Mechanics Channel by Mark Barkey
Mechanics Channel by Mark Barkey
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Відео

AEM535-FEA 01-2022_24inch_schedule80_Hypermesh
Переглядів 5042 роки тому
Creation of schedule 80 Pipe; 24 inch OD; updated for Hypermesh 2022
AEM250 distance introduction FA23 SP24
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For AEM 250-distance students to see how to access the course shell (Blackboard) and explain how the course will be conducted.
AEM 637 plotting plate with crack stress distribution
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plotting crack tip stress field; range of applicability; comparison to plate with a hole
AEM 637 plotting plate with hole stress distribution
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using excel to plot stress distribution for elasticity solution of an infinite plate containing a hole
AEM 637 Problem 5 4 18 Part A
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AEM 637 Problem 5 4 18 Part A
AEM 637 Problem 5 4 18 Part B
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AEM 637 Problem 5 4 18 Part B
AEM 637 Problem 4 18 6
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Checking 3-D elasticity equations for Mechanics of Materials stress/strain fields
AEM 637 Problem 4-7.1
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Theory of Elasticity: Deformation fields for tension-torsion stress state.
AEM 637 Problem 4-19.4
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eigenvalues and eigenvectors for elastic torsion problem, circular cross-section
AEM 637 Problem 3 4 1
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example problem
AEM 637 Problem 3 3 7
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example problem
AEM637 generalized plane eigen problem example
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AEM637 generalized plane eigen problem example
AEM 637 Problem 2-16.2
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Example problem/homework problem, determination of displacement fields from strain fields; plane elasticity; small strains; system of partial differential equations
AEM 637 overview for distance students
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AEM 637 overview for distance students
648 2021 final hints part 5
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648 2021 final hints part 5
648 2021 final hints part 4
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648 2021 final hints part 4
648 2021 final hints part 3
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648 2021 final hints part 3
648 2021 final hints part 1
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648 2021 final hints part 1
648 2021 final hints part 2
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648 2021 final hints part 2
2021 Plasticity normality flow rule in regular stress space
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2021 Plasticity normality flow rule in regular stress space
2021 J2 flow theory uniaxial part2
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2021 J2 flow theory uniaxial part2
2021 J2 flow theory uniaxial part1
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2021 J2 flow theory uniaxial part1
AEM250 Overview Fall 2021
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AEM250 Overview Fall 2021
29 structural yield surface
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29 structural yield surface
28 Intro to multiaxial plasticity for fatigue analysis
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28 Intro to multiaxial plasticity for fatigue analysis
26 dicussion of Socie multiaxial fatigue damage
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26 dicussion of Socie multiaxial fatigue damage
25 introduction to multiaxial fatigue
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25 introduction to multiaxial fatigue
24 4 30 partial solution cyclic neuber
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24 4 30 partial solution cyclic neuber
23 vehicle design process and proving grounds
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23 vehicle design process and proving grounds

КОМЕНТАРІ

  • @raniyanausheenbaker
    @raniyanausheenbaker 19 днів тому

    Thank you

  • @dendisephanie4974
    @dendisephanie4974 25 днів тому

    the value on point A = 500, is this assumed or can be determined before?

  • @thamerhazber
    @thamerhazber Місяць тому

    I want the pdf of lecture please

  • @solomonidowu340
    @solomonidowu340 2 місяці тому

    Thank you so much for this content, Prof. Pls, how can I join or visit your personal website website to get the material file used in this lecture. Awaiting your response, Sir.

  • @SagarBangera-em7yw
    @SagarBangera-em7yw 2 місяці тому

    which book do you refer sir ?

  • @stitaswain7349
    @stitaswain7349 4 місяці тому

    Thank you so much for great kectures. Just a ailly doubt i always havea is whatbis the difference between in the subjects theory of elasticty\plasticity and continuum mechanics?

    • @mbarkey.mechanics
      @mbarkey.mechanics 4 місяці тому

      Continuum Mechanics is a general approach for all continuous media--solids, fluids, deformable dynamic bodies, etc. You can think of elasticity being continuum mechanics specialized to elastic materials, and likewise plasticity. Historically, however, elasticity and plasticity come first; then the more generalized framework of continuum mechanics was developed.

