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Acceleration on Smooth Inclined Plane

Acceleration of a body sliding down a frictionless inclined plane.
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Derivation

The situation

A body slides down a smooth (frictionless) inclined plane of angle θ\theta. What is its acceleration?

Derivation

Forces on the body:

  • Weight mgmg vertically downward
  • Normal reaction NN perpendicular to the surface
  • No friction (smooth surface)

Resolve weight along and perpendicular to the incline:

  • Component along incline (down the slope): mgsinθmg\sin\theta
  • Component perpendicular to incline: mgcosθmg\cos\theta

Perpendicular to incline (no acceleration in this direction):

N=mgcosθN = mg\cos\theta

Along the incline (Newton's Second Law):

mgsinθ=mamg\sin\theta = ma

a=gsinθ\boxed{a = g\sin\theta}

Understanding the result

The acceleration depends only on θ\theta and gg — not on the mass. A heavy block and a light block slide down the same frictionless incline with exactly the same acceleration. This is the same result as free fall — mass cancels because both the gravitational force and inertia are proportional to mass.

How θ\theta affects acceleration

θ\thetaa=gsinθa = g\sin\theta
0° (flat)00 — no motion
30°30°g/2=5g/2 = 5 m/s²
45°45°g/27.1g/\sqrt{2} \approx 7.1 m/s²
60°60°g3/28.7g\sqrt{3}/2 \approx 8.7 m/s²
90°90° (vertical)gg — free fall

At θ=90°\theta = 90°, the incline becomes a vertical wall and the body is in free fall — consistent.

Normal force on the incline

N=mgcosθN = mg\cos\theta

At θ=0°\theta = 0°: N=mgN = mg (flat surface, full weight supported) At θ=90°\theta = 90°: N=0N = 0 (vertical wall, no support)

The normal force decreases as the slope steepens.

Remember
For an object projected up a smooth incline, the deceleration is also $g\sin\theta$ (gravity component still acts down the slope). The time to reach the top and the distance covered follow from the equations of motion with $a = -g\sin\theta$.