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Ductility - Science topic

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Ductility curve tells the susceptibility of a material towards solidification cracking. The slope of the curve is expressed in terms of Critical strain rate for temperature drop but the curve is between strain vs temperature. Why is it so ?
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Hi Ravi,
(No need to call me sir).
Yes, you really only need to concentrate on the value of ductility at each temperature in terms of strain. This should be compared to the level of strain in the material as it cools. If the applied strain is greater than the ductility, the material will tear.
Best wishes,
Simon
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hi. i am trying to emulate a simulation on ballistic impact on gelatin block. i use regular steps usually used for impacts. but something is off.
each time impact occurs, there is a great stress and cavity in the impact face. but after the first few elements, it appears as if the ball just goes through the block with no effect. the PEEQ visualization doesn't even show any number (all 0 blue) despite obvious deformation. the article and project both assume block as linear plastic-elastic
what is going wrong?
settings:
_Step:
dynamic explicit step with mass scaling of 10000 (computation time is still slow)
_Interaction:
general contact with friction coeff 0.2 and normal hard contact (0 friction and no normal were tested too). surface to surface always gave errors
ball is constraint to a RP in its center as rigid body (coupling always gave errors and kept ball in place. as if locking it)
_Assembly:
nothing important. no constraints there.
_Property:
density and isotropic elastic
ductile damage with evolution.
plastic strain ( rate dependent Johnson-cook and isotropic were both tried)
hyper-elastic would give errors if used with plastic
_Mesh:
more fine element in the impact zone, with explicit linear setting. hourglass was tested on viscous, enhanced and default. deletion is on.
_Load:
pre-defined field of velocity in initial step towards block face
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The issue likely arises from incorrect material parameters (e.g., yield stress too high), insufficient mesh refinement in the impact zone, overly high mass scaling (causing unrealistic dynamics), or improper contact settings (e.g., inadequate stiffness or alignment). Verify material plasticity parameters, refine the mesh, reduce mass scaling, and ensure contact interactions are correctly defined.
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Is there any specific relationship between elongation percentage and dimple size during ductile failure?
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There is no simple linear relationship between elongation percentage and dimple size during ductile failure, but some general trends can be observed:
  1. Larger dimple sizes are often associated with higher ductility and elongation. Materials with higher ductility tend to form larger, deeper dimples on the fracture surface due to more extensive plastic deformation before fracture.
  2. The relationship is complex and influenced by multiple factors:
  • Temperature: Higher temperatures generally lead to increased ductility and larger dimple sizes
  • Microstructure: Finer microstructures typically result in smaller dimples but may contribute to higher overall ductility
  • Strain rate: Higher strain rates may lead to smaller dimples and potentially lower ductility
3- Dimple size distribution is often asymmetric, with many small dimples and fewer large ones, complicating the analysis
4- As elongation increases, dimples tend to become more elongated rather than simply larger
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I would like to know how chemical composition for a low carbon steel allow will effect the DBTT behavior? Which elements determine ductile or brittle fracture based on their weight percent. Any literature reference
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The DBTT of low carbon steel is influenced by both the carbon content and the presence of alloying elements or impurities. Elements like manganese and nickel can lower the DBTT and improve toughness, while higher levels of carbon, phosphorus, sulfur, and oxygen tend to raise it, making the steel more brittle at lower temperatures. The following studies may be helpful: https://doi.org/10.1007/s11223-019-00075-8; https://doi.org/10.3390/ma14071634; https://doi.org/10.1007/s12540-021-01053-z; The effect of chemical composition on the DBTT in low-carbon steel alloys plays a decisive role in determining the microstructure of the material. Generally, low-carbon steels exhibit a ferrite-pearlite microstructure, and refining the grain size can lower the DBTT, thereby improving impact toughness. For instance, a finer grain structure significantly enhances resistance to brittleness. This phenomenon can be explained by the Hall-Petch relationship, which states that as grain size decreases, the material's yield strength increases, and the fracture stress rises accordingly. Additionally, the inclusion of elements like aluminum or manganese in the chemical composition of low-carbon steels also affects the DBTT. For example, an increase in manganese content enhances the ductility of the steel, lowering the transition temperature. The addition of aluminum can further reduce the DBTT in ferritic structures, improving the material's thermal resilience. These factors can be optimized according to the steel's intended applications and required strength characteristics.
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Which is better: a DBTT as a point or as a temperature range? What factors affect it?
Based on my research, I noticed that the DBTT of some aluminide coatings is a point, while for others, the hardness gradually reduces as temperature increases, resulting in a DBTT that spans a range. I want to analyze the factors that cause this effect and understand Which type is better for service applications?
In some Ni-aluminide samples with a DBTT at a specific point, the hardness of the specimen increases before reaching the DBTT. How can this fact be explained? Is there a relationship between having a DBTT at a specific point and the observed increase in hardness before it?
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I found these results for Ni aluminide coating, I was wondering if you provide some similar for Fe-aluminide and Ti-aluminide coatings. Thank you
Why does NiAl's strength increase before the DBTT?
This occurs due to stoichiometry deviations and aluminum consumption during oxidation, which harden the material.
Is the DBTT of Ni-aluminides a point?
For NiAl, the DBTT is around 760°C but can vary due to factors like stoichiometry deviations, strain rate, grain boundary strengthening, and the solubility of elements like Cr.
What improves ductility at the DBTT—slip systems or dislocations?
In Ni-Aluminide coating, Ductility improvement at the DBTT is linked to dislocation movement, particularly (100) dislocations. The activation energy for the ductile-to-brittle transition is tied to vacancy diffusion, where vacancy movement influences the material's behavior. Additionally, some researchers suggest that the DBTT is more of a phase transition than simple thermal activation, as it also relates to stress handling at grain boundaries.
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Hello
I want to verification low cyclic fatigue in a bar under cyclic load.
Is the fracture strain different in uniaxial and cyclic loading?
In my model, damage starts when the PEEQ reaches the fracture strain, and the bar fails at a very low number of cycles compared to the experimental test.
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The PEEQ values for monotonic and cyclic loading will undoubtedly differ. In cyclic loading, plastic strain accumulation is generally higher, as it depends largely on the number of cycles endured and the specific loading protocol. In contrast, for monotonic loading, PEEQ may be relatively lower, since the specimen isn't subjected to reversed loading. This could explain why your numerical model shows premature failure compared to the experimental data. For more insights into PEEQ (at fracture) variation under different stress states in mild steel subjected to monotonic loading, you may refer to our article: https://doi.org/10.1016/j.engfracmech.2023.109638.
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How do these effects change when the surface layer becomes ductile at high temperature?
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CYS remains virtually unchanged when small surface cracks appear in the material, whereas YS can decrease several times.
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In nanocrystalline metals, the size of their crystalline grains affects how strong, ductile, and hard they are. Smaller grains often mean stronger metals but can reduce ductility. Controlling grain size during manufacturing could help optimize these properties for specific applications.
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Hello,
- Regarding strength, we have two different cases depending on the grain size:
1- Hall-Petch Relationship: This relationship states that as the grain size decreases, the strength and hardness of the metal increase. This is because grain boundaries act as barriers to dislocation motion, making it harder for the material to deform.
2- Inverse Hall-Petch Breakdown: At extremely small grain sizes (typically below 10-15 nm), the strengthening effect can reverse. This is due to mechanisms like grain boundary sliding becoming more prominent, leading to softening.
- Concerning ductility, nanocrystalline metals can become more brittle because there are fewer dislocations within the grains to allow for plastic deformation.
- To make a balance between strength and ductility, having a bimodal grain size distribution could be a solution, with both small (for example, 10-20 nm) and slightly larger grains (more than 100 nm up to 1-2 µm). This can improve ductility while maintaining high strength. The very small grains contribute significantly to the strength of the material due to the Hall-Petch effect while the slightly larger grains enhance ductility by providing pathways for dislocation movement and accommodating more plastic deformation without leading to premature failure.
Hope this helps.
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Where is the interface energy G_c set for the ductile damage model in DAMASK3.0-alpha3? I have seen the critical energy release rate or interface energy G_c in almost all DAMASK damage models, but the anisotropic brittle model and the toughness model only have the settings of critical load g_crit and critical displacement s_crit? And what is the function of the parameter damage diffusion D?
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Hello,
I'm employing a ductile damage model in Abaqus, but there's a possibility of two failure modes: crack formation or localized buckling. While I've been able to detect cracking failures in some cases, I haven't observed any instances of buckling failure in others. Given the complexity of the model, I've opted for the explicit solver in Abaqus. I'm curious if the explicit solver can accurately predict local buckling failures.
Thank you
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Your explicit simulation will give you the dynamic response. If you simulate a quasi-static process in a severly reduced time(and thus a much higher loading rate), it's quite possible that you delay or prevent buckling phenomena.
I'd recommend running the simulation with a linear elastic material and check if you will eventually see some buckling. If nothing happens, try to apply the load more slowly (or reduce the mass scaling, if you used that).
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I have fabricated chitosan acetate films and exploring their TS, Young's modulus and percent elongation/ductility. But they have shown a fluctuating trends. Generally it has been said that with the increasing TS value the ductility have shown a decreasing trend and vice-versa regarding the subjected samples. Though there is a very irragular relationship between the TS and Young’s modulus. But I am verymuch confused about the unexpected behaviour of the considered biopolymeric samples like chitosan-acetate films regarding the TS, Young's modulus and ductility. Therefore, if you are an expert in this particular field please justify the reason behind the seance.
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Thanks to all for your valuable comments
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I saw there are isoductile and anisoductile damage types in damask 2.0, what are their counterparts in damask 3.0. If I want to simulate the ductile damage of aluminum, how can I set it up in the material file of damask 3.0?
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Not sure which alpha version you are using:
For alpha-8:
import damask
g = damask.GeomGrid.load('Polycrystal.vti')'
g.initial_conditions['phi'] = 1.0 # assuming none of the points are damaged (pristine material), you can obviously change that.
g.save('Polycrystal.vti')
For alpha-7:
import damask
g = damask.Grid.load('Polycrystal.vti')'
g.initial_conditions['phi'] = 1.0 # assuming none of the points are damaged (pristine material), you can obviously change that.
g.save('Polycrystal.vti')
Hope this helps!
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I am working on a project in openLCA using the ecoinvent database and need to enter data for a 500mm ductile iron pipe. The necessary life cycle inventory information for this pipe is available in another database - ozlc2019. How can I utilize the ductile iron pipe data from ozlc2019 in my ecoinvent project in openLCA?
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I see two solutions: first you calculate a the results in ozlc2019 database for the ductile iron pipe only then a) either try to export, than import it to ecoinvent or b) create a spreadsheet where you can combine the results of the two calculations. By the way it is not recommended to use separate databases because they might have profound underlying modeling differences which makes the data incompatible. I rather try to remodel the pipe production process in ecoinvent than trying to import something ffrom another database to it...
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Hi,
I am interested in performing crack initiation and propagation analysis considering high-temperature creep for metals using Abaqus. I know that Abaqus has creep analysis capability with Abaqus/standard and damage modeling capability for ductile metals. However, after defining creep in the material card, I am not able to use ductile damage initiation and evolution anymore.
The error I got was:
"The option *damage initiation, criterion=shear cannot be used in conjunction with *creep"
My question on this matter is three-fold:
1) Is there any Abaqus built-in way to model creep + damage?
2) why is creep analysis not implemented in Abaqus/explicit? Is it because of computational accuracy or efficiency?
3) if there is no built-in models, what is the best way to move forward. Should I consider writing a UMAT/VUMAT subroutine considering both creep and failure, or write a CREEP subroutine and link it to a UMAT/VUMAT failure subroutine?
