Angular acceleration of a rod - 2

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The discussion revolves around the angular acceleration of a rod in rotational equilibrium before and after a string is cut. Initially, the tension in the string and the force from the spring are balanced, leading to a force equation that yields F = Mg/2. Upon cutting the string, the rod rotates about its end, necessitating a recalculation of forces and torques. It is clarified that the spring force remains constant immediately after the cut, which affects the angular acceleration calculations. Ultimately, the solution is validated, confirming that the approach to finding angular acceleration about the center of mass is appropriate.
Vibhor
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Homework Statement



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Homework Equations

The Attempt at a Solution


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Initially the rod is in rotational equilibrium , so net torque about CM is zero .

From torque equation about CM , we get

Tension T in the left string = Force F (kx) in the spring

Doing a force balance gives us T+F=Mg

2F=Mg

F=Mg/2

Now when the string is cut , force equation in vertical direction is Mg - F = Ma

Torque equation about the CM is F(L/2) = (ML2/12)α

F = Mg/2 since force exerted by spring remains same just after right string is cut .

Using value of F in the above two eqs gives a = g/2 and α = (3g/L)

Have I approached it correctly ?
 

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Vibhor said:
Have I approached it correctly ?
No. When the cord is cut, the rod will rotate about its end at A. It is best to do your calculation about that end. Then you will see that the force exerted by the spring changes when the cord is cut.
 
kuruman said:
No. When the cord is cut, the rod will rotate about its end at A. It is best to do your calculation about that end. Then you will see that the force exerted by the spring changes when the cord is cut.

Just after the cord is cut , the spring length doesn't change instantaneously , which means force exerted by spring doesn't change immediately when the cord is cut .

I don't see how spring force is different before and just after cord is cut .
 
Vibhor said:
Just after the cord is cut , the spring length doesn't change instantaneously , which means force exerted by spring doesn't change immediately when the cord is cut .
That is true. I was thinking about another situation when a stated that the force changes. For this problem, the angular acceleration for rotations about the CM is the one that makes sense. Your solution looks good.
 
Thanks
 
Last edited:
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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