Fracture Strength by Griffith

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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Пікірлер: 9

  • @chaoviteliang8813
    @chaoviteliang88137 жыл бұрын

    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
    @Osmancarrisot10 жыл бұрын

    Great Explanation Congratulations Prof Ramesh.

  • @blackdice1001
    @blackdice100110 жыл бұрын

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

  • @Luiz-uy7eu
    @Luiz-uy7eu11 жыл бұрын

    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 KZread Subtitles doesn't work properly so I have struggled to understand some words.

  • @yeldos89
    @yeldos8911 жыл бұрын

    Griffith is the man

  • @learneasyonline
    @learneasyonline8 жыл бұрын

    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.

  • @pavansainarasimha6741
    @pavansainarasimha6741 Жыл бұрын

    why not for ductile materials ?

  • @anahitaemami9438
    @anahitaemami94388 жыл бұрын

    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

    2 жыл бұрын

    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 :)