GRE Physics Companion: Power
Power problems are usually short once the correct form is recognized.
The central relations are
and
For the net force,
Figure 1. A compact strategy for GRE power problems. First decide whether the question
concerns average power, instantaneous force-velocity power, energy rate, or efficiency.
1 High-value GRE facts
- Average power is work divided by elapsed time.
- instantaneous power is dW∕dt.
- For a force acting on a particle,
- A force perpendicular to velocity delivers zero instantaneous power.
- Negative power means that the force removes mechanical energy from the particle.
- The area under a P versus t graph is work.
- A kilowatt-hour is energy, not power.
- For constant net power,
- For collinear motion at constant power,
- If drag satisfies FD ∝ v2, then the power required to overcome drag satisfies P
D ∝ v3.
Part I: Original GRE-style problems
Problem 1: average power
A machine does 18 kJ of work in 6.0 s. Its average power is
- 0.33 kW
- 3.0 kW
- 6.0 kW
- 18 kW
- 108 kW
Problem 2: force and velocity
A 100 N force acts on a particle moving at 5.0 m∕s. The angle between force and velocity is 60∘.
The power delivered by the force is
- 0 W
- 100 W
- 250 W
- 500 W
- 1000 W
Problem 3: perpendicular force
A particle moves in uniform circular motion under a central force. The instantaneous power
delivered by the central force is
- negative
- zero
- proportional to v
- proportional to v2
- impossible to determine
Problem 4: braking power
A braking force of magnitude 4000 N acts opposite a CAR moving at 15 m∕s. The instantaneous
power of the braking force is
- −60 kW
- −15 kW
- 0
- 15 kW
- 60 kW
Problem 5: lifting
A 60 kg person climbs a vertical height of 5.0 m in 4.0 s. Taking g = 9.8 m∕s2, the average
mechanical power against gravity is closest to
- 0.37 kW
- 0.74 kW
- 1.5 kW
- 2.9 kW
- 7.4 kW
Problem 6: kilowatt-hour
One kilowatt-hour is equal to
- 3.6 × 103 J
- 3.6 × 104 J
- 3.6 × 105 J
- 3.6 × 106 J
- 3.6 × 109 J
Problem 7: constant power
A motor delivers constant mechanical power P to a vehicle moving in a straight line. Neglecting all
resistive forces, the drive force at speed v is
- Pv
- P∕v
- P∕v2
- v∕P
- independent of v
Problem 8: quadratic drag
A vehicle moves at steady speed through a regime in which the drag force is proportional to v2.
If its speed is doubled, the mechanical power required to overcome drag is multiplied
by
- 2
- 4
- 6
- 8
- 16
Problem 9: efficiency
A motor has efficiency η = 0.80 and must deliver 4.0 kW of useful mechanical output. The required
input power is
- 3.2 kW
- 4.0 kW
- 4.8 kW
- 5.0 kW
- 8.0 kW
Problem 10: power-time graph
The power delivered to a system increases linearly from 0 to 100 W during a 4.0 s interval. The
work done during the interval is
- 50 J
- 100 J
- 200 J
- 400 J
- 800 J
Problem 11: kinetic energy rate
A 2.0 kg particle moves in one dimension at 6.0 m∕s and has acceleration 3.0 m∕s2 in the same
direction. The net instantaneous power is
- 12 W
- 18 W
- 24 W
- 36 W
- 72 W
Problem 12: constant net power from rest
A 4.0 kg particle starts from rest and receives constant net power 200 W for 5.0 s. Its final speed is
closest to
- 5.0 m∕s
- 11.2 m∕s
- 15.8 m∕s
- 22.4 m∕s
- 50 m∕s
Part II: Complete worked solutions
Solution 1
Average power is
Thus
| Pavg | =  | (8)
|
| = 3000 W | (9)
|
| = 3.0 kW. | (10) |
Answer: (B).
Solution 2
Use
Therefore
| P | = (100)(5.0) cos 60∘ | (12)
|
| = 250 W. | (13) |
Answer: (C).
Solution 3
In uniform circular motion, the central force is perpendicular to the velocity:
Therefore
Answer: (B).
Solution 4
The force is opposite the velocity, so
Thus
| P | = Fv cos 180∘ | (17)
|
| = −(4000)(15) | (18)
|
| = −60 000 W | (19)
|
| = −60 kW. | (20) |
Answer: (A).
Solution 5
The work done against gravity is
| W | = mgh | (21)
|
| = (60)(9.8)(5.0) | (22)
|
| = 2940 J. | (23) |
Average power is
| Pavg | =  | (24)
|
| = 735 W | (25)
|
| = 0.735 kW. | (26) |
Answer: (B).
Solution 6
Use
| 1 kWh | = (1000 J∕s)(3600 s) | (27)
|
| = 3.6 × 106 J. | (28) |
Answer: (D).
Solution 7
For force parallel to velocity,
Therefore
Answer: (B).
Solution 8
If
then
Doubling speed gives
Answer: (D).
Solution 9
Efficiency is
Thus
Answer: (D).
Solution 10
Work is the area under the power-time graph. The graph is a triangle:
Answer: (C).
Solution 11
Net power can be written as
The acceleration and velocity are parallel, so
| Pnet | = mav | (38)
|
| = (2.0)(3.0)(6.0) | (39)
|
| = 36 W. | (40) |
Answer: (D).
Solution 12
Constant net power changes kinetic energy according to
Starting from rest,
| Kf | = (200)(5.0) | (42)
|
| = 1000 J. | (43) |
Then
For m = 4.0 kg,
| 2vf2 | = 1000, | (45)
|
| vf2 | = 500, | (46)
|
| vf | = 22.4 m∕s. | (47) |
Answer: (D).
2 GRE checklist
Before calculating, identify what kind of power is being asked for.
- If total work and elapsed time are given, use Pavg = ΔW∕Δt.
- If force and velocity are given, use P = F ⋅ v.
- If kinetic energy is changing, use Pnet = dK∕dt.
- If a power-versus-time graph is given, find the signed area.
- If efficiency is involved, distinguish input power from useful output power.
- If constant power drives collinear motion, remember F = P∕v.
- If resistance is proportional to v2, remember that required power scales as v3.
- Check whether the sign of power should be positive, zero, or negative.
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.