. The above syste-
matic summary shows that future research directions of
energy field-assisted green machining technology for
HSDMmaymainlyfocusonthefollowingpoints:
(1)Fortoolcoatingswithdifferentapplicationrequire-
ments, the elemental composition and thickness of
coatings should be explored with three processing
scenarios: rough machining, semi-finishing, and
finishing.Thus, the optimumworking conditions canbe
appliedto thevariousprocessingmethodsofdifficult-to-
machinemetalmaterials,whichcanprolongthetoollife
intheenergyfield-assistedHSDMprocess.
(2)Itisnecessary to utilize multi-energyfieldsynergy
toassist the manufacturingof difficult-to-machine metal
materials, and cutting force, vibration, and temperature
sensingtechnologycanbeusedassignalinputsourcesto
controlthe ultrasonicandCMQLparametersinrealtime
under different processing conditions, which can realize
the adaptive intelligent control of difficult-to-machine
metalmaterialsinlarge-scalemanufacturing.
(3)Toaddresstheproblemofhighcarbonemissionsin
themachiningprocess,amulti-energyfieldcollaborative
and multi-dimensional carbon-efficient concept for
HSDM is proposed, which considers both efficient
material removal and surface quality assurance and
realizes green intelligent machining using multi-energy
fieldsatalowtotalenergyconsumptionoftheprocess.
Nomenclature
Abbreviations
B&F Back-and-forth
CA Coldair
CCD Centralcompositedesign
CFD Computationalfluiddynamics
CL Conventionalmelting
CM Conventionalmilling
CMQL Cryogenicminimumquantitylubrication
CMQLAM Cryogenic minimum quantity lubrication energy field-
assistedmilling
CVD Chemicalvapordeposition
DHC Doublehelixchannel
DSC Doublestraightchannel
FEM Finiteelementmethod
HAZ heat-affectedzone
H.F Highfeedmilling
HM Helicalmilling
HPDL High-powersemiconductorlaser
HSDM High-speeddrymilling
LAM Laser-assistedmilling
LCO2Liquidcarbondioxide
L.F Lowfeedmilling
LMO Localmisorientation
LS Singlelaserscanning
JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 57
MQL Minimumquantitylubrication
Nd:YAG Neodymium-dopedyttriumaluminumgarnet
NMQL Nanofluidminimumquantitylubrication
NURBS Non-uniformrationalB-spline
OoW Oil-on-water
PCBN Polycrystallinecubicboronnitride
PVD Physicalvapordeposition
SCCO2Supercriticalcarbondioxide
SEM Scanningelectronmicroscope
SLM Selectivelasermelting
SSC Singlestraightchannel
S&T Spatialandtemporal
TAM Thermal-assistedmachining
TC4 Ti–6Al–4V
UVAM Ultrasonicvibration-assistedmilling
XRD X-raydiffraction
Variables
AVibrationamplitude
dLHeatsourcesize
fVibrationfrequency
fzFeedpertooth
NzNumberoftips
PciCoordinatetoolpoint
PliInitialcoordinatepoint
PLLaserpower
PLiEndcoordinatepoint
rRadiusofthecuttingtool
rcSumoftheradiusofthecuttingtool
RExpectedfilletradius
Sa Averageroughness
Sq Surfacerootmeansquareroughness
tCuttingtime
vcCuttingspeed
vfFeedspeed
VLLaserscanningspeed
x,y,zTipdisplacements
xcl Distance between the tool center and the laser heat source
center
xLDistancebetweenspotandtool
ωrAngularvelocityofthespindle
αiToolradiusangle
αpAxialcuttingdepth
αeRadialcutwidth
βToolrotationangle
θInitialphaseofthevibrationsignal
xiDistance between the initial coordinate point of the heat
sourceandtheendcoordinatepoint
AcknowledgementsThisworkwassupportedbytheNational KeyR&D
Program of China (Grant No. 2020YFB2010500). The authors gratefully
acknowledgethereviewersandeditorsfortheirinsightfulcomments.
