Niraj Chawake
Niraj Chawake
  • Видео 65
  • Просмотров 242 432
17. State of Strain at a Point | Displacement Tensor, Rotation Tensor and Strain Tensor
The Basics of Mechanical Behavior of Materials
This video deals with
1. Displacement of points in continuum
2. State of strain at a point
3. Normal and Shear displacements
4. Displacement Tensor
5. Strain Tensor
6. Rotation Tensor
7. Relation between engineering shear strain and tensorial component of strain
8. Infinitesimal strain theory
Просмотров: 942

Видео

66. Creep deformation of Materials | Generalized creep equation | Deformation mechanisms maps
Просмотров 1,3 тыс.9 месяцев назад
Basics of Mechanical Behavior of Materials This video deals with 1. Generalized form of a creep equation 2. Mukherjee-Bird-Dorn relation 3. Stress exponent (n) 4. Inverse grain size exponent (p) 5. Creep mechanisms and their identification using n and p values 6. Deformation mechanisms maps
65. Creep deformation of materials | Creep mechanisms | Power law creep
Просмотров 4,7 тыс.Год назад
Basics of Mechanical Behavior of Materials This video deals with 1. Creep mechanisms 2. Diffusion creep | Diffusion based creep mechanisms 3. Dislocation creep | Dislocation based creep mechanisms 4. Coble creep | Nabarro Herring creep 5. Grain boundary diffusion and Lattice diffusion 6. Dislocation creep | Dislocation based creep mechanisms 7. Cross slip | Climb 8. Grain boundary sliding 9. Po...
64. Creep deformation | Creep in materials | Creep failure
Просмотров 4,7 тыс.Год назад
Basics of Mechanical Behavior of Materials This video deals with 1. Creep deformation of materials 2. Definition of creep 3. Creep curve 4. Stages of creep: Primary creep, Secondary creep and Tertiary creep 5. Minimum creep rate or steady state creep rate 6. Temperature dependence of creep 7. Stress dependence of creep 8. Stress exponent, Activation energy for creep 7. Power law creep
63. Fracture Mechanics | LEFM Vs EPFM | J integral
Просмотров 8 тыс.Год назад
Basics of Mechanical Behavior of Materials This video deals with 1. Stress ahead of a crack tip 2. Brief introduction to Irwin's model and Dugdale model 3. Crack opening displacement and crack tip opening displacement 4. Linear elastic plastic mechanics vs Elastic plastic fracture mechanics 5. Brief introduction to J-Integral (nonlinear strain energy release rate) 6. Fracture terminologies: Duc...
62. Fracture Modes and Stress Concentration
Просмотров 3,1 тыс.Год назад
Basics of Mechanical Behavior of Materials This video deals with 1. Different Fracture Modes: Mode I, Mode II and Mode III 2. Opening mode, Shearing mode, Tearing mode 3. Plane stress and Plane Strain condition of Fracture 4. Fracture Toughness variation due to specimen thickness 5. Notch Effect or Crack effect 6. Stress Concentration and Stress Concentration Factor 7. Notch Effect: Triaxial st...
61. Fracture Mechanics | Strain Energy Release Rate & Fracture Toughness
Просмотров 4,6 тыс.Год назад
Basics of Mechanical Behavior of Materials This video deals with 1. Strain Energy Release Rate and Critical Strain Energy Release Rate 2. Crack Extension Force 3. Stable and Unstable Cracks 4. Fracture Toughness 5. Stress Intensity Factor 6. De Havilland Comet Crash-case study-Fracture Mechanics
60. Griffith theory of fracture | Griffith theory of brittle fracture
Просмотров 8 тыс.2 года назад
This video deals with 1. Understanding the discrepancy between Theoretical Cohesive strength and experimentally observed cohesive strength. 2. Griffith consideration of inherent cracks present in materials to evaluate cohesive strength 3. Griffith's theory for brittle materials 4. Role of surface energies and relaxation energies towards fracture 5. What are Surface cracks (sharp cracks and thro...
59. Fracture & Theoretical Cohesive Strength of Materials
Просмотров 4,2 тыс.2 года назад
This video deals with 1. Some failure case examples: Aloha aircraft, Liberty Ships, Liberty bells, Titanic, the Space shuttle Columbia 2. Strength Vs Wire length (role of flaws) Leonardo da Vinci's experiment 3. Fracture surfaces 4. Theoretical cohesive strength of Materials
