Conference PaperPDF Available

Woven Nitinol Fabric Strips Characterized in Tension via Finite Element Analysis and Geometric Modeling

Authors:
  • Deft Dynamics

Abstract and Figures

Nitinol in the form of wires, tubes, and plates have been explored extensively; however, the characteristics of Nitinol as a woven fabric have so far been little-studied analytically. It would be easier to design such a fabric if conventional fabric models were known to apply to Nitinol fabrics, potentially with modifications required by Nitinol’s unique properties. A 25 mm wide Nitinol narrow fabric has been manufactured using traditional weaving equipment using a proprietary process that achieves a uniform and tight weave. Heat-treatment and straight shape-set is applied to a single Nitinol wire and the woven Nitinol fabric at 600°C for 30 minutes. The 0.25 mm Nitinol wire constituent was tested using differential scanning calorimetry (DSC) to determine the transition temperatures (Mf, Ms, As, and Af), which were found on average to be 54.5°C, 66.9°C, 88.7°C, and 103.5°C respectively. Both the Nitinol wire and fabric were tested in a temperature-controlled chamber (testing temperatures ranged from room temperature to 200°C) in which the tensile stress-strain characteristics were observed. It was determined that existing analytical models can be employed to accurately estimate the overall tensile stiffness of woven Nitinol fabrics in a small-strain regime. Additionally, it was confirmed that the tensile loading of woven Nitinol fabric can be modeled in MSC.Adams with beam elements. In combination with the geometric model presented, woven Nitinol fabric behavior can be predicted from the experimental behavior of the constituent Nitinol wire.
Content may be subject to copyright.
1 Copyright © 2020 by ASME
Proceedings of the ASME 2020 Conference on Smart Materials, Adaptive Structures and Intelligent Systems
SMASIS2020
September 14-16, 2020, Irvine, California, USA
SMASIS2020-2290
MACHINE DESIGN FOR MULTISCALE NITINOL ANNEALMENT PROCESS AND
END PRODUCT PERFORMANCE ANALYSIS
Amanda Skalitzky Stuart Coats
Auburn University Auburn University
Auburn, Alabama, USA Auburn, Alabama, USA
Ramsis Farag Austin Gurley David Beale
Auburn University Deft Dynamics Auburn University
Auburn, Alabama, USA Birmingham, Alabama, USA Auburn, Alabama, USA
ABSTRACT
The functional properties of Nitinol (NiTi) are set by
composition, production process, and post-production heat
treatment and cold working. Post-production heat treating is
dependent on two main parameters: anneal temperature and
aging time. Most heat-treating processes performed by
researchers generally consist of simple temperature soaks at
specified aging times. However, there are drawbacks to this
method. More complex heat treatments can result in
performance improvements, but they are difficult to implement
and often proprietary to manufacturers and therefore not widely
used by researchers. By designing a Continuously-Fed heat
treatment System (CFS), this work demystifies this complex
heat-treatment process by rapidly heat-treating NiTi wire
samples across a range of annealing temperatures, soak times,
and tensions with little human intervention. This automated
process ensures samples are created in a consistent manner and
results in a much more consistent end-product when compared
to conventional heat-treating methods. Using the CFS, a gamut
of samples with varying annealing temperatures (400-550°C)
and aging times (1-3 minutes) were created with 0.25mm
diameter high-temperature actuator wire initially in the ‘as-
drawn’ condition. Differential Scanning Calorimetry (DSC)
analysis was performed to determine how the transition
temperature(s) change with the various heat-treating parameters
and the mechanical properties of the wire were determined
utilizing a tensile test. The experimental results demonstrate the
benefits of the CFS and are compared to those of a more
conventional heat treatment process. Experimental results show
that high-performance Nitinol actuator behavior can consistently
be achieved using the CFS. Optimal heat treatment processes
can be determined quickly experimentally.
INTRODUCTION
The term Shape Memory Alloy (SMA) refers to an alloy
that undergoes a microstructural phase change that may be
initiated through the application of mechanical stress or by
varying the material temperature [1]. There are many different
types of SMAs, including iron-manganese-silicon, copper-
aluminum-silicon, copper-zinc-aluminum, and Nitinol (nickel-
titanium). Nitinol is a very popular SMA due to a good balance
of cost, stability, and thermos-mechanical performance [2]. It is
composed of nickel and titanium, with a ratio varying tightly
between 49 and 51 atomic percent nickel [3]. Although the cost
of Nitinol is higher than that of some other SMAs, the benefits
of altering the memory-recovery temperature and overall
functional properties through various methods such as the
production processes, alloy variation, and annealing temperature
and aging time supersede the higher cost. Additionally, Nitinol
has a unique ability to undergo large amounts of stress and strain
during thermo-mechanical loading and has the capability to
recover large inelastic strains near 8% before experiencing any
permanent deformation [4].
Nitinol has two different transformation mechanisms,
shape-memory and super-elastic, which occur during a reversible
phase change from an Austenite (B2) to Martensite (B19’)
microstructure. A chang e in te mperat ure r esults i n the phase
transformation responsible for the shape memory property while
a stress-induced transformation is responsible for the super-
elastic property. There is an additional phase known as the R-
phase, which occurs when the material is annealed at a certain
range of temperatures and appears during the cooling cycle,
generally in between the Austenite and Martensite phases [5]. It
2 Copyright © 2020 by ASME
occurs when Nitinol has a high dislocation density (the material
has been cold worked) and/or when there are Ni-rich precipitates
(the material has undergone a heat treatment process). This
phase does not allow for large strain transformations and causes
a two-stage transformation behavior [6].