Conflict of InterestThe authors declare that they have no conflict of
interest.
Open AccessThis article is licensed under a Creative Commons
Attribution 4.0 International License, which permits use, sharing,
adaptation,distribution,andreproductioninany mediumor formatas long
asappropriate creditisgiven tothe originalauthor(s)and source,alinkto
the Creative Commons license is provided, and the changes made are
indicated.
Theimagesorotherthird-partymaterialinthisarticleareincludedinthe
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JinZHANGetal.Energyfield-assistedhigh-speeddrymillingofdifficult-to-machinematerials 65
... It is also noteworthy to mention the utilization of high-speed dry machining on very demanding materials. The work by Jin Zhang et al., published in 2023 [25], provides an indepth analysis of the characteristics and challenges associated with high-speed dry milling techniques when applied to difficult-to-machine materials, including titanium alloys, nickel and high-strength steels. A study was conducted to investigate the milling of these materials by varying the process parameters, such as speed and depth of cut. ...
... The employment of energy-assisted machining techniques has been shown to enhance efficiency, reduce tool wear, and improve surface quality. These methods typically involve the use of technologies such as laser applications or ultrasonic vibrations, which is explored in greater detail in forthcoming sections [25]. ...
... Despite its many limitations, dry machining offers a significant advantage in that it eliminates all types of cutting fluids. From an environmental and economic standpoint, it remains a viable option, provided the process is carried out effectively to avoid material losses, as it is a method with reduced capabilities [25]. Cutting fluids contribute significantly to environmental pollution and incur high costs in terms of acquisition, maintenance, and disposal, which can sometimes amount to twice their initial cost [26]. ...
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This document presents a review on cooling and lubrication methods in machining. A systematic search of information related to these methods was carried out based on the PRISMA (Preferred Reporting Items for Systematic Reviews and Meta-Analyses) methodology. The importance of the sustainability of machining processes is highlighted, as they represent between 10 and 17% of the total manufacturing cost of the final part and have negative environmental and health impacts. Although dry machining completely eliminates the use of cutting fluids, in many cases it produces unsatisfactory results due to the increase in temperature inside the tool, which requires prior analysis to ensure its viability compared to conventional techniques. On the other hand, semi-dry machining, which significantly reduces the volume of cutting fluids, is a more competitive alternative, with results similar to those of conventional machining. Other sustainable cooling and lubrication methods are also being investigated, such as cryogenic and high-pressure cooling, which offer better machining results than conventional processes. However, they have a high initial cost and further research is needed to integrate them into industry. While the combination of these cooling and lubrication methods could lead to improved results, there is a notable lack of comprehensive studies on the subject.
... In recent years, many field-assisted machining technologies have also been studied to improve the cutting performance of challenging materials. Zhang et al. [13] summarized the advantages and challenges of field-assisted processing technologies in recent years, providing valuable insights for addressing the machining challenges of ATI 718 plus. ...
... In the AB segment, the material undergoes plastic deformation, following the JC constitutive model. When it reaches point B, the material reaches the damage initiation (13) [15,27] are listed in Table 6. ...
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ATI 718plus is a novel nickel-based high-temperature alloy that delivers superior mechanical properties and higher working temperatures compared to the In718 superalloy. In order to study the machinability of ATI 718plus, a combination of experiments and finite element simulation is used to explore the mechanism of serrated chip formation and the evolution of microstructure under high-speed cutting conditions. Firstly, the Johnson-Cook constitutive model parameters of the ATI 718plus alloy were obtained through a split Hopkinson pressure bar experiment. Secondly, we established a 2D orthogonal cutting model on the AdvantEdge FEM platform by implementing the Johnson-Cook constitutive model and damage model via a custom subroutine. Through the comparison of orthogonal cutting experimental data and finite element simulation results, we verified the accuracy of the finite element model and analyzed the mechanism of serrated chip formation. Finally, combining the multi-physics field distribution of different parameters from the finite element simulation and EBSD test results, it is revealed that the microstructural evolution mechanism during the high-speed cutting of ATI 718plus involves grain lamellar refinement induced by CDRX and grain growth induced by DDRX. The interaction of these two processes results in different forms of microstructures. Under specific cutting parameters, a superfine grain layer with a thickness of 10 µm was formed on the machined surface, which holds great referential significance for our control and improvement of the surface properties in cutting machining.