Thanks,
Shiyao
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Hi Shiyao,
I believe you need to use CREEP subroutine in which you can define the creep constitutive equations (depending on which creep model you want to use). You can also include creep damage equations in the subroutine.
I believe ABAQUS only accept one subroutine file, so creep and damage have to be in the same subroutine file.
Regards,
Wu
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Hello all, I am trying to implement Lemaitre ductile damage model through user material subroutine VUMAT. I have coded all the necessary algorithm in subroutine VUMAT. when i submitted the job, its complited successfully . but it shows: ERROR in job messaging system: Error in connection to analysis
i have tried also to run it from abaqus command line prompt and it shows : system error code 3
could you help me please ? i'am using abaqus 2017 linked with visual studio ultimate 2013 update 5 +intel parallel studio 2017 update 2
thank you
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Hi, usually, this problem occurs when I switch on the wifi or internet connections. As I remember, some parameters of ipv6 should be changed.
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I have a four-story steel structure
When conducting a pushover analysis and examining the results, the structure's ductility ratio at the performance point did not exceed 1, and the equivalent damping remained at 5% according to the FEMA400 EL method.
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The main problem is with ETABS algorithm which can not consider and draw bi-linear curve truly. Take your curve and use excel to draw bi-linear curve instead of drawing it in SAP or ETABS.
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I'm working on alumina coating on GGG40 ductile iron. I use the dip coating technique for coating. The solution contains ethanol, distilled water, aluminum chloride, and ammonium. The gel coats steel well but some oxidation problem occurs on iron. I'm guessing it is about Cl but I couldn't fix it. Do you have any ideas?
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I do know what your purpose is.
I think if you could dip coat of pure Al on iron and then oxidate the Al coat to form Al2O3.
Dip coat of Al will not envole water, Cl, whic would lead to iron corrision.
This is a guess.
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hello,
I am doing Pushover analysis of a G+15 Storied building by ETABS Software. I want to check the structural ductility according to FEMA 440 and level of structural performance according to ATC-40 of this building. I would very grateful if anyone share calculation process by using ETABS software Results.
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Here are the steps to check structural ductility and performance level according to FEMA 440 and ATC-40 using ETABs results for a G+15 building pushover analysis:
Run pushover analysis in ETABS up to the target displacement. Make sure to record base shear and roof displacement at each analysis step.
Plot the pushover curve of base shear vs roof displacement. From this curve, determine the yield and ultimate displacement (Δy and Δu).
Calculate ductility factor μ as Δu/Δy.
Check ductility requirements for seismic force-resisting systems according to FEMA 440 Table C2-3. Requirement is ductility factor μ ≥ 2 for Special Moment Frames.
Determine performance point as the intersection of demand curve with design spectrum. Note the spectral displacement SD1 and acceleration SA1.
Calculate post-yield stiffness degradation index Iγ using equation from FEMA 440.
Plot Iγ vs ductility factor μ on ATC-40 Figure 6.2-1 graph. Read off the expected performance level.
Cross check performance level does not exceed the Collapse Prevention (CP) level for Life Safety objective as per ATC-40 Section 6.4.1.
Tabulate results including pushover curves, μ, Iγ values and determined performance level for reporting.
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I'm modeling an over-reinforced concrete beam using CDP for a 4-point bending test in ABAQUS, and I'm encountering some unexpected behavior. As it's an over-reinforced concrete, I expect to see brittle failure, with the concrete crushing at the top mid-portion, followed by a sudden drop in load on the load-displacement curve. However, what I'm observing is quite different.
I've conducted both load-controlled and displacement-controlled tests, and regardless of the approach, I'm seeing compressive stresses (S33, von Mises, and others) at and near the load points and boundary restraints significantly higher than the ultimate compressive strength of the concrete (as can be seen in the attached screenshot). I've even checked the stresses at integration points using the probe value function, and they still show stress levels above the concrete's ultimate compressive strength
I've tried different mesh sizes and element types, but these changes haven't had a substantial impact. Because of this issue, IMO I'm unable to achieve the brittle failure I expected, as the concrete compressive stresses never seem to reach the ultimate compressive strength at the top mid-portion. Instead, I'm getting ductile failure with reinforcement yielding especially the top reinforcement yielding at the location of the load points.
Has anyone encountered a similar problem or have any suggestions on how to address this issue and obtain the desired brittle failure behavior in my simulation?
Any help will be greatly appreciated.
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If the top reinforcement is equal to bottom reinforcement then this will act as steel beam and this typical behaviour can be experienced
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article with my own views on construction and earthquake.
For me the way seismic loads are transmitted onto the reinforced concrete building structure is as follows.
1. Ground acceleration.
2. Mass inertia.
3. Base ternosity
4. Torque. Torque when applied to elastic columns, shows a different behaviour than if applied to walls, and different if applied to rigid near walls with high dynamics. That is, it has a different coefficient of behaviour q. in terms of ductility, base shear, structural dynamics and capacity in elastic displacement before it exhibits leakage.
A stiff wall has high dynamic and low ductility and is more difficult to fail than an elastic substructure. It still triples the loads it takes down to the base, but due to a larger cross-section the loads received by the elongated wall are less.
A large part of the earthquake behaviour of the structure also has to do with the shape of its faces. Modern architectural needs call for buildings with high ceilings and large openings and a reduction in the number of load-bearing elements. That is, they require non-framed structures made of columns which have a different behaviour and do not show large torsional deformations.
The moment if applied to columns has the following behaviour. It does not download large moments to the base, it consumes energy due to elastic behaviour, and stores energy in the frame which is discharged in the other direction in the next loading cycle. But it has no momentum.
If the torque is applied to stiff near-walls with high momentum and the acceleration is high, then it puts too much torque on the base, which is impossible to be absorbed by the connecting beams which it breaks.
If the torque is applied to stiff near walls with high momentum and the acceleration is large, then it downloads too large a moment to the base, which can be absorbed by the basement walls.
If the acceleration is too large the basement walls do pick up the moment, but there is little or a large withdrawal of the entire footprint of the building.
At this stage we have lost the support of much of the building's base from the foundation soil, and the static loads are left unsupported and their weight force creates an opposing moment to the building's overturning moment.
This can result in the following effects. a) The basement walls and the stiff wall cross-section may be able to take up these loads of the counter-rotating moments and the foundation may experience from a slight recoil to total overturning.
And b) shear failure of one of the two cross-sections, the one that is weaker.
The patent does what it does in this situation.
It presses the structure into the ground so that the moments are taken up by the ground preventing them from transferring to the basement walls.
But this would create a vulnerable rigid superstructure wall which would fail by shear failure for many reasons.
Firstly it would fail the concrete overlay by shear failure due to the over tensile strength of the steel in tension and the low shear strength of the concrete which develops at the concrete-steel interface in the mechanism of aggregation.
Second, in the mechanism of ''congruence'', the critical failure region occurs near the base where the wall takes down large loads. This means that when splitting the direction of the normal tensile forces over the critical failure region, we will also have a potential difference to the adhesion of the top and bottom so that premature shear failure of the bottom of the overlay concrete due to low congruence.
Conclusion We have to prevent tension on one side of the wall because only then we will prevent 1) the critical failure region, 2) the shear failure of the overlay concrete and 3) the potential difference
QUESTION How do we remove the tension?
We eliminate the tension by the method of prestressing + prestressing tendon contact with the soil using strong soil anchors for this purpose.
With this method we take the tensile force from the top level and send it directly into the ground, ensuring the disappearance of the critical failure zone, the disappearance of the tensile stresses from the wall body which only compresses, the disappearance of the potential difference, the deflection of the wall moments into the ground and the prevention of them being driven into the basement wall and beams. Prestressing also helps the stiff wall to become even more dynamic and stiff in order to reduce the deformations at the nodes to zero. Prestressing also increases the friction of the aggregates resulting in an increase in the dynamic of the cross-section with respect to the base shear. The embedment in the ground with expanding mechanisms and the subsequent filling of the boreholes in which the mechanisms are placed with reinforced concrete ensure a strong foundation and soil samples to know their quality.
These are the reasons why in this first experiment with a natural acceleration of 2.41g the test piece did not show the slightest damage.
Once I removed the packing bolts under the seismic base, and eliminated the preload from the tendons the results of the specimen behavior were different and fishy.
Take a closer look at the damage.
άρθρο με τις δικές μου απόψεις για τις κατασκευές και τον σεισμό.
Για εμένα η σειρά που μεταδίδονται τα σεισμικά φορτία πάνω στην κτίριο κατασκευή από οπλισμένο σκυρόδεμα είναι η εξής.
1. Επιτάχυνση εδάφους.
2. Αδράνεια μάζας.
3. Τέμνουσα βάσης
4. Ροπή. Η ροπή όταν εφαρμοσθεί σε ελαστικά υποστυλώματα, παρουσιάζει διαφορετική συμπεριφορά, από ότι αν εφαρμοστεί σε τοιχία, και διαφορετική αν εφαρμοστεί σε δύσκαμπτα κοντά τοιχώματα με μεγάλη δυναμική. Έχει δηλαδή διαφορετικό συντελεστή συμπεριφοράς q. ως προς την πλαστιμότητα, την τέμνουσα βάσης, την δυναμική της κατασκευής και την ικανότητα στην ελαστική μετατόπιση πριν παρουσιάσει διαρροές.
Ένα δύσκαμπτο τοίχωμα έχει μεγάλη δυναμική και μικρή πλαστιμότητα και αστοχεί πιο δύσκολα από ένα ελαστικό υποστύλωμα. Ακόμα τριπλασιάζει τα φορτία που κατεβάζει στην βάση, όμως λόγο μεγαλύτερης διατομής τα φορτία που παραλαμβάνει το επιμήκη τοίχωμα είναι λιγότερα.
Μεγάλο ρόλο στην συμπεριφορά της κατασκευής στον σεισμό έχει να κάνει και με το σχήμα των κατόψεων της. Οι σύγχρονες αρχιτεκτονικές ανάγκες θέλουν υψίκορμα κτίρια με ελεύθερες κατόψεις και μεγάλα ανοίγματα και με μείωση των φερόντων στοιχείων. Δηλαδή απαιτούν μη πλαισιακές κατασκευές από υποστυλώματα οι οποίες έχουν άλλη συμπεριφορά και δεν παρουσιάζουν μεγάλες στρεπτομεταφορικές παραμορφώσεις.
Η ροπή αν εφαρμοστεί σε υποστυλώματα έχει την εξής συμπεριφορά. Δεν κατεβάζει μεγάλες ροπές στην βάση, καταναλώνει ενέργεια λόγο ελαστικής συμπεριφοράς, και αποθηκεύει ενέργεια στον κορμό του την οποία εκτονώνει προς την άλλη κατεύθυνση στον επόμενο κύκλο φόρτισης. Όμως δεν διαθέτει δυναμική.
Αν η ροπή εφαρμοστεί σε δύσκαμπτα κοντά τοιχώματα με μεγάλη δυναμική και η επιτάχυνση είναι μεγάλη, τότε κατεβάζει πάρα πολύ μεγάλες ροπές στην βάση, οι οποίες είναι αδύνατον να παραληφθούν από τους συνδετήριους δοκούς τους οποίους σπάει.
Αν η ροπή εφαρμοστεί σε δύσκαμπτα κοντά τοιχώματα με μεγάλη δυναμική και η επιτάχυνση είναι μεγάλη, τότε κατεβάζει πάρα πολύ μεγάλες ροπές στην βάση, οι οποίες είναι δυνατόν να παραληφθούν από τα τοιχώματα υπογείου.
