A uniform rod(m,l) is standing vertically on a horizontal frictionless surface. Gravity is downwards and uniform. I give its upper end a little push and off it goes. I want to find the Normal Force(and all other variables) as a function of time.
Here's what I do :
mg−N=ma
Where a is downward acceleration(and the only) of centre of mass wrt ground.
Next, I think of conservation of energy. I assume it rotates θ from vertical
mgl2(1−cosθ)=K.E.
I have problem writing expression of its Kinetic Energy. I have studied about instantaneous centre of rotation.
So, I can write its speed and rotational kinetic energy about it as K.E.? Also How do I find relation between ω (angular velocity about that instantaneous centre) and velocity of rod?
Answer
This is what I did and I think is simple and right :
Assume v linear speed of centre of mass downwards and ω angular speed around it. Use the fact the bottom point has no vertical speed to find relation between v and ω. And I am done.
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