58. Twinning in crystals | Deformation twinning in fcc and bcc
Просмотров 4,2 тыс.2 года назад
Basics of Mechanical Behavior of Materials This video deals with 1. Slip Vs Twinning 2. Twinning in fcc materials 3. Twinning in bcc materials 4. Twinning and anti-twinning sense in bcc materials 5. Shear strain developed during twinning 6. Annealing twin and Mechanical twin 7. Stacking fault energy
57. Grain boundary model, geometrically necessary dislocations & statistically stored dislocations
Просмотров 3 тыс.2 года назад
This video deals with 1. Low angle grain boundaries (LAGB) and high angle grain boundaries (HAGB) 2. Pure tilt and pure twist boundaries 3. Edge dislocation model for symmetric tilt LAGB 4. Boundary energy with the angle of misorientation 5. Concept of geometrically necessary dislocations (GNDs) and statistically stored dislocations (SSDs)
56. Grain boundary strengthening and Hall-Petch Relation
Просмотров 4,4 тыс.2 года назад
This video deals with 1. Role of grain boundaries to resist dislocation motion 2. Dislocation pile up at boundaries 3. Model to explain Hall-Petch relation 4. Importance of friction stress and Hall-Petch coefficient 5. Utility of Hall-Petch equation 6. Inverse Hall-Petch relation 7. Critical value of grain size for retaining strength 8. Grain growth in nanograined materials even at ambient cond...
55. Grain boundaries in polycrystalline materials
Просмотров 2,1 тыс.2 года назад
This video deals with 1. Grain boundaries in a crystalline material 2. Angle of misalignment or misorientation 3. High and Low angle grain boundaries 4. Role of grain boundaries during plastic deformation 5. Equicohesive temperature
54. Precipitation hardening and Dispersion strengthening
Просмотров 4,3 тыс.2 года назад
This video deals with the 1. Precipitates 2. Formation of precipitates (includes Ostwald ripening) 3. Nature of precipitates (coherent, semicoherent, incoherent) 4. Bowing mechanism (Orowan) and shearing mechanism (cutting) 5. Dispersion strengthening Special Thanks Professor Sudhanshu S Singh
53. Cottrell atmosphere and Yield point phenomenon
Просмотров 6 тыс.2 года назад
This video deals with 1. Cottrell atmosphere 2. Yield point phenomenon and Luder's band 3. Strain aging 4. Portvin Le Chatelier effect 5. Snoek Effect
52. Solid solution strengthening and different interactions
Просмотров 2,1 тыс.2 года назад
52. Solid solution strengthening and different interactions
51. Solid solution strengthening and dislocations interactions with solutes
Просмотров 2,1 тыс.2 года назад
51. Solid solution strengthening and dislocations interactions with solutes
50. Strain hardening stages in fcc single crystal
Просмотров 4 тыс.2 года назад
50. Strain hardening stages in fcc single crystal
49. Dislocations Intersections Jogs and Kinks
Просмотров 7 тыс.2 года назад
49. Dislocations Intersections Jogs and Kinks
48. Image force on dislocations
Просмотров 1,6 тыс.2 года назад
48. Image force on dislocations
47. Stacking faults in bcc
Просмотров 1,7 тыс.2 года назад
47. Stacking faults in bcc
46. Superlattice dislocations and Antiphase boundaries
Просмотров 2,8 тыс.2 года назад
46. Superlattice dislocations and Antiphase boundaries
45. Lomer Cottrell locks
Просмотров 4,9 тыс.2 года назад
45. Lomer Cottrell locks
44. Stacking faults in FCC
Просмотров 6 тыс.2 года назад
44. Stacking faults in FCC
43. Five independent slip systems for ductility
Просмотров 1,9 тыс.2 года назад
43. Five independent slip systems for ductility
42. Frank Read Source of dislocations
Просмотров 5 тыс.2 года назад
42. Frank Read Source of dislocations
41. Dislocations Interactions, Dislocations Stable configurations and Taylor relation
Просмотров 2,4 тыс.2 года назад
41. Dislocations Interactions, Dislocations Stable configurations and Taylor relation
40. Strain hardening and dislocation interaction
Просмотров 2 тыс.2 года назад
40. Strain hardening and dislocation interaction
39. Strain energy and Line tension of dislocation
Просмотров 1,9 тыс.2 года назад
39. Strain energy and Line tension of dislocation
38. Strain energy of dislocation
Просмотров 3,1 тыс.2 года назад
38. Strain energy of dislocation

