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Lecture 20 on Mechanical Vibrations/Structural Dynamics-AM

9.5K views · May 17, 2018 · Education

Comments · 17

  • @simonlugwisha4327 · 2 years ago

    such an amazing breakdown of the concept

  • @slnkrc08 · 2 years ago

    Thank you so so much. Finally I understand the concept :))

  • @eleampere · 2 years ago

    Thank you professor <3

  • @davidestig5662 · 7 years ago

    Thanks professor for sharing this lecture!

    1

  • @assiamerabet3555 · 5 years ago

    Thank you sir

  • @mohammadnoori7787 · 5 years ago

    The natural frequency does not change, however the frequency of the damped system is a function of damping ratio.  Wd=sqrt(1-zeta^2)*wn where wS is the frequent the damped system, which mistakenly sometimes is referred to as damped natural frequency, zeta is the damping ratio and an is the natural frequency.

    1

  • @mustafaalmayali5347 · 4 years ago

    Thank you professor <br><br>I think that the response of constant load must be :<br>U(t)= F./k (cos wn t - 1 )<br>Because the integration of sin is (- cos)

    2

  • @engsameeralotaibi6925 · 6 years ago

    sr you are the best .

  • @channelUCAprGak8H5 · 5 years ago

    thank you so much for sharing to us this lesson we need it so much .. thanks

  • @RD-tg9xx · 5 years ago

    Consider the undamped natural frequency of a single-degree-of-freedom linear <br>spring-mass system. If energy dissipation is added to this system, explain whether the fre- <br>quency of damped vibration will differ from the undamped one, and if so, in what manner?

  • @yıkık1sinema7 · 5 years ago

    Professor I will ask you something. Where can I find examples for Duhamel Integral? thanks...

  • @abusalisheik6681 · 6 years ago

    Professor can you share research writing classes

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