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Rolling down an incline

Intermediate

Rolling bodies accelerate slower than sliding ones due to rotational energy.

Key relationa = g sinθ/(1+I/mR²)

a = g sinθ/(1 + I/mR²). Smaller I/mR² means faster descent.

Worked example

Solid sphere (2/5): a = 0.71 g sinθ. Ring: 0.5 g sinθ.

Common mistake

Mass and radius cancel out.

In more detail

A body rolling down an incline without slipping converts potential energy into translational and rotational kinetic energy. The acceleration depends on how the mass is distributed.

Real-world uses

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Frequently asked questions

Which body reaches the bottom first?

The one with the smallest moment of inertia relative to its mass, such as a solid sphere.

Does the radius matter?

Not for a given shape, since the acceleration is independent of radius for the same shape.

Does the mass of the rolling ball change the acceleration?

No. The mass cancels, so the acceleration depends only on the slope angle and the shape of the object through I/mR².

Related topics in Rotational Motion

Newton's second law for rotation · Rotational kinetic energy · Rolling without slipping · Race of rolling bodies · Work and power in rotation · Angular momentum of a particle

← All Rotational Motion topics