Unit: Energy and Momentum of Rotating Systems

Lesson Preview

Think of a car's tires spinning out on snow covered roads, or a bowling ball sliding down the lane before it starts rolling smoothly. These everyday examples illustrate the difference between rolling with and without slipping.

An object rolling on a surface has two independent motions: translational velocity vCMv_\text{CM} of its center of mass and angular velocity ω\omega. For a radius RR, we saw previously that the rolling without slipping condition is

vCM=ωRv_\text{CM} = \omega R

When this equality fails, the object is rolling while slipping.

Detecting Slip

Compare vCMv_\text{CM} to ωR\omega R at any instant.

Pure Rolling: vCM=ωRv_\text{CM} = \omega R

The contact point has zero velocity relative to the surface.

vcontact=vCMωR=0v_\text{contact}=v_\text{CM} - \omega R=0
Compiling TikZ diagram...

Overspinning: vCM<ωRv_\text{CM} < \omega R

The wheel spins faster than needed. The contact point slides backward relative to the surface. This occurs when wheels spin on ice.

vcontact=vCMωR<0v_\text{contact}=v_\text{CM} - \omega R<0
Compiling TikZ diagram...

Underspinning: vCM>ωRv_\text{CM} > \omega R

...

... continued in the full lesson.

Ready to Start Learning?

Sign up now to access the full Rolling with Slipping (Energy) lesson and our entire curriculum!