Комментарии

  • @sixy5195
    @sixy5195 12 часов назад

    It was great, thanks for the clear explanation

  • @kamalalagarsamy3783
    @kamalalagarsamy3783 Месяц назад

    In the case of edge dislocation, we extra have half plane that creates the dislocation line. In screw dislocation, what does make dislocation line?

    • @nirajchawake
      @nirajchawake Месяц назад

      In the case of an edge dislocation, you can visualize a dislocation line using an extra half-plane of atoms. Screw dislocation line is harder to imagine. I recommend looking at more pictures, videos, and simulations to better understand the displacements they (both dislocations) cause in the lattice. A straightforward way to think of a dislocation line is as the boundary between the slipped and unslipped regions. This will help to understand the nature of burgers vector and dislocation line vector.

  • @himanshushekhar4524
    @himanshushekhar4524 Месяц назад

    Sir, as you said that in some case it is difficult to identify the point Y i.e yield point, then we have to obtain the point P. In both the case there should be three point on the stress-strain curve naa??? Either A,B & Y or A B &P. Why are you showing all four point on single Stress vs Strain diagram??? And one more question is there , in case where we are unable to identify point Y, we identify the point P. The point P we call proff stress can we call it Yield stress , vice-versa????

    • @nirajchawake
      @nirajchawake Месяц назад

      Himanshu, These points are useful when considering plasticity under various conditions. Points A and B are particularly valuable for theoretical work on the onset of plasticity. In contrast, points Y and P are mainly relevant for practical applications. To fully understand the definition of yield and the utility of Point P, I recommend reading textbooks by R. M. Christensen.

    • @himanshushekhar4524
      @himanshushekhar4524 Месяц назад

      @@nirajchawake thankyou very much sir😊

  • @anjaliprajapati1204
    @anjaliprajapati1204 Месяц назад

    Very nice lectures sir. Thank you so much for taking such a wonderful lectures. I have one small request, can you please tell the refrences (books,papers etc) which you have used for these lectures.

    • @nirajchawake
      @nirajchawake Месяц назад

      I used various books on mechanical behaviour of Materials by Dieter, Meyers and Chawla, Hosford, Courtney.

  • @lallamendbruno
    @lallamendbruno Месяц назад

    Hi i dont get what happen if there is an incoherent phase, what effect does it have on the dislocation motion, does a dislocation can travel through it ? And thus what is the effect on the hardening if there is a non coherent phase ?

    • @nirajchawake
      @nirajchawake Месяц назад

      Please check this video ruclips.net/video/oqCln00adzM/видео.htmlsi=xaJ6GrRsqFyloRT_

  • @cookiemaria780
    @cookiemaria780 Месяц назад

    Thank you so much for also covering fracture mechanics!! It was a great explanation. I really enjoy all of your lecture videos! 😃😄

  • @juancarlosalvarezhostos7138
    @juancarlosalvarezhostos7138 Месяц назад

    What I do not understand is how to define the sign of \hat{t}?? Is it pointing in or pointing out the screen plane???

  • @maitreyeephukan4663
    @maitreyeephukan4663 Месяц назад

    Amazing video!

  • @zhenccc
    @zhenccc Месяц назад

    this is so helpful. clearly explained. thank you so much!!

  • @abhinavtiwari395
    @abhinavtiwari395 Месяц назад

    Sir ye topic elastic energy dislocation hai kya

  • @gauravm8152
    @gauravm8152 2 месяца назад

    Can you please make a video on what happens at atomic level during tensile testing of ductile and brittle materials (explaining all phenomena like elastic deformation, upper and lower yield point, slip deformation, necking, cup and cone fracture, etc)?

  • @wowineedyou
    @wowineedyou 2 месяца назад

    thank you! this video is really helpful, i wrote my final task about Hall-Petch relationship based on your video and got an excellent mark!