Αν η επιτάχυνση είναι πολύ μεγάλη τα τοιχώματα του υπογείου παραλαμβάνουν μεν την ροπή, αλλά παρατηρείται μια μικρή ή μεγάλη ανάκληση όλου του εμβαδού της βάσης του κτιρίου.
Σε αυτή την φάση έχουμε χάσει την στήριξη μεγάλου μέρους της βάσης του κτιρίου από το έδαφος θεμελίωσης, και τα στατικά φορτία μένουν αστήρικτα και η δύναμη του βάρους τους δημιουργεί μια αντίρροπη ροπή προς την ροπή ανατροπής του κτιρίου.
Αυτό μπορεί να επιφέρει τα εξής αποτελέσματα. α) Τα τοιχώματα του υπογείου και η διατομή του δύσκαμπτου τοιχώματος να μπορέσουν να παραλάβουν αυτά τα φορτία των αντίρροπων ροπών και η βάση να παρουσιάσει από μια μικρή ανάκληση μέχρι και ολική ανατροπή.
Και β) να αστοχήσει διατμητικά μια εκ των δύο διατομών, αυτή που είναι πιο αδύναμη.
Η ευρεσιτεχνία τι κάνει σε αυτή την κατάσταση.
Πακτώνει την κατασκευή στο έδαφος ώστε οι ροπές να τις αναλάβει το έδαφος αποτρέποντας την μεταφορά τους στα τοιχώματα του υπογείου.
Όμως αυτό θα δημιουργούσε ένα ευάλωτο δύσκαμπτο τοίχωμα ανωδομής το οποίο θα αστοχούσε από διατμητική αστοχία για πολλούς λόγους.
Πρώτον θα αστοχούσε το σκυρόδεμα επικάλυψης από διατμητική αστοχία λόγο της υπέρ αντοχής του χάλυβα στον εφελκυσμό και την μικρής αντοχής του σκυροδέματος στην διάτμηση η οποία αναπτύσσεται στην διεπιφάνεια σκυροδέματος και χάλυβα στον μηχανισμό της συνάφειας.
Δεύτερον στον μηχανισμό της συνάφειας η κρίσιμη περιοχή αστοχίας εμφανίζεται κοντά στην βάση όπου το τοίχωμα κατεβάζει μεγάλα φορτία. Αυτό σημαίνει ότι κατά τον διαχωρισμό της φοράς των ορθών δυνάμεων εφελκυσμού πάνω στην κρίσιμη περιοχή αστοχίας, θα έχουμε και διαφορά δυναμικού προς την πρόσφυση του πάνω και κάτω μέρους οπότε και πρόωρη διατμητική αστοχία του κάτω μέρους του σκυροδέματος επικάλυψης λόγο μικρής συνάφειας.
Συμπέρασμα Πρέπει να αποτρέψουμε τον εφελκυσμό στην μια παρειά του τοιχώματος γιατί μόνο τότε θα αποτρέψουμε 1) την κρίσιμη περιοχή αστοχίας, 2) την διατμητική αστοχία του σκυροδέματος επικάλυψης και 3) την διαφορά δυναμικού
ΕΡΏΤΗΣΗ Πως καταργούμε τον εφελκυσμό?
Καταργούμε τον εφελκυσμό με την μέθοδο της προέντασης + της πάκτωσης του τένοντα προέντασης με το έδαφος χρησιμοποιόντας για τον σκοπό αυτό ισχυρές αγκυρώσεις εδάφους.
Με αυτή την μέθοδο αναλαμβάνουμε την δύναμη εφελκυσμού από την ανώτατη στάθμη και την στέλνουμε απευθείας μέσα στο έδαφος, εξασφαλίζοντας την εξαφάνιση της κρίσιμης περιοχής αστοχίας, την εξαφάνιση των εντάσεων εφελκυσμού από το σώμα του τοιχώματος το οποίο μόνο θλίβεται, την εξαφάνιση της διαφοράς δυναμικού, την εκτροπή των ροπών του τοιχώματος μέσα στο έδαφος και την αποτροπή στο να οδηγηθούν στο τοίχωμα του υπογείου και στους δοκούς. Ακόμα η προένταση βοηθάει το δύσκαμπτο τοίχωμα να γίνει ακόμα ποιο δυναμικό και δύσκαμπτο με σκοπό να μηδενίσει τις παραμορφώσεις στους κόμβους. Η προένταση αυξάνει και την τριβή των αδρανών υλικών με αποτέλεσμα να έχουμε αύξηση της δυναμικής της διατομής ως προς την τέμνουσα βάσης. Η πάκτωση στο έδαφος με μηχανισμούς που διαστέλλονται και η μετέπειτα πλήρωση των οπών των γεωτρήσεων στις οποίες τοποθετούνται οι μηχανισμοί με οπλισμένο σκυρόδεμα, εξασφαλίζουν ισχυρή θεμελίωση και δείγματα εδάφους για να ξέρουμε την ποιότητά τους.
Αυτοί είναι οι λόγοι για τους οποίους σε αυτό το πρώτο πείραμα με φυσική επιτάχυνση 2,41g το δοκίμιο δεν παρουσίασε την παραμικρή βλάβη.
Μόλις αφαίρεσα τους κοχλίες πάκτωσης κάτω από την σεισμική βάση, και εξάλειψα την προένταση από τους τένοντες τα αποτελέσματα της συμπεριφοράς του δοκιμίου ήταν διαφορετικά και ψαθυρά.
Δέστε από κοντά τις βλάβες.
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Dear Doctor James Lewis
The purpose of modern seismic regulation is to build structures that: a) In frequent earthquakes with a high probability of occurrence, nothing will happen, b) In earthquakes with a medium probability of occurrence, minor, repairable damage will occur, and c) In very strong earthquakes with a low probability of occurrence, no loss of life will occur. So we should not use the term "absolute" in seismic structures. We should use the term 'quality' structures which means applying at least the requirements of all modern regulations. The quality of construction and its safety is also a function of the economic situation of countries, among other factors. It is understandable that poor countries cannot be compared with countries where they have expensive modern seismic regulations. Conclusion... there is no absolute seismic planning today, and we should not refer to absolute seismic planning, but to quality planning. So there is a great need today to invent a more modern anti-seismic design that corresponds to absolute anti-seismic design, with lower construction costs.
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The material data (in the property section) we need to consider in the ABAQUS simulation should be tensile test data (to assign the ductile damage parameters) or compression test data.?
The application or the product we are simulating is particularly for compression application (Assume it is Auxetic Structure).
Please help me in this regard..!
Regards,
Saiyad
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Yeah,
Thank you for the answer Junxian Chen .
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It is conjectured that the infilled frames performed better.
How such an unfavourable element (infill) which detrimentally adds to the stiffness of the structure and causes the absorption of more seismic force, and at the same time is not strong enough to last for the entire seismic event, and even is not ductile to absorb seismic energy, could improve the overall performance.
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I fully agree with Dr. Punashri. Further, if some kind of minimum reinforcement (horzontal, and possibly verical as well) is added in the inill walls, they will perform much better. Lateral collapse of infill is avoided in this manner. These bars should be properly anchored in the columns
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What are their significance in measuring ductility? If they are different then why they are?
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Professor William Callister wrote the famous book "Materials Science and Engineering: An Introduction".
Go to the chapter that discusses mechanical behavior of metals. You will find the answer there.
Long story short... elongation is about the change in length. Reduction in area is about the change in the cross-sectional area at the point of fracture.
The magnitudes of elongation and reduction in area will, in general, be different.
Best regards.
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Dear All,
I am totally new to countium mechanics and damage models.I need to implement a local damage model with von misses plasticity based on section 2.2.1. Damage Model in this article :https://www.frontiersin.org/articles/10.3389/fmats.2019.00181/full
However I am not sure how to implement a local damage model in Abaqus and where to start.Would be much more appreciated if anybody can help me!
Kind Regards,
Pardis
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The stiffness degradation you intend to use from reference article can be employed in CDP of ABAQUS. You can refer to these articles to develop your own damage parameters from constitutive relations.
You can also refer to this article where they have used CDP for other similar type of material at nano-scale.
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Hey experts,
i have a question regarding the Damage Initiation criterion in ABAQUS in the "Damage for traction Separation laws" tab. When in General should the maximum principal stress and when should the maximum nominal stress be the damage Initiation criterion? I would appreciate a general answer explaining the advantages and disadvantages of the two options. I can imagine it also depends on the ductility of the material?
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The maximum principal stress criterion is appropriate for brittle materials that fracture under tension or compression, such as ceramics or some composites. In this case, the maximum principal stress criterion is useful because it considers the state of stress in all three dimensions, and is sensitive to the orientation of the applied load. This criterion assumes that the material fails when the maximum principal stress reaches a critical value.
On the other hand, the maximum nominal stress criterion is appropriate for ductile materials that deform plastically before fracturing, such as most metals. In this case, the maximum nominal stress criterion is useful because it accounts for plastic deformation and the stress triaxiality effects. This criterion assumes that the material fails when the maximum nominal stress reaches a critical value. Advantages of using the maximum principal stress criterion include its sensitivity to the orientation of the applied load, and its suitability for brittle materials that fail under tension or compression. However, this criterion does not consider the effects of plastic deformation and is therefore not appropriate for ductile materials. Advantages of using the maximum nominal stress criterion include its ability to account for plastic deformation and the stress triaxiality effects, making it suitable for ductile materials. However, this criterion does not consider the orientation of the applied load, and may not be suitable for brittle materials that fracture under tension or compression. In general, the choice between using maximum principal stress and maximum nominal stress as the damage initiation criterion in ABAQUS should be based on the material behavior and the type of loading. For materials that exhibit both brittle and ductile behavior, it may be necessary to use a combination of these criteria to accurately model the material response.
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I have the attached load-deflection curve for an RC beam tested under a three-point loading test up to failure. What is the appropriate way/ most acceptable method to determine the cracking load, stiffness, and rotational ductility?
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Sorry. I am not an expert in that field.
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I want to remove the material from the workpiece to study the chip behaviour with certain set of process parameter like feed rate , depth of cut, grit velocity.
I have applied the material property and considered grit as rigid body.
But I am not getting any material removal phenomenon but material is under going plastic deformation using johnson cook plastic model for ductile material and applied all the d1-d5 values and the A, B, n strain rate and temperature values.
So what else I can do in damage criteria to remove the material.
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There are several factors that can affect the material removal phenomenon during machining, and it may be difficult to pinpoint the specific cause of the issue you are experiencing without more information. Here are a few things you might consider:
  1. Check your process parameters: Make sure that your process parameters, such as feed rate, depth of cut, and grit velocity, are appropriate for the material you are machining and the desired level of material removal.
  2. Consider the type of cutting tool: The type of cutting tool you are using can have a significant impact on the material removal phenomenon. For example, using a sharp tool with a high cutting speed may result in more efficient material removal compared to using a dull tool with a low cutting speed.
  3. Check the temperature and strain rate: The temperature and strain rate at the cutting edge can affect the material removal phenomenon. Make sure that you are using the correct values for the material you are machining, and consider adjusting these values if necessary.
  4. Check the material properties: Make sure that you have accurately characterized the material properties of the workpiece and that you are using the correct material model in your simulations.
  5. Consider other factors: There may be other factors that are affecting the material removal phenomenon, such as the presence of defects in the workpiece or the type of cutting motion being used.
I hope these suggestions are helpful. If you are still having difficulty achieving the desired material removal phenomenon, it may be helpful to seek the guidance of an expert in the field or to consult with the manufacturer of your cutting tool or machine.
