Animated Solution for Physics - Rotational Motion: A disc of mass M and radius R is rolling with angular speed ω on a horizontal plane as shown. The magnitude of angular momentum of the disc about the origin O is
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Visualized Solution
Visualizing the Rolling Disc
Disc of mass M and radius R is rolling on the x-axis.
Angular speed is ω.
LO=LCM+r×pCM
Angular momentum about a fixed point O is the sum of:
1. Spin angular momentum about CM: LCM
2. Orbital angular momentum of CM about O: r×pCM
Pure Rolling Condition
For pure rolling on a stationary surface:
v=Rω
LCM=ICMω
Spin angular momentum:
ICM=21MR2
Direction of ω is into the page (clockwise).
∣LCM∣=21MR2ω
Lorbital=r×pCM
Orbital angular momentum:
pCM=Mv=MRω
Perpendicular distance from O to the line of velocity is R.
∣r×pCM∣=pCM×R=(MRω)R=MR2ω
LO=LCM+Lorbital
Both vectors point into the page.
LO=21MR2ω+MR2ω
LO=23MR2ω
LO=(21+1)MR2ω
LO=23MR2ω
The Way Forward
What if the disc was slipping?
What if we calculated angular momentum about a point on the x-axis?
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The Sigma Insight: Torque and Angular Momentum
Solution Diagram
The Anatomy of Angular Momentum
When a rigid body like a disc is both translating and rotating, its total angular momentum about any fixed point in space is not just a single simple term. It is a beautiful vector sum of two distinct physical phenomena.
Imagine you are standing at the origin O, watching this disc roll past you. You see two things happening simultaneously: the disc is spinning around its own center, and the center of the disc is moving linearly past you.
Mathematically, this is expressed by the master equation:
LO=LCM+r×pCM
Here, LCM is the spin angular momentum (the rotation of the disc about its own center of mass), and r×pCM is the orbital angular momentum (the angular momentum of the center of mass itself, treated as a point particle, about the origin).
Decoding the Spin
Let's break down the first term, the spin angular momentum. For a symmetric body rotating about its center of mass, this is simply the moment of inertia multiplied by the angular velocity:
LCM=ICMω
For a uniform solid disc, the moment of inertia about its central axis is ICM=21MR2.
The disc is rolling forward, which means it is rotating clockwise. If you curl the fingers of your right hand in a clockwise direction, your thumb points directly into the page (or screen). Therefore, the magnitude of the spin angular momentum is 21MR2ω, and its direction is into the page.
The Orbital Contribution
Now, let's look at the orbital term, r×pCM. The center of mass of the disc is moving in a straight horizontal line. Because the disc is undergoing pure rolling, the velocity of the center of mass is intimately tied to its angular speed by the relation v=Rω.
The linear momentum of the center of mass is pCM=Mv=MRω.
To compute the cross product r×pCM, we don't need to do complicated matrix math. We can use the geometric definition: the magnitude is simply the momentum multiplied by the perpendicular distance from the origin to the line of motion.
The center of mass moves along a horizontal line at a constant height R above the x-axis. Therefore, the perpendicular distance is exactly R.
∣r×pCM∣=(MRω)×R=MR2ω
What about the direction? Using the right-hand rule for the cross product (fingers from r curling towards pCM), your thumb again points directly into the page.
The Grand Summation
We have found our two pieces of the puzzle. Both the spin angular momentum and the orbital angular momentum point in the exact same direction (into the page). Because they are collinear, we can simply add their magnitudes together algebraically to find the total angular momentum about the origin:
LO=21MR2ω+MR2ω
LO=23MR2ω
This elegant result shows that the translational motion of the rolling disc contributes twice as much to the total angular momentum about the origin as its own internal spinning does!