Finding Final Velocity of a Falling Rotating Rod

AI Thread Summary
The discussion centers on calculating the final velocity of a falling rotating rod with a heavy gold ball attached. The initial confusion arises from the need to consider the moments of inertia, but participants clarify that the lightweight rod can be ignored, treating the system as a point mass. The approach involves using energy conservation principles, specifically equating gravitational potential energy to kinetic energy. The final velocity at the top of the rod when it strikes the ground is determined to be 8.85 m/s. The conversation emphasizes that mass cancels out in the equations, simplifying the calculation.
blue5t1053
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Problem:
A rigid assembly is made of a light weight rod 2 m long and a heavy gold ball which is attached at the middle of the rod. The rigid assembly initially rests with one end on the ground in a vertical position. If released what speed does the top of the rod have when it strikes the ground?

Equations:
Rotational \ Inertia \ for \ a \ thin \ rod \ about \ central \ axis; \ \ I = \frac{1}{12} M L^{2}

Rotational \ Inertia \ for \ a \ thin \ rod \ about \ non-central \ axis; \ \ I = \frac{1}{12} M L^{2} + M R(from \ center)^{2}

Rotational \ Inertia \ for \ a \ sphere; \ \ I = \frac{2}{5} M r^{2}

My Work:
Any help where to start? I am lost. I know that the final answer is 8.85 m/s.
 
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blue5t1053 said:
Rotational \ Inertia \ for \ a \ thin \ rod \ about \ central \ axis; \ \ I = \frac{1}{12} M L^{2}

Rotational \ Inertia \ for \ a \ thin \ rod \ about \ non-central \ axis; \ \ I = \frac{1}{12} M L^{2} + M R(from \ center)^{2}

Rotational \ Inertia \ for \ a \ sphere; \ \ I = \frac{2}{5} M r^{2}

Hi blue5t1053! :smile:

You're making this too complicated … no wonder you don't know where to start. :rolleyes:

When a question uses words like "lightweight" and "heavy", it means that you can ignore the lightweight one.

So you don't need to consider moments of inertia … the rod is lightweight, so it counts as 0, and the ball is heavy, so you can regard it as a point.

So this is just a point mass. :smile:

(But is the ground frictionless, or is the rod attached to the ground? :confused:)

Now try it … ! :smile:
 
I am to assume that the ground is frictionless and that it will rotate from where the rod had made contact with the ground.

I can't find any way to calculate it without mass. What principle would I use to find it? I tried using angular velocity, but I couldn't make it work.
 
Would this be right?

m*g*h = \frac{1}{2} * m * v^{2}

9.8 \frac{m}{sec^{2}} * 1 m = \frac{1}{2} * v^{2}

\sqrt{\frac{9.8 \frac{m}{sec^{2}} * 1 m}{\frac{1}{2}}} = v

v = 4.427 \frac{m}{sec} \ ; \ then *2 m \ for \ top \ of \ rod

v = 8.85 \frac{m}{sec}
 
Hi blue5t1053! :smile:

You don't need the mass … it will be the same on both sides of any equation … it always cancels out.

Draw a diagram showing the rod at a typical angle θ.

Since you don't know the value of the normal force… and you'd rather avoid calculating it … get an angular acceleration by taking moments about the bottom of the rod! :smile:
 
blue5t1053 said:
Would this be right? …

(I forgot you were only asked to find the final velocity! :redface:)

Yes, that looks fine! :smile:
 
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