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If the fracture stress of one piece is higher than its yield stress, does it brittle fracture or ductile?
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If fracture stress exceeds yield strength, then the material has already deformed plastically (note that plastic strain at yield is 0.2% due to offset). Being on the right side of these curves implies defect(s) in the material should be below a size that does not cause premature fracture before yield strength is reached. I hope this helps.
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The typical failure modes of cylindrical samples in splitting tensile strength and beams in flexural strength were observed. It has been found that the sample of the mixes with 100% OPC was split into two parts, brittle failure. When the 12.5% OPC is replaced with silica fume, minor cracks were observed up to the full depth of the samples without splitting into two halves. Is it the ductile behavior in the samples because of silica fume incorporation or any other reason? Need a valuable discussion
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Thank you very much Dr. Shashikant Kumar for a nice discussion
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I major in geoscience and I find such unique patterns in either rocks or the muddy sediment or even the CaCO3 paste. I feel puzzle about that why the different fracture modes produced the same fracture morphology. In my opinion, fracture in rocks may be a brittle fracture, while the fracture in desiccation paste may be more ductile. I believe this topic have been well studied in material science. Could you plz give me some advice?
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This is very intresting observations. What you defined as different fracture modes? There were static, quasi-static or dynamic loads?
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Dear all
I am using A3003P plate and rigid nail in a drop test,
in Abaqus always a rigid nail passed through A3003P plate but actual test results are not pierced.
damage evolution was calculated by my ss-curve area
UTS : 177MPa , Plastic strain : 0.19512mm
but it was pierced
So I adjusted the elastic modulus to 1000GPa and damage evolution to 50mm but it was pierced again
The attached file is my ss-curve and test conditons.
The velocity is just before the crush, plate thickness is 1.5mm, elements characeristic length is 1mm
how don't pierce it?
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U need 2 use Johnson Cook Damage model
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Hi, I want to model ductile damage in abaqus so I need material parameters for steel ss400 and st57. I would appreciate if you could help me.
Abaqus
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ِِِِِِِDear Seyed Saeed Askariani ,I read your report. I think it is useful and I will definitely use your report after verifying my new job and I may ask some questions.
Best regard.
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Is it possible through "hardening" process? Also, how it could change the microstructure of α-ferrite ?
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There are two ways to increase steel's strength at the expense of its ductility: cold working and hardening. Any steel can be cold worked, but hardening only works for steels with a carbon content above 0.3%.
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Hi,
I am looking for damage model data based on traction-separation law for A249 304L stainless steel tubes to input into abaqus model ?(damage initiation and evolution). Does anyone knows where I can get those data from?
Regards
Reza
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Mohammadreza Arjmandi Did you figure out how to calculate those parameters?
i really want to know,,,
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Why is tensile strength more important in joint strength analysis of Friction Stir Welding (FSW)? Why not other mechanical properties, such as yield strength, ductility, etc., are considered in the analysis? Is there any connection that TS is more important than other properties?
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the yield strength is the minimum stress under which a material deforms permanently. in fsw as this is done on aluminium alloys or soft materials, where stress is very less and the material is ductile, therefore yield strength mean less and are not the properties which matter.
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Including the full range of ductile, hard, brittle alloys and composite materials.
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Yes, basically cutting relates to shear of the material. Higher the shear strength higher will be the difficulty to cut the material. e.g. Cast iron is easier to machine than steel, because CI is weak in shear where as steel has good shear strength.
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I have to work on crack formation to simulate ductile fracture in ABAQUS by using UEL. Can you please suggest to me some explanation videos?
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Dear Yassine Hersi,
I hope this can help you:
step one:
Programming the user element by means of the "uel subroutine" in ABAQUS. You save the file "userfile.f".
step two:
In the input "jobfile.inp" you must identify the user elements, and define their properties, and degrees of freedom. For example:
*USER ELEMENT, TYPE=U1, NODES=3, COORDINATES=2, PROPERTIES=8, VARIABLES=60
1,2
*ELEMENT, TYPE=U1, ELSET=CZ
** PLACE HERE THE COHESIVE ELEMENTS
12360,1376,2923,1325
…….
*UEL PROPERTY, ELSET=CZ
1700,…..
Step three:
If abaqus subroutine is enabled in your computer, you run the uel subroutine in the command window writing this:
Abaqus job= jobfile user=namefile
Best regards
Susana
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All these are refractory Metals with higher than 2450 deg C melting point.
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  1. The Answer appears to be in the variation of Shear Modulus and Peierls Stress values of these elements (G ) in GPA)
W: 164 1.7-2.1
Mo: 158 4.6
Ta: 62.8 5.4
Nb: 47.2 8.7
REF:Size-dependent plasticity in an Nb25Mo25Ta25W25 refractory high-entropy alloy
The higher shear modulus values of W,Mo doesn't permit adjacent layers to slip thereby high CRSS(Critically Resolved Shear Stress) and low Peierls Stress inducing brittleness. While low shear modulus values, LOW CRSS(Critically Resolved Shear Stress) and high Peierls Stress of Ta,Nb permit easy shear or slip enabling ductility.
thanks & regards,
g.sudhakar
phd(materials engg),HCU.
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See for example,
Usually strength and ductility cannot simultaneously increase unless some mechanism converts ductility-raising metastable phase to strength rising phase under sufficient elongation, as the case for Austenite to Martensite transformation in transformation-induced plasticity (TRIP) steel. To my knowledge, Cu-ZN brass usually does not form Martensite, so it is alloying that is responsible. Strength increase may be attributed to solid solution strengthening, but how to explain the ductility rise?
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That's a Very Good Question. Yes it's true that strength and ductility are generally vary inversely , in this particular context Cu is FCC and Zn is HCP. FCC has 12 slip systems while HCP has only 3 slip systems. The more the slip systems higher the ductility and vice versa. FCC metals are very ductile and HCP metals are brittle.
The anamoly lies in tradeoff between ductily and brittleness. While HCP is contributor to strength while FCC to ductility. While former has little influence,but latter has greater influence by which we observe elongation and strength increase in single phase alpha region. Beyond >35%,beta phase steps in the influence of HCP Zn is more predominating than FCC Cu by which elongation decreases and strength increases(alpha + beta) region. Beyond >45%,fully beta prime HCP. Both strength and ductility fall.
thanks & regards.
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Hello, we want o make biopolymer composite wires using 3D printing (using our solution and not a ready filament of course) and I wonder which biopolymer or even a plasticizer is recommended in order to get ductile wires. Most of what we produce is brittle wires for now. Thanks in advance.
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You need to be very careful with your selection because of extractables and leachables. It depends on your application (patient contact/long term vs short term). Maybe take a closer look at some of the USP Class VI or ISO 10993 rated Polyurethane based photopolymer resins but you might need to use a top down printer to reduce the need for supports depending on the length of the wire and overall geometry. These usually contain some degree of PEGDMA. Also be careful of what type of photointiator you are planning on using.
The end result after curing is typically a polymer with low molecule weight photolites left over that can migrate easily out of the polymer itself after curing and through skin, food packaging and other similar examples. A lot of work is being done to reduce extractables and leachables but applications such as long and or short term skin contact (intact skin vs rating for contact with mucosal membranes) has been successful if you look around at some offerings from some of the larger 3d printing names in the industry.
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I am interested in learning a bit about the background of how the behaviour factors, which are used in Eurocode 8 to calculate the design base shear for a structure, were developed. As I understand it, and please correct me if I am wrong, the factors implcitly comprise several different components:
- first, a reduction in seismic forces to account for system ductility in accordance with the equal displacement principle,
- secondly, a further reduction to account for overstrength of the structural elements,
- and thirdly, some component that accounts for the performance for the structural system.
Can anyone enlighten me as to how the values in the Eurocode were obtained and/or point me towards some appropriate literature. I would also be content with information pertaining to the R valued used in the US as this is somewhat similar.
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You may also find more information in this paper
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waste gypsum is used to stabilize the mud block. will it be helpful?
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Kindly see also the following very good RG link:
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additive manufacturing,deformation,metals
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Yes, sure. Technologies of additively manufactured metals has varying success and complexity for different alloys. For example, for metals and alloys with high chemical activity and affinity for oxygen (aluminum, titanium, magnesium, zirconium, etc.), the production of products using these technologies is much more difficult than for metals with lower chemical activity (iron, copper, nickel, cobalt, molybdenum, etc.).
There are other features of 3D printing technologies for different alloys, for example, associated with subsequent heat treatment (porosity elimination by hot isostatic pressing, hardening, tempering, dispersion strengthening, normalization, etc.).
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It is apparent that increasingly testing of disc shaped samples using a ball or hemispherical indenter is being advocated for measuring materials properties. It should be apparent that at the start of loading the disc must deform to take on the shape of the ball. This is a relatively high deformation process. For very brittle samples there is insufficient ductility available and cracking occurs. For ductile materials there is the risk of the strain introduced modifying the properties. Thus, the structure when the measurement is taken is significantly altered. In both cases the results obtained may not be representative
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I completely agree with Jonathan David Parker and Mark Petkov . This question should interest the Project
Personally, I think that small punch tests should never replace the uniaxial test. Nevertheless, there would be a role for small punch tests when (1) material is limited and (2) the problem being investigated requires large strains.
The "large strain" issue is the key point to Jon's question.
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A lot of papers show HEAs have excellent combination of strength and ductility as well as corrosion resistance, i.e. Ni-Co-Cr-Fe-Al-Ti HEAs. The microsstructure and chemical composition are very similar to superalloys. Has Ni-Co-Cr-Fe-Al-Ti HEA been used in industrial?
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Dear Hanlin, thank you for sharing this very interesting technical question with the RG community. I found a statement in a relevant literature reference that (citation): "Over the last decade, the concept of high entropy alloy (HEA) has attracted world-wide attention for the design of novel metallic materials." For more detailed information about these interesting and unusual materials please have a look at the following useful articles which might help answering your question:
On the Path to Optimizing the Al-Co-Cr-Cu-Fe-Ni-Ti High Entropy Alloy Family for High Temperature Applications
This paper is freely accessible as public full text on RG, so that you can download it as pdf file.
Also potentially useful:
Understanding Phase Stability of Al-Co-Cr-Fe-Ni High Entropy Alloys
(please see attched pdf file)
Good luck with your work and best wishes!
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As we all know, with the increase of drawing strain, the tensile strength of cold drawn pearlitic steel wires gradually increased while the ductility decreased. However, from the view of engineering stress-strain curve, the elongation of steel wires did not decrease with the increase of drawing strain. So, how to establish the relationship between drawing strain and tensile ductility of cold-drawn pearlitic steel wires?
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Stress-strain curve from literature is only suitable for steels in a normalized state (tempered at approx. 800°C). As soon as you deform the steel for the first time, it is work hardened and the stress-strain curve changes. This means that after every further cold drawn without intermediate annealing there is a new stress-strain curve. Of course you won't find any such curves in literature.
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I am research scholar at SVNIT, Surat, India and working in the field of Design of Reinforced Concrete (Industrial) Chimney. I need a minimum of 5 international reviewer from academics for my research paper titled as "Moment-Curvature Relationships for RC Chimney Sections". In this paper moment-curvature diagrams are plotted using three different design standards namely IS: 4998 - 2015, ACI: 307 - 08 and CICIND 2011 and results are compared in terms of strength, ductility and energy absorption. Please let me know if anyone can review my paper.
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Hi dear Megha Bhatt
Do you need 5 international reviewers to suggest them to the journal you are going to submit to?
The best way is to choose from the authors that you have referenced their papers in your article. And since you used Indian standards, it is better to select reviewers from your own country (who do not live in India currently).
