Let us consider a giant piano of mass m. The piano is pushed up by a force F to a delivery truck using an inclined plane elevated at an angle θ as shown in the figure.
The weight mg of the piano has two components mgsinθ and mgcosθ as shown in the figure.
The normal force on the inclined plane is N=mgcosθ
If μ be the coefficient of friction, the frictional force is f=μN=μmgcosθ
Since we are trying to push the piano upward, the force of friction will be downward along the slope of the plane.
As shown in the figure, total downward force along the slope of the plane will be f+mgsinθ
Since the piano is pushed up by force F , the net upward force will be
Fnet=F−(f+mgsinθ)⇒Fnet=F−(μmgcosθ+mgsinθ)⇒Fnet=F−mg(μcosθ+sinθ)
Initially the body is at rest and the static friction will come into play.
Substituting F=3530N,m=345kg,g=9.8m/s2,θ=40°,μ=0.52 for static friction,
Fnet=3530−345×9.8(0.52cos40°+sin40°)⇒Fnet=9.9N
Thus, the piano will start to move upward.
Substituting μ=0.15 for kinetic friction,
Fnet=3530−345×9.8(0.15cos40°+sin40°)⇒Fnet=968.2N
Answer: 3530N will be enough to move the piano up the ramp.
The net force during static friction = 9.9N
The net force during kinetic friction = 968.2N
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