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Fracture Strength by Griffith

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  • เผยแพร่เมื่อ 2 เม.ย. 2012
  • Engineering Fracture Mechanics by Prof. K. Ramesh, Department of Applied Mechanics, IIT Madras. For more details on NPTEL visit nptel.iitm.ac.in
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ความคิดเห็น • 9

  • @chaoviteliang8813
    @chaoviteliang8813 7 ปีที่แล้ว

    This is such a good class!! I am so fortunate to listen to Prof. Ramesh's teaching, which greatly helped me understanding fracture mechanics concepts!

  • @Osmancarrisot
    @Osmancarrisot 10 ปีที่แล้ว

    Great Explanation Congratulations Prof Ramesh.

  • @blackdice1001
    @blackdice1001 10 ปีที่แล้ว

    What Luiz said. This is a great help, thank you.

  • @pavansainarasimha6741
    @pavansainarasimha6741 ปีที่แล้ว

    why not for ductile materials ?

  • @Luiz-uy7eu
    @Luiz-uy7eu 11 ปีที่แล้ว

    Amazing how some really good classes as this can have so few views and feedback. There is some real good information here that is hard to find anywhere else. Too bad that the TH-cam Subtitles doesn't work properly so I have struggled to understand some words.

  • @yeldos89
    @yeldos89 11 ปีที่แล้ว

    Griffith is the man

  • @anahitaemami9438
    @anahitaemami9438 8 ปีที่แล้ว +1

    time 18:28: the plot is for -Ua (not the +Ua written there) and so Ut = Us - Ua . Can anyone give more explanations about that ?

    • @geetamonpara8116
      @geetamonpara8116 3 ปีที่แล้ว

      This may be long overdue. But here it goes. Here he is considering deformation under constant strain, which implies that the strain energy decreases as the crack grows. This is mentioned in detail in the previous lecture under constant displacement approach. Hence, Ua is negative. As a result, net change in energy is Us (increase due to surface energy) - Ua (decrease due constant strain condition). Hope this helps :)

  • @learneasyonline
    @learneasyonline 8 ปีที่แล้ว

    10:50 take a cycle Tyre for example just could not stop me laugh.Beautiful sir ! Love your lecture sir,very very detailed and very cool explanations.