  • @kar-dt1hk
    @kar-dt1hk 5 місяців тому

    can you please send me this inp file ,

  • @senecastevens3399
    @senecastevens3399 6 місяців тому

    why do we also multiply by the transpose?

  • @Vassilis-dt1ru
    @Vassilis-dt1ru 6 місяців тому

    this was a great video and a solid explanation, I was looking for a way to always find the principal directions for the saint venant problem !

  • @ing.erickosorio2887
    @ing.erickosorio2887 6 місяців тому

    Hi professor Berkey, I have a quick question, I find your courses really interesting keep up the good job. My question is, what is the source or reference for the SN curve equation you showed for steel Ferrus metal (1.62*Su*N^-0.085). And also would that be a feasible equation for assessing the fatigue of a steel plate? Thank you so much.

    • @mbarkey.mechanics
      @mbarkey.mechanics 6 місяців тому

      I don't recall the original source, but I lectured from Bannantine, Fundamentals of Fatigue Analysis. It would be referenced there. It is an equation you might use if nothing else is available. If you have actual data then use it. Happy studies.

  • @sagarjaiswal2448
    @sagarjaiswal2448 6 місяців тому

    It was a great explanation. I am wondering why the components of shear stress in radial direction is not considered? As its also making angle dtheta from the radial direction.

  • @rajendraganguli7790
    @rajendraganguli7790 7 місяців тому

    Sir,, Volume is very low , can you please try to improve it

    • @mbarkey.mechanics
      @mbarkey.mechanics 7 місяців тому

      Sorry, I am not able to remake any videos at this time and any post processing improvements that I could do are also ones that you could do. Happy Studies!

    • @rajendraganguli7790
      @rajendraganguli7790 5 місяців тому

      @@mbarkey.mechanics ok Sir.. and Thanks for the great video, it helped me.

  • @mitchellngwena4142
    @mitchellngwena4142 7 місяців тому

    Thank you very much sir your content has been helping a lot lately in my studies

  • @RDunya
    @RDunya 8 місяців тому

    Thank you so much for taking the time to share your knowledge with us.

  • @ompabaletserametse8643
    @ompabaletserametse8643 8 місяців тому

    Thanks !

  • @mishrashubham7659
    @mishrashubham7659 8 місяців тому

    Hi Mark Barkey, that's a very classic explanation there. I would love to know more about your work in this field for my comprehension.

  • @vilivont4436
    @vilivont4436 8 місяців тому

    Great lecture, thanks a lot.

  • @mustaphachiad
    @mustaphachiad 9 місяців тому

    Thank you Sir for this interesting fatigue course

  • @shravanbhadoria4104
    @shravanbhadoria4104 9 місяців тому

    Thanks Dr. Mark.

  • @komaldipen
    @komaldipen 9 місяців тому

    put your mibile number here.

  • @shravanbhadoria4104
    @shravanbhadoria4104 9 місяців тому

    Sir, if the body undergoes pure translation and rotation then will the Jacobian be 1? Since the body has not undergone any deformation that is d(xi) = dx, which means the J should be 1. Please provide your input on this. Thanks!

    • @mbarkey.mechanics
      @mbarkey.mechanics 9 місяців тому

      (rigid) Translations are easy to see that J=1. You have to be careful with equations for rotations.. If the equations are not written in a certain way, you may not notice that the points go through a rigid rotation. You have to be careful with standard FEA codes. Explicit codes would usually account for large deformations and translations.

  • @ing.erickosorio2887
    @ing.erickosorio2887 9 місяців тому

    Hi professor Barkey. How can we tell when we have a stress singularity rather than a real stress concentration? I've run FEA models where I always get a crazy amount of stress in connections between elements. But those are really small localized points, some people ask me to crazy reinforced those areas to see if we can get rid of the high peak in stresses. In my mind that peak would not be important since it's in very small localized point and probably von mises it's not even applicable due to the constraint in connections and the possible development of tri axial state of stress. What do you think about it ? how would you approach those issues? Thank you so much

    • @mbarkey.mechanics
      @mbarkey.mechanics 9 місяців тому

      Crack like stress distributions are distinctive. You can see some in the next series of examples. Connections, MPCs, and point constraints can all cause local stress disturbances and are hard to alleviate. Auto companies will often use standard element sizes and connection techniques so that they deal with known modelling errors.

