Spring Pulley System: Find Max Velocity of Block

AI Thread Summary
The discussion revolves around calculating the maximum velocity of a block in a spring-pulley system involving a disk, a block, and a spring. Participants clarify the setup, emphasizing that the spring is relaxed when the block is released and that the string is massless. The equations of motion and forces acting on the block, disk, and spring are analyzed, with a focus on the relationship between acceleration, tension, and gravitational force. There is a consensus that conservation of energy should be applied, including the elastic potential energy of the spring, to find the maximum velocity. The need for clearer definitions and assumptions regarding the system's parameters is also highlighted.
Chem Austronaut
Messages
2
Reaction score
0

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


[/B]

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!
 
Physics news on Phys.org
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!
 
I multiplied the values first without the error limit. Got 19.38. rounded it off to 2 significant figures since the given data has 2 significant figures. So = 19. For error I used the above formula. It comes out about 1.48. Now my question is. Should I write the answer as 19±1.5 (rounding 1.48 to 2 significant figures) OR should I write it as 19±1. So in short, should the error have same number of significant figures as the mean value or should it have the same number of decimal places as...
Thread 'Calculation of Tensile Forces in Piston-Type Water-Lifting Devices at Elevated Locations'
Figure 1 Overall Structure Diagram Figure 2: Top view of the piston when it is cylindrical A circular opening is created at a height of 5 meters above the water surface. Inside this opening is a sleeve-type piston with a cross-sectional area of 1 square meter. The piston is pulled to the right at a constant speed. The pulling force is(Figure 2): F = ρshg = 1000 × 1 × 5 × 10 = 50,000 N. Figure 3: Modifying the structure to incorporate a fixed internal piston When I modify the piston...
Thread 'A cylinder connected to a hanging mass'
Let's declare that for the cylinder, mass = M = 10 kg Radius = R = 4 m For the wall and the floor, Friction coeff = ##\mu## = 0.5 For the hanging mass, mass = m = 11 kg First, we divide the force according to their respective plane (x and y thing, correct me if I'm wrong) and according to which, cylinder or the hanging mass, they're working on. Force on the hanging mass $$mg - T = ma$$ Force(Cylinder) on y $$N_f + f_w - Mg = 0$$ Force(Cylinder) on x $$T + f_f - N_w = Ma$$ There's also...
Back
Top