... Mac et al. [116] attempted to improve both TL and SR by heating the workpiece material while maintaining high v values. Zhang et al. [117] comprehensively reviewed related techniques, such as laser-assisted machining. ...
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Advancements in machine tools have enabled high-speed machining (HSM) of mold and die (M&D) in the hardened state, offering improved sustainability compared to conventional methods. The M&D industry is often referred to as “the mother of manufacturing” because nearly all mass-produced discrete parts are fabricated using M&D. Meanwhile, the Industry 5.0 concept, introduced by the European Commission, has emerged as a comprehensive framework for guiding industrial development. This study presents a systematic literature review on the application of HSM in M&D fabrication within the context of an Industry 5.0 environment. The review covers 183 research articles. The obtained findings are grouped based on 11 assessment indexes aligned with the three pillars of Industry 5.0: sustainability, resilience, and human well-being. The study also identifies gaps between the literature and current industrial practices. Finally, future research directions are proposed to facilitate the comprehensive implementation of Industry 5.0 in M&D machining workshops.
... The actual processing of difficult-to-machine materials is subject to complex multifield coupling, including mechanical forces, thermal forces, electromagnetic forces and chemical reactions [26][27][28][29]. Qi et al. [30] established the mapping relationship between the multi-physical field (equivalent plastic strain, temperature) and the microstructure evolution of Inconel 718 during the cutting process, and the study indicated that high cutting speed contributes to grain refinement, and that high temperature and equivalent plastic strain are the main factors for grain refinement. ...
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Improving the surface quality and controlling the microstructure evolution of difficult-to-cut materials are always challenges in high-speed machining (HSM). In this paper, surface topography, defects and roughness are assessed to characterize the surface features of 7050 aluminum alloy (Al 7050) under HSM conditions characterized by high temperature, strain and strain rate. Based on multi-physical field coupling, the mechanism of microstructure evolution of Al 7050 is investigated in HSM. The results indicate that the surface morphology and roughness of Al7050 during HSM are optimal at fz = 0.025 mm/z, and the formation of surface defects (adherent chips, cavities, microcracks, material compression and tearing) in HSM is mainly affected by thermo-mechanical coupling. Significant differences are observed in the microstructure of different machined subsurfaces by electron backscatter diffraction (EBSD) technology, and high cutting speeds and high feed rates contributed to recrystallization. The crystallographic texture types on machined subsurface are mainly {110}<112> Brass texture, {001}<100> Cube texture, {123}<634> S texture and {124}<112> R texture, and the crystallographic texture type and intensity are significantly affected by multi-physical field coupling. The elastic–plastic deformation and microstructural evolution of Al7050 alloy during the HSM process are mainly influenced by the coupling effects of multiple physical fields (stress–strain field and thermo-mechanical coupling field). This study reveals the internal mechanism of multi-physical field coupling in HSM and provides valuable enlightenment for the control of microstructure evolution of difficult-to-cut materials in HSM.
... Multi-energy field-assisted machining is a new and emerging machining technology that uses multiple energy sources to improve material removal processes. The technique involves the combined use of several types of energy (electrical, magnetic, ultrasonic, etc.) to increase machining efficiency or machining accuracy [31,32]. For example, Zheng et al. [33] focused on optimising the laser parameters during CFRP machining. ...
