Deriving SHM: Help Needed for Challenging Problem in Textbook

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The discussion revolves around deriving the harmonic oscillator differential equation for a mass-spring system with friction. The problem involves a block attached to a spring, moving on a board with static and kinetic friction as it slides back and forth. The key challenge is calculating the total force acting on the block as a function of its position, particularly when it moves to the left while experiencing friction. Participants are encouraged to focus on the forces involved and how they relate to the block's motion. Assistance is sought to navigate the complexities of the derivation.
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This is actually the problem in the textbook.
I'm trying to derive the harmonic oscillator differential equation for this system, but It seems like it's very very challenging.

could anyone help me out?

Following is the question and figure from the textbook.







Homework Statement



A block of mass m is attached to a fixed support by a horizontal spring with force constant k and negligible mass. The block sits on a long horizontal board, with which it has coefficient of static friction μs and a smaller coefficient of kinetic friction μk. The board moves to the right at constant speed v. Assume the block spends most of its time sticking to the board and moving to the right, so the speed v is small in comparison to the average speed the blok has as it slips back toward the left.
Derive the harmonic oscillator differential equation for the system.





Homework Equations



F=ma
F(sp)=-kx
E=K+U


The Attempt at a Solution




I couldn't figure out.



( The figure has a copyright from the textbook).
I will delete this post if it could cause the copyright problem.
 

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Your differential equation is relevant when the block moves to the left. It is sliding (with friction) and accelerated by the spring. Can you calculate the total force which acts on the block as function of its position?
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
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