GRE Physics Companion: Beats, Interference, and Coherence
For two coherent waves,
For nearby frequencies,
For path difference,
Figure 1. A compact strategy: decide whether the problem concerns fixed-phase interference,
nearby-frequency beats, or finite coherence; then work with amplitudes first and intensities second.
1 High-value GRE facts
- Superpose amplitudes before squaring for coherent waves.
- Equal amplitudes and zero phase difference give maximum reinforcement.
- Equal amplitudes and phase difference π give complete cancellation.
- Δϕ = (2π∕λ)Δr + ϕ0.
- In-phase sources constructively interfere at Δr = mλ.
- In-phase sources destructively interfere at Δr = (m + 1∕2)λ.
- fbeat = |f1 − f2|.
- Tbeat = 1∕fbeat.
- Unequal beat amplitudes give nonzero minima.
- Narrow bandwidth implies long coherence time.
Part I: Original GRE-style problems
Problem 1: equal-amplitude constructive interference
Two coherent waves each have amplitude
and zero phase difference. The resultant amplitude is
- 0
- A∕2
- A
- 2A
- 4A
Problem 2: destructive interference
Two equal-amplitude coherent waves cancel completely when their phase difference
is
- 0
- π∕2
- π
- 2π
- 4π
Problem 3: equal-source intensity maximum
Each of two equal coherent sources individually produces intensity
At complete constructive interference, the total intensity is
- I0
- 2I0
- 3I0
- 4I0
- 8I0
Problem 4: path difference
Two in-phase sources have wavelength
Complete destructive interference occurs at path difference
- 0
- λ∕4
- λ∕2
- λ
- 2λ
Problem 5: beat frequency
Two tones have frequencies
and
The beat frequency is
- 2 Hz
- 4 Hz
- 8 Hz
- 442 Hz
- 884 Hz
Problem 6: beat period
If the beat frequency is
the beat period is
- 0.05 s
- 0.10 s
- 0.20 s
- 1.0 s
- 5.0 s
Problem 7: unequal beat amplitudes
Two nearby-frequency waves have amplitudes
and
The minimum beat-envelope amplitude is
- 0
- A
- 2A
- 5A
- 8A
Problem 8: coherent visibility
Perfectly coherent sources have intensities
The fringe visibility is
- 0.20
- 0.40
- 0.60
- 0.80
- 1.00
Problem 9: incoherent averaging
If the relative phase of two sources varies randomly and rapidly compared with the averaging time,
the average interference term is approximately
- maximum
- minimum
- zero
- infinite
- equal to I1I2
Problem 10: coherence-time estimate
A source has bandwidth
Using
the coherence time is approximately
- 0.001 s
- 0.010 s
- 0.10 s
- 1.0 s
- 100 s
Problem 11: coherence length
For the source in Problem 10, take wave speed
The coherence length is approximately
- 0.03 m
- 0.30 m
- 3.0 m
- 30 m
- 300 m
Problem 12: partial coherence
Two equal-intensity fields have
Their maximum possible fringe visibility is
- 0.30
- 0.49
- 0.70
- 1.00
- 1.40
Part II: Complete worked solutions
Solution 1
In phase, the amplitudes add:
Answer: (D).
Solution 2
For equal amplitudes, complete destructive interference occurs at
The simplest choice is
Answer: (C).
Solution 3
Constructive interference doubles the amplitude. Since intensity is proportional to amplitude
squared,
Answer: (D).
Solution 4
For in-phase sources, destructive interference occurs at
The smallest positive value is
Answer: (C).
Solution 5
Answer: (B).
Solution 6
Answer: (C).
Solution 7
For unequal amplitudes,
Answer: (C).
Solution 8
| 𝒱 | =  | (26)
|
| =  | (27)
|
| = 0.60. | (28) |
Answer: (C).
Solution 9
Rapid random phase variation gives
Thus the stable interference term averages away. Answer: (C).
Solution 10
Answer: (B).
Solution 11
Answer: (C).
Solution 12
For equal intensities,
Therefore
Answer: (C).
2 GRE checklist
- Add coherent amplitudes first, then determine intensity.
- Use phase difference, not source separation alone.
- Convert path difference to phase using 2π∕λ.
- Beat frequency is the absolute frequency difference.
- The average of the two frequencies is not the beat frequency.
- Unequal beat amplitudes give incomplete minima.
- Random phase variation removes the stable interference term.
- Use coherence estimates only at the level justified by the bandwidth convention.
References
References
[1] PhysicsLibrary, M06-12, Acoustic Resonance in Pipes and Helmholtz Resonators.
[2] PhysicsLibrary, M06-10, Fourier Analysis, Wave Packets, and Dispersion.
[3] A. P. French, Vibrations and Waves, W. W. Norton, 1971.
[4] L. E. Kinsler, A. R. Frey, A. B. Coppens, and J. V. Sanders, Fundamentals of
Acoustics, 4th ed., Wiley, 2000.