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Question

Figure shows a spring fixed at the bottom end of an incline of inclination 37. A small block of mass 2 kg starts slipping down the incline from a point 5.8 m away from front end of the spring. The block compresses the spring by 20 cm, stops momentarily and then rebounds through a distance of 1 m up the incline. The spring constant of the spring ( in N/m) is (Take g=10 m/s2)

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Solution

FBD of block for downward and upward motion along the incline:


When the block is going down ,
Resolving all forces along the plane, we get
Net force =mgsin37μN
=mgsin37μmgcos37
Distance covered along the plane =5.8 m+0.2 m=6.0 m
So, work done by all forces on the block =F×d
=(mgsin37μmgcos37)×6.0
... (1)

This work done is stored as potential energy in the spring compression =12kx2=12k(0.2)2 ... (2)

When block rebounds, this P.E is utilized in the motion of the block. In return (rebound) journey, the friction force remains same, but acts in opposite direction of motion.
New net force along the plane
=mgsin37+μmgcos37
Now it moves for a distance of 1 m
Work done by forces =(mgsin37+μmgcos37)×1.0 ... (3)

(a) Equating (1) and (3):
(mgsin37+μmgcos37)=6(mgsin37μmgcos37)
7μmgcos37=5mgsin37
μ=5mgsin377mgcos37
μ=57tan37=0.54
μ=0.54

(b) Equating (2) and (3), we get
12kx2=mgsin37+μmgcos37
k(0.2)2=2mg(sin37+μcos37)
k=2×2×10(0.6+0.54×0.8)0.04
k=40×1.0320.04=1032 N/m
Stiffness k=1032 N/m

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