Superposition Principle and Resultant Amplitude of Two Waves

Physics · Wave Optics · NEET

The superposition principle says: when two or more waves meet at a point, the total displacement is just the sum of the individual displacements. For two waves of equal amplitude a with a phase difference phi, the resultant amplitude is R = 2a cos(phi/2), so the intensity is I = 4I0 cos2(phi/2). Memory hook: "waves just ADD up" — same phase means they help each other (R = 2a), opposite phase means they cancel (R = 0).
Superposition of Two Waves: Resultant R = 2a cos(phi/2)phi = 0 (in phase)R = 2a (constructive)phi = pi (opposite)R = 0 (destructive)Key resultsR = 2a cos(phi/2)I = 4I0 cos2(phi/2)phi = 0 -> I = 4I0phi = pi -> I = 0phi = (2pi/lambda) x path diff
Two coherent waves add by superposition. In phase (phi = 0) their amplitudes combine to R = 2a with intensity 4I0; fully out of phase (phi = pi) they cancel to R = 0. The general result is R = 2a cos(phi/2) and I = 4I0 cos2(phi/2).

Your doubts, answered

Is the superposition principle only for light waves?

No. Superposition is a general wave property. You first met it in Class 11 for waves on a string and sound waves, and it also works for water ripples, electric fields, and light. It says the medium point moves by the algebraic sum of what each wave alone would produce. In Wave Optics we simply apply this same rule to two light waves to explain interference.

What is the resultant amplitude of two waves formula?

For two waves of the same amplitude a and same frequency, meeting with a phase difference phi, the resultant amplitude is R = 2a cos(phi/2). If the two waves have different amplitudes a1 and a2, use the vector-addition form: R = sqrt(a1^2 + a2^2 + 2 a1 a2 cos phi). Both come straight from adding the two wave equations.

Why is the resultant amplitude 2a cos(phi/2) and not just a + a = 2a?

The plain sum 2a only happens when the two waves are perfectly in step (phi = 0), because cos(0) = 1. For any other phase difference the waves are shifted, so at a given instant one is not at its peak when the other is. The factor cos(phi/2) accounts for this shift. At phi = pi (fully opposite), cos(pi/2) = 0, so R = 0 and the waves cancel.

Do amplitudes add or do intensities add?

For coherent waves (fixed phase relation), you add the DISPLACEMENTS (amplitudes as vectors) first, then square to get intensity: I = 4I0 cos2(phi/2). For incoherent sources (rapidly changing phase), the cross term averages to zero and the INTENSITIES simply add: I = I1 + I2. This is why two separate bulbs never make a visible interference pattern.

If two waves cancel, where does the energy go?

Energy is not destroyed. Superposition only redistributes energy across the screen. Where the waves cancel (dark point) the energy is missing, but at points of constructive interference the intensity rises to 4I0, which is double the 2I0 you would expect from just adding two sources. Averaged over the whole pattern, the total energy is conserved.

⚠️ The NEET trap
At two coherent sources of equal intensity I0 each, the brightest point has intensity 2 I0 (just add the two).
For coherent waves you add amplitudes first: R = 2a, so I_max = (2a)^2 is proportional to 4I0, NOT 2I0. Intensities add to 2I0 only for INCOHERENT sources.
🧠 Coherent = add amplitudes then square (4I0). Incoherent = add intensities (2I0). Check coherence before you add.

Real NEET questions

NEET 2026

In Young's double slit experiment, using monochromatic light of wavelength lambda, the intensity of light at a point on the screen where the path difference is lambda is K units. The intensity of light at a point where the path difference is lambda/3 will be

A · K/4
B · K
C · 2K
D · K/2
Solution: Use resultant intensity I = I_max cos2(phi/2), where phase difference phi = (2 pi / lambda) x path difference. Step 1: at path difference = lambda, phi = 2 pi, so cos2(phi/2) = cos2(pi) = 1, giving I = I_max = K. So I_max = K. Step 2: at path difference = lambda/3, phi = (2 pi / lambda)(lambda/3) = 2 pi/3, so cos2(phi/2) = cos2(pi/3) = (1/2)^2 = 1/4. Step 3: I = K x 1/4 = K/4. Answer A.
NEET 2016

The interference pattern is obtained with two coherent light sources of intensity ratio n. In the interference pattern, the ratio (I_max - I_min)/(I_max + I_min) will be

A · sqrt(n)/(n+1)
B · 2 sqrt(n)/(n+1)
C · sqrt(n)/(n+1)^2
D · 2 sqrt(n)/(n+1)^2
Solution: From superposition, amplitudes add and cancel: I_max = (sqrt(I1) + sqrt(I2))^2 and I_min = (sqrt(I1) - sqrt(I2))^2. Step 1: I_max - I_min = 4 sqrt(I1 I2) and I_max + I_min = 2(I1 + I2). Step 2: ratio = 4 sqrt(I1 I2) / (2(I1 + I2)) = 2 sqrt(I1 I2)/(I1 + I2). Step 3: put I1/I2 = n, divide top and bottom by I2: = 2 sqrt(n)/(n + 1). Answer B.

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Frequently asked

What is the principle of superposition of waves?

When two or more waves overlap at a point in a medium, the resultant displacement at that point is the algebraic (vector) sum of the displacements produced by each wave separately. Each wave travels as if the others are not present.

What is the formula for resultant amplitude of two waves?

For equal amplitudes a with phase difference phi: R = 2a cos(phi/2). For unequal amplitudes a1 and a2: R = sqrt(a1^2 + a2^2 + 2 a1 a2 cos phi). The resultant intensity is proportional to R squared.

What is the maximum and minimum resultant amplitude?

Maximum amplitude is R = a1 + a2 when phi = 0 (waves in phase, constructive). Minimum amplitude is R = |a1 - a2| when phi = pi (waves out of phase, destructive). For equal amplitudes the minimum is zero.

Why do coherent sources give I = 4I0 but incoherent give 2I0?

Coherent waves have a fixed phase, so amplitudes add: R = 2a and I_max is proportional to 4I0. Incoherent waves have a rapidly changing phase, so cos(phi) averages to zero and only intensities add, giving 2I0 everywhere with no pattern.

What is the difference between resultant displacement and resultant amplitude?

Resultant displacement is the instantaneous sum y = y1 + y2 and it changes with time. Resultant amplitude R = 2a cos(phi/2) is the fixed peak value of that combined wave at a given point, set only by the phase difference phi.