Angular Speed of Pulley (Spring, Pulley, Ramp)

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Homework Help Overview

The discussion revolves around determining the angular speed of a pulley system involving a spring, a block on an incline, and the associated energies. Participants are analyzing the relationships between potential energy, kinetic energy, and the moment of inertia in the context of rotational and translational motion.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the equations for kinetic energy and potential energy, questioning the contributions of both the block and the pulley to the overall energy of the system. There is an emphasis on understanding the roles of translational and rotational kinetic energy.

Discussion Status

Multiple interpretations of the energy relationships are being explored, with some participants suggesting a reconsideration of the total mechanical energy of the system. Guidance has been offered to clarify the contributions of different forms of energy, but no consensus has been reached on the correct approach.

Contextual Notes

Participants note the complexity of the problem due to the presence of both linear and rotational motion, as well as multiple forms of energy. There is an acknowledgment of the initial conditions and the confusion arising from the setup of the problem.

Ticklez_Panda
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Homework Statement


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---Find Angular Speed---


Homework Equations


I = 1/2 mR^2
Ug = mgdsinθ
Us = 1/2 kd^2
KE = 1/2 I w^2

The Attempt at a Solution


Moment of inertia of reel = 1/2mR2
Kinetic energy of the reel = 1/2 mv2 = 1/2(1/2mR2) w2
KE = mgdsinθ (potential due to gravity) + 1/2kd2 (spring potential)
w = sqrt(4(mgdsinθ + 1/2kd2) / mR2)
This answer is incorrect, I'm wondering where I went wrong. Please help if you are able to. Cheers!
 
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You are forgetting that the block will also have non-zero KE.
 
Ticklez_Panda said:
Moment of inertia of reel = 1/2mR2
Kinetic energy of the reel = 1/2 mv2 = 1/2(1/2mR2) w2
KE = mgdsinθ (potential due to gravity) + 1/2kd2 (spring potential)
w = sqrt(4(mgdsinθ + 1/2kd2) / mR2)
This answer is incorrect, I'm wondering where I went wrong. Please help if you are able to. Cheers!

You have not considered the kinetic energy of the block.

There are two types of kinetic energies to be taken into account.

1) Rotational kinetic energy of the reel given by (1/2)Iω2
2) Translational kinetic energy of the block given by (1/2)mv2
 
Tanya Sharma said:
You have not considered the kinetic energy of the block.

There are two types of kinetic energies to be taken into account.

1) Rotational kinetic energy of the reel given by (1/2)Iω2
2) Translational kinetic energy of the block given by (1/2)mv2

Kinetic energy of the block must be equal to the spring energy? I assume this since the block will fall with potential due to gravity, during this fall it will gain kinetic energy and it is the accumulated energy that will transfer into the spring. Which means that 1/2mv^2 = 1/2kd^2.

So it would follow that w = sqrt(4(mgdsinθ + 1/2kd2 - 1/2mv^2) / mR2)
 
Ticklez_Panda said:
Kinetic energy of the block must be equal to the spring energy? I assume this since the block will fall with potential due to gravity, during this fall it will gain kinetic energy and it is the accumulated energy that will transfer into the spring. Which means that 1/2mv^2 = 1/2kd^2.

So it would follow that w = sqrt(4(mgdsinθ + 1/2kd2 - 1/2mv^2) / mR2)

This is incorrect understanding...

Start afresh...

Initially,when the block is 'd' distance up the incline what is the total mechanical energy of the system ?
 
Tanya Sharma said:
This is incorrect understanding...

Start afresh...

Initially,when the block is 'd' distance up the incline what is the total mechanical energy of the system ?

Initially ΔEint= 0 because the spring is not compressed and the block is attached to the reel. When the reel is wound counterclockwise the block begins to rise, it gains potential energy due to gravity and the pulley experiences kinetic energy as it rises. I'm not quite sure where to go from here. I'm a bit confused that the pulley is what were are seeking the speed of. Generally it's been about the speed of the block so far in the course.
 
Well, the problem is intentionally set up so as to confuse you. Instead of one potential energy, it has two. Instead of one kinetic energy, it has two. Instead of purely linear motion, it has linear and rotational, which are kinematically related.

Yet you can solve it exactly as the other you did. Find the full potential energy. The full kinetic energy. Their sum is constant.
 
I will let voko guide the OP.
 

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