The temperature where the various phase changes occur
are often referred to as the transition temperatures and can be
seen on the phase diagram in Figure 1. When no external stress
is applied and the Nitinol is heated, it begins to transition from
the Martensite phase into the Austinite phase. This is known as
the Austenite-start-temperature (
𝐴!
). As the material continues
to be heated, the material eventually transforms entirely into
Austenite phase, which is referred to as the Austenite-finish-
temperature (
𝐴"
). While cooling under a stress-free state, the
temperature at which the phase transformation from Austenite
back to Martensite begins is referred to as the Martensite-start-
temperature (
𝑀!
). The temperature at which this phase
transformation is complete is called the Martensite-finish-
temperature (
𝑀
"
). Above a certain temperature known as the
Martensite-deformation-temperature (
𝑀#)
Martensite can no
longer be induced with stress alone and as a result the material is
permanently deformed [7]. The upper and lower temperature
bounds of the R-phase transformation are known as the R-phase-
start-temperature (
𝑅!
) and the R-phase-finish-temperature (
𝑅"
)
[8].
Figure 1: Nitinol phase diagram.
HEAT-TREATMENT EFFECT
Nitinol can be purchased in many different forms such
as-drawn or straight-annealed. As-drawn Nitinol means the
material has been heavily cold-worked by the manufacturer. The
cold work provides creates an internal strain field in the
crystalline structure resulting in the alloy possessing a higher
yield stress and ultimate tensile strength. However, once a heat-
treatment is performed by the user, the alloy becomes annealed.
This lowers the yield stress and ultimate strength when atomic
diffusion that is accelerated by being held at elevated
temperature releases the internal strain field between the crystals
[9]. If the annealing temperature and aging time is too high, it
will cause the material to recrystallize and therefore have a lower
ultimate tensile strength and extremely high yield strains.
Additionally, in the recrystallized state, it should be noted that
although the material has a high strain to failure, the reversible
recovery strain drops well below 8% [10]. Therefore, it is
important for most applications that take advantage of the shape-
memory or super-elastic effects to ensure recrystallization does
not occur.
There are benefits to working with as-drawn wire such
as easier shape-setting and higher strengths as compared to
straight-annealed Nitinol material. If as-drawn Nitinol is
utilized, the heat-treatment process is the most common process
utilized to alter the thermal and mechanical properties of Nitinol.
Heat-treatment refers to both the annealing temperature and
aging time which crucially effect the behavior of the Nitinol [11].
The temperature at which the reversible phase
transformation from Austinite to Martensite initiates can be
altered through annealing at various temperatures, aging times,
and various quenching profiles after heat treatment [12]. As the
annealing temperature increases, the transformation temperature
does as well, which causes an increase in the endothermic and
exothermic peaks of the DSC curve [13].
SYSTEM DESIGN
The Continuously Fed heat-treatment System (CFS)
comprises four main elements: a temperature-controlled furnace,
a tension-controlled wire feeder, a quenching bath, and a
feedback control computer which can be seen in Figure 2.
During operation, untreated wire is pulled through the furnace at
a continuous slow speed under regulated tension. The soak time
is determined by the speed and oven size and the wire is
quenched immediately upon exiting the furnace. A s equenc e o f
desired sample lengths, temperatures, soak times, and tensions
are provided to the control computer and it autonomously
generates these samples and spools them for the operator to
perform post heat-treatment tests.
Figure 2: Diagram of the Continuously fed heat-treatment system
architecture
The furnace was designed using a modified Neycraft
JFF-2000 Fiber Furnace which was selected due to its large size
which allowed for the heat-treatment of longer sections of wire.
Additionally, the systems’ electrical simplicity allowed for
straightforward modification of the internal temperature
3 Copyright © 2020 by ASME
controller. This furnace was then outfitted with a new
temperature controller to provide more precise temperature
control (within 1°C of the desired temperature) than the original
manufacturer equipment which consisted of a knob that
controlled oven duty cycle and a temperature display. The new
temperature controller was developed by replacing the existing
oven electronics with a high voltage relay connected to the
furnace’s internal resistance heater, a K-type thermocouple and
thermocouple amplifier, and a Teensy 3.2 microcontroller
implementing closed-loop PID control. The Teensy 3.2 was
implemented because of its low cost, high processing speed, ease
of programming, and modularity.
In addition to the temperature controller, three NEMA
17 geared stepper motors, paired with DeftStep stepper-servo
drivers (Figure 3), were attached to an external frame to allow
for the continuous feeding of Nitinol wire through the thermal
chamber of the furnace using spools of 3D-printed polymer
attached to the output shaft of the motors. NEMA 17 motors
offer high torque output per cost when used with a planetary
gearbox as in this application. The DeftStep drivers provide an
easy conversion from a traditional stepper motor into a more
useful stepper-servo motor. The drivers also allow for relatively
simple configuration and communication when using a USB-
based microcontroller such as a Teensy and modification of the
stepper driver firmware allowed for direct speed control.
Additionally, these drivers employ current chopping, direct
control of current, which not only increases the bandwidth of the
motor, but also allows for the use of currents twice as high as the
motor specification for short periods of time resulting in even
higher torque output.