Finally, bear in mind that usually, journals have their reviewers. If they can't find proper reviewers, they will opt from your suggested ones.
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Dear researchers
i tested CA6NM turbine steel for impact angle on slurry erosion jet rig. At 90 degree angle i am getting higher erosion rate whereas, at lower impact angle i am getting lower erosion rate? i am not able to under stand why this is happen though this is ductile material.
i saw papers in which lower erosion rate happens at 90 degree and higher erosion rate is happen in small impact angles.
please help why i am getting this type of results
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That is a good question.
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Has anyone modeled aortic valve calcium plaque crack/failure/fracture? What crack model works the best? Can you also guide me to a good resource where I can find reliable fracture parameters? TIA
Note: I am looking into the 'concrete smeared cracking model', 'concrete damaged plasticity model', and also ductile fracture models. The issue is I have not found any reliable source clearly stating the material property/ a range of property (since calcium deposit material property can vary based on age and some other hemodynamic factors). So I am unable to test out those models.
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I want to know, what will be the ductility and energy dissipation of simple H/I steel section for cyclic loading. How the steel section is different than RC section for cyclic loading.
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If we increase or decrease the ductility of 1060 grade aluminum tube then then what is the effect on the corrosion property.
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Dear Sir Abdulaziz Albannai ,
Thank you for replying me.
This is Refrigerant aluminum tube. Pitting corrosion occur in the bend position.
we know that bend property depends on ductility of a materials. But maximum pitting corrosion occur in the bend position.
So have any relation pitting corrosion and ductility?
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Carbon,basalt,glass are mostly used fiber Reinforced polymers. Even there is incresed in Strength of the concrete ,these materials are not efficient in the point of ductility and crack width when compared to controlled concrete. Any suggestions and updates ?
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Dear Christi,
I just came across your very interesting technical question. I fully agree with the other expert RG members in that there is no single "perfect" FRP (= Fiber-Reinforced Polymer). The variety of known FRPs is just too large. For a highly instructive overview of this field please have a look at the following useful article:
Fiber-Reinforced Polymer Composites:
Manufacturing, Properties, and Applications
This paper has been published Open Access, so that it is freely accessible as pdf file (see attachment).
A large number of other helpful references about this topic can also be found and accessed by searching the "Publications" section of RG. Simply search for the term "Fiber-Reinforced Polymer Composites" and then click on "Publications":
A large number useful articles about this topic have been posted by RG members, many of them even as public full texts.
I hope this helps. Good luck with your research work and best wishes!
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The target is removing or decreasing free carbon on the external surface of gray and ductile iron.
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Yes, the heat treatment in open atmosphere is an effective method for decrease carbon on surface graphitic cast iron
according to my published paper
Novel Approach for Using Ductile Iron as Substrate in Bimetallic Materials for Higher Interfacial Bonding Bearings
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Hello
I want to use ductile damage model in abaqus to simulate the deep drawing of square part. To reach this goal i need to enter values of stress triaxiality and fracture strain during the deep drwing process. I know stress triaxiality = -P/Q wich (P=-1/3(S1+S2+S3)) and Q= von mises equivalent stress. But i don't know how to get the values of the principale stresses and fracture strain experimentally
I get also the values of (S1,S2,S3,von mises) from ODB field output and calculated the stress triaxiality but i don't know if the results are good or not.
Could you help me please?
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Hi,
You can mount a strain gauge on your part. Each set of measurements give you three values. Then the rest of the stress tensor components can be found using the equilibrium equations. When you have all the stress components, you would be able to calculate principal stresses.
Good luck
Farzad
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How do I obtain these ductile damage parameters(initiation and evolution) to apply in abaqus in order to have damage criteria. I have experimental data form a steel device that is subjected to a hysteresis loop. So I can get the dissipative energy from the area of the force displacement graph. But i can't find a solution to apply these parameters in order to simulate the damage criteria. Do you think ductile damage is a good application for this example or should I do other damage criteria and how do I get the parameters for that damage criteria? Thank you.
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Please find the attached file.
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For strengthening of existing URM buildings, which techniques can we opt to get better seismic performance in terms of high strength, deformability, and energy absorption capacity?
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Pls see our article where we made a comparative table showing different strengthening technique for URM with cost and strength effectiveness...further we proposed a bed-joint concept to overcome the de-bonding issues.
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Seismic design takes advantage of larger damping owing to structure ductility to reduce the design load by R factor (of 3 to 8 value). Apparently, both seismic and wind governing loads are derived from similarly rare event at about 500 years return period, although some recent codes use 2/3 of MCE 2500yrs for seismic. But why only seismic design allows some structural yielding and acceptable damage, while wind design should remain elastic? Is there some concept that I misunderstand?
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The main difference between the two loads lie in the prediction of their occurrence. While wind loads could be predicted with much accuracy(including the time of occurrence & intensity levels), unfortunately we have not yet developed any methodologies that enable prediction of time-specific or intensity specific occurrence of earthquakes at a site. Only probabilistic seismic hazard analyses (PSHA) are undertaken for better prediction of earthquake occurrence.
Secondly it is highly uneconomical and impractical to design a structure to remain elastic for a highly uncertain event such as earthquake. Therefore, the ductility of the structure is called for( by introducing R factor) while designing the structure for a much lower level of earthquake. Further it shall be noted that during earthquakes, structures are permitted to undergo different damage states depending on the return periods of the earthquake event.
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For my high wear scenario, TUNGSTEN DISULFIDE WS2 looks to be a promising coating material. I have coated my substrate (ductile iron castings) with ws2 nano poweder using dipping method. However, in our tests coating comes off after few hours. Scratch test post dipping showed good adhesion.
I want to know from experts here.
1. What is best method to achieve good adhesion between ws2 and ductile iron for sliding application (coated casting on mild steel).
2. Which technology can be scalable as my coating will be 10k parts per month.
I have looked at sputtering but that seems expensive foror large quantities.
Any guidance appreciated
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Dear Jay Paresh Mehta many thanks for asking this very interesting technical question. Apparently large areas can be coated with tungsten disulfide by chemical vapor deposition but I really don't know how this is scalable and what the costs are:
Preparation and Photoluminescence of Tungsten Disulfide Monolayer
In this context please also have a look at the following potentially useful articles which migth help you in your analysis:
Friction of Tungsten-Based Coatings of Steel under Sliding Contact
and
The replacement of cadmium coating on parts of the weapon with tungsten-disulphide coating
All three articles have been posted by the authors as public full texts on RG, so they can bee freely downloaded as pdf files.
I'm afraid that these references will not provide a satisfactory answer to your question, but perhaps they contain some useful hints.
Good luck with your work and best wishes, Frank Edelmann
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I'm wondering which type of casting defect has happened and what are remedies?
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Dear Mohammad Farshbaf Ahmadipour,
The problem is known - the presence of a defect in the surface. This type of defect is typical in the following cases: - Presence of moisture in the mold; - poor adaptation of the vomit; - poor separation of air and gases from the mold; - lack of sufficient channels for removal of air and gases from the mold; - low hydrostatic pressure during casting; - low casting temperature unlikely but not switched off; - basket thinness of the metal due to loss of chemical elements or low casting temperature; and other. Nebivadase also turns off the temperature of the heated mold, it has a strong influence on the quality of the casting.
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Hi,
I am trying to complete a force-displacement curve for a concrete prism with a weak section in the middle (5mm long) with fx = 90% of fx for damage localization
to study the mesh sensitivity in ABAQUS.
However, the curve returns with very brittle behaviour and with much higher ductility but the ultimate strength is about the same. This can be due to anything that I have modelled (boundary conditions, face-to-face tie constraints or load application).
Both the model in ABAQUS and the comparison will be attached in this question. Any advice is greatly helpful. Thank you
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I advice you to change the particle size distribution
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I am using Inox 1.4310 (X10CrNi18-8) as the material for the blank in a punching operation,
However I need the Ductile Damage (Fracture strain, stress triaxiality, strain rate) and Shear Damage (Fracture strain, stress triaxiality, strain rate) as well as plasticity.
Thank you
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In microstructural images recorded using SEM, voids in metals are sufficiently well visible to do e.g. image analysis to automatically characterize these voids, see e.g.
Do voids nucleate at grain boundaries during ductile rupture? - ScienceDirect
However, I am wondering whether it is possible to identify voids solely from EBSD recordings. Any suitable orientation map/algorithm or experimental options in the EBSD software to to be able to extract the void area from EBSD recordings?
Cheers, LE
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Dear Lennard Euler thank you for your interesting technical question. Please have a look at the following potentially useful articles which might help you in your analysis:
1. Do Voids Initiate at Grain Boundaries During Ductile Rupture?
and
2. Recent Advances in EBSD Characterization of Metals
(Review article)
Please find attached both articles as pdf files.
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Respected all,
I am going through a formula of critical depth of cut for ductile to brittle transition cutting of carbon fibre reinforced epoxy composite.
dc= 0.15 (E/H) (K1c/H)^2
here Hardness value is needed to be added in MPa as E is in MPa, K1c is in MPa.
The value of E is 155.6 GPa, K1c is 250 MPa mm^1/2
Can you please help me with the hardness. Many papers say that it is Rockwell hardness of 68-74. Some say that Knoop hardness of 143 GPa. I have tried inputting the values. However, I am not getting the correct solution. Can you please help me with the same. I have tried a lot but couldn't get the solutions. Thank you.
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Which hardness scale is much suitable for the CFRP/GFRP/KFRP Epoxy composites?
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tensile rest was carried out at different temperature starting from room temperature to 850°C. it is observed that yield strength and ultimate tensile strength remain unaffected until 650°C but ductility starts increasing after 550°C and maximum at 650°C and thereafter decreases. YS unaffected could be due to kear wilsdrop lock. similarly the ultimate tensile strength may be due to work hardening of the material. After 650°C, it is decreased due to onset of dynamic recovery.
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The standard heat treatment for this alloy appears to be aimed at increased creep resistance and elevated temperature service rather than conventional lower temperature tensile strength. • The standard heat treatment as utilized on the as received material has a high-temperature solution cycle aimed at setting the grain size and partially dissolving the prior particle boundaries. • Slow cooling is employed to allow large section sizes to be processed with reduced risk of quench cracking. • A slow or interrupted cooling rate through the gamma prime precipitation and growth range was used to set the large gamma-prime size and distribution. • The ageing cycle used for this material is believed to stabilize the gamma-prime and secondary carbide phases for optimum high-temperature performance.
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both of SAC and DDC occurs after PWHT or in welding procedure when reheating from previously weld pass, butt I guess Although that mechanism is different, temperature range that occurs is different...!!!
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Hi, my darling
This is a good question and certainly has a good answer, too. However, I do not know the answer, and I must think about that.
Seriously, What is different between this two ways of the cracking process?
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As per my previous concepts, the ductility of concrete in uni-axial compression decreases as the compressive strength increases.(As from the stress strain diagram, a low strength concrete fails at higher strain levels)
But when we talk about the structural elements i.e, Flexure members, Compression members numerous sources on the internet say " That the ductility of the concrete increases with the increase in the compressive strength" What could be a good justification to this? Please answer in the light of following:
1) Is it because we have improved shear strength attributed with higher strength?
2) The curvature ductility increases with the increase in compressive (Fig Attached below)
So can someone argue, that a column in pure axial state , its ductility decreases, but when we have some eccentricity ( i.e, bending) the ductility increases
Thanks in Advance!
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Usually, the more compressive strength concrete has, the less its ductility becomes.
