Rotational Motion Two Questions

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Homework Help Overview

The discussion revolves around two physics problems related to rotational motion and energy conservation. The first problem involves a bucket of water suspended by a rope around a pulley, focusing on the forces acting on the system as the bucket falls. The second problem concerns a mass attached to a cord wrapped around a wheel, where participants explore the tension in the rope and the moment of inertia of the wheel.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the application of conservation of energy and rotational kinematics equations to analyze the problems. There are attempts to derive equations for tension and acceleration, with some participants questioning the assumptions made in their calculations.

Discussion Status

Several participants have provided guidance on how to approach the problems, including suggestions to consider the rotational dynamics of the pulley and the relationship between linear and angular quantities. There is ongoing exploration of the necessary equations and concepts, with some participants expressing uncertainty about specific steps.

Contextual Notes

One participant notes the absence of the angle of incline in the second problem initially, which is later clarified. There is also a mention of the potential confusion caused by combining two questions in one thread, indicating a possible constraint on the discussion format.

hunansux
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Homework Statement



A 16.0 kg bucket of water of is suspended by a rope wrapped around a pulley, which is just a solid cylinder 0.300 m in diameter with mass 12.0 kg. The cylinder is pivoted on a frictionless axle through its center. The bucket is released from rest at the top of a well and falls 12.0 m to the water. Neglect the weight of the rope.

Homework Equations



Conservation of Energy, Rotational Kinematics Equations

The Attempt at a Solution



Solving for tension in the rope (wrong):

Ft - Fg = ma

Speed of the bucket as it hits the water (also wrong..):

mgyi + (mvi^2)/2 = mgyf + (mvf^2)/2

While the bucket is falling, what is the force exerted on the cylinder by the axle?

^^ No idea how to do that ****.



Problem 2

A 15.0 kg mass is attached to a cord that is wrapped around a wheel of radius r = 9.0 cm (Fig. P8.60). The acceleration of the mass down the frictionless incline is measured to be 2.00 m/s2. Assume the axle of the wheel to be frictionless.

Questions:
Determine the tension in the rope.
Determine the moment of inertia of the wheel.
Determine the angular speed of the wheel 2.00 s after it begins rotating, starting from rest.

This is really similar to the previous one and since I couldn't figure that out... I thought I'd see if you guys could help me.
 
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for the second question u haven't mentioned the angle of incline.if the angle of incline is y. then we have the force equation as

mgsiny-T=m x 2.00m/s2.

also from the rotation of the wheel,
2.00m/s2=alpha x radius of wheel.(gives u the angular acc)

now
tau=I x alpha gives u the MI,

and find out the angular velocity from omega=alpha x t.
...
 
Whoops my bad the angle is 37 degrees it was in the picture not the prompt though! Sorry

Edit: "tau= I x alpha" How do I find the torque and the alpha? Sorry for the dumb question I'm sure it has an incredible easy solution... I just got moved in a AP Physics class from Honors so I'm missing a lot.
 
Last edited:
hunansux said:
Whoops my bad the angle is 37 degrees it was in the picture not the prompt though! Sorry

Maybe there's a problem with my pc,but I don't see any pic,nor any links!
 
The picture is from my textbook haha I didn't mean online! Thanks for the help though. I got the first part of the second question
 
hunansux said:
Whoops my bad the angle is 37 degrees it was in the picture not the prompt though! Sorry

Edit: "tau= I x alpha" How do I find the torque and the alpha? S


tau is the product of the tension and the radius of cylinder...
alpha is obtained from the previous eqn(see my original soln)
 
haha I guess I should have googled tau I assumed it was another way of saying torque... anyway thanks for the help! I still need help one number one. No idea what I did wrong I followed the example we did in class... might have been sleeping though haha. Anyway thanks!
 
welcome to pf!

hi hunansux! welcome to pf! :wink:

(btw, not a good idea to put two questions in the same thread)
hunansux said:
A 16.0 kg bucket of water of is suspended by a rope wrapped around a pulley, which is just a solid cylinder 0.300 m in diameter with mass 12.0 kg. The cylinder is pivoted on a frictionless axle through its center. The bucket is released from rest at the top of a well and falls 12.0 m to the water. Neglect the weight of the rope.

Solving for tension in the rope (wrong):

Ft - Fg = ma

Speed of the bucket as it hits the water (also wrong..):

mgyi + (mvi^2)/2 = mgyf + (mvf^2)/2

While the bucket is falling, what is the force exerted on the cylinder by the axle?

try again, using the kinetic energy or angular momentum of the pulley :smile:
 
Thanks for the help I'll try that too. I sent my teacher an email no response though :( Would it have been better to make two threads?
 
  • #10
hunansux said:

Homework Statement



A 16.0 kg bucket of water of is suspended by a rope wrapped around a pulley, which is just a solid cylinder 0.300 m in diameter with mass 12.0 kg. The cylinder is pivoted on a frictionless axle through its center. The bucket is released from rest at the top of a well and falls 12.0 m to the water. Neglect the weight of the rope.

Homework Equations



Conservation of Energy, Rotational Kinematics Equations

The Attempt at a Solution



Solving for tension in the rope (wrong):

Ft - Fg = ma

Speed of the bucket as it hits the water (also wrong..):

mgyi + (mvi^2)/2 = mgyf + (mvf^2)/2

While the bucket is falling, what is the force exerted on the cylinder by the axle?

^^ No idea how to do that ****.

You can solve this by finding the acceleration, a, of the bucket, and then by use kinematics.

Alternatively, you can use conservation of energy.

Let's look at using conservation of energy.

You had written: mgyi + (mvi 2)/2 = mgyf + (mvf 2)/2.

This neglects the kinetic (rotational) energy of the pulley.

The Kinetic Energy of a rotating object is: (1/2)I(ω2), where I is the object's moment of inertia, and ω is the object's angular velocity (in radians/second).

So you should have written something like:

mgyi + (½)m(vi)2 + (½)I(ωi)2 = mgyf + (½)m(vf)2 + (½)I(ωf)2.

Of course, vi, ωi, and yf are all zero.

You need to find the moment of inertia of a solid cylinder. Also relate the speed of the bucket to the angular velocity of the pulley.
 
  • #11
Thanks for the help sammy. Any idea on how to do that third part? I'm struggling with that.
 
  • #12
hunansux said:
Thanks for the help sammy. Any idea on how to do that third part? I'm struggling with that.

The third part ... Do you mean, "While the bucket is falling, what is the force exerted on the cylinder by the axle? " ?

The linear acceleration of the cylinder is zero, so the net force on the cylinder is zero.

The downward forces on the cylinder are:
1. The tension in the rope.

2. The weight of the cylinder = mg of the cylinder.​

The upward force on the cylinder is provided by the axle, and is equal (but opposite) to the sum of the two downward forces.

Next question to be asked is: "What is the tension in the rope?" No, it's not equal to the weight of the bucket. If it were, the bucket wouldn't accelerate downward!

T - (mb)*g = (mb)*a, where T is the tension, mb is the mass of the bucket, a is the acceleration of the bucket (assumed to be negative, the way I wrote it).

Do you know the acceleration?

vf 2 - vi 2 = 2*(a)*(yf - yi)
 
  • #13
Thanks everyone for the help got a chance to talk to my teach today. He helped with the rest! Admins can close this if they'd like to!
 

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