Figure 3: Neema 17 stepper motor (left) and DeftStep stepper-servo
driver (right)
The first motor was used to control the speed of the wire
through the furnace. The second was used to control the tension
on the wire throughout the annealing process, as measured with
two load cells attached to the base of this motor. The load cells
utilized were straight bar load cells due to the desired mounting
of the motor and the direction of the force due to the wire tension.
The third motor was used for wire take-up onto a final spool for
storage while the annealing process was in progress. Upon
exiting the furnace, the wire was immediately quenched in room-
temperature water using a constantly flowing overhead
quenching shower providing continuous quenching of the wire
after the heat-treatment process.
The annealing process was then specified by the
temperature of the furnace and the time that the wire was in the
thermal chamber. Once manufactured, the CFS allowed for
continuous heat treating of long wire lengths. The entire CFS
can be seen in Figure 4.
Figure 4: Render of the Continuously Fed Nitinol Heat Treating
System
EXPERIMENTAL SETUP
The heat-treating process developed is referred to as
Continuously Fed (CF) heat-treating. This process involves
heating the furnace up to the desired annealing temperature, then
commanding the motor speed and tension. The motor speed was
determined using the desired aging time and the tension was
controlled to 1N for all heat treatments presented in this work.
This allowed for thermal expansion to be neglected during this
process. The tension of 1N was chosen for the because during
the initial heat-treating runs, it was determined that tensions
above 5N led to the wire breaking in the thermal chamber of the
furnace. Due to the novelty of this heat-treating scheme it was
decided that 1N tension would be used and further research could
explore higher tensions. As the wire is fed through the oven, it
is heat-treated continuously and then immediately quenched with
room temperature water to complete the heat treatment process.
During this process the wire was kept straight so the desired
trained shape could be achieved. This system allows for much
more ideal control of the wire’s trained shape, annealing
temperature, and aging time when compared to the conventional
method.
The conventional heat-treating process is referred to as
non-Continuously Fed (non-CF) heat-treating, also known as
conventional heat-treatment. This is the traditional process of
placing the wire in a fixture to hold its desired straight shape and
putting the fixture into the furnace at the desired temperature.
After the desired aging time was reached, the fixture and wire
were removed and then quenched in room temperature water to
complete the heat-treating process. However, this conventional
method has several issues. Opening the door of the furnace
4 Copyright © 2020 by ASME
reduces the temperature significantly and causes the resulting
wire to be trained at a lower than desired temperature.
Additionally, the thermal expansion of the wire is not
appropriately accounted for with the fixture. The conventional
method does not allow for sections larger than the width of the
fixture to be trained making it not suitable for applications
requiring long lengths of heat-treated wire.
Differential Scanning Calorimetry (DSC) analysis was
performed on the heat-treated wire to determine the transition
temperatures of the wire and to determine if any R-phase was
present. The transition temperatures were necessary to
determine the affects the annealing temperatures and aging times
had on the Nitinol wire. It was decided that DSC analysis was
only to be performed on the heat-treated CFS wire since the
change in the transition temperature is a function of the aging
temperature and time [12, 14]. The annealed and aged Nitinol
wire was tested in a DSC machine in accordance to ASTM
F2004-17 [15]. This standard calls for the Nitinol wire to be
precisely cut and placed into a DSC pan between 25 and 45 mg
in mass. The testing procedure began with the sample at 0°C,
heated to 160°C, and then cooled back down to 0°C at a ramp
rate of 10°C/min. The temperatures were chosen to ensure the
sample was cooled to 30°C below the
𝑀
"
and heated 30°C above
the
𝐴"
. The data recorded by the DSC Q2000 includes testing
time, temperature (
), heat flow (mW), and heat capacity (mJ).
This test determined the Nitinol wires’
𝑀!
,
𝑀
"
,
𝐴!
, and
𝐴"
temperatures, as well as if there was any
𝑅!
and
𝑅"
present
(Figure 5).
Figure 5:Example DSC results with construction lines to determine
phase transitions
The tensile testing machine used was an Instron-5560
equipped with a 1kN load cell. The tensile tests were performed
with a grip separation of 150mm and an extension rate of
5mm/min. The data recorded consisted of force and extension
from the initial position using the load cell and crosshead motion
respectively. This was then converted to a stress-strain curve
using the geometry of the treated wire. ASTM F-2516 states that
a class C extensometer should be used for strain measurement
when testing Nitinol wires thicker than 0.2mm; however, at the
time of this testing, this capability was not available [16].
EXPERIMENTS
A tensil e test was performed for the 0.25mm high-
temperature actuator wire at the various annealing temperatures,
aging times, and heat-treatment methods for a total of 30 sample
variations (Tabl e 1).
Ta bl e 1: Annealing temperatures and aging times
Tem p (°C)
Aging Times
(minutes)
Heat-Trea tmen t Sy ste m
400
1, 2, 3
CFS
Conventional
425
1, 2, 3
CFS
Conventional
450
1, 2, 3
CFS
Conventional
475
1, 2, 3
CFS
Conventional
500
1, 2, 3
CFS
Conventional
The range of tested annealing temperatures were
determined after performing an initial tensile test on wire heat-
treated over a range of 350-550°C. Annealing temperature above
500°C (for this specific wire and aging times) resulted in
extremely high yield strains. Wire annealed at 550°C
demonstrated a 40%-50% yield strain and decrease in UTS,
which only occurs if the Nitinol recrystallizes, rendering it
useless for most actuator applications. The annealed wire would
be useful in applications where actuation stroke is more
important than blocking force, however this would be examined
in future work. An example can be seen in Figure 6 for the aging
time of 1 minute; it was determined annealing the wire at
temperatures higher than 500°C would not be included in the
analysis.
