A block of mass M is kept on a rough horizontal surface. The coefficient of static friction between the block and the surface is µ. The block is to be pulled by applying a force to it. What minimum force is needed to slide the block? In which direction should this force act?..Concept of Physics - 1 , HC VERMA , Chapter 6:Friction "
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Solution :
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Let P be the force applied to it at an angle θ
From the free body diagram "
R+Psinθ-mg=0
R=-PSinθ+mg
mR=Pcosθ
From equation (i), μ(Psinθ-Pcosθ)
P=μmg/μSinθ+cosθ
Applied force should be minimum when msinθ+cosθ is maximum.
Again,
(μsinθ+cosθ) is maximum when its derivative is zero.
(d/dθ)(μsinθ+cosθ)=0
μCosθ-sinθ=0
θ=tan⁻¹μ\
So, P=μmg/μSinθ+cosθ
=μmglCosθ/(μsinθ+cosθ)/cosθ
By dividing the numerator and denominator by cosθ, we get
P=μmgsecθ/1+μtanθ
=μmgsecθ/1+tan²θ
=μmg/secθ
=μmg/√1+tan²θ
=μmg/(1+μ²)
Hence minimum force is μmg/√1+u² at an angle q=tan⁻¹μ
********************************************
Let P be the force applied to it at an angle θ
From the free body diagram "
R+Psinθ-mg=0
R=-PSinθ+mg
mR=Pcosθ
From equation (i), μ(Psinθ-Pcosθ)
P=μmg/μSinθ+cosθ
Applied force should be minimum when msinθ+cosθ is maximum.
Again,
(μsinθ+cosθ) is maximum when its derivative is zero.
(d/dθ)(μsinθ+cosθ)=0
μCosθ-sinθ=0
θ=tan⁻¹μ\
So, P=μmg/μSinθ+cosθ
=μmglCosθ/(μsinθ+cosθ)/cosθ
By dividing the numerator and denominator by cosθ, we get
P=μmgsecθ/1+μtanθ
=μmgsecθ/1+tan²θ
=μmg/secθ
=μmg/√1+tan²θ
=μmg/(1+μ²)
Hence minimum force is μmg/√1+u² at an angle q=tan⁻¹μ
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F cos θ =μ N
=μ(mg-Fsinθ)
F= μmg/(cos θ +μsinθ)
For minimum force (cos θ +μsinθ) should be maximum
and maximum value of (cos θ +μsinθ) is √(1+μ2)
so F min =μmg/√(1+μ2)
and for the direction of force let
(cos θ +μsinθ) =√(1+μ2)(1/√(1+μ2) cos θ + μ/√(1+μ2) sinθ)
=√(1+μ2)sin(θ +φ) where tanφ =1/μ
so sin(θ +φ) =1
θ +φ =pi/2
θ =pi/2 -φ
= pi/2 -tan-1(1/μ)
=tan-1(μ)
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