Superposition and Wave Interference

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Questions and Answers

When two waves with identical frequency and wavelength superpose in a medium, what condition leads to complete destructive interference?

  • The waves are $\pi$ radians out of phase and possess equal amplitudes. (correct)
  • The waves are $\pi/2$ radians out of phase.
  • The waves have different wavelengths.
  • The waves are in phase.

In the context of wave superposition, which of the following is NOT a characteristic of linear waves?

  • Their amplitudes are much smaller than their wavelengths.
  • They always exhibit constructive interference. (correct)
  • They can pass through each other without being altered.
  • They obey the superposition principle.

Consider two identical waves traveling in the same direction. If the phase difference between them is $\phi$, what value of $\phi$ will result in the largest possible amplitude for the resultant wave?

  • $\phi = 0$ (correct)
  • $\phi = 3\pi/2$
  • $\phi = \pi$
  • $\phi = \pi/2$

When analyzing the interference of sound waves using a tube with adjustable path lengths, what condition regarding the path length difference ($\Delta r$) ensures constructive interference at the receiver?

<p>$\Delta r$ is equal to zero or an integer multiple of the wavelength. (A)</p> Signup and view all the answers

What is the resultant amplitude when two waves having amplitudes $A_1$ and $A_2$ and a phase difference of $\pi$ radians interfere?

<p>$|A_1 - A_2|$ (D)</p> Signup and view all the answers

In the context of wave superposition, how does the interaction of two nonlinear waves typically differ from that of two linear waves?

<p>Nonlinear waves do not necessarily pass through each other unaltered. (D)</p> Signup and view all the answers

Given two sinusoidal waves with the same frequency, wavelength, and amplitude $A$, what is the amplitude of the resultant wave when their phase difference is $\phi = \pi/2$?

<p>$\sqrt{2}A$ (A)</p> Signup and view all the answers

Two sound waves of the same frequency are traveling in the same medium. If the path length from the source to the receiver differs by half a wavelength, what type of interference will occur at the receiver?

<p>Destructive interference (D)</p> Signup and view all the answers

Consider two identical pulses, one upright and one inverted, traveling towards each other on a string. At the moment they completely overlap, what can be said about the displacement of the string?

<p>The displacement is zero. (C)</p> Signup and view all the answers

When two waves interfere, and the resultant wave has a larger amplitude than either individual wave, what term describes this phenomenon?

<p>Constructive interference (B)</p> Signup and view all the answers

Two identical sound sources emit waves in phase. At a certain point, the path difference to the listener is one and a half wavelengths. What will the listener hear?

<p>A quieter sound due to destructive interference (B)</p> Signup and view all the answers

How does the superposition principle apply to waves passing through the same point in a medium?

<p>The resulting wave's amplitude is the algebraic sum of individual wave amplitudes. (A)</p> Signup and view all the answers

Which of the following conditions must be met for two waves to exhibit complete destructive interference?

<p>They must have the same amplitude and be 180 degrees out of phase. (C)</p> Signup and view all the answers

In a scenario where two identical waves are superimposing, and the resulting wave has an amplitude of zero, what is their phase difference?

<p>$\pi$ radians (C)</p> Signup and view all the answers

For two sound waves with equal amplitudes to have maximum constructive interference, what must be the difference in their path lengths from the sources to the point of interference?

<p>An integer multiple of the wavelength (C)</p> Signup and view all the answers

If two identical pulses on a string, one upright and one inverted, meet and completely overlap, what happens to the energy of the pulses at the point of overlap?

<p>The energy is instantaneously zero at the point of overlap. (A)</p> Signup and view all the answers

Consider a scenario where waves are interfering. Under what condition is the superposition considered constructive?

<p>When the resultant wave's amplitude is greater than at least one of the individual waves (D)</p> Signup and view all the answers

Two identical speakers emit sound waves with a wavelength of 2 meters. If a person is positioned such that one speaker is 5 meters away and the other is 6 meters away, will they experience constructive or destructive interference?

<p>Constructive interference (D)</p> Signup and view all the answers

The superposition principle is most directly applicable to which type of waves?

<p>Linear waves (A)</p> Signup and view all the answers

If two identical waves are superimposed and the resultant wave's amplitude is twice the amplitude of each individual wave, what can be concluded about their phase relationship?

<p>They are in phase. (C)</p> Signup and view all the answers

Flashcards

Superposition Principle

The algebraic sum of individual waves' values at any point.

Linear Waves

Waves that obey the superposition principle; small amplitudes relative to wavelength.

Nonlinear Waves

Waves that do not obey the superposition principle; often large amplitudes.

Interference

Waves combine in the same region, creating a resultant wave.

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Constructive Interference

The displacement is in positive y direction; the resultant wave has greater amplitude than individual.

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Destructive Interference

Caused by waves displacements in opposite direction.

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Interference Tube

A simple device to show interference of sound waves.

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Path Length

The distance an wave travels from source to receiver.

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Constructive Interference Condition

When cos(φ/2) = ±1; φ is an even multiple of π.

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Destructive Interference Condition

When cos(φ/2) = 0; φ is an odd multiple of π.

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Study Notes

  • Superposition and interference are wave phenomena involving combinations of traveling waves
  • Analyzing such wave combinations relies on the superposition principle

Superposition Principle

  • The resultant value of the wave function is the algebraic sum of the values of the wave functions of individual waves

Linear Waves

  • Waves that obey the superposition principle
  • Characterized by having amplitudes much smaller than their wavelengths

Nonlinear Waves

  • Waves that violate the superposition principle
  • Often characterized by large amplitudes

Interference

  • It is the combination of separate waves in the same region of space to produce a resultant wave

Constructive Interference

  • Occurs when the displacements caused by overlapping pulses are in the same direction

Destructive Interference

  • Occurs when the displacements caused by overlapping pulses are in opposite directions

Sinusoidal Waves

  • Superposition principle applied to two sinusoidal waves traveling in the same direction in a linear medium

Wave Functions

  • Formulas to consider waves traveling to the right with the same frequency, wavelength, and amplitude but differing in phase:
  • y1 = A sin (kx - ωt)
  • y2 = A sin (kx - ωt + φ)
  • k = 2π/λ
  • ω = 2πf
  • φ is the phase constant

Resultant Wave Function

  • Formula y = 2A cos(φ/2) sin (kx - ωt + φ/2) shows that resultant wave is sinusoidal
  • Frequency and wavelength are the same as the individual waves
  • Amplitude of resultant wave is 2A cos(φ/2)
  • Phase is φ/2

Constructive Interference Condition

  • Crests and troughs of individual waves coincide
  • Waves are said to be everywhere in phase

Interference of Sound Waves

  • Setup involves a loudspeaker sending sound into a tube with a T-shaped junction
  • Sound splits in two directions, reaching a receiver through two paths

Path Length

  • The distance along any path from speaker to receiver
  • The lower path length(₁), is fixed
  • The upper path length (r₂), can be varied

Path Length Difference

  • The difference in path lengths (Δr = r₂ - r₁) determines interference
  • Two waves reach the receiver in phase when Δr is zero or an integer multiple of the wavelength λ so, (Δr = nλ, where n = 0, 1, 2, 3, ...)

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