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Several challenges arise during edge trimming of carbon fibre-reinforced polymer (CFRP) composites, such as the formation of machining-induced burrs and delamination. In a recent development, appropriate-quality geometric features in CFRPs can be machined using special cutting tools and optimised machining parameters. However, these suitable technologies quickly become inappropriate due to the accelerated tool wear. Therefore, the main aim of our research was to find a novel solution for maintaining the machined edge quality even if the tool condition changed significantly. We developed a novel mechanical edge-trimming technology inspired by wobble milling, i.e., the composite plate compression is governed by the proper tool tilting. The effectiveness of the novel technology was tested through mechanical machining experiments and compared with that of conventional edge-trimming technology. Furthermore, the influences of the tool tilting angle and the permanent chamfer size on the burr characteristics were also investigated. A one-fluted solid carbide end mill with a helix angle of 0° was applied for the experiments. The machined edges were examined trough stereomicroscopy and scanning electron microscopy. The images were evaluated through digital image processing. Our results show that multi-axis edge-trimming technology produces less extensive machining-induced burrs than conventional edge trimming by an average of 50%. Furthermore, we found that the tool tilting angle has a significant impact on burr size, while permanent chamfer does not influence it. These findings suggest that multi-axis edge trimming offers a strong alternative to conventional methods, especially when using end-of-life cutting tools, and highlight the importance of selecting the optimal tool tilting angle to minimize machining-induced burrs.
... Dry cutting is considered the most promising route for sustainability in metal cutting and has been gaining significant attention in research during recent years [15]. Several techniques have been employed for improving the performance of dry cutting and optimizing its outcomes to reach the outcomes of wet machining, such as texturing tools [16] coating tools [17,18] energy-assisted hybrid machining [19,20]. Among the important optimizing routes in dry machining is using structured tools or textured cutting tools. ...
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Efficient lubrication and cooling are crucial in machining operations to enhance tool life and workpiece quality. Sustainable methods like minimum quantity lubrication (MQL) and dry cutting often face limitations in cooling efficiency and chip evacuation, especially under high-speed conditions or when machining difficult-to-cut materials such as stainless steel. This study introduces the novel pressurized injection lubrication (PIL) technique designed to address these challenges by optimizing lubrication, cooling, and chip evacuation during the turning operations of stainless steel 304. Using flaxseed oil as the lubricant, the PIL system employs a 0.26 mm stream diameter at a pressure of 16 bar to provide the necessary cooling and lubrication to the cutting zone. Cutting temperature and surface roughness were selected as the primary responses. Experimental runs were designed using the Taguchi L9 method. Analysis of variance showed that the lubrication method significantly affected the cutting temperature, with a contribution percentage approaching 94%. The experimental results demonstrated that PIL reduced the cutting temperature by up to 55%, while MQL reduced it by about 48%, both compared to dry cutting at the highest utilized speed. The lubrication method was also found to be the most significant factor affecting surface roughness, with a contribution percentage of 72.8%. Experimentally, PIL improved surface roughness by a maximum of 16.2% compared to MQL. Additionally, PIL maintained low oil consumption (0.9 l/h) and energy usage (< 0.017 kWh). The cost-effective PIL setup, priced under 65 USD, underscores its potential as a sustainable and efficient alternative for machining processes. The system’s components are readily available, facilitating easy integration into existing metal-cutting machines. Finite element analysis (FEA) modeling was used to predict residual stresses under different lubrication methods. The FEA model indicated that PIL and MQL reduced residual stresses by about 81.2% and 76.6%, respectively, compared to dry cutting at a speed of 500 rpm. These findings suggest that PIL can significantly enhance machining performance and sustainability, offering a viable solution to modern manufacturing challenges.