Figure 6: Tensile testing results for various annealing temperatures to
include 550C
5 Copyright © 2020 by ASME
Five tensile tests were conducted for each sample
variation, then averaged to determine the stress-strain behavior.
The 400°C annealed wire using the CFS system at the various
aging times were compared to those of the conventional system
(Figure 7). The CFS heat-treated wire demonstrates that as the
aging time is increased, the yield strain and the UTS decreases.
For the conventional heat-treatment system, the yield strain
increases as the aging time increases, but the UTS is random.
However, there is not a drastic difference and therefore, the aging
times at 400°C should be increased.
Figure 7: Tensile testing results for 400C annealed wire at various
aging times
The 425°C annealed wire using the CFS system at the
various aging times were compared to those of the conventional
system (Figure 8). The CFS heat-treated wire demonstrates that
as the aging time is increased, the yield strain and the UTS
decreases. For the conventional heat-treatment system, the yield
strain is almost 3% higher than the CFS wire. The reason for the
higher strain is a result of having to open the door of the furnace
which reduces the temperature significantly and causes the
resulting wire to be trained at a lower than desired temperature
and the thermal expansion of the wire is not appropriately
accounted for with the fixture.
Figure 8: Tensile testing results for 425C annealed wire at various
aging times
The tensile testing results of the CFS heat-treated wire
were then compiled and interpolated using a cubic interpolation
scheme to allow for simple analysis. The yield stress results
show that increasing the aging temperature has an appreciable
effect on the yield strength of the Nitinol wire as seen in Figure
10. As the temperature increases, the tensile strength decreases.
Aging time has a similar effect, albeit less sensitive than the
aging temperature. These results have an intuitive relationship
which shows that the higher the temperature of the Nitinol wire
at the quenching point the lower the yield stress.
Figure 9: Surface showing interpolated yield stress of the aged Nitinol
wires
The yield strain results follow a generally similar trend
to that of the yield strength with respect to the aging temperature
as seen in Figure 10 (i.e. higher temp, lower yield strain).
However, the aging time results are much different. The longer
the wire remains in the thermal chamber before quenching, the
higher the yield strain. These results can be used to “design” the
desired Nitinol properties at yield which would allow easier
implementation of Nitinol in various applications.
Figure 10: Surface showing interpolated yield strain of the aged
Nitinol wires
6 Copyright © 2020 by ASME
RESULTS AND DISCUSSION
The one-minute aging time at various temperatures
using the CFS demonstrate that as the annealing temperature
increases, the strain failure rate and UTS decrease (Figure 11).
This data is extremely consistent when compared to that of the
conventional heat-treatment system.
Figure 11: Tensile testing data for various annealing temperatures at
one-minute aging
The two-minute aging time at various temperatures
using the CFS demonstrate the strain failure rate is slightly lower
at all temperatures than the one-minute aging. Additionally, as
the annealing temperature increases, the strain failure rate and
UTS decrease (Figure 12). This data is extremely consistent
when compared to that of the conventional heat-treatment
system.
Figure 12: Ten s il e t es t in g d at a f or v a ri o us a n ne al i ng t e mp er a tu re s a t
two-minute aging
The three-minute aging time at various temperatures
using the CFS demonstrate the strain failure rate is slightly lower
at all temperatures than the one-minute and two-minute aging.
Additionally, as the annealing temperature increases, the strain
failure rate and UTS decrease (Figure 13). This data is extremely
consistent when compared to that of the conventional heat-
treatment system.
Figure 13: Ten s il e t es t in g d at a f or v a ri o us annealing temperatures at
three-minute aging
Ultimately, it can be concluded that the CFS heat-
treatment system produces extremely consistent stress-strain
curves and follows a pattern throughout. The conventional
system that is used by most produces random data that various at
each temperature and aging time.
DSC Analysis
DSC analysis was conducted on the following
annealing temperatures: 400°C, 425°C, 450°C, 475°C, and
500°C. Each of these temperatures were aged for 1 minute, 2
minutes and 3 minutes and the transition temperatures were
determined. DSC analysis was also performed on the wire with
the 550°C annealing temperature. These results showed that
with an aging time of 3 minutes, the R-phase present in some of
the higher temperatures was no longer present due to the
recrystallization that occurred with these heat-treating
parameters. It can be seen after performing DSC analysis on
the various annealed and aged wire, the transition temperatures
at multiple iterations of tests on the various annealed and aged
wire, the transition temperatures were determined. DSC results
for a 1-minute aging time (Figure 14) show that as the annealing
temperature increased, so did the
𝐴!
and
𝐴"
temperatures. The
𝑀!
and
𝑀
"
temperatures did change; however, this change was
marginal at most and was considered to be insignificant. As
expected, the R-phase was present in the higher temperature
samples beginning at 500°C.
7 Copyright © 2020 by ASME
Figure 14: DSC results for various annealing temperatures with a
1-minute aging time
The DSC results for an aging time of 2 minutes (Figure
15) were broadly similar to the 1-minute aging time. However,
the overall location of the transition temperatures was higher due
to the longer aging time leading to the Nitinol reaching a higher
temperature.
