Rotational Motion of a long pole

AI Thread Summary
A 3.3m long pole balanced vertically will rotate about its tip when given a slight push. The speed of the upper end just before it hits the ground can be calculated using energy conservation principles, where the initial potential energy converts into translational and rotational kinetic energy. The correct formula for the speed of the tip involves considering the pole's rotational kinetic energy about the pivot point at its base. The moment of inertia for the pole about the end is I = 1/3 ML^2, which simplifies the calculations. The discussion emphasizes the importance of correctly applying the principles of rotational motion and energy conservation to find the speed at the tip.
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A 3.3m long pole is balanced vertically on its tip. It is given a tiny push. What will be the speed of the upper end of the pole just before it hits the ground? Assume the lower end does not slip.

mgh=.5mv^2 + .5Iw^2 Initial PE = final KE translation + final KE rotational
v=rw, I=.33mr^2

Combine these equations and I got
v=(1.5gh)^(1/2)

Now I think this is the speed of the CM, located 1.65m above the ground (h=1.65). So to find the speed of the tip I covert v into radians per second and then multiply that by 3.3 to find speed of the tip.

Is this method correct? The book contains no answer.
 
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Your basic idea of using energy conservation is correct, but the details are not. The total KE of the rod as it hits the ground can be viewed as a combination of the translational KE of the CM plus the rotational KE about the CM. (I_{cm} = 1/12 M L^2)

A simpler approach is to realize that the stick is in pure rotational about the pivot point, thus the KE of the rod is just the rotational KE about the pivot point. (I_{end} = 1/3 M L^2)
 
Thanks for your help.
 
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