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The study addresses the machinability of heat-treated Ti1023 titanium alloy and maps strategic operating conditions for reduced cutting forces, improved surface roughness, and elevated material removal rates during end milling operations. An experimental study employing a full factorial design is utilized to investigate the effects of milling process variables, cutting speed, feed rate, and axial depth of cut, on the machinability indices, namely cutting force, surface roughness, and material removal rate. Correlations between the milling process parameters and the machinability indices were established based on the experimental data, employing a least-squares method for nonlinear modeling. The formulation of a multi-objective optimization problem was undertaken with the aim of improving the machinability of the heat-treated Ti1023 alloy, considering the objectives of reduced cutting forces, improved surface roughness, and maximum material removal rate. A population-based multi-objective multiverse optimization (MOMVO) algorithm was implemented to generate Pareto optimal solutions and compared with non-dominated sorting genetic algorithm II and feasibility enhanced particle swarm optimization. The findings highlight the efficacy of the MOMVO in exploring diverse solutions across the solution space. The Pareto optimal solutions were ranked on their desirability and used to map optimal operating conditions, providing an intuitive guide for practitioners to determine appropriate parameters for efficient and effective milling of heat-treated Ti1023 alloys for aerospace applications.
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Cutting fluid plays a cooling-lubrication role in the cutting of metal materials. However, the substantial usage of cutting fluid in traditional flood machining seriously pollutes the environment and threatens the health of workers. Environmental machining technologies, such as dry cutting, minimum quantity lubrication (MQL), and cryogenic cooling technology, have been used as substitute for flood machining. However, the insufficient cooling capacity of MQL with normal-temperature compressed gas and the lack of lubricating performance of cryogenic cooling technology limit their industrial application. The technical bottleneck of mechanical—thermal damage of difficult-to-cut materials in aerospace and other fields can be solved by combining cryogenic medium and MQL. The latest progress of cryogenic minimum quantity lubrication (CMQL) technology is reviewed in this paper, and the key scientific issues in the research achievements of CMQL are clarified. First, the application forms and process characteristics of CMQL devices in turning, milling, and grinding are systematically summarized from traditional settings to innovative design. Second, the cooling-lubrication mechanism of CMQL and its influence mechanism on material hardness, cutting force, tool wear, and workpiece surface quality in cutting are extensively revealed. The effects of CMQL are systematically analyzed based on its mechanism and application form. Results show that the application effect of CMQL is better than that of cryogenic technology or MQL alone. Finally, the prospect, which provides basis and support for engineering application and development of CMQL technology, is introduced considering the limitations of CMQL.
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The present study aimed to implement a sustainable machining method to improve energy efficiency in helical milling (HM) of AISI 1020. Therefore, ultrasonic vibration is integrated with conventional helical milling to reduce cutting forces. A model was developed for power consumption in terms of cutting forces in x, y and z directions, tangential and axial feed speeds. Series of plain and ultrasonic vibration helical milling (UVHM) experiments are conducted using 10 and 8 mm diameter mill cutters at different working conditions and experimental results for cutting forces are collected. Formation of chip and its geometry are investigated using the cutting trajectories of the bottom cutting edges of the cutter. Cutting forces and power consumption are estimated related to chip geometry in plain and UVHM processes and compared. In UVHM, the axial force is reduced by around 47% as the ultrasonic vibration is applied in the axial direction and the power consumption is reduced by 34%. The results showed that ultrasonic vibration has a significant effect on chip morphology, cutting force and power consumption, indicating that ultrasonic vibration assisted machining has a wide application in manufacturing. The process parameters are optimised as 2000 rpm of cutter rotational speed, 156 rpm of cutter orbital speed and 0.3 mm of axial depth of cut using 8 mm diameter cutter and the chip thickness, chip depth and power consumption are found to be 0.3969 mm, 0.2665 mm and 835.6 W respectively at optimal working condition.
