How Is Acceleration Calculated for a Freely Falling Yoyo?

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The discussion focuses on calculating the linear acceleration and tension of a freely falling yoyo, modeled as a uniform disk. Using Newton's Second Law, the derived acceleration is 2/3 g, while the tension in the rope is (1/3)Mg. The calculations involve net force and torque equations, with the moment of inertia for a cylinder taken into account. Participants note the importance of considering both the inner and outer radii of the yoyo, as the problem simplifies by assuming the string is wound around the outer radius. The conversation highlights the complexity of accurately modeling the yoyo's dynamics in this scenario.
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A yoyo is allowed to drop freely with a string held fixed in place at the top. Assume that the yoyo is a uniform disk of mass M and radius R.

1) Use Newton's Second Law to find the linear acceleration of the yoyo and the tension in the rope.

My answer key says that the answers are 2/3 g for acceleration and (1/3)Mg for tension

I have the net force = ma, and net torque = I*alpha.

so

Net force : mg - T = ma
Net torque = I*alpha

since this is a cylinder

I = (1/2)MR^2

I also know that torque is F*R

I have (1/2)M*R^2*alpha = F*R

F = (1/2)M*R*alpha
Ma = (1/2)M*R*alpha
a =(1/2)*alpha *R

alpha = a/R

so a= (1/2)a

This is not true.

I know how to find tension. I plugged in the correct value for a into the mg-T=ma. But I can't find the acceleration.
 
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Isn't there something else you know about the construction of that yo-yo?
 
I know that the yoyo is a cylinder that spins counter clockwise going down and clockwise going up. It is attached to a fixed place a tthe top. I don't know what I am missing.
 
vu10758 said:
I know that the yoyo is a cylinder that spins counter clockwise going down and clockwise going up. It is attached to a fixed place a tthe top. I don't know what I am missing.
Isn't there an inner radius for the axle and an outer radius for the cylinder?
 
Yes. So I have to include both in the problem. The given R is the outer radius, and the inner radius is not explicitly mentioned.
 
vu10758 said:
Yes. So I have to include both in the problem. The given R is the outer radius, and the inner radius is not explicitly mentioned.
I don't see how you can do the problem without it. Maybe the problem assumes the string is wound around the outside of the cylinder. If that is the case, then the problem can be done with α = a/R. That is not very realistic for a yo-yo, but it does simplify the calculation.

That is what they assumed to get their answer. I wouldn't call this a yo-yo. It's just a cylinder with a string wrapped around it, but the problem can be done and their answer is OK. I will go back to the first post and look at what you did. You were off to a good start.

vu10758 said:
A yoyo is allowed to drop freely with a string held fixed in place at the top. Assume that the yoyo is a uniform disk of mass M and radius R.

1) Use Newton's Second Law to find the linear acceleration of the yoyo and the tension in the rope.

My answer key says that the answers are 2/3 g for acceleration and (1/3)Mg for tension

I have the net force = ma, and net torque = I*alpha.

so

Net force : mg - T = ma
Net torque = I*alpha

since this is a cylinder

I = (1/2)MR^2

I also know that torque is F*R <== this F is T

I have (1/2)M*R^2*alpha = F*R = T*R

F = (1/2)M*R*alpha = (1/2)M*a = T
Ma = Mg - (1/2)M*R*alpha = Mg - (1/2)M*a
Ma + (1/2)M*a = Mg
(3/2)M*a = Mg
a = (2/3)g
T = (1/2)M*a = (1/2)M*(2/3)g = (1/3)M*g

-----------------------------------------------------------------------------------
a =(1/2)*alpha *R == The rest is replaced ==

alpha = a/R

so a= (1/2)a

This is not true.

I know how to find tension. I plugged in the correct value for a into the mg-T=ma. But I can't find the acceleration.

Sorry if I led you astray. I just didn't get this being a yo-yo problem.
 
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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