  • @kaliprasad1925
    @kaliprasad1925 2 месяца назад

    Very nice explanation.

  • @pedrodeoliveiracamargo2413
    @pedrodeoliveiracamargo2413 2 месяца назад

    Fantastic

  • @nigel3436
    @nigel3436 3 месяца назад

    tks i got it easily with ur lecture

  • @user-fd4jh9qx8y
    @user-fd4jh9qx8y 3 месяца назад

    Where can I get the solution of cubical equation?

  • @vishabjeetsingh2643
    @vishabjeetsingh2643 3 месяца назад

    Sir, b2 berger vector is flowing from slip plane to another slip plane. How is that possible? Because t2 is the dislocation line, it should have two separate planes in its both ends, one sliped and the other unslipped.

  • @clem5474
    @clem5474 3 месяца назад

    This was a great explanation.

  • @HarshYadav-qi9mm
    @HarshYadav-qi9mm 3 месяца назад

    Hello, why is it shear stress vs gamma strain, and not stress vs strain?

    • @nirajchawake
      @nirajchawake 3 месяца назад

      Our objective is to establish a connection between stress and strain behavior and the motion of dislocations. In this context, we understand that dislocations glide or slip along specific planes, resulting in shear strain. These movements are governed by the shear stress acting on these glide planes. Therefore, for simplicity, we concentrate on investigating shear stress and shear strain in this scenario.

  • @PempheroSiliyatheMrEngineer
    @PempheroSiliyatheMrEngineer 4 месяца назад

    Well explained Sir..... I got the whole concept.... Thanks

  • @sangeetkoreo
    @sangeetkoreo 5 месяцев назад

    sir at 5:05 why are you taking counter clockwise from reference line A? It will be clockwise Please clear this doubt

  • @ganapathysenthilkumar2655
    @ganapathysenthilkumar2655 5 месяцев назад

    Great lecture sir , greetings

  • @jaya622
    @jaya622 5 месяцев назад

    preparing for exams based on your lectures

  • @jaya622
    @jaya622 5 месяцев назад

    Thank you for the valuable lectures

  • @vivektripathi4832
    @vivektripathi4832 5 месяцев назад

    Thanks a lot

  • @himanshushekhar4524
    @himanshushekhar4524 5 месяцев назад

    Since Stress is function of strain. If we apply some force on a material having some certain cross-sectional area and it doesn't show any deformation (strain). So what would be stress , zero???? Or force applied divided by cross-sectional area.??

    • @nirajchawake
      @nirajchawake 5 месяцев назад

      Let's consider a steel cylinder with dimensions: length 100 mm and radius 10 mm, under a tensile load of 1 N, with an elastic modulus of 200 GPa. To determine the stress and strain, we apply basic definitions: Stress = Force/Area = 1 N / (π × 10^2) mm^2 = 0.0032 MPa Strain = Stress / Elastic modulus = 0.0032 MPa / 200 GPa = 1.6E−8 This yields a strain of 1.6E−8, which can also be expressed as the change in length/original length: Change in length = 1.6E−8 × 100 mm = 1.6E−9 m = 1.6 nm Despite being a minute value, it demonstrates that even small forces induce an elastic response in terms of stress and strain. Thus, the statement, "forces acting on a body causing stresses in it but won't cause strains," is inaccurate. As materials inevitably respond to stress with associated strains.

    • @himanshushekhar4524
      @himanshushekhar4524 5 месяцев назад

      @@nirajchawake Thankyou so much sir for responding..... One more thing is here ,you used the word "Inaccurate" . Were you wanted to use insignificant??? Because here how inaccurate will make sense?? We are getting accurate value,by putting all the data you mentioned in reply.

  • @kartiksgame2335
    @kartiksgame2335 6 месяцев назад

    Thankyou sir

  • @kartiksgame2335
    @kartiksgame2335 6 месяцев назад

    thank you sir

  • @kartiksgame2335
    @kartiksgame2335 6 месяцев назад

    thanks sir

  • @kartiksgame2335
    @kartiksgame2335 6 месяцев назад

    just wow

  • @kartiksgame2335
    @kartiksgame2335 6 месяцев назад

    this one lecture is enough to make me watch all your lectures sir

  • @5leafclover_
    @5leafclover_ 7 месяцев назад

    Thanks sir

  • @himanshushekhar4524
    @himanshushekhar4524 7 месяцев назад

    Would you please redefine X bar in Y(plastic strain)

  • @himanshushekhar4524
    @himanshushekhar4524 7 месяцев назад

    thankyou very much sir for these series of lectures!!!!!!!