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Surface roughness of conventional (CL) Ti6Al4V and selective laser melting (SLM) Ti6Al4V was investigated and contrasted using the method of conventional milling (CM) and ultrasonic-assisted milling (UAM) in this paper. Compared with the CL Ti6Al4V, results indicated that surface roughness of the SLM Ti6Al4V using the CM and UAM can be reduced by up to 37.5% and 18.3%, respectively. The surface roughness of SLM Ti6Al4V and CL Ti6Al4V using the UAM compared with that of CM can be reduced up to 23.3% and 19.1%, respectively. It was found that SEM topography(1500 ×) of the CL Ti6Al4V and the SLM Ti6Al4V has no prominent difference under the condition of CM or UAM. Moreover, it was observed that the SEM topography of the machined SLM Ti6Al4V or CL Ti6Al4V can be effectively improved using the UAM rather than the CM. Finally, the improvement mechanism of surface roughness was discussed and analyzed.
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In order to study the influence of spindle speed and amplitude on the surface integrity, TC18 titanium alloy samples were milled by the process of conventional milling and longitudinal ultrasonic vibration assisted milling. The experimental data were obtained by dynamometer, thermometer, scanning electron microscope, X-ray diffractometer, and three-dimensional surface topography instrument for observation and analysis. The results show that the spindle speed has a significant effect on the cutting force, cutting temperature, surface morphology, and surface residual stress. Compared with conventional milling, the surface micro-texture produced by longitudinal ultrasonic vibration assisted milling is more regular, and the cutting force and cutting temperature can be reduced by 34.1% and 19.5%, respectively. Then, the surface residual compressive stress and surface roughness can be increased by 50.9% and 163.88%, respectively. In addition, a certain depth of plastic deformation layer can be formed under the surface of ultrasonic vibration machining, and the depth of deformation layer increases with the increase of amplitude, and when the amplitude is 4 μm, the depth of plastic deformation can reach about 5.2 μm. This study lays a theoretical foundation for further research and optimization of ultrasonic milling technology for difficult machining materials.
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In the traditional micromilling (TMM) of Inconel718 alloy, due to the influence of material plasticity and size effect, relatively large burr will be produced. In order to hinder the burr forming in micromilling, ultrasonic vibration in feed direction is applied to the workpiece to complete vibration cutting. Combined with trajectory simulation and cutting experiment, the burr formation mechanism of TMM and ultrasonic vibration assisted micromilling (UVAMM) was studied. The results show that when the ratio of amplitude (A) to feed per tooth (ƒz) is greater than 0.5, continuous cutting changes to intermittent cutting in the vibration cutting process. The fractured area with dimples on the burr increases with the increase of amplitude. Compared with TMM, UVAMM improves chip breaking ability, facilitates the propagation of burr crack, and effectively inhibits the formation of burr. When the chip breaking condition is reached, the burr shape is usually tearing or flocculent. Under the conditions of low speed (n), large ƒz, and large A, the burr suppression is more obvious.
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A polycrystalline diamond (PCD) tool is employed in cutting various titanium alloys because of its excellent properties. However, improving the cutting performance of titanium alloys is still a challenge. Here, an experimental investigation on the influence of ultrasonic vibration-assisted machining (UVAM) of Ti6Al4V titanium alloy on the cutting performance and action mechanism was studied using a PCD tool. Cutting force, machined surface, surface adhesion, and wear morphology were analyzed. The results indicated that UVAM can effectively improve cutting performance. It was found that there was serious adhesion and wear of slight fragments close to the cutting edge after ultrasonic-assisted dry milling. Furthermore, the action mechanism of UVAM in improving cutting performance was discussed and analyzed from the perspective of intermittent cutting.