  • @BillelHamza-ck2vx
    @BillelHamza-ck2vx 9 місяців тому

    Dear Prof Mark, first Thanks a lot for your videos, I have a small question.. at 22:20 what does it mean look at half life and why?

    • @mbarkey.mechanics
      @mbarkey.mechanics 9 місяців тому

      If the specimen lasted 50,000 cycles, the half-life would be 25,000 cycles. Most materials would be stabalized by then and you would examine this hysteresis loop. Of course, to find the half-life cycle, you must first test to find the failure cycles.

  • @JMTechnicalCornerexploration
    @JMTechnicalCornerexploration 9 місяців тому

    Thank you very much for your fruitful lectures. Could you please give me your email address? Actually I am working on fatigue analysis of mooring line. I have already got load history. But i can't determine the number of cycles as i have several same stress levels in diagram. I would be grateful if you give me your email address. Thank you

  • @vilivont4436
    @vilivont4436 9 місяців тому

    Great.

  • @vilivont4436
    @vilivont4436 9 місяців тому

    Great lecture, thank you a lot.

  • @nicolaspinto822
    @nicolaspinto822 9 місяців тому

    legend

  • @armelledecameracafe1640
    @armelledecameracafe1640 9 місяців тому

    Does the method for closing the non closed hysteresis loops (from 15:) is equivalent to apply the rainflow counting to the mirrored signal ?

    • @mbarkey.mechanics
      @mbarkey.mechanics 9 місяців тому

      By mirrored signal, do you mean repeating it back to largest peak? If so, no, since for unclosed loops the damage is usually taken to be one-half the closed loop damage. If you mean something else, let me know. But I don't think any method of artificially closing unclosed loops and counting half damage would be like any other technique.

  • @shravanbhadoria4104
    @shravanbhadoria4104 9 місяців тому

    Thanks Prof. Mark!

  • @pging8328
    @pging8328 9 місяців тому

    Thanks for your video. It looks like it requires a lot of manual calculation. Is there a table of these figures readily available for each different type of beam?

    • @mbarkey.mechanics
      @mbarkey.mechanics 9 місяців тому

      yes, for standard shapes there are tables. However, by understanding the calculation, you can learn why the beam is designed the way that it is.

  • @brianjo9945
    @brianjo9945 10 місяців тому

    Thank you

  • @이대영-x9v
    @이대영-x9v 10 місяців тому

    Thanks that you give me such a nice lectures. I feel that your ingenuity enlighting every dark corners of my knowledge.

  • @bayikancanozturk
    @bayikancanozturk 11 місяців тому

    thank you

  • @bayikancanozturk
    @bayikancanozturk 11 місяців тому

    Thank you so much!!

  • @emreercelik
    @emreercelik 11 місяців тому

    wonderful lecture, thank you professor.

  • @vilivont4436
    @vilivont4436 11 місяців тому

    Great lecture.

  • @aliejax6343
    @aliejax6343 Рік тому

    Dear Sir, thank you very much for very useful lectures. I have a question if you could please answer. For a case of simply supported beam subjected to UDL, the moment is zero at the supports but when writing boundary conditions are vertical faces near supports, we take the integration of bending stresses equal to zero. Why cannot we directly put bending stress expression to be equal to zero? Thank you in anticipation.

    • @mbarkey.mechanics
      @mbarkey.mechanics 11 місяців тому

      I think the answer you want is based on the mathematics: We have taken a 3-D problem and reduced it to 2-D, then invoked a stress function approach to make that math easier...so we have given up some elegance for practicality. But consider the deeper philosophical answer: even our 3-D problem is a representation of what we think of reality...find a actual simply supported beam with a uniform distributed load and look at the supports--which are a finite width--what location there has a totally zero bending stress distribution? Maybe that approximation of no net resulting bending moment is OK after all! We can continue this discussion through to finite element analysis, and I can counter with relativistic mechanics and quantum mechanics. And even then we end up with the same question--is our simplification good enough?

