Rotational Dynamics involving a pulley, spring, and block

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SUMMARY

The discussion focuses on a physics problem involving a block on an incline connected to a spring via a pulley. The block has a mass of 9.00 kg, the incline angle is 51.0 degrees, and the coefficient of kinetic friction is 0.200. The spring constant is 40.0 N/m, and the pulley is a solid cylinder with a radius of 0.550 m. After analyzing the forces and deriving equations, the correct acceleration of the block after sliding 0.425 m down the incline is determined to be 3.00 m/s².

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Knowledge of rotational dynamics and moment of inertia
  • Familiarity with spring mechanics and Hooke's Law
  • Ability to analyze free body diagrams
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  • Study the concept of effective mass in rotational systems
  • Learn about the relationship between tension and spring force in dynamic systems
  • Explore the equations of motion for blocks on inclined planes
  • Investigate the principles of torque and angular acceleration in pulleys
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JennV
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Homework Statement



A block of mass m = 9.00 kg is situated on an incline of angle θ = 51.0^{\circ} with coefficient of kinetic friction \mu_k = 0.200, and is connected to a light spring of spring constant k = 40.0 N/m via a light rope passing over a massive pulley as shown. The block is released from rest when the spring is unstretched. The uniform solid cylindrical pulley is mounted on a frictionless axle and has the same mass as the block and a radius R = 0.550 m. The light rope which connects the spring to the block slides over the pulley without slipping.

Find the acceleration of the block at the instant it has slid a distance of x = 0.425 m parallel to the incline. (Take the positive direction to be down the incline.)

Diagram:
http://img72.imageshack.us/img72/8755/ch11qrotdyn.jpg

Homework Equations



mgsin(theta)
uk*mgcos(theta)
ma
0.5*Kx^2
Solid uniform cylinder moment of inertia = 0.5*MR^2

The Attempt at a Solution



I drew free body diagrams for each objects. & derived a equation to solve for acceleration:

m(block)gsin(theta)-ukm(block)gcos(theta)-0.5*kx^2 = 0.5m(pulley)a + m(block)a

But the acceleration that I got was really high, so I believe that it is wrong.

My question is: does the tension of the string between the spring and pulley proportional to the extension of the spring which is 0.5kx^2 ?
 
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Hi JennV! :smile:

(have a mu: µ and a theta: θ and try using the X2 and X2 icons just above the Reply box :wink:)
JennV said:
m(block)gsin(theta)-ukm(block)gcos(theta)-0.5*kx^2 = 0.5m(pulley)a + m(block)a

nooo …

i] the force from the spring is kx, not kx2/2 (that's the PE)

ii] the pulley isn't moving, it's only rotating, so you can't use the mass …

you either need the "effective mass" (if you know how to work that out),

or you need to call the tension either side of the pulley T1 and T2, and do two separate equations, F = ma for the block, and τ =Iα for the pulley …

what do you get? :smile:
 
tiny-tim said:
Hi JennV! :smile:

(have a mu: µ and a theta: θ and try using the X2 and X2 icons just above the Reply box :wink:)


nooo …

i] the force from the spring is kx, not kx2/2 (that's the PE)

ii] the pulley isn't moving, it's only rotating, so you can't use the mass …

you either need the "effective mass" (if you know how to work that out),

or you need to call the tension either side of the pulley T1 and T2, and do two separate equations, F = ma for the block, and τ =Iα for the pulley …

what do you get? :smile:


Thank you so much tiny-tim for replying! But I actually already have derived the answer myself and it was 3.00! YAY! =D
 

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