Yahoo...Finally I arrived the answer...It turns out that I had been replacing v2 by ω2l2 instead of ω2l2/4 in the final step ...?:)?:)?:)
Thanks pals... And sorry for wasting your precious time..if I did.
Here's my solution anyway...
Considering the body to be centred at the mid point of the middle leg of the 'H', we have,
mgl/2 =mv2/2 + [(ml2/12 + ml2/4 + ml2/4)ω2]/2
which on simplifying and putting v=ωl/2 gives:
ω=(12g/17l)^0.5...
Thanks BvU for your help..! :smile::smile::smile:
In the first place, I do know the parallel+perpendicular axis theorems. :wink:
But the formula says that we have to use the MoI about the COM of the object, not about the axis about which it is rotating.
Saying this, I want to also add that it's...
Yes.! That's right! The correct answer is V/3R
Pardon, but I didn't understand your solution. You conserved angular momentum about point of contact ?
OK..., let me clear my basics first of all..,
I suppose no matter about what point we are conserving angular momentum, we always use velocity...
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Respected Physics Gurus/experts...!
I am confused in the application of Kinetic energy Expression, i.e, KE = (1/2)MVCM2+(1/2)ICMω2
I had been trying out this question actually(it's pretty simple though:-p)...---
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