    • @aliejax6343
      @aliejax6343 11 місяців тому

      @@mbarkey.mechanics thank you Professor. I get it now

  • @aliejax6343
    @aliejax6343 Рік тому

    Dear Sir, thank you very much for very useful lectures. I have a question if you could please answer. For a case of simply supported beam subjected to UDL, the moment is zero at the supports but when writing boundary conditions are vertical faces near supports, we take the integration of bending stresses equal to zero. Why cannot we directly put bending stress expression to be equal to zero? Thank you in anticipation.

  • @vilivont4436
    @vilivont4436 Рік тому

    Really great lecture, thank you a lot.

  • @mrmagoo-i2l
    @mrmagoo-i2l Рік тому

    Excellent videos, I hope you haven’t given up making them.

    • @mbarkey.mechanics
      @mbarkey.mechanics Рік тому

      Thanks. In my current role as Department Head, my duties have not allowed as much time for video development...but I will get back to it some day again. Happy Studies.

  • @gulafshabhatti9410
    @gulafshabhatti9410 Рік тому

    Thank you for amazing explanation. Can you please refer me a book for this.

  • @aliyyekara6135
    @aliyyekara6135 Рік тому

    I am thankful for your lecture series Professor. Your lectures are very instructive, helpful, amazing.

  • @NOVERDOSAPUTRA
    @NOVERDOSAPUTRA Рік тому

    may i know, what is distance between base plate and bottom of column

  • @vipin3557
    @vipin3557 Рік тому

    Timestamp 28

  • @prithvi-y4v
    @prithvi-y4v Рік тому

    Can mem never be greater than 2? I have about 500points to process and there are instances where my memory is greater than 10. Also, can you please tell me how to count half cycles ?

    • @mbarkey.mechanics
      @mbarkey.mechanics Рік тому

      Yes, the memory storage for can be greater than 2. ASTM rainflow forces the start of the sequence with the largest peak (or valley) and so there would never be any un-closed loops in following this procedure. However, if you are doing 'real time' rainflow processing then there can be instances where you do not have control of the start of the time history. This case is discussed in my lectures. The usual implementation is to go ahead and close all un-closed loops and assign half damage to those loops that were artificially closed. In the German literature, this is known as a 'residue' of the time history and you can find literature addressing this in detail.

    • @prithvi-y4v
      @prithvi-y4v Рік тому

      @@mbarkey.mechanics thank you for the response! Can you please point me to the lecture which speaks about rainflow processing in 'real time'. Also for the residual cycles, is there any standard algorithm to follow?

    • @mbarkey.mechanics
      @mbarkey.mechanics Рік тому

      @@prithvi-y4v I don't remember which lecture, but the procedure is just as I have described above.

  • @DesireeLekamge
    @DesireeLekamge Рік тому

    me about to cry becasue this is so much better than my lectures( still grateful for both tho)

  • @DesireeLekamge
    @DesireeLekamge Рік тому

    Hi Mr, at 33:10, would the di be in the small circle?

  • @DesireeLekamge
    @DesireeLekamge Рік тому

    i love this page! THANK YOU, if i have any questions r u able to reply? i am studying this currently! ill look into all videos of yours.

  • @mathunt1130
    @mathunt1130 Рік тому

    Have you not thought about deriving this using modern notations? I think a lot of confusion can be avoided in this way.

    • @mbarkey.mechanics
      @mbarkey.mechanics Рік тому

      My lectures are prepared for the audience I give them to, and the notation used varies with that audience. I encourage you to make your own lectures to your satisfaction.

  • @wuxiao0715
    @wuxiao0715 Рік тому

    Great explanation! BTW, at 35:00, I think we should write duj/dei(ej)(ei), instead of duj/dui(ei)(ej).