Example: Rotational Angular Momentum of a Bicycle Wheel
A bicycle wheel has a mass of 0.8kg and a radius of 32cm. If the wheel rotates in the xz plane, spinning clockwise when viewed from the +y axis, and making one full revolution in 0.75 seconds, what is the rotational angular momentum of the wheel?
Facts
Mass of bicycle wheel = 0.8kg.
Bicycle wheel has a radius of 32cm.
Bicycle wheel is spinning clockwise when viewed from the +y axis.
Bicycle wheel rotates in the xz plane.
Bicycle wheel completes one full revolution in 0.75 seconds.
Lacking
The rotational angular momentum of the wheel
Approximations & Assumptions
No friction in the bearings therefore angular speed is constant
Ignore the spokes of the bicycle
Representations
Equation for moments of inertia for a hoop: $I=MR^{2}$
$\omega = \frac{2\pi}{T}$
$\vec{L}_{rot} = I \vec{\omega}$
Solution
We know from the right hand rule that because the wheel is moving clockwise in xz plane that the direction of $\vec{\omega}$ is -y.
We are trying to find the rotational angular momentum and to do so we must find $I$ and $\vec{\omega}$ to fill into the following equation: $\vec{L}_{rot} = I \vec{\omega}$
We can find $I$ by knowing the mass of the wheel and radius of the wheel.
$I = MR^{2} = (0.8kg)(0.32m)^2 = 0.082 kg \cdot m^2$
We can find $\omega$ because we know that one revolution is equal to $2\pi$ and that this revolution is completed in 0.75seconds.
$\omega = \frac{2\pi}{0.75s} = 8.38 s^{-1}$
We now have values for $I$ and $\omega$ and can find the rotational velocity by filling into $\vec{L}_{rot} = I \vec{\omega}$
$\mid\vec{L}_{rot}\mid$ = $(0.082 kg \cdot m^2)(8.38 s^{-1}) = 0.69 kg \cdot m^2/s$
Therefore the rotational angular momentum is equal to:
$\vec{L}_{rot} = \langle 0, -0.69, 0 \rangle kg \cdot m^2/s$