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The latest development of CMQL technology was reviewed, and the key scientific problems in the research results were clarified. Firstly, the application forms and technology characteristics of CMQL equipment in cutting processes were systematically analyzed from traditional setting to innovative design. Secondly, the cooling and lubrication mechanism of CMQL and the influence mechanism on cutting thermo-force evolution and workpiece surface quality were revealed. Furthermore, CMQL application performances in turning, milling and grinding for typical difficult-to-machined metals were systematically analyzed based on the action mechanism and application form. The effect of CMQL on restraining thermal-mechanical coupling damage and improving quality was better than that of cryogenic and MQL alone. Finally, the limitations of the technology and the development direction were analyzed, which provides the reference for the engineering applications of CMQL technology. © 2022, China Mechanical Engineering Magazine Office. All right reserved.
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Micromilling of difficult-to-machine materials like Ti-6Al-4V alloy suffers from drawbacks such as tool wear and catastrophic tool breakage due to the tiny diameter of the micro tool. Hence, in this paper, an effort has been made to prolong tool life and improve surface quality via hybridization of water and CuO nanofluid-based MQL with PVD coated (AlTiN/TiAlN) and uncoated WC micro end-mill in micromilling of Ti-6Al-4V alloy. The results exhibited minimum surface roughness at lower concentration (0.25 vol%) of CuO nanofluids with AlTiN coated WC tool and diminished tool wear and built-up edge formation at higher concentration (1 vol%) water-based CuO nanofluids. Under various environmental conditions, the average size of the top burr width was determined on both the up and down milling sides. The minimum average burr width of 9.93 μm was obtained in up milling using 0.25 vol% CuO nanofluids condition with AlTiN coated tool. In the case of down milling, the minimum burr width was 10.58 μm when using 0.25 vol% CuO nanofluids with TiAlN coated tool. Furthermore, significant improvements in tool life and surface quality have been observed through the hybridized sustainable environments obtained by the combined utilization of MQL and coated tools.
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Poor surface traits, short insert life, high manufacturing costs, and low productivity are associated with the machining of nickel alloys. Cutting fluids have well-known positive and negative effects on machinability performance. As a result, the machining industry has developed green cutting environments such as vegetable oil assisted minimum quantity lubrication (MQL) and cryogenic cooling. Despite the fact that MQL and cryogenic approaches can replace mineral oil-based flooding, their lack of lubrication and cooling properties at high speeds have prompted a search for a new hybrid approach (CO2 + MQL) that provides adequate cooling/lubrication (C/L). Moreover, as of now, no information concerning the effects of hybrid cooling on milling of Nimonic-80A is existing. To test the viability, the machining of Nimonic-80A under hybrid C/L was compared to other cutting environments (MQL and cryogenic). As crucial machinability factors, temperature, power consumption, surface and subsurface characteristics were thoroughly examined. Hybrid condition curtailed the burr formation, which paves the way for a reduction in specific cutting energy (SCE). The experimental results indicate that the hybrid condition considerably decreases the temperature and SCE by 34–53% and 17–19% in comparison with the MQL condition. Peak widening and intensity reduction were seen in the XRD examination, but no phase transition was found. Smaller grain size shows the superiority of hybrid environment.
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Longitudinal ultrasonic vibration-assisted milling (LUVAM) was performed to improve the machinability and surface quality of titanium alloys Ti-6Al-4V under dry conditions. Effects of ultrasonic amplitude on the three-component cutting forces, cutting temperature, surface topography and 3D surface roughness (Sa and Sq) were investigated. The results show that, the cutting forces in both longitudinal and feed directions decrease with the increasing amplitude from 0 to 6 µm, as well as the average and maximum cutting temperature. Accordingly, the surface topography of Ti-6Al-4V becomes more uniform when ultrasonic amplitude reaches to 6µm. Sa and Sq decrease by 35.1% and 34.0%, respectively, when the ultrasonic amplitude increases from 0 to 6 µm. The machinability and surface quality of Ti-6Al-4V are improved via this dry LUVAM, duo to the thermal-mechanical coupling resulted from large-amplitude ultrasonic vibration. The established approaches have potential applications in dry or near dry cutting of difficult-to-machine alloys with LUVAM.