Figure 15: DSC results for various annealing temperatures with a
2-minute aging time
DSC results for a 3-minute age time (Figure 16) while
generally consistent with the previous two age times, the R-
phase is present at lower annealing temperatures. Additionally,
the higher age time resulted in the
𝐴!
and
𝐴"
temperatures having
a larger overall range than the other two age times.
Figure 16: DSC results for various annealing temperatures with a
3-minute aging time
The results of the DSC testing were then compiled and
interpolated using the same scheme as the tensile testing data.
This allows for quick analysis of the whole test matrix (Figure
17). These results show that as the aging temperature increases,
so does
𝐴!
. The same is true for the aging time. This leads to the
conclusion that the higher the temperature at the quenching time
the higher
𝐴!
is.
Figure 17: Surface showing interpolated Austenitic start temperature
of the aged Nitinol wires
Similarly, to
𝐴!
,
𝐴"
also increases as the annealing
temperature and time in the thermal chamber increases (Figure
18). This is because the transition temperatures generally remain
quite close to each other regardless of the aging process. These
results, like the tensile testing results, allow for the “design” of
the properties of the Nitinol wires allowing for easy
implementation of specific properties.
8 Copyright © 2020 by ASME
Figure 18: Surface showing interpolated Austenitic finish temperature
of the aged Nitinol wires
CONCLUSION
In conclusion, the Continuously Fed heat-treatment
System resulted in rapid sample creation at a higher quality heat
treatment than the conventional method: The annealing
temperature was much more consistent throughout the heat-
treating process. Precise speed control of the wire allowed for
the annealing time to be more accurate for each sample. Ten sion
control of the wire allowed for the thermal expansion of the
Nitinol to be all but neglected as the system actively changes the
wire tension as the material expands. Additionally, the tension
control removed the need for the manufacturing of a fixture
which, if poorly manufactured, could lead to incorrectly trained
shapes after heat treating. The continuous quenching system
placed after the exit of the furnace made the transition between
the heated wire and the cooled wire much faster than the
conventional method. All of these contributed to improved
sample consistency. The tensile testing data shows that the CFS
had overall much lower strain at failure that is more consistent
with trained wire produced by manufacturers (with the exception
of the lower annealing temperatures, which if aged for longer
would likely produce results more similar to the higher annealing
temperatures). DSC results showed that the novel heat treatment
process was consistent with those of previous researchers. Being
able to create long sections of straight trained wire allows for
Nitinol wires to be used on much larger applications for a much
lower cost as the user is no longer limited by the size of their
furnace. In future work, different tension on the heat-treated
wire will be utilized to determine if the tension affects the overall
functional properties of the wire. Additionally, different
diameter wire will be utilized, and multiple stage heat-treatments
will be performed. These results will then be compared to the
conventional heat-treatment wire as well as the single stage
continuously fed wire.
REFERENCES
[1]
S. e. Cai, "Effect of heat treatment temperature on nitinol
wire," Applied Physics Letters, vol. 105, pp. 105-109,
2014.
[2]
A. Skalitzky, A. Gurley, D. Beale and K. Kubik, "Design
and Analysis of SMA Woven Fabric," Smart Marterials,
Adaptive Structures, and Intelligent Systems, vol. 8206,
pp. 1-8, 2018.
[3]
J. Eaton-Evans, J. M. Dulieu-Barton, E. Little and I. A.
Brown, "Observations during mechanical testing of
Nitinol," J. Mechanical Engineering Science, vol. 222, no.
Part C, pp. 97-105, 2008.
[4]
M. Drexel, G. Selvaduray and A. Pelton, "The Effects of
Cold Work and Heat Treatment on the Properties of Nitinol
Wire," in International Conference on Shape Memory and
Superelastic Technologies, Pacific Grove, 2006.
[5]
J. Shaw, C. Churchill and M. Iadicola, "Tips and Tricks for
Characterizing Shape Memory Alloy Wire - Part 1 -
Differential Scanning Calorimetry and Basic Phenomena,"
Experimental Characterization of Active Materials Series,
pp. 55-62, 2008.
[6]
S. Yoon and D. Yeo, "Phase Transfromations of Nitinol
Shape Memory Alloy by Varying with Annealing Heat
Treatment Conditions," in Smart Materials, Nano-, and
Micro-Smart Systems, Sydney, 2004.
[7]
T. Duer ig an d A. Pelton, "Ti -Ni Shape Memory Alloys,"
Materials Properties Handbook: Titanium Alloys, vol. 1,
pp. 1035-1048, 1994.
[8]
W. H u an g a n d W. T oh , " Tr a in in g tw o-way shape memory
alloy by reheat treatment," Journal of Materials Science
Letters, vol. 19, pp. 1549-1550, 2000.
[9]
J. Fuentes, G. P and J. Strittmatter, "Phase change behavior
of nitinol shape memory alloys: Influence of heat and
thermomechnical treatments," Advanced Engineering
Materials, vol. 4, pp. 437-451, 2002.
[10]
K. e. a. Gall, "The influence of aging on critical
transformaton stress levels and martensite start
temperatures in NiTi: part II," Engineering Material
Te ch no l og y, vol. 121, pp. 28-37, 1999.
[11]
D. Miller and D. Lagoudas, "Influence of cold work and
heat treatment on the shape memory effect and plastic
strain development of NiTi," Materials Science and
Engineering, vol. A308, pp. 161-175, 2001.