  • @user-un3on3vp7x
    @user-un3on3vp7x 7 месяцев назад

    why the n of dislocation creep is 0? won't more grain boundaries serve as the barrier and stop the dislocation gliding? By the way, I really live on with your videos😭😭😭😭 thank you so much

  • @3drhinomodeling143
    @3drhinomodeling143 7 месяцев назад

    Hello

  • @3drhinomodeling143
    @3drhinomodeling143 7 месяцев назад

    Excellent explanation. Specially I was looking how to proof symmetry of strain tensor.

  • @ankitprasad5382
    @ankitprasad5382 7 месяцев назад

    Bhaiya tell us something more about motion of kinked and joged dislocation:conservative and non-conservative

  • @user-un3on3vp7x
    @user-un3on3vp7x 7 месяцев назад

    cannot understand why the power of the ra is 2 but not 3 in the misfit volume

  • @not_a_handle150
    @not_a_handle150 8 месяцев назад

    Thanks for such quality content sir, do you conduct any courses on nptel?

  • @user-bh7md4th5m
    @user-bh7md4th5m 8 месяцев назад

    Thank you very much for your teaching

    • @nirajchawake
      @nirajchawake 8 месяцев назад

      Glad that it is useful to you

  • @luckysingh-ry4ew
    @luckysingh-ry4ew 8 месяцев назад

    can u please share notes

    • @nirajchawake
      @nirajchawake 8 месяцев назад

      please email me at nchawake[at]iitk[dot]ac[dot]in

  • @mohamedyassineelloumi8057
    @mohamedyassineelloumi8057 8 месяцев назад

    Very informative lecture, Sir. I am a student and I have creep data I want to apply the time-temperature superposition principle to generate a master curve. is it possible to get the code file? Thank you

  • @popescugsw1558
    @popescugsw1558 8 месяцев назад

    HELLO. I AM STUDYING METALLURGY AND MATERIALS ENGINEERING IN TURKEY. I WANT TO USE SOME OF THE PHOTOS IN THIS VIDEO IN MY FINAL THESIS. DO YOU HAVE A STUDY RELATED TO THIS I WOULD LIKE TO REFER TO?

    • @nirajchawake
      @nirajchawake 8 месяцев назад

      We don't have studies related to this. Please feel free to use photos by giving proper credits. Also, if you use photos/images from the video which I have taken from other sources, please see the references mentioned at the bottom of slides for them.

  • @jordankemguimatio5109
    @jordankemguimatio5109 8 месяцев назад

    You shown how to determine C-values of the compliance Matrix for an isotrope cubic material. Thanks ! What about for anisotrope and orthotrope Material?

  • @negarrahbar4813
    @negarrahbar4813 8 месяцев назад

    32:41', in screw dislocation, as also shown in the pictures, the movement of the dislocation line is perpendicular to the dislocation line. Still, in the yellow box, the text says it parallels the dislocation line! Why? Is that a mistake in the text or did I not get it correctly?

    • @nirajchawake
      @nirajchawake 8 месяцев назад

      May be a mistake there. Dislocation always moves perpendicular to the dislocation line (or its tangent vector).

    • @negarrahbar4813
      @negarrahbar4813 8 месяцев назад

      Thank you for the clarification. Great educational videos, especially the visualisations.

  • @Physicist_Dost
    @Physicist_Dost 9 месяцев назад

    Very usefull for physics students also....sir could you plz tell us few reference books

  • @user-un3on3vp7x
    @user-un3on3vp7x 9 месяцев назад

    sorry professor, I have no idea why there are only two 2 fold symmetry in orthorhombic. I think there are three. BTW, I really love your videos, they are really really helpful.

  • @siddharthjena2189
    @siddharthjena2189 9 месяцев назад

    Cleared many confusions.. Thank you sir

  • @padmapriyakannan3019
    @padmapriyakannan3019 9 месяцев назад

    These videos are absolutely amazing. Thank you!