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6. Torque & the Time Rate of Change of Angular Momentum 

MIT OpenCourseWare
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MIT 2.003SC Engineering Dynamics, Fall 2011
View the complete course: ocw.mit.edu/2-003SCF11
Instructor: J. Kim Vandiver
License: Creative Commons BY-NC-SA
More information at ocw.mit.edu/terms
More courses at ocw.mit.edu

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2 сен 2013

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Комментарии : 11   
@georgesadler7830
@georgesadler7830 2 года назад
Professor Vandiver, thank you for another deep derivation of Torque and the Time Rate of Change of Angular Momentum. This is a different way of teaching dynamics in comparison to just a list of formulas. I am really understand mechanics better when it's taught this way.
@gohan100100
@gohan100100 7 лет назад
I believe a mistake was made at 27:08 in the 7th lecture of the Engineering Dynamics playlist. When computing the kinetic energies at time 1 and 2 the magnitude of the velocity squared should've been used. Because the velocity had a component in the R hat direction, the magnitude of the velocity squared is (Rdot + R * thetaDot)^2.
@NeiderNadid
@NeiderNadid 7 лет назад
there is not mistake because at time 1 and 2 the velocity in R direction is zero.
@gohan100100
@gohan100100 7 лет назад
neider nadid at 10:50 the velocity of A with respect to O was given as Rdot Rhat + R*thetadot Thetahat. Why would the component of velocity in the R hat direction be zero at t1 and t2?
@NeiderNadid
@NeiderNadid 7 лет назад
in the interval (t1,t2) the velocity is non zero due down movement, but at t2 the cord stopping and at t1 the is in rest.
@gohan100100
@gohan100100 7 лет назад
neider nadid Awesome! Thank you.
@Upgradezz
@Upgradezz 3 года назад
Was my question as well
@hdheuejhzbsnnaj
@hdheuejhzbsnnaj 2 года назад
Really not the way to teach such interesting material. This way of teaching is very 1920.
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