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Formulas/physics/Laws Of Motion/Minimum Force to Move a Body

Minimum Force to Move a Body

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 mm rests on a rough horizontal surface with coefficient of static friction μ\mu. A force FF is applied at angle α\alpha above the horizontal. What is the minimum force needed to just move the body, and at what angle α\alpha should it be applied?

Setting up

Forces on the body:

  • Weight mgmg downward
  • Normal reaction NN upward
  • Applied force FF at angle α\alpha above horizontal
  • Limiting friction μN\mu N opposing horizontal motion

Vertical equilibrium:

N+Fsinα=mgN + F\sin\alpha = mg

N=mgFsinαN = mg - F\sin\alpha

Horizontal — on verge of sliding:

Fcosα=μN=μ(mgFsinα)F\cos\alpha = \mu N = \mu(mg - F\sin\alpha)

Fcosα=μmgμFsinαF\cos\alpha = \mu mg - \mu F\sin\alpha

Fcosα+μFsinα=μmgF\cos\alpha + \mu F\sin\alpha = \mu mg

F(cosα+μsinα)=μmgF(\cos\alpha + \mu\sin\alpha) = \mu mg

F=μmgcosα+μsinαF = \frac{\mu mg}{\cos\alpha + \mu\sin\alpha}

Finding the minimum force

To minimise FF, maximise the denominator f(α)=cosα+μsinαf(\alpha) = \cos\alpha + \mu\sin\alpha.

Differentiate and set to zero:

dfdα=sinα+μcosα=0\frac{df}{d\alpha} = -\sin\alpha + \mu\cos\alpha = 0

tanα=μ\tan\alpha = \mu

αopt=tan1(μ)\alpha_{opt} = \tan^{-1}(\mu)

This is the angle of friction λ\lambda. The optimal angle equals the angle of friction.

Minimum force

Substitute tanα=μ\tan\alpha = \mu into FF:

At α=tan1(μ)\alpha = \tan^{-1}(\mu): sinα=μ1+μ2\sin\alpha = \frac{\mu}{\sqrt{1+\mu^2}}, cosα=11+μ2\cos\alpha = \frac{1}{\sqrt{1+\mu^2}}

cosα+μsinα=11+μ2+μ21+μ2=1+μ21+μ2=1+μ2\cos\alpha + \mu\sin\alpha = \frac{1}{\sqrt{1+\mu^2}} + \frac{\mu^2}{\sqrt{1+\mu^2}} = \frac{1+\mu^2}{\sqrt{1+\mu^2}} = \sqrt{1+\mu^2}

Fmin=μmg1+μ2\boxed{F_{min} = \frac{\mu mg}{\sqrt{1+\mu^2}}}

Why lifting the force reduces the required push

When the force is purely horizontal (α=0\alpha = 0): F=μmgF = \mu mg — the full friction must be overcome.

When the force is tilted upward: the upward component reduces the normal force NN, which reduces friction μN\mu N. 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

AngleRequired force
α=0°\alpha = 0° (horizontal)F=μmgF = \mu mg
α=αopt=tan1(μ)\alpha = \alpha_{opt} = \tan^{-1}(\mu)F=μmg1+μ2<μmgF = \frac{\mu mg}{\sqrt{1+\mu^2}} < \mu mg
α=90°\alpha = 90° (straight up)F=mgF = mg (just lifting the body)

The minimum force is always less than μmg\mu mg (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.