What is the coefficient of kinetic friction between the block and the incline?

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SUMMARY

The discussion focuses on calculating the coefficient of kinetic friction between a 2.00-kg block and a rough incline, connected to a spring with a spring constant of 100 N/m. The block moves 20.0 cm down the incline before coming to rest, and the equations of motion involve potential energy (PE), kinetic energy (KE), and frictional forces. Key equations include Ff = μFn and the relationship between gravitational forces and the incline's angle. The solution requires understanding the energy transformations and the work done against friction.

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alevis
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Homework Statement


A 2.00-kg block situated on a rough incline is connected to a spring of negligible mass having a spring constant of 100 N/m. The block is released from rest when the spring is unstretched, and the pulley is frictionless. The block moves 20.0 cm down the incline before coming to rest.
Find the coefficient of kinetic friction between block and incline.

Homework Equations


PE = KE
F= ma
Ff = \muFn
\mu = Ff/Fn

PE = KE

The Attempt at a Solution



Ff = mgsin\theta
Fn = mgcos\theta
\mu = (mgsin\theta)/mgcos\theta
stuck!

mgh = 1/2mv2
 
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You know, that's not really an attempt at a solution. You need to show more than some equations slapped together. Explain what you have done and why. We can't read your mind!

Did you draw a digram of all the forces on the block? Always start with that.
 
alevis said:

Homework Statement


A 2.00-kg block situated on a rough incline is connected to a spring of negligible mass having a spring constant of 100 N/m. The block is released from rest when the spring is unstretched, and the pulley is frictionless. The block moves 20.0 cm down the incline before coming to rest.
Find the coefficient of kinetic friction between block and incline.

Homework Equations


PE = KE
F= ma
Ff = \muFn
\mu = Ff/Fn

PE = KE

The Attempt at a Solution



Ff = mgsin\theta
Fn = mgcos\theta
mgh = 1/2mv2

Because of friction your two energy equations are not quite correct. You could try thinking of it this way: The potential energy at the start goes into the work to overcome friction and the energy stored in the spring. That's assuming that you put your reference level for the potential energy where the mass stops.
 

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