Rotational Mechanics - Pulley and Bucket

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SUMMARY

The discussion focuses on calculating the linear acceleration of a falling bucket connected to a cylindrical pulley system. The problem involves a 4.91 kg pulley with a radius of 0.338 m and a 3.80 kg bucket, with gravity set at 9.81 m/s². The initial approach incorrectly considered only the torque from the bucket's weight without accounting for the combined mass of the bucket and the pulley. The correct method involves treating both masses as a single system to derive the linear acceleration accurately.

PREREQUISITES
  • Understanding of rotational dynamics and torque
  • Familiarity with Newton's second law (F=ma)
  • Knowledge of moment of inertia for a cylinder
  • Ability to apply angular acceleration to linear acceleration conversions
NEXT STEPS
  • Study the relationship between torque and angular momentum in rotational systems
  • Learn about the moment of inertia for various shapes, particularly cylinders
  • Explore the concept of net force in systems with multiple masses
  • Practice problems involving pulley systems and combined mass dynamics
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Students studying physics, particularly those focusing on mechanics and rotational dynamics, as well as educators seeking to clarify concepts related to pulley systems and acceleration calculations.

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Homework Statement



Problem:
"A cylindrical 4.91 pulley with a radius of 0.338 m is used to lower a 3.80 kg bucket into a well. The bucket starts from rest and falls for 4.06 s. The acceleration of gravity is 9.81 m/s². What is the linear acceleration of the falling bucket? Answer in units of m/s²."

Givens:
<br /> \\ m_{p}=4.91 kg\\<br /> <br /> \\ r=0.338 m\\<br /> <br /> \\ m_{p}=3.80 kg\\<br /> <br /> \\ v_{i}=0 m/s\\<br /> <br /> \\ \Delta t=4.06 s\\<br />

Unknown:
<br /> \\ a_{t}=?<br />

Homework Equations



<br /> \\ a_{t} = r\alpha\\<br /> <br /> \\ \Tau\=\I\alpha = Fd sin \theta\\<br /> <br /> \\ I_{cylinder}\=\frac{1}{2} r^2\\<br /> <br />

The Attempt at a Solution


<br /> \\ \tau = F_{g}r = I\alpha\\<br /> \\ m_{b}gr = \frac{1}{2}mr^2\alpha\\<br /> \\ \alpha = \frac{2m_{b}g}{m_{p}r}\\<br /> \\ a_{t} = \frac{2m_{b}g}{m_{p}\\<br />

Now, I thought that was a perfectly logical way to get the answer, but when I submitted it, the answer was wrong. Can anyone tell me what I'm doing wrong here?

Edit: And I seem to be having difficulties putting breaks into my TeX, heh.
 
Last edited:
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torque is equal to the rate of change of angular momentum. That is-- T=d/dt(Lp+Lb)
I think that should work out.
 
your approach just doesn't take into account the mass of the bucket.
 
Ja4Coltrane said:
your approach just doesn't take into account the mass of the bucket.

What do you mean by this? I used the mass of the bucket to calculate F_{g}, which I used to find the torque that I could divide by I to find \alpha.
 
Well that makes sense if Fg just acted on the pulley. If it acts over the whole system, there is some difference.
T=dL/dt=d(Lp+Lbucket)/dt=d(Iw+mvr)/dt
does that make sense? now you can distribute the d/dt to get your answer.
 
I am going to try to put Ja4Coltrane's math into more conceptual terms.

Note: Remember those mass/pulley systems. This problem is just a rotational analogy.

1st: You are correct that the only force is the wieght (mg) of the bucket. However F=ma and there are two masses here. Now F is a net force so it is F=Fg - torque

The two masses are the rotational mass (I) of the cylinder (which you included) but also includes the mass of the bucket (which you forgot).

2nd: Treat both masses as one system and set Fg= both masses x(acceleration).

3. use some algebra and turn angular acceleration into (translational) acceleration. I have a feeling that some factors of r might cancel out.

I hope this is helpful although the mathematical explanation is suffecient for all calculus lovers.
 
Last edited:

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