Minimum force needed to move a body on a rough horizontal surface, applied at optimal angle.
Class 11Class JEE
Derivation
The problem
A body of mass m rests on a rough horizontal surface with coefficient of static friction μ. A force F is applied at angle α above the horizontal. What is the minimum force needed to just move the body, and at what angle α should it be applied?
Setting up
Forces on the body:
Weight mg downward
Normal reaction N upward
Applied force F at angle α above horizontal
Limiting friction μN opposing horizontal motion
Vertical equilibrium:
N+Fsinα=mg
N=mg−Fsinα
Horizontal — on verge of sliding:
Fcosα=μN=μ(mg−Fsinα)
Fcosα=μmg−μFsinα
Fcosα+μFsinα=μmg
F(cosα+μsinα)=μmg
F=cosα+μsinαμmg
Finding the minimum force
To minimise F, maximise the denominator f(α)=cosα+μsinα.
Differentiate and set to zero:
dαdf=−sinα+μcosα=0
tanα=μ
αopt=tan−1(μ)
This is the angle of friction λ. The optimal angle equals the angle of friction.
Minimum force
Substitute tanα=μ into F:
At α=tan−1(μ): sinα=1+μ2μ, cosα=1+μ21
cosα+μsinα=1+μ21+1+μ2μ2=1+μ21+μ2=1+μ2
Fmin=1+μ2μmg
Why lifting the force reduces the required push
When the force is purely horizontal (α=0): F=μmg — the full friction must be overcome.
When the force is tilted upward: the upward component reduces the normal force N, which reduces friction μN. Less friction means less force needed horizontally.
But tilting too much reduces the horizontal component — inefficient again. The optimal angle balances these two effects.
Comparison
Angle
Required force
α=0° (horizontal)
F=μmg
α=αopt=tan−1(μ)
F=1+μ2μmg<μmg
α=90° (straight up)
F=mg (just lifting the body)
The minimum force is always less than μmg (the force needed when pushing horizontally).
Note
This result applies to pulling (force above horizontal). For pushing (force below horizontal), the normal force increases, friction increases, and the required force is always greater than $\mu mg$. Pulling is always more efficient than pushing on a flat surface.