[12]
M. Losertova, M. Stencek, D. Matysek, O. Stefek and J.
Drapala, "Microstructure evolution of heat treated NiTi
alloys," in 27th Joint Seminar Development of Materials
Science in Research and Education, Ostrava-Poruba,
2017.
[13]
H. Sadiq, M. Wong, R. Al-Mahaidi and X. Zhao, "The
effects of heat treatment on the recovery stresses of shape
9 Copyright © 2020 by ASME
memory alloys," Smart Materials and Structures,
vol. 19,
pp. 1-7, 2010.
[14]
G. e. a. Eggeler, "On the effect of aging on martensite
transformations in Ni-ri
ch NiTi shape memory alloys,"
Smart Marterials and Structures, vol. 14, pp. 186-
191,
2005.
[15]
A. F2004-17, "Standard Test Method for Transformation
Tem pe rat ur e of Nickel-Titanium Alloys by Thermal
Analysis," 2017. [Online]. Available:
https://doi.org/10.1520/F2004-17. [Accessed 1 September
2018].
[16]
A. F2516-18, "Standard Test Method for Tension Testing
of Nickel-Titanium Superelastic Materials," 2018.
[Online]. Available: https://compass-astm-
org.spot.lib.auburn.edu/EDIT/html_annot.cgi?F2516+18.
[Accessed 5 March 2020].
... Both forward and reverse transformations are associated with latent heat release and absorption, respectively. Full-field measurement methods, such as Infra-Red Thermography (IRT) and Digital Image Correlation (DIC), can provide quantitative information about the temperature and displacement, respectively, at each point on the surface [18,19]. martensite, as well as the reverse transformation (martensite to austenite) [13]. ...
... Both forward and reverse transformations are associated with latent heat release and absorption, respectively. Full-field measurement methods, such as Infra-Red Thermography (IRT) and Digital Image Correlation (DIC), can provide quantitative information about the temperature and displacement, respectively, at each point on the surface [18,19]. -maximum longitudinal strain; -stress to start martensitic transformation (austenite to single-variant martensite); -stress at finish of martensitic transformation; -stress to start reverse transformation (single-variant martensite to austenite); -stress at finish of reverse transformation; -martensite yield stress; ℎ -martensite hardening parameter. ...
Article
Full-text available
Nitinol (NiTi) alloys are gaining extensive attention due to their excellent mechanical, superelasticity, and biocompatibility properties. It is difficult to model the complex mechanical behavior of NiTi alloys due to the solid-state diffusionless phase transformations, and the differing elasticity and plasticity presenting from these two phases. In this work, an Auricchio finite element (FE) model was used to model the mechanical behavior of superelastic NiTi and was validated with experimental data from literature. A Representative Volume Element (RVE) was used to simulate the NiTi microstructure, and a microscale study was performed to understand how the evolution of martensite phase from austenite affects the response of the material upon loading. Laser Powder Bed Fusion (L-PBF) is an effective way to build complex NiTi components. Porosity being one of the major defects in Laser Powder Bed Fusion (L-PBF) processes, the model was used to correlate the macroscale effect of porosity (1.4–83.4%) with structural stiffness, dissipated energy during phase transformations, and damping properties. The results collectively summarize the effectiveness of the Auricchio model and show that this model can aid engineers to plan NiTi processing and operational parameters, for example for heat pump, medical implant, actuator, and shock absorption applications.
... FEA can simulate complex geometries both with internal and external structures. A considerable amount of work on investigating and mechanical response of NiTi wires, actuator springs, and stents is noted in the literature [12,32] One dimensional j o u r n a l o f m a t e r i a l s r e s e a r c h a n d t e c h n o l o g y 2 0 2 3 ; 2 5 : 3 2 5 8 e3 2 7 2 also been performed on investigating the mechanical and functional response of NiTi [19,33e35]. Additive manufacturing has enabled the manufacturing of complex and near-net-shaped lattice structures. ...
Article
Full-text available
The additive manufacturing (AM) of nitinol (NiTi) has gained considerable attention due to the capability of this material and processing combination to produce complex structures with desired shape memory or superelastic properties. Finite element analysis models were developed in this work to simulate the load-bearing capability of Laser Powder Bed Fusion (PBF-LB) produced NiTi lattice structures. The Auricchio numerical method, with exponential hardening law, was implemented within the FEA model to take account of the martensite-austenite reorientation upon change of stress state. The strut diameter and the unit cell side length were varied which in turn varied the lattice relative density. The lattice structures were subjected to 7 % compressive strain under isothermal conditions. The highest energy absorption efficiency of 40 % was achieved from the lattice structure with a strut diameter of 2 mm, a 6 mm unit cell side length, and a relative density of 42 %; however, the highest specific peak stress was recorded within the lattice structure having a strut diameter of 2.5 mm, a 4 mm unit cell side length, and a relative density of 62 %. Transient analysis was performed by varying the compression rate from 0.25 mm/s to 1 mm/s. For all loading conditions, the energy absorption increased linearly until a stable stress plateau was reached. Moreover, for these examined compression rates, the maximum stress absorption efficiencies varied within the range of 25 %–33 %.
... This is associated with low hardening, and the lattice transforms completely into martensite. The crystalline phase of detwinned martensite occurs at lower temperatures and higher stresses, whereas the crystallization of austenite occurs at higher temperatures and lower stresses [7]. As seen in Fig. 1, when the material is deformed at constant (room) temperature, initially it follows the Hooke's law with the stiffness (EA) as that of the austenite phase. ...
