Rotational Kinetic Energy: Pole Balanced Vertically

AI Thread Summary
The discussion focuses on calculating the speed of the upper end of a vertically balanced pole just before it hits the ground, using conservation of energy principles. The initial approach incorrectly used the full height of the pole (h) instead of the height of the center of mass (l/2) in the energy equation. The correct method involves recognizing that the center of mass of the pole falls a distance of l/2, leading to the correct angular velocity (w) calculation. The final speed of the upper end of the pole is determined to be 7.27 m/s. Understanding the center of mass is crucial for solving similar problems involving rotational kinetic energy.
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Homework Statement



A 1.80m long pole is balanced vertically with its tip on the ground. It starts to fall and its lower end does not slip. What will be the speed of the upper end of the pole just before it hits the ground? [hint: Use conservation of energy]

l=1.890m


Homework Equations



mgh=1/2I(w)^2
v=wr

The Attempt at a Solution



So I know how to do the problem but I don't quite understand it.

The original method I used to solve the problem was:

mgh=1/2I(w)^2
mgh=(1/2)(1/3m(l^2))(w^2)
*masses cancel to get:
gh=(1/6)(ml^2)(w^2)
Solve for w:
sqrt((6gh)/l^2)=w

However this got me the wrong answer and I realized instead of plugging in h, you must use l/2. Why is this? Is there an equation or something I am missing?

Correct Solution:

sqrt((6g(l/2))/l^2)=w
sqrt((6(9.8m/s^2)(1.8m/2))/(1.8^2)=w
w=4.04rad/s
v=rw
= 1.8m(4.04rad/s)
=7.27m/s

Thanks!
 
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Here you should consider the center of mass of the falling rod.It is located at the geometric center of the rod.
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