Conversation of energy to determine angular velocity

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Homework Help Overview

The problem involves using the conservation of energy to determine the angular speed of a spool after a bucket has fallen a certain distance. The scenario includes a 3.00 kg bucket and a 5.00 kg spool, with the string unwinding as the bucket descends.

Discussion Character

  • Exploratory, Assumption checking, Mixed

Approaches and Questions Raised

  • Participants discuss the potential energy of the bucket and its conversion to the rotational kinetic energy of the spool. There are attempts to derive the angular velocity using energy equations, with some questioning the moment of inertia used in calculations.

Discussion Status

Some participants have pointed out potential errors in the calculations, particularly regarding the moment of inertia of the spool. There is acknowledgment of the need to correct these values, which may lead to a viable answer aligning with the multiple choice options provided.

Contextual Notes

Participants note that the problem is from a textbook and involves specific values for mass and radius, which are critical for the calculations. There is also a mention of the multiple choice nature of the question, which influences the discussion on correctness.

deltaOmega
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Homework Statement


[From Serway College Physics; Ch 8, problem 52] Use conversation of energy to determine the angular speed of the spool shown in the figure after the 3.00 kg bucket has fallen 4.00 m, starting from rest. The light string attached to the bucket is wrapped around the spool and does not slip as it unwinds.

qPxF9.png


For variables:
m_{bucket} = 3.00 kg
m_{spool} = 5.00 kg
r = 0.600 m

Homework Equations


I_{spool} = \frac{1}{2} mr^2
PE = mgh
KE_{r} = \frac{1}{2} m \omega^2
PE_i + KE_i = PE_f + KE_f
v_t = r \omega

The Attempt at a Solution


I've seen variants of this question all over the web, including this site, but none of them were helpful to me.

Obviously the only thing driving the bucket down is gravity, which will unwind our spool. So potential energy is:

PE = m_{bucket} g h
PE = (3 \text{kg})(9.8 \text{N/kg})(4 \text{m})
PE = 117.6 \text{J}

Since potential energy is unwinding the spool, then the spool's kinetic rotational energy (KE_{r} = \frac{1}{2} m \omega^2) should be equal to the potential energy (PE_{bucket} = KE_{r}).

I tried to derive the angular velocity from this with:
117.6 \text{J} = \frac{1}{2} m_{bucket} v^2 + \frac{1}{2} I_{spool} \omega^2
117.6 \text{J} = \frac{1}{2} m_{bucket} (r \omega)^2 + \frac{1}{2} (\frac{1}{2} m_{spool} r^2) \omega^2
117.6 \text{J} = \frac{1}{2} (3.00 \text{kg})(0.600 \text{m})^2 \omega^2 + \frac{1}{2} ( \frac{1}{2} (5.00 \text{kg})(0.600 \text{m})^2) \omega^2
117.6 \text{J} = 0.54 \omega^2 + 0.162 \omega^2
117.6 \text{J} = 0.702 \omega^2
167.52 = \omega^2
12.9 \text{m/s} = \omega

However, this cannot be right, as the question is multiple choice and only offers the following answers: 7.12, 8.66, 9.12, 10.9, or 11.8.

Help would be appreciated.
 
Last edited:
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deltaOmega said:

Homework Statement


[From Serway College Physics; Ch 8, problem 52] Use conversation of energy to determine the angular speed of the spool shown in the figure after the 3.00 kg bucket has fallen 4.00 m, starting from rest. The light string attached to the bucket is wrapped around the spool and does not slip as it unwinds.

qPxF9.png


For variables:
m_{bucket} = 3.00 kg
m_{spool} = 5.00 kg
r = 0.600 m

Homework Equations


I_{spool} = mr^2
PE = mgh
KE_{r} = \frac{1}{2} m \omega^2
PE_i + KE_i = PE_f + KE_f
v_t = r \omega

The Attempt at a Solution


I've seen variants of this question all over the web, including this site, but none of them were helpful to me.

Obviously the only thing driving the bucket down is gravity, which will unwind our spool. So potential energy is:

PE = m_{bucket} g h
PE = (3 kg)(9.8 N/kg)(4 m)
PE = 117.6 J

Since potential energy is unwinding the spool, then the spool's kinetic rotational energy (KE_{r} = \frac{1}{2} m \omega^2) should be equal to the potential energy (PE_{bucket} = KE_{r}).

I tried to derive the angular velocity from this with:
117.6 J = \frac{1}{2} m_{bucket} v^2 + \frac{1}{2} I_{spool} \omega^2
117.6 J = \frac{1}{2} m_{bucket} (r \omega)^2 + \frac{1}{2} (\frac{1}{2} m_{spool} r^2) \omega^2
117.6 J = \frac{1}{2} (3.00 kg)(0.600 m)^2 \omega^2 + \frac{1}{2} ( \frac{1}{2} (5.00 kg)(0.600 m)^2) \omega^2
117.6 J = 0.54 \omega^2 + 0.162 \omega^2
117.6 J = 0.702 \omega^2
167.52 = \omega^2
12.9 m/s = \omega

However, this cannot be right, as the question is multiple choice and only offers the following answers: 7.12, 8.66, 9.12, 10.9, or 11.8.

Help would be appreciated.

Hello deltaOmega. Welcome to PF !

It seems to me that your moment of inertia for the spool is incorrect.
 
Oops, it should be \frac{1}{2} m r^2, as used in the work later.
 
deltaOmega said:
Oops, it should be \frac{1}{2} m r^2, as used in the work later.
So that's OK ?

What is (1/2)(1/2)(5)(0.6)2 ?

It's not 0.162
 
I think you mean conservation of energy, not conversation.
 
SammyS said:
So that's OK ?

What is (1/2)(1/2)(5)(0.6)2 ?

It's not 0.162

Well, that's embarassing. That ends up being 0.45, which changes the final answer to 10.9 rad/s, corresponding with one of the multiple choice answers. Thanks.
 

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