Article
Full-text available
Over the recent years, Nitinol (Ni-Ti) shape memory alloys have gained popularity in the medical, aerospace and energy sectors, due to their superelasticity, shape memory effect, low stiffness, good biocompatibility and corrosion resistance. Compared to steels and other common metallic materials, it is difficult to model the mechanical behavior of Ni-Ti due to the inherent functional properties caused by the diffusion-less solid-state phase transformations. With the help of Laser Powder Bed Fusion (L-PBF) process, these transformational characteristics can be controlled. This will ultimately lead to controlling the mechanical and thermal properties for specific applications. In this work, Finite Element Analysis (FEA) was conducted to replicate the actual mechanical phenomenon occurring in Nitinol. Models were generated for simulating the superelastic and plastic behaviors, and were validated against actual experimental data. The ability to model the complex mechanical response of Nitinol will enable exploration into the sensitivity of material response to phase volumes, material composition, and strain rate. Robust models of these phenomenal also provide the potential for tailoring in-silico the microstructure required for specified desired macroscopic material properties.
Article
Advancements in e-textiles, sensors, and actuators have propelled wearable technologies toward wide-spread market use, however the physical interface between these technologies and the human body has remained a functional challenge. Prior research has found that system-body interface challenges produce wearing variability, or variation in system placement, orientation, and tightness in relation to a body both between use trials and between users, resulting in large variation and deterioration in system performance. We break down the mechanics of common system-body interface challenges through a summary of design principles critical to any system interfacing with the human body. Additionally, we present an active interface based on shape memory materials that dimensionally adapts to its user's dimensions. An experimental investigation of these active system interfaces considers the impact of design variables often overlooked in the design process. Recommendations are provided to optimize interfaces for the requirements for a given wearable technology. Additionally, we illuminate methods to reduce wearing variability for a range of users to produce consistent system-body interaction across a user population. Through these active interfaces, we advance a broad range of wearable technologies, including wearable sensing, motion tracking, haptics, and wearable robotic devices.
Article
This work reexamines traditional shape memory alloy (SMA) loading paths commonly used in SMA-based actuator applications and presents a novel, superimposed condition in which SMA generates substantial forces upon heating and cooling. This atypical effect, which is investigated with a textile-based actuator, was found to be prominent at the completion of material phase transformation, at which point thermal expansion/contraction became the dominant force-generating mechanism. We demonstrate that amplification of generated forces can be accomplished by varying the applied thermal load, applied structural strain, as well as actuator architecture. Specifically, we present SMA knitted actuators as an actuator architecture that increases the effect by aggregating SMA wires within a complex strain profile-effectively providing a larger operational window for the effect to propagate. The amplification of blocking forces through this novel operational procedure suggests reconsidering traditional blocking force design paradigms and opens untapped actuator application spaces, such as the highlighted medical and aerospace wearable technologies.
Conference Paper
Full-text available
Shape Memory Alloys (SMAs) are often used for robotic, biomedical, and aerospace applications because of their unique ability to undergo large amounts of stress and strain during thermomechanical loading compared to traditional metals. While SMAs such as NiTi have been used in wire, plate, and tubular forms, NiTi as a woven dry fabric has yet to be analyzed for use as protective materials and actuators. Applications of SMA fabric as a “passive” material include shields, seatbelts, watchbands and window screens. Applications as an “active” material include robotic actuators, wearable medical and therapy devices, and self-healing shields and screens. This paper applies a macro-mechanical model from composites analysis to NiTi plain woven fabric to determine the effective elastic constants. The fabric model is based on actual weave geometry, including the presence of open gaps and wire cross-sectional area, and with the same diameter and alloy in the warp and weft. A woven NiTi ribbon has been manufactured (Figure 1) using a narrow weaving machine and has been tested in uniaxial tension. Planar fabric constants were measured at a range of temperatures. The analytically and experimentally derived constants for various weave patterns and cover factor combinations are presented and compared. It was determined that in uniaxial tension the fabric behaves like a collection of unidirectional wires, but has 78% of the rigidity, on average, across all test temperatures. This result is predicted by the fabric model with a 16% error, demonstrating that the proposed analytical model offers a useful tool for design and simulation of SMA fabrics.
Article
Full-text available
Superelastic behavior of off-stoichiometric NiTi alloys is significantly affected by microstructure changes due to heat treatment. Applying appropriate thermal treatments important effects on microstructural changes, transformation temperatures and thermomechanical properties of final NiTi products can be achieved. The experimental samples of NiTi alloy with 55.8 wt.% Ni were submitted to heat treatment and the microstructures before and after the treatment were observed. The thermal regimes consisted of annealing treatment at 600 °C for 1 hour followed by water quenching and of ageing at eight different temperatures (250, 270, 290, 300, 350, 400, 450 and 500 °C) for 30 minutes. Microstructure features studied by means of optical and scanning electron microscopies, EDX microanalyses, X-ray diffraction analyses and microhardness measurement, have shown that higher ageing temperatures led to microstructure changes and corresponding increase in microhardness.
