GRE Physics Companion: Angular Momentum of Particle Systems
The core relations are
and
For a particle system with central internal forces,
Figure 1. A compact strategy for angular-momentum problems. State the origin, compute cross
products or perpendicular lever arms, then connect torque to the change in angular momentum.
1 High-value GRE facts
- Angular momentum depends on the chosen origin.
- L = r⊥p for a particle.
- Torque is the time rate of change of angular momentum.
- Zero external torque implies constant total angular momentum.
- angular impulse equals ΔL.
- A central force has zero torque about its force center.
- In the center-of-mass decomposition, LO = RCM × P + LCM.
- Radial motion contributes no angular momentum about the center.
- For planar polar motion, L = mr2𝜃.
- For fixed-axis rigid body rotation, Lz = Izω.
Part I: Original GRE-style problems
Problem 1: perpendicular motion
A particle has momentum magnitude p and moves along a line whose perpendicular distance from
the origin is b. Its angular-momentum magnitude about the origin is
- p∕b
- bp
- b∕p
- p2b
- zero
Problem 2: radial motion
A particle moves directly away from the origin. Its angular momentum about the origin
is
- mrv
- mrv∕2
- mv∕r
- zero
- dependent on acceleration
Problem 3: torque
A force F acts parallel to the position vector r. The torque about the origin is
- rF
- rF∕2
- zero
- F∕r
- mrv
Problem 4: angular impulse
A constant torque 5 N m acts for 3 s. The change in angular momentum magnitude
is
- 5 kg m2∕s
- 8 kg m2∕s
- 15 kg m2∕s
- 25 kg m2∕s
- 75 kg m2∕s
Problem 5: central force
A particle moves under a central force. Which quantity is necessarily conserved about the force
center?
- linear momentum
- angular momentum
- kinetic energy for every central force
- speed
- position
Problem 6: center-of-mass decomposition
A system has RCM = 2ex m, total momentum P = 3ey kg m∕s, and LCM = 4ez kg m2∕s. Its
angular momentum about the origin is
- 2ez
- 4ez
- 6ez
- 10ez
- 12ez
Problem 7: planar polar motion
For a particle in planar polar coordinates, angular momentum magnitude about the origin
is
- mṙ
- mr𝜃
- mr2𝜃
- mr2ṙ
- m𝜃∕r
Problem 8: areal velocity
For a particle of mass m with angular momentum magnitude L under a central force, the areal
velocity is
- L∕m
- L∕(2m)
- 2L∕m
- m∕(2L)
- zero
Problem 9: origin shift
Two origins differ by constant vector a. If total linear momentum is zero, then the total angular
momentum about the two origins is
- always different
- identical
- opposite
- related by a factor of two
- undefined
Problem 10: internal forces
For two particles with equal-and-opposite central internal forces, the pair’s total internal torque
about any origin is
- zero
- twice either individual torque
- always parallel to the force
- proportional to total mass
- nonzero unless the origin is the center of mass
Problem 11: fixed-axis rigid body
A rigid body rotates about a fixed z axis. Its axial angular momentum is
- Mω
- Iz∕ω
- Izω
- Izω2
- MrCMω
Problem 12: zero external torque
If the net external torque on a particle system is zero and internal torques cancel, then
- every particle velocity is constant
- total linear momentum must be zero
- total angular momentum is constant
- kinetic energy must be constant
- all forces vanish
Part II: Complete worked solutions
Solution 1
Use the perpendicular-distance form:
Answer: (B).
Solution 2
Radial motion has r parallel to p, so
Answer: (D).
Solution 3
If F is parallel to r,
Answer: (C).
Solution 4
Answer: (C).
Solution 5
A central force gives zero torque about its center, so angular momentum is conserved. Answer:
(B).
Solution 6
| LO | = RCM × P + LCM | (9)
|
| = (2ex) × (3ey) + 4ez | (10)
|
| = 10ez kg m2∕s. | (11) |
Answer: (D).
Solution 7
Answer: (C).
Solution 8
Answer: (B).
Solution 9
Use
If P = 0, the two angular momenta are identical. Answer: (B).
Solution 10
The pair torque is
For a central force, the two vectors are parallel, so the cross product is zero. Answer:
(A).
Solution 11
For fixed-axis rotation,
Answer: (C).
Solution 12
From
zero external torque implies constant total angular momentum. Answer: (C).
2 GRE checklist
- State the origin before computing angular momentum or torque.
- Use r⊥p when the geometry is simpler than a full cross product.
- Apply the right-hand rule to determine vector direction.
- Connect angular impulse to ΔL.
- For system problems, distinguish external torque from internal torque.
- Recognize central forces immediately as zero-torque forces about their center.
- Use the center-of-mass decomposition when translation and internal motion coexist.
- Do not use L = Iω as an unrestricted three-dimensional Vector Identity.
References
References
[1] J. R. Taylor, Classical Mechanics, University Science Books, 2005.
[2] D. Kleppner and R. Kolenkow, An Introduction to Mechanics, 2nd ed., Cambridge
University Press, 2014.
[3] OpenStax, University Physics, Volume 1, Rice University, 2016.