Spring Pulley System: Find Max Velocity of Block

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Homework Help Overview

The problem involves a spring-pulley system with a disk and a block, where the goal is to determine the maximum velocity of the block as it descends. The setup includes a disk with a mass, a block attached to a string, and a spring with a specific spring constant.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the relationship between the forces acting on the block, the spring, and the disk. There are attempts to derive expressions for acceleration and velocity, with some questioning the validity of using certain kinematic equations due to non-constant acceleration. Others suggest using conservation of energy to relate the variables.

Discussion Status

Some participants have provided interpretations of the setup and raised questions about missing information, such as the initial state of the spring. There is acknowledgment of the need to include elastic energy in the analysis. Multiple interpretations of the problem are being explored, with no explicit consensus reached yet.

Contextual Notes

Participants note potential confusion regarding the description of the system, particularly the term "cordless string" and the configuration of the disk and spring. There is also mention of the spring being relaxed at the moment the block is released, which is a crucial assumption in the analysis.

Chem Austronaut
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Homework Statement



We have a system, consisting of a Disk radius R, with weight M, with a cordless string attached on its edge, at one edge of this cordless string we have a block of mass m, at the other end, we have the string attached to a spring with one end fixed to the floor, with spring constant k, also, the disk is on an axle, so it's mid air, and their is no friction between the disk and the axle. What is the max velocity of the block?

Homework Equations



Let's say the positive y direction is downward, we have the string to spring on the left, and the block of mass m attached to the right which will be released (at which the spring will also be in the relaxed state) so we choose the direction of the angular velocity to be clockwise, (towards suspended block)

Fnet y of spring: T1 = kx

Fnet y of Disk: T1 + T2 + Mg - N (axle on disk) = 0

Fnet y of block mass M: mg - T2 = may

tau (net) = T2R - T1R = Ialpha

Vy^2 = Voy^2 + 2ay (delta y)

The Attempt at a Solution


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We can find the acceleration of the block, by relating it with the following atan = ay = alphaR

Thus alpha = ay/R

Substituting alpha in Tau net we get

T2R - T1R = MR^2(ay/R) ==> ( I used I = MR^2) , cancellation of R and solving for T2 = May + kx (I put T1 = kx)

Plugged this in for Fnet of block mg - (May + kx) = may

My result for ay = (mg - kx)/ (m + M) , now I can use Vy^2 to solve for a V but I get an equation in terms of X, m, M, g, K, and H (delta y) how do i go about finding Vy max of block with Voy = 0, at what point is the force of spring and force of w of block such that the block has a max v?

My result ( I think it's wrong or I'm missing something) Vy = sqrt( 2ayh) using ay derived above..What am I missing to find the max Vy of block? What roles do mg and kx play in control of blocks speed, angular speed, and distance H displaced by block, also how can I relate delta x of spring (sorry I just realized its a bad idea to use x in kx, since we are only dealing with y dir. My apologies.) with the change in H of block? Can you? Thanks I advanced!
 
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I can't decipher the description of the set-up. What's a 'cordless string'? In what way is it attached to the disk if it's also attached (at one edge?!) to a block and at one end to a spring? Is the disk vertical or horizontal? Do you mean the string runs over the disk, as in a pulley? Is the string vertical each side of the disk?
 
pulleyspring.JPG

Is this the set-up?
I think some data are missing. Is the spring relaxed when the block is released?
When using conservation of energy, you have to include also the elastic energy of the spring. The formula Vy^2 = Voy^2 + 2ay (delta y) is not valid, as the acceleration is not constant.

And welcome to PF :)
 
Last edited:
My interpretation of the setup is the same as ehild's.
Chem Austronaut said:
My result for ay = (mg - kx)/ (m + M)
I agree with your acceleration (though I would have used ##I = \frac{1}{2}MR^2## for the moment of inertia of a disk). If Vy is a maximum what does that say about ay at that instant? Once you apply that condition you can get the x value at which Vy_max occurs. If you have a relation between Vy and x then you can plug in your x value and find Vy_max. But as mentioned above, you can't use the constant acceleration kinematic equations.

One way to get a relation between Vy and x is to use energy conservation between the initial state and Vy_max case. I think you'll have to make some assumption on the initial x of the spring (probably that it is relaxed and xo = 0). Don't forget that x and H are related to each other, so that's another variable you can substitute out.
 
ehild said:
View attachment 75877
Is this the set-up?
I think some data are missing. Is the spring relaxed when the block is released?
When using conservation of energy, you have to include also the elastic energy of the spring. The formula Vy^2 = Voy^2 + 2ay (delta y) is not valid, as the acceleration is not constant.

And welcome to PF :)

My apologies harupex, i was writing this on my ipad at the time, i meant massless, not cordless, so that T1s aren't affected by the mass of the string, Ehild is the interpretation is the one I'm talking about. and yes, the condition is such that the spring is relaxed when the block is released.

Thank you :) it's a pleasure.Thank you folks, ill rework the situation and get back to you asap, happy thanksgiving!
 

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