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The ductility of structural elements and reinforced concrete structures is characterized by their ability to deform beyond the leakage limit, without significantly reducing their strength.
According to § 5.2.1 of EC8 there is a design option of the available ductility of the building.
Reinforced concrete buildings can be studied with two different design methods.
a) To be designed with the necessary ductility which means to have the required - necessary ability to consume seismic energy, but without losing their resistance to earthquake loads.
b) To be designed with low ductility, with low energy consumption, but with very high dynamic strength.
They are two different design methods that can not work together, because ductility allows inelastic deformation, while dynamic strength requires rigid walls of diaphragm function.
A pillar that deforms elastically or inelastically, cannot work together with a rigid elongated wall to resist seismic loads, because the elongated rigid wall resists from the beginning of the deformation, while the pillar recedes, due to its elasticity. or the ductility inelasticity, which follows.
As I mentioned before, according to § 5.2.1 of Eurocode 8, (EC8) there are three design options with different available ductility with a corresponding increase in dynamic strength when the ductility decreases, or in other words, an increase in ductility as the dynamic strength of the construction decreases .
I will strongly disagree with the Eurocodes 8. They can not work together flexibility, ductility and dynamics as they plan today.
Only the design that I suggest to you in the photos achieves a combination of flexibility, ductility and dynamics together. https://www.youtube.com/watch?v=IO6MxxH0lMU
In the dynamics of structures we study the structures in dynamic strain as a consequence of seismic movement of the ground. What my method is studying is how it will help the response dynamics of structures in terms of dynamic equilibrium equation, , using external dynamic response factors, with and without damping.
A short pillar and a normal pillar do not resist the earthquake together, because the short pillar receives all the stresses on its own because it is rigid, while the normal pillar gives way to elasticity.
The result is that the short column fails first because it is unable to pick up all the earthquake loads on its own. The same goes for a wall and a pillar. The wall as more rigid than the pillar receives all the tension on its own, and will be the first to fail.
How Eurocode 8 does not allow short columns but allows design with columns and walls together is worth mentioning.
My opinion is that either you have to design dynamically, or with available ductility
Both dynamically and ductility contribute to the reduced reaction of the structure to the earthquake.
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Within the elastic displacement phase all the energy of the earthquake is stored in the trunks of the beams and columns and returns in the opposite direction, like the spring. We have no failures in elasticity. When the displacement grows larger than the elastic limit we have inelastic displacement with leaks - cracks. To manage the inability of seismic designs to control the inevitable inelastic displacement, they built the Ductility mechanism. They are unable to control the deformation. This is the problem, and Ductility just manages it better. But it does not solve the problem of deformation which causes from failures to collapse of structures.
Seismic damping consists of different damping mechanisms. 1) The horizontal seismic damping (bearings) limit the acceleration of the ground to pass on the construction. 2) Ductility is also this mechanism of seismic damping, because with the small failures on the trunks of the beams that it allows to be made, it releases seismic energy. 3) Hydraulic systems create seismic damping by converting the kinetic energy of the earthquake into thermal energy through its liquids which are heated when compressed by the displacement of the piston. 4) Elasticity is the vestibule of inelasticity and it also consumes seismic energy because heat is produced in the steel molecules when it receives stresses. There are other seismic damping systems that each operate differently in different areas of the structure to provide basically less instantaneous high seismic intensities on the structure. When we talk about dynamics this is something else. It is not seismic damping. It is a force against another force The design method I suggest involves something completely new and that is that it receives power from an external factor (that of the soil) and transfers it to the structure to help the structure respond dynamically against seismic forces, in order to have a balance of forces and not failure. This external force factor can be used to increase the dynamics of structures. It is not a seismic damping mechanism. So some who try to compare bearings with the external factor dynamics offered by my patent are misplaced because they compare two different things that have nothing to do with each other. However, if we want to use the invention as a seismic damping mechanism before it acts dynamically, then we simply place a seismic damping mechanism on the patent mechanism which will resiliently resist seismic shifts by drawing the reaction force from the ground before the main mechanism of the patent action dynamically to stop the inelastic displacement of the construction. In the dynamics of structures we study the structures in dynamic stress as a consequence of seismic movement of the ground. What my method is studying is how it will help the dynamic response of structures in the dynamic equilibrium equation, using external dynamic response factors, with and without damping.
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I want to determine the percentage of ductile and brittle fracture for some samples from impact test.
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In SEM it is possible to distinguish ductile zone and calculate the percentage.
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In metals and alloys, generally when the stress generated exceeds yield (ductile) strength, it is implied yielding or failure occurs.
Similarly, in the case of finite element analysis of elastomers, what is the best parameter used to predict failure of elastomer under static loading?
1. Stress
2. Strain or
3. Strain energy
Third, similar to the Goodman relation in metals, what is the industrially used relation for fatigue life prediction of elastomers?
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The traditional thinking is in stress limits and small deformations. The stretch-strain curve of elastomers becomes quite steep when approaching the limiting stretch. Therefore, the stress at rupture is less certain. But the limiting stretch is. Unfortunately you will hardly find tabulated values.
However, you can find some large deformation theories for limiting chain extensibility material models like the van der Waals rubber model. Then you can find that the square root of the trace of the left and right Cauchy Green tensor is limited to approx. 8.8. (The eigenvalues/proper values of this tensor are the squares of stretch.)
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How does it lead to Strengthening but not at the cost of ductility.?
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It is often stated that “Grain boundary strengthening has the advantage that the ductility of the material does not decrease with decreasing grain size and increasing strength.” (Rösler, Harders, Bäker, Mechanical Behavior of Engineering Materials). This is an exception to the generally observed inverse relation between strength and toughness.
In this context it is important to differentiate between toughness, which requires a pre-existing crack or notch and ductility, which is the ability of the material to plastically deform and is usually determined in a tensile test, e.g. by the fracture strain.
Fine-grained structures usually have smaller potential flaws, which increases the stress to fracture.
Grain boundaries can also act as barriers to crack propagation, the different crystallographic orientations cause the crack change direction, and cracks can be bridged in fibrous grain structures.
For fracture to occur in a tensile test of a semi-brittle material, slip bands have to nucleate at the yield stress, these have to nucleate micro-cracks, and these micro-cracks have to propagate.
Cottrell (A.H. Cottrell, Theory of brittle fracture in steel and similar metals, Trans. AIME 212 (1958) 192-203.) developed a model in which the stress for propagating a microcrack that was initiated at the intersection of two slip planes can be calculated to $\sigma_{f} \approx \frac{4 G \gamma_{m}}{k_{y}} d^{-1 / 2}$
with $\sigma_{f}=$ fracture stress $G=$ shear modulus $\gamma_{m}=$ plastic work done around a crack as it moves through the crystal $\begin{aligned} k_{y} &=\text { dislocation locking term from Hall-Petch relation \\ d &=\text { grain size } \end{aligned}$.
Which is similar to the Hall-Patch equation.
For more, see e.g. chap. 7.2.2. of Hertzberg, Vinci, Hertzberg, Deformation and Fracture Mechanics of Engineering Materials or p.325 of Haasen, Physical Metallurgy.
Hope this helps,
Erik
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Hi,
I am doing the thesis on the performance based design of the Reinforced concrete tall structure under high wind and low seismicity by using MIDAS GEN Software. The structure has designed for the least possible sizes and material. But still the ductility factor(D/D1) for the overall structure is less than 1. In Midas gen, is it how we will verify the ductility or is there any other procedure is check the ductility?
Thanks and Regards
Anupama Kamani
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Please check the attached paper. The ductility demand is calculated in the paper.
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These beams have the same deep as the waffle has, and they have been detailed just like a beam for seismic requirements.
Can these beams and columns act as a ductile frame?
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Thank you Patlola
Madhusudhan
I have asked this question from ACI TECHNIQUE STAFF and they have answered:
yes as below:
Can you tell why NOT??
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I am not an expert at materials science. However, when I look at the literature, I read a process called cold spraying. This process is basically spraying a ductile powder (e.g. copper) onto a solid substrate at a high velocity to improve surface ductility of the substrate. Now, what I am wondering is if surface embrittlement is unavoidable if a brittle powder (glass, PMMA, metallic glass, ceramic) can be sprayed onto a solid substrate. I'm preparing a research proposal where any suggestion would be much valuable and appreciated.
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It goes without saying that the hard and brittle materials that are applied to a soft surface make the surface hard and brittle. If you hit this brittle surface, the metallic substrate under the layer is plastically deformed and the layer crumbles. However, it does not mean that this surface has to fail if the component is subjected to other loads. If you think that, for example, when the coated rod is elastically bent, the brittle layer always breaks before the metallic base material, then it is not always the case. In this case, not only the ductility of the layer, but also its strength and its modulus of elasticity play an important role. I know of cases where the steel substrate broke earlier than the brittle layer on its surface under cyclic alternating loads (in the elastic range). The "secret" lay in the layer's low modulus of elasticity. So, in other words, the word "brittle" doesn't always mean "bad".
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Hey friends,
I am trying to apply ductile damage in a bending cyclic test on a pin. Using Static General Step.
I can run the simulation till the end without damage, but when I apply the ductile damage to the material, I get converge problems. It only runs until the elimination of the first elements and then gets aborted, with the usual message of “Too many attempts made for this increment”.
This is a simulation of an experimental test, I wish to simulate the full failure of the pin.
Looking at the job diagnosis, some contact occurrences: Overclosures, Maximum contact force error, Maximum penetration, points now slipping, points now sticking warnings show for Nodes around the eliminated elements, and warnings like zero pivots, and negative eigenvalues are shown.
I apply the ductile damage parameters, Fracture Strain, and Damage evolution in tabular form (D,displacement) that I simplified to just two lines (D=0 and D=1).
On the step module I am using NGeom: On and automatic stabilization, with dissipated energy fraction of 0.01.
I am using Reduced Integration linear elements C3D8R, with Stiffness Hourglass Control and max degradation of 0.998.
I think the problem is either with the damage parameter definition or the mesh definition.
Can somebody help me? I have read and tried of everything, but I can’t seem to get pass this problem. If you have a question regarding the model definition I will be glad to answer.
Thank you very much, Diogo Cabrita.
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Thank you all, I fixed the problem by using fracture energy instead of displacement in damage evolution. Also I let it run even if the abaqus froze and it goes to the end. I have another problem now that is the sitfness degradation on the unloading phases, it seems to unload elastically when the elements are already damaged and I wanted it to unload with a less stiff rate. I don't know how to consider this, if anyone has a suggestion I would like to know. Thank you again, Diogo
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Dear researchers
As you know, one of the challenges of using nonlinear procedures is to determine the behavior of plastic hinges of members with deformation controlled action that this behavior is assigned to the plastic hinge by a force-deformation curve and its relations using parameters modeling. various researches has shown that the uncertainties in these modeling parameters significantly affect the structural responses.
Also, the acceptance criteria of different performance levels relating to the mentioned force-deformation curve are needed for performance-based design of structures.
There are two questions now:
1- Are force-deformation curves presented in ASCE 41-13 suitable only for nonlinear static analysis (push over)? or also is applicable for nonlinear dynamic analysis?
2- Given that the acceptance criteria presented in ASCE 41-13 are derived based on the mentioned force-deformation relations in this code (a, b and c modeling parameters), what acceptance criteria can be used to evaluate the structure at the IO, LS and CP performance levels if the other force-deformation relations presented in the technical literature (such as Lignos and Hartloper relations for beams and columns of moment frames, respectively) are utilized for concentrated plasticity modeling?
The mentioned curves (Lignos and Hartloper relations) are mostly used in structural modeling to study the structural collapse, in which the collapse is determined by the criteria mentioned in FEMA p-695 and as a result, acceptance criteria in accordance with these behavior curves have not been researched.
