GRE Physics Companion: Energy Methods for Particle Systems
The two formulas to recognize immediately are
and
For two particles,
1 High-value GRE facts
- Total kinetic energy is the sum of the kinetic energies of all particles.
- K = KCM + Krel.
- internal forces cancel from the net force but not generally from work.
- Actual external work uses the displacement of each force application point.
- Fext,net ⋅ dRCM is pseudowork and tracks KCM.
- Zero total momentum does not imply zero total kinetic energy.
- If no net external force acts, V CM is constant.
- An explosion can increase Krel while leaving KCM unchanged.
- For two particles, use reduced mass for relative kinetic energy.
- In uniform gravity, the system potential is MgY CM.
Part I: Original GRE-style problems
Problem 1: center-of-mass velocity
Two particles move along a line. Particle 1 has mass 2m and velocity +v, while particle 2 has mass
m and velocity −v. The center-of-mass velocity is
- −v
- −v∕3
- 0
- +v∕3
- +v
Problem 2: zero momentum
A system has total momentum zero. Which statement must be true?
- Its total kinetic energy is zero.
- Its center-of-mass kinetic energy is zero.
- Every particle is at rest.
- Its relative kinetic energy is zero.
- No internal forces act.
Problem 3: kinetic-energy decomposition
A system has total kinetic energy 50 J and center-of-mass kinetic energy 18 J. Its relative kinetic
energy is
- 18 J
- 32 J
- 50 J
- 68 J
- 900 J
Problem 4: reduced mass
Two particles have masses m and 3m. Their reduced mass is
- m∕4
- 3m∕4
- m
- 3m
- 4m
Problem 5: internal force work
Which statement is correct for equal-and-opposite internal forces?
- Their net internal work is always zero.
- They cancel from the net force, but their total work need not vanish.
- They can never change relative kinetic energy.
- They are always nonconservative.
- They cannot store potential energy.
Problem 6: explosion at rest
A system initially at rest explodes into two fragments in the absence of external impulse. Which
quantity must remain zero?
- total kinetic energy
- relative kinetic energy
- center-of-mass velocity
- speed of each fragment
- internal energy change
Problem 7: actual work versus pseudowork
A constant external force F moves one particle of a two-equal-particle system through distance d,
while the second particle remains fixed. The actual external work is Fd. The center of mass
moves
- 0
- d∕4
- d∕2
- d
- 2d
Problem 8: pseudowork
For the system in Problem 7, the center-of-mass pseudowork is
- 0
- Fd∕4
- Fd∕2
- Fd
- 2Fd
Problem 9: uniform gravity
For particles in a uniform gravitational field,
This equals
- Mg∕Y CM
- MgY CM
- M2gY
CM
- gY CM∕M
- zero
Problem 10: two-fragment momentum
A 2 kg fragment moves at +6 m∕s after an explosion from rest. The second fragment has mass 3 kg.
Its velocity is
- −9 m∕s
- −6 m∕s
- −4 m∕s
- +4 m∕s
- +9 m∕s
Problem 11: explosion kinetic energy
For the fragments in Problem 10, the total kinetic energy is
- 12 J
- 24 J
- 36 J
- 60 J
- 72 J
Problem 12: isolated spring pair
Two particles connected by an ideal spring form an isolated system. Which quantity is necessarily
constant?
- each particle’s kinetic energy
- the spring potential energy
- Krel
- KCM
- each particle’s speed
Part II: Complete worked solutions
Solution 1
The total mass is
The total momentum is
Thus
Answer: (D).
Solution 2
If total momentum is zero,
Thus
and
The particles can still move relative to one another.
Answer: (B).
Solution 3
Use
Thus
Answer: (B).
Solution 4
The reduced mass is
| μ | =  | (13)
|
| =  | (14)
|
| = m. | (15) |
Answer: (B).
Solution 5
Newton’s third law makes the pair forces equal and opposite, so they cancel from the net system
force.
Their work is
which need not vanish.
Answer: (B).
Solution 6
With no external impulse, total momentum is constant.
The initial system is at rest, so
and therefore
after the explosion.
Answer: (C).
Solution 7
For equal masses,
If particle 1 moves by d and particle 2 remains fixed,
Answer: (C).
Solution 8
Pseudowork is
Using
we obtain
Answer: (C).
Solution 9
By definition,
Therefore
Multiplying by g,
Answer: (B).
Solution 10
Momentum conservation gives
Thus
Answer: (C).
Solution 11
The kinetic energy is
| K | = (2)(62) + (3)(42) | (29)
|
| = 36 + 24 | (30)
|
| = 60 J. | (31) |
Answer: (D).
Solution 12
An isolated system has no net external force, so
is constant.
Therefore
is constant.
The spring can exchange energy with relative motion, so Krel and Us need not be individually
constant.
Answer: (D).
2 GRE checklist
For particle-system energy problems:
- Compute the center-of-mass velocity when momentum information is available.
- Use K = KCM + Krel.
- For two particles, consider the reduced mass.
- Do not assume internal work vanishes.
- Distinguish actual external work from pseudowork.
- Use momentum conservation for explosions and internal releases.
- In uniform gravity, replace ∑
migyi with MgY CM when useful.
- State the system boundary before assigning internal and external interactions.
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.