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Ductility - Science topic
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Questions related to Ductility
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 ?
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

Is there any specific relationship between elongation percentage and dimple size during ductile failure?
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
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?
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.
How do these effects change when the surface layer becomes ductile at high temperature?
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.
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?
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
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.
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?
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?
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
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




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.
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?
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.
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.


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.
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
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.
What are their significance in measuring ductility? If they are different then why they are?
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
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?
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?

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.

If the fracture stress of one piece is higher than its yield stress, does it brittle fracture or ductile?

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
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?
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?


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
Is it possible through "hardening" process? Also, how it could change the microstructure of α-ferrite ?
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
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?
Including the full range of ductile, hard, brittle alloys and composite materials.
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?
All these are refractory Metals with higher than 2450 deg C melting point.
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?
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.
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.
waste gypsum is used to stabilize the mud block. will it be helpful?
additive manufacturing,deformation,metals
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
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?
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?
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.
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
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.
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.
If we increase or decrease the ductility of 1060 grade aluminum tube then then what is the effect on the corrosion property.
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 ?
The target is removing or decreasing free carbon on the external surface of gray and ductile iron.
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?

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.
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?
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?
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
I'm wondering which type of casting defect has happened and what are remedies?

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
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
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
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.
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.
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...!!!
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!


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.
I want to determine the percentage of ductile and brittle fracture for some samples from impact test.
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?
How does it lead to Strengthening but not at the cost of ductility.?
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
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?

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.
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.





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.


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?
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
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
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?
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!
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?
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
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?
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
I am looking about any useful review paper about fracture mechanics (brittle and ductile)....Have one you any suggestions?
Why cannot a direct conversion be made between the ductility measures of elongation and reduction in area using the assumption of constant volume?
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.
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?
Wanted to compare the behaviour between ductile and non ductile detailed RCC frame specimen
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
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?
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??
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?

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.
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?
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.


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?
do someone has any resource about repairing leakage in as cast pipe and fittings?for example welding, powder or polymer repairing agents.
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
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?