Superposition and interference · Physics Class 11–12 | StemPy Lab
Course 14.2·Lesson 1 of 3
Superposition and interference
When two waves meet, the displacement at each point is the sum of their displacements. This is the principle of superposition. Two waves of the same frequency with a phase difference ϕ add to a wave of amplitude 2acos(ϕ/2), so they can help each other or cancel.
about 30 min1 simulation2 practice questions1 Python program5 questions to check yourself
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Two pulses on one rope
Two children hold the ends of a long skipping rope. Each one flicks the rope once. Two pulses run towards each other. What happens when they meet? Do they bounce off each other? Do they crash and stop?
Neither. Look at the picture.
Two columns of three pictures of a rope. Left column, two pulses on the same side: before they meet, one moves right and one moves left; when they overlap exactly, the rope rises twice as high; after they have passed, both pulses go on unchanged. Right column, one pulse up and one pulse down: when they overlap exactly, the rope is flat for an instant; afterwards both pulses go on unchanged. Dashed curves show each pulse alone and the solid curve shows the rope, which is their sum.
On the left, both pulses are on the same side. When they overlap, the rope rises twice as high as one pulse. On the right, one pulse is up and one is down. When they overlap exactly, the rope is flat for an instant. In both cases the pulses then move on, with the same shape as before. Each pulse passes through the other as if the other was not there.
The principle of superposition
This is a rule for waves on a rope, on water, in air and in many other places. When two or more waves are at one point at the same time, the displacement there is the sum of the displacements of each wave:
y=y1+y2
We call this the principle of superposition. Displacements on opposite sides have opposite signs, so they can cancel.
In the flat moment on the right, where did the energy go? It did not vanish. The rope is flat, but it is moving. The energy is all kinetic for that instant. A moment later the pulses appear again.
Two waves with a phase difference
Now take two long waves on the same string, with the same amplitude a, the same wavelength and the same frequency. The second is shifted by a phase differenceϕ:
y1=asin(kx−ωt),y2=asin(kx−ωt+ϕ)
Add them. A rule of trigonometry, sinA+sinB=2sin2A+Bcos2A−B, gives
y=2acos2ϕsin(kx−ωt+2ϕ)
The sum is again a wave of the same wavelength and frequency. Its amplitude is
A=2acos2ϕ
(Take the size of this; an amplitude is never negative.) Let us look at three cases.
ϕ=0: the waves are in phase. A=2a. They help each other fully. This is constructive interference.
ϕ=π: the waves are out of phase. A=0. They cancel. This is destructive interference.
Between these, A lies between 0 and 2a. For ϕ=60∘ and a=3mm, A=2×3mm×cos30∘=5.2mm.
When the two amplitudes are different, a1 and a2, the sum is still a wave of the same frequency, with
A2=a12+a22+2a1a2cosϕ
For a1=a2=a this gives the same answer as before.
Intensity
The energy a wave carries each second through each square metre is its intensity. It grows as the square of the amplitude: I∝A2. So two equal waves in phase, with twice the amplitude, give four times the intensity of one wave. Two waves out of phase give none. The energy is not lost. It goes to the places where the waves are in phase.
If the amplitudes are a1 and a2, the largest and the smallest intensities are in the ratio
IminImax=(a1−a2)2(a1+a2)2
Path difference and phase difference
Two sources in step send out waves of wavelength λ. At a point, one wave has come a distance x1 and the other x2. The difference Δx=x2−x1 is the path difference. One wavelength of path is a whole cycle, 2π, of phase. So
ϕ=λ2πΔx
A path difference of 0, λ, 2λ and so on gives constructive interference. A path difference of λ/2, 3λ/2 and so on gives destructive interference.
Practise with new numbers
Try it in Python
The program adds two waves point by point along a string. Then it compares the largest value of the sum with the formula 2acos(ϕ/2).
Common mistakes
Adding amplitudes in every case.a1+a2 is right only when the waves are in phase.
Thinking that waves which cancel destroy energy. The energy moves to other places, or into motion of the medium.
Forgetting the half angle. For equal waves, A=2acos(ϕ/2), not 2acosϕ.
Adding intensities when the waves are in step. Add the displacements first, then square.
Remember these
Superposition: the displacements of waves at a point add, y=y1+y2.
Pulses pass through each other unchanged.
Equal waves with a phase difference ϕ: A=2acos(ϕ/2).
In phase: A=2a. Out of phase: A=0.
Intensity I∝A2. Phase difference ϕ=λ2πΔx.
Check yourself
Try each one on your own first. If you are stuck, open a hint. Then check with Show the answer.
A pulse 2cm high meets a pulse 5cm deep on a rope, on the other side. What is the displacement of the rope where they overlap exactly?
Two equal waves of amplitude a meet with a phase difference of 90∘. What is the amplitude of the sum?
Two waves arrive at a point with a path difference of 1.5λ. Do they help each other or cancel?
Two equal waves in phase give an intensity I. What intensity does one of them give alone?
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