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1. Seismic codes suggest simplified force-deformation models in order to estimate the inelastic behavior both in monotonic and cyclic loading. The monotonic F-δ curve is considered as the envelope and the skeleton curve of F-δ loops under cyclic loading. The real inelastic behavior under cyclic loading depends on the material and the dynamic loading, e.g. reinforced concrete under seismic loading. So, stiffness and strength deterioration should be considered under cyclic loading in the concentrated plasticity modeling technique.
2. Uncertainties about deformation capacity are high beyond the point C of the F-δ curve. Even in the Collapse Prevention performance level (before point C), the ultimate deformations shows significant dispersion in experimental cyclic tests (e.g. reinforced concrete). Consequently, appropriate acceptance criteria for different performance levels and for different materials can be found in seismic codes (ASCE 41-13, FEMA, Eurocode, EN 1998-3, etc) or in other technical literature using model safety factors to scale down the proposed mean values to mean plus standard deviation ones.
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I have seen in literature and myself experienced high ductility in some pulse electrodeposited Ni and Ni alloys such as Ni-Co and Ni-W thin films. This high ductility is due to the superplastic behavior of these thin films with ultra fine grain microstructure of grain size <50 nm. As per literature, this property is attributed to the grain boundary sliding mechanism of these ultra fine grains. However, I seen most of this literature about super plasticity of pulse electroplated thin films on FCC metal thin films such as Ni, Cu and there alloys.
My main question is whether the crystal structure, slip systems etc. matters for achieving superplastic behavior in electroplated thin films or just an equiaxed ultra fine grain structure is required with a random texture?
If we only require an equi axed UFG structure to achieve super plasticity, then can we pulse electrodeposit any brittle thin films such as CdTe, InSb or Bi2Te3 with some enhanced ductility?
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Ok
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In order to run a ductile damage simulation and determine stress triaxiality and failure strain for AISI 304L, we need to test several notched flat specimens of the same material. How can we select these specimens? I mean parameters like thickness and notch radius?
We use a plate with thickness of 12 mm for forming simulation
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Consider material as D3 material and following are the properties I am looking for:
Mechanical
· Young’s Modulus
· Poisson’s Ratio (NU) 
· Shear Modulus (G)
· Structural Damping Coefficient (GE)
· Mass Density (RHO)
Stress Strain Related Properties
· Stress-stain (H)
· Initial Yield Point
· Initial Fraction Angle
· Exponent
· Strain Rate Level
Strength Properties
· Yield Strength
· Ultimate tensile strength
· Tsai-Wu Interaction Coefficient
Strength Limit
· Tension (ST)
· Compression (SC)
· Shear (SS)
Strain Limit
· Tension (XT)
· Compression (XC)
· Shear (XS)
Durability
· Fatigue Strength Coefficient
· Fatigue Strength Exponent
· Fatigue ductility Coefficient
· Fatigue Ductility Exponent
· Cylindrical Yield Strength
· Cylindrical Strength Coefficient
· Cylindrical strain Hardening Exponent
· Fatigue Limit Strength in Bending
· Fatigue Limit Strength in Torsion
Formability
· Work Hardening
· Forming Limit
· Plastic Strain Ratio
· Initial Strain
· Hardening Exponent
· Strength Coefficient
Thermal
· Temperature (TREF)
· Specific Heat (CP)
Electromagnetic
· Electrical conductivity
· Resistivity
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Harsha:
As heat treatment can dramatically change the microstructure and phases present, together with their distribution and in many cases with their crystal structure, most of the properties that you mention will change. In particular, in your list, the mechanical properties, stress-strain related properties, strength limit, strain limit, durability and formability will be affected, with the notable exception that the elastic properties - Young's modulus, Poisson's ration and Shear modulus - will only be marginally changed, if at all. I doubt if there will be much effect either on the thermal and electrical properties in this steel, but the latter can be sensitive to variations in the defect population and to the presence of small precipitates. However, steels are obviously good thermal and electrical conductors and so any change due to heat treatment will likely be marginal.
However, as heat treatment is invariably used to change the plastic deformation properties, and tool steels can be extremely brittle (if not heat-treated properly), it is essential that you perform the heat treatment correctly - presumably you will need to quench and temper the steel - in order to get the desired combination of strength and ductility.
ROR
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It has been reported that materials with both high strength and ductility could be produced through adding impurity elements. Mass production is however very difficult. Why and how could this be improved?
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Strength-ductility trade-off is a big challenge in materials field. Recently, many interesting works have been conducted to overcome this issue. One of the important group of alloys are high entropy alloys (HEA) and its derivatives. They show remarkable strength and ductility combination at room temperature. From, iron-carbon alloy family, TWIP steel also showed some remarkable hardening. Interestingly, TWIP steel and HEAs can be mass produced by conventional methods. Casting, solution annealing, hot working and cold working of HEAs are possible. There should be many works available in literature which talks about mechanical behavior of HEAs and hot deformation characteristics of HEAs. To me it looks like in future it will be possible to mass produce these high strength-ductility materials. I can share with you one of our work on CrCoNi HEA :
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I was wondering what the difference is between the glass transition temperature and the ductile/brittle transition temperature? I know that Tg is the temperature where a polymer will go from a glassy state to a viscoelastic state. From my understanding when a polymer is under the Tg value it will be brittle and glassy. When a polymer is above the Tg value it will act rubbery and ductile. Is this correct?
I also know that the ductile/brittle transition temperature is the minimum temperature in which a material has the ability to absorb a specific amount of energy without fracturing. In other words it is the temperature in which a material will fail and crack because it has become so brittle.
I am just getting confused because I am trying to determine the temperature at which polyethylene will crack in the freezer and I don't know which value to use. For example, polyethylene has a glass transition temperature of -90°C, but it can crack if it is in a temperature of -70°C (DBTT). It does not make sense to me that polyethylene would crack while it is still in the viscoelastic state.
If anyone can explain the difference and clarify this up for me that would be great. Also, if anyone knows what value I should use to determine the cracking point of polymers due to freezing please let me know. Thanks!
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Dear Elizabeth,
There are some relations between glass transition and ductile/brittle transition which depends on the type of the polymers. They me be the same or there are some mathematical equations between Tg (glass transition) and Tb(brittle transition). It needs to explain with some graphs and mathematical equation.
I have attached some articles and one text which explain in details. I hope they would be useful.
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I am modelling an impact on a Ti64 block. The impacting particles are rigid and the Johnson-Cook material has been used for the block.
I am wondering how to calculate erosion; I want to analyze the effect of impact angle, and I know it from experiments, where the erosion increases as the angle increases and reaches a peak in around 40 degrees and then it begins to decrease as the angle increases. But, using SPH, it just increases and reaches its peak around 90 degrees; as a matter of fact it behaves like a brittle material rather than a ductile matterial. I use Vol Fail in post processing to calculate erosion, giving the Effective plastic strain a threshold of 0.14. But the results do not correspond to those of experiments. Is there another way to calculate erosion or the problem is with the modelling?
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You may want to use the damage parameters in Johnson Cook model instead of defining only the plastic strain as the failure criteria.
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Im trying to model the failure of polycarbonate using the Johnson-cook model for ductile metals in Abaqus, I have found literature in which the parameters for the constitutive equation were given, but I havent found any resource with values for the fracture model, does anyone have any knowledge or could point me in the right direction?
Cheers!
Alex
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Dear Alexander,
Refer this paper for your query.
The strain rate sensitivity of the yield stress fell into two behaviors, either a progressive increase in terms of strain rate or an increase with a transition in the intermediate strain rate range. It can relate materials constant idea using model.
Ashish
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In the ductile materials, the reversed yielding helps in absorbing energy and facilitating the fatigue crack propagation. How does the crack propagate in brittle materials where such a mechanism is unavailable?
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Brittle solids containing cracks are thought to be highly risky for engineering applications. Cracks accelerate failure and add to the complexity of failure prediction, thus causing many disasters. stress intensity factor (SIF) by Irwin (1957), who set up the crack propagation criterion in linear elastic fracture mechanics (LEFM); J-integral (Rice, 1968) in elastic plastic fracture mechanics (EPFM); and fracture process zone (FPZ) models (Bazant and Cedolin, 1979, Hillerborg et al., 1976). Popular continuum-based numerical methods (e.g., the finite element method (FEM), finite difference method (FDM), boundary element method (BEM), and numerical manifold method (NMM) often use the SIF as the most widely accepted criterion, which can be calculated by the J-integral, the stiffness derivative method (Parks, 1974), or methods based on nodal displacement near a crack tip (Fu et al., 2012). However, the calculation of the SIF in the presence of pre-existing cracks or near boundaries is inaccurate. Moreover, the SIF is difficult to determine in a non-homogeneous material, although solutions are found in functionally graded materials
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Dear All
Anyway can you provide (if available) any document/ research paper/any industrial case study the Impact/effect of “beryllium” addition in ductile iron melt, or anybody worked on this ? I shall be happy o get this information or any reference document,
Regards
Amitava Sengupta
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„Beryllium has been added to austenitic cast iron in amounts up to about 4%, where it greatly increases the tempering resistance of austenite and its hardness through the uniform precipitation of beryllium carbide (Be2C)“. Eugen Piwowarsky: Hochwertiges Gußeisen: seine Eigenschaften und die physikalische Metallurgie seiner Herstellung (High quality cast iron: its properties and the physical metallurgy of its production) Springer-Verlag, 02.07.2013 (e-book)
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I am looking about any useful review paper about fracture mechanics (brittle and ductile)....Have one you any suggestions?
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Ahmed:
The topic of fracture mechanics is somewhat broad to describe in one review paper but there are several books that I can recommend. The first book written on the topic was John Knott's Fundamentals of Fracture Mechanics (Halstead Press, 1973) which I can send you a copy of, if you want it. However, by far the best recent text is Ted Anderson's Fracture Mechanics: Fundamentals and Applications (CRC Press, now in its 4th ed., 2017). This is a truly educational description of the mechanics of linear elastic and nonlinear elastic fracture mechanics - there's not too much on the materials science of fracture, but his description of the mechanics is excellent.
ROR
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Why cannot a direct conversion be made between the ductility measures of elongation and reduction in area using the assumption of constant volume?
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In principle, you can directly correlate these two parameters until the volume constancy is maintained during tensile deformation, i.e., up to the UTS level or the uniform elongation values. Beyond, this level volume constancy is lost due to generations of voids/cracks within the materials and the deformation becomes highly localized and non-uniform (the so-called "necking" phenomenon). Once necking occurs, the necked area deforms under a complex triaxial state of stress, the elongation becomes very sensitive to specimen geometry and gauge length.
On the contrary, RA, at least in principle, is independent of the specimen gauge length.
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I'm working with Strenx 700 Steel. It is a low carbon steel (0.12% wt carbon). I'm looking for good heat treatment in order to improve its ductility.
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Hi, I investigated some different routes to optimize the mechanical and also corrosion properties of low carbon steel with 0.12% C. It may be helpful.
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1_ is the deformation based method ( that depend on the deformation at the ultimate load and the deformation at the steel reinforcement yielding) suitable to calculate the ductility for the flexural concrete members that reinforced by two types of reinforcements such as the conventional steel reinforcements and the FRP for example? and why?
2- what is the difference between the deformability based method that proposed by Jeager (1995) and developed by the (CAN/ CSA S-806 12) and the energy baesd method that suggested by Naaman and Jeong?
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Hi, FRP is an elastic high strength brittle material but since it ruptures in very high loads, it allows the RC member bends without facing shear failure.
