Superposition: Question 7

Syllabus 8.2, 8.3

Structured AS 9 marks

Two dippers, S1S_1 and S2S_2, oscillate in phase in a ripple tank, producing coherent water waves of wavelength 2.4 cm2.4\text{ cm}. A point PP on the water surface is 25.2 cm25.2\text{ cm} from S1S_1 and 19.2 cm19.2\text{ cm} from S2S_2.

(a) State the condition, in terms of path difference and wavelength λ\lambda, for constructive interference to occur at a point, and the condition for destructive interference to occur. [2]

(b) State two conditions that S1S_1 and S2S_2 must satisfy for a stable, observable interference pattern to be produced on the water surface. [2]

(c) Calculate the path difference between the two waves arriving at PP. [2]

(d) Determine, showing your working, whether the interference at PP is constructive, destructive, or neither. [3]

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Worked solution

Part (a): Conditions for constructive and destructive interference

Constructive interference occurs at a point where the path difference between the two waves is a whole number of wavelengths: path difference=nλ,n=0,1,2,\text{path difference} = n\lambda, \qquad n = 0, 1, 2, \dots

Destructive interference occurs at a point where the path difference is an odd number of half-wavelengths: path difference=(n+12)λ,n=0,1,2,\text{path difference} = \left(n+\tfrac12\right)\lambda, \qquad n = 0, 1, 2, \dots

Part (b): Conditions for a stable interference pattern

For S1S_1 and S2S_2 to produce a stable, observable interference pattern, they must be coherent, which requires:

  • the same frequency (and hence the same wavelength), and
  • a constant (non-varying) phase difference between them.

(In this case, being driven in phase from the same oscillator ensures both conditions are met.)

Part (c): Path difference at PP

The path difference is the difference between the two distances from the sources to PP: Δ=S1PS2P=25.219.2=6.0 cm\Delta = |S_1P - S_2P| = |25.2 - 19.2| = 6.0\text{ cm}

Check (recompute independently): starting from 19.2 cm19.2\text{ cm} and adding 6.0 cm6.0\text{ cm} gives 19.2+6.0=25.2 cm19.2+6.0=25.2\text{ cm}, matching the given distance from S1S_1, consistent.

So the path difference is Δ=6.0 cm\Delta = \boxed{6.0\text{ cm}}.

Part (d): Type of interference at PP

Express the path difference as a number of wavelengths, using λ=2.4 cm\lambda = 2.4\text{ cm}: Δλ=6.02.4=2.5\frac{\Delta}{\lambda} = \frac{6.0}{2.4} = 2.5

Check (recompute independently): 2.4×2.5=2.4×2+2.4×0.5=4.8+1.2=6.02.4 \times 2.5 = 2.4\times2 + 2.4\times0.5 = 4.8+1.2=6.0, confirms 6.0/2.4=2.56.0/2.4=2.5 exactly.

Since 2.5=2+122.5 = 2 + \tfrac12, the path difference is (2+12)λ\left(2+\tfrac12\right)\lambda, an odd number of half-wavelengths. By the condition stated in part (a), this means the two waves arrive at PP exactly out of phase, so the interference at PP is destructive.

Final answers

  • (a) Constructive: path difference =nλ=n\lambda; destructive: path difference =(n+12)λ=(n+\tfrac12)\lambda
  • (b) Same frequency/wavelength; constant phase difference (coherent)
  • (c) Path difference =6.0 cm= \boxed{6.0\text{ cm}}
  • (d) 6.0 cm=2.5λ=(2+12)λ6.0\text{ cm} = 2.5\lambda = (2+\tfrac12)\lambda, so the interference at PP is destructive