Conference Paper
Full-text available
Shape memory and superelastic capabilities coupled with good biocompatibility give Nitinol the ability to provide functionality seldom possible with traditional engineering alloys. In this study the effect of heat treatments of 300 ∼ 550°C for 2 ∼ 180 minutes on Ti-50.8%Ni (at.%) wire of 30% and 50% cold work was investigated. Transformational and mechanical properties were characterized through the bend and free recovery (BFR) method and tensile testing. Thermally activated precipitation and annealing processes occurred. Annealing processes tended to increase the slope and the total strain recovery of the BFR plots. Two TTT diagrams were constructed illustrating the trends in the Austenite Finish Temperature (Af ) of the wires. A maximum precipitation rate occurred at approximately 450°C. Precipitation strengthening was evident in both 30% and 50% cold-worked wires. However, only in the former did an increase in UTS occur. Recrystallization began at approximately 450°C for both wires.
Article
Full-text available
In-situ synchrotron X-ray diffraction has been used to study the influence of the heat treatment temperature on the subsequent micromechanical behavior of nitinol wire. It was found that increase in the heat treatment temperature rotated the austenite texture from the {332}B2 fiber towards the {111}B2 fiber, and the texture of the Stress-Induced Martensite phase changed from the ( 1¯40)B19' to the ( 1¯20)B19' fiber accordingly. Heat treatment at a low temperature reduces the internal residual strains in the austenite during super-elastic deformation and therefore improves the materials fatigue performance. The development of internal residual strains in austenite is controlled by transformation induced plasticity and the reversal martensite to austenite transformation.
Article
Full-text available
We investigate the effect of 450 °C aging on the microstructure and on the martensitic transformations in a Ni-rich (50.8 at.% Ni) NiTi shape memory alloy using transmission electron microscopy (TEM), x-ray diffraction (XRD), neutron diffraction (ND) and differential scanning calorimetry (DSC). On cooling from the high temperature phase, DSC charts show two distinct peaks after short aging times, three peaks after intermediate aging times and two peaks again after long aging times (2–3–2 transformation behaviour). After 1.5 h 450 °C aging, three DSC peaks were obtained on cooling from the high temperature phase. The first peak on cooling represents the formation of R-phase and the second peak is associated with the formation of B19'. Due to a macroscopic microstructural heterogeneity a second B19' peak (overall third peak) occurs at lower temperatures. We discuss our results in the light of recent remarks on burst-like events during the growth of thermoelastic martensite and on the effect of oxidation on NiTi microstructures.
Article
Full-text available
The influence of annealing temperatures on the thermo-mechanical behavior of NiTi alloy in terms of transformation temperatures, mechanical properties at ambient temperature and the recovery stress under constrained end conditions were investigated experimentally. An attempt is made to correlate results obtained from the DSC test and tensile test at room temperature with results from recovery stresses at elevated temperatures. It is found that annealing the alloy above the recrystallization temperature (600 °C) reduces the maximum recovery stress significantly, even though the alloy still exhibits thermal transformations and a stress-induced martensite plateau at an annealing temperature above 600 °C. A pre-strained amount above approximately 2.4% strain is sufficient to achieve the maximum recovery stress at constrained end conditions. It is recommended that the alloy used in this study be annealed at temperatures below 450 °C in order to produce the desired thermo-mechanical properties in the alloy for applications that exploit the shape memory effect.
Article
Phase transformations and crystal structures of nitinol shape memory alloy are investigated by varying with heat treatment conditions through DSC (differential scanning calorimetry) and XRD (X-ray diffraction). Heat treatment conditions are considered as heat treated times of 5min, 15min, 30min, and 45min as well as heat treated temperatures of 400°C, 500°C, 525°C, 550°C, 575°C, 600°C, 700°C, 800°C, and 900°C. In addition, tensile tests are conducted to investigate thermomechanical behaviors of nitinol shape memory alloy through material testing system by varying with heat treated temperatures and environmental temperatures. According to these results, heat treatment conditions are found to be significantly affected on phase transformations, crystal structures, and thermomechanical behaviors of nitinol shape memory alloy.
Article
Superelastic and shape memory capabilities of Nitinol are strongly dependent on the alloy composition, its heat treatment, and mechanical deformation history. The current article presents a review of the behaviour of Nitinol and describes a characterization study conducted to determine the mechanical properties of the material, both by means of differential scanning calorimetry (DSC) and by mechanical testing at a range of temperatures. Values for key transformation temperatures are found using both techniques. It is concluded that mechanical deformation during sample preparation for DSC measurements may have led to material property modifications and hence erroneous phase transformation temperature values. It is shown that mechanical testing can provide a means of benchmarking DSC data.
Article
An experimental study was performed to determine the effect of aging on martensitic transformations in NiTi. Polycrystalline and single crystal NiTi ([100], [110], and [111] orientations) were both considered. Stress-induced transformations in single crystals of the [110] and [111] orientations. Solutionized and over-aged single crystals exhibited a strong orientation dependence of the critical stress required to trigger the transformation, {sigma}{sub cr}. The Schmid law was able to accurately predict the orientation dependence of {sigma}{sub cr} in the solutionized and over-aged single crystals. Peak-aged single crystals demonstrated a much weaker orientation dependence of {sigma}{sub cr} and in general, the Schmid law was not obeyed. By considering the local stress fields outside of the semi-coherent precipitates, the decrease in the orientation dependence of {sigma}{sub cr} was accounted for. The martensite start temperatures, M{sub s}, in aged single crystal and polycrystalline NiTi were much higher than in solutionized samples. In peak-aged NiTi the increase was primarily attributed to the local stress fields outside the coherent precipitates which create preferential nucleation sites for the martensite. In the over-aged NiTi the increase in M{sub s} was primarily attributed to the decrease in the average Ni concentration of the matrix surrounding the coarsened precipitates.