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Wanted to compare the behaviour between ductile and non ductile detailed RCC frame specimen
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Finite element analysis using any open source or commercial software
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Hi,
I was wondering the things shown in the title.
As you know, pure Li metal has some ductility and it adhere on other metal such as steel, copper etc. when i put some pressure on Li and other metal layers. anybody knows the mechanism or principle of this? i tried giving pressure (stainless steel roller) on the stacking of Li and copper or stainless steel to have bimetal brazed layers, and the reproducible is every day different. it is like, one day it just adhere with small pressure that i feel like even Li surface is sticky, and the other day it never adhere on the substrate. i tested temperature control and it looks not that much concerned. i also tried tin plating on stainless steel substrate before and Li plating directly on the stainless steel as well. In parallel, i should set up this way.
if anybody knows this, please let me know.
thanks
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Fracture surface after Uni-axial tensile testing of pure aluminium sub-size tensile specimen shows the presence of elongated dimples instead of equi-axed dimples. What could be the reason behind this? Does it imply that the material failed by shear?
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Akash:
It depends on the size and geometry of your test specimens.
Elongated dimples which form in shear are very common in uniaxial tensile test fracture surfaces. The classical example is the "cup-and-cone" failure mode. In the center of the samples - the "cup" - where the stress-state is dominated by the applied tensile stresses, the process of ductile dimple formation occurs by microvoid coalescence, i.e., voids nucleate at particles (either by the particle cracking or separation at the particle/matrix interfaces); these voids then grow, primarily driven by the triaxial stresses at the center of the sample, until they coalesce or more likely the separating ligaments between the voids "neck down" due to plastic instability. Nominally the same process occurs near the surface of the sample - the "cone" - but now the process is dominated by the near-surface shear stresses. The result is the coalescence of voids formed around particles in shear, which naturally results in elongated dimples.
As you describe your aluminum sample as "sub-size", it is highly likely that the process of microvoid coalescence is dominated by the near-surface shear stresses, in which case elongation dimples would be the result.
ROR
P.S. It is interesting to note here that the formation of dimples both in tension and in shear can even occur at the center of a uniaxial tensile sample in the "cup" region. In many low-alloy steels, the initial voids responsible for their microvoid coalescence ductile fracture are formed at inclusions, e.g., MnS inclusions which readily debond from the matrix. These voids then grow under the triaxial stresses, as described above, but the necking down between these larger voids by a plastic instability can occur by shear-induced microvoid coalescence of cracks in the much smaller carbide particles. The latter is know as a void sheet instability.
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As per multiple sources, a seismic event happened on 2019-12-20 11:39:52 (UTC) which jolt Afghanistan, Pakistan and even parts of India. The epicenter of the event was 51 km of Jarm, Afghanistan(36.534°N 70.437°E210.2) with an intermediate focal depth of 210.2 km and a magnitude of 6.4..
I was wondering that at a depth of 200 km in the upper mantle, the temperature ranges between 900 to 1600 F. At this temperature it is assumed to be ductile natured lithosphere. But for generation events like this, we would need solid and brittle. the lithosphere. How the lithosphere maintains its solidity at such depth and temperatures and a brittle mood fault like feature can accumulate such huge stresses which can produce such devastating earth quacks??
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Dear colleagues, thank you very much for your interesting question and answer.
I trying to give another explanation to the Mukhtiar´s question, may I share this work of Hagen and Azevedo entitled “Deep and Ultra-Deep Earthquakes Worldwide, Possible Anomalies in South America” in which the authors explain the possible origin of the ultra-deep earthquakes that occur in South America.
I suggest you pay attention to the fact that, although there are more than a few places in the world where there are phenomena of ultra-deep earthquakes, statistically only in three of them the authors can it be alleged that they are such as a systematic phenomenon: the border of the Pacific Ocean that include the North Pacific, South Pacific, and South America.
Also, please, pay attention that in the South America study-case, the ultra-deep earthquakes happened in the interior of the continent. Hagen and Azevedo explain that the reason for those existences was an anomaly created in the asthenosphere as part of the process of the South America collision with the Nazca plate. They proposed that South America has a lithospheric-slab buried in the region with an approximate depth between 500 - 670 km.
Although beyond the scope of this answer, it would be interesting to observe that the southernmost limit in South America of ultra-deep earthquakes is interpreted as the boundary of the “flat-slab subduction”, a phenomenon that ultimately favors Andean growth and uplift, e.g., Espurt, N., F. Funiciello, J. Martinod, B. Guillaume,V. Regard, C. Faccenna, and S. Brusset (2008), Flat subduction dynamics and deformation of the South American plate: Insights from analog modeling, Tectonics, 27, TC3011, doi:10.1029/2007TC002175.
Best regards,
Mario E. Sigismondi
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Dear all,
it is said that, Toughness, in contrast to resilience, is how much energy can be absorbed and still keep going. In the case of materials, the amount of energy that the material can absorb plastically before fracturing is the toughness.In the figure below, we can see that a material can have a high tensile strength (ceramics) and yet have a small toughness. In addition, materials can be extremely ductile (unreinforced polymers) and also have a small toughness. So, a large toughness (metals) is obtained by having a high tensile strength and a high ductility. My question is, can this be applied to soil diagrams as well? Do you know any paper that addresses this?
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Dear Mohamad Jamali moghadam, I think it is done via a damping process used in soil mechanics, similar to the technique used for oil exploration by geophysisists. My Regards
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In EC8, for the response-history analysis, in the first step the raw ground motion record must be scaled to S*ag , for the site of interest. Then, the ground motion record should be matched to the elastic spectrum. For instance, If I want to account for a ductility factor q=2, is it correct to multiply with 0.5 the matched record in the load combinations, in order to account for the ductility.
Another option whould be to match the raw groud motion record to the design spectra for q=2, and then use the matched record (unfactored) in the design. However I am not sure if this is correct.
Any advice/guidance will be greatly appreciated.
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Mohamed,
Thank you for taking the time to send a detailed answer to my question. Your explanation is much appreciated.
I am intending to do the linear time history analysis for the problem. The behaviour factor (q) that I am using is this analysis is taken as 1.5 or 2, case for which EC8 allows an elastic analysis of the structure. As you mentioned to reduce the maximal ground acceleration, can I simply divide the raw ground motion record with the q factor before performing any matching with the target/elastic spectra (I am using SeismoMatch for this step), or it would be more appropriate to obtain the matched ground motion and then to reduce the seismic input in the load combinations.
Kind regards,
George
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Good afternoon,
My question is on what are the recent advancements and improvements in the estimation of ductility demand and behaviour factor relations? Of course we have Miranda and Bertero (1994), we have Priestley, Calvi and Kowalski book on DDBD etc, but what are the new findings in the last 5 years?
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Good afternoon.
I recommend a recently published research on the state of the art of equivalent viscous damping.
Any questions are available
best regards
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Hello,
I am modelling a vascular tissue (intima) cut by a sharp instrument in Abaqus. The scheme of my model in on the picture. The instrument will be translated and simultaneously oscillated with ultrasonic frequency. The tissue is cut just below the metal stent struts.
I can figure out the nonlinear properties of my tissue (Mooney-Rivlin coefficients deduced from experimental data of simple tension) and the loading conditions but the problem is - how to define damage properties for soft tissue in Abaqus? More precisely, I want to find out what “material behaviours” in material definition should I introduce except for the "mechanical-elasticity-hyperelastic".
All the "cutting" models I've found use “Johnson-Cook formulation” or “Ductile damage” but I think they are only for metals. “Traction-separations laws” can’t be implemented because they require the predefined crack path and it is not possible because I can’t predict this path.
This problem is more similar with a “bullet impact in gelatin” – the material is damaged by an instrument but the instrument can be translated in course of the impact https://www.sciencedirect.com/science/article/pii/S175161611630412X
I tried to make the research by myself but I still have several questions:
1. As I have the complete test data maybe it is sufficient for damage modelling to indicate elastic and plastic behavior of the tissue?
2. What “material behaviours” would you recommend me to define in this case?
Thank you in advance,
Nikita.
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Thank you very much! It is indeed the method that I finally used.
Unfortunately, this type of model (with inserted cohesive elements) is not working for unhomogenoius materials so if you have any advice or solution - it would be very helpful!
The problem is the following: when I add another material inside the model with inserted cohesive elements it does not complete because of аn exessive deformation ratio or distortion of elements. I give two examples below:
1) the vascular tissue with holes calculates perfectly
2) the vascular tissue with a metallic stent in these holes gives deformation in the bottom of the model (wrong place) and the analysis ends with an error.
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I am currently working on post-earthquake retrofitting of non-ductile and ductile RC frames experimentally...is it possible to numerically simulate them in SAP2000? How would I retain the damaged frame in SAP2000 for retrofitting?
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I have prepared the damaged model in SAP2000 by splitting the member where the damage has occurred. The stiffness has been reduced up to the point of failure. Now how should i retrofit keeping in view the splitted parts of member.
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do someone has any resource about repairing leakage in as cast pipe and fittings?for example welding, powder or polymer repairing agents.
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Dear Mehardad,
Blowhole is a cavities defect always located in the cope part of the mould in poorly vented pockets and undercuts. Blowhole is divided into pinhole and subsurface blowhole type. Pinhole is very tiny hole while subsurface blowhole only can be seen after machining. Reason, gases entrapped by solidifying metal on the surface of the casting, which results in a rounded or oval blowhole as a cavity associated with slag’s or oxides. Sand inclusion, sand burning, cold lap or cold shut, misrun, gas porosity, mismatch defects, distortion , thermal defects can occur during welding. Possible causes are due to Inadequate core venting, excessive release of gas from core, excessive moisture absorption by the cores, low gas permeability of the core sand, moisture content of sand too high, or water released too quickly, gas permeability of the sand too low sand temperature if too high, bentonite content if too high and too much gas released from lustrous carbon producer. by reducing this all causes blowhole in ductile iron welding can be stopped.
Remedies
Improve core venting, provide venting channels, ensure core prints are free of dressing, Reduce amounts of gas, use slow-reacting binder and reduce quantity of binder. It is better to use a coarser sand if necessary (soft sand permeability problem), apply dressing to cores, thus slowing down the rate of heating and reducing gas pressure, dry out cores and store dry, thus reducing absorption of water and reducing gas pressure, reduce moisture content of sand, Improve conditioning of the sand, reduce bentonite and carbon carrier content, reduce sand temperature, installing a sand cooler if necessary etc.
Hope it help you out.
Ashish
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Hello
I have a project with this title "investigation of burst Pressure in a Pressure vessels based on the ductile Damage Criterion". and we decided to use Lemaitre criteria for this simulation, to  reach this goal I need  to write VUMAT subroutine in abaqus , but I don't have any information on how to write this code or about its parameters, i need a template of VUMAT subroutine or a complete example of vumat or a file that completely describe how to write this user subroutine. Please help me  best regard I am Arkan from Tehran, Iran
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go through the link
i will explain the constitutive relation and the corresponding VUMAT.
hope this help
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is there any example of a ceramic that is ductile at its bulk form?
if yes, then how is it possible? why ceramics' brittleness explained for dislocation immobility in terms of differently-charged ions do not hold here?
can geopolymers be as ductile as their organic counterparts at sufficiently high temperature?
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  1. The two most common chemical bonds for ceramic materials are covalent and ionic. For metals, the chemical bond is called the metallic bond. The bonding of atoms together is much stronger in covalent and ionic bonding than in metallic. That is why, generally speaking, metals are ductile and ceramics are brittle.
  2. metallic bond can increase ductility.