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Wave Motion: Superposition, Reflection, Transmission, Refraction, and Standing Waves

Study Guide - Smart Notes

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Wave Motion

Principle of Superposition

The principle of superposition states that when two or more waves traverse the same medium simultaneously, the resultant displacement at any point is the algebraic sum of the displacements due to each wave. This principle is fundamental to understanding complex wave phenomena such as interference and standing waves.

  • Composite Waves: When multiple waves overlap, the resulting wave is called a composite or complex wave.

  • Fourier's Theorem: Any complex wave can be represented as a sum of simple sinusoidal waves (harmonics). For example, a square wave can be constructed from a series of sine waves with different frequencies and amplitudes.

  • Example: The first five terms of the Fourier series for a square wave are: $y(x) = \sin(x) + \frac{1}{3}\sin(3x) + \frac{1}{5}\sin(5x) + \frac{1}{7}\sin(7x) + \frac{1}{9}\sin(9x)$

Superposition of three waves and their sum

  • Physical Example: Surface ripples on water pass through each other, reinforcing or canceling out at different points in space and time.

Water surface showing superposition of ripples

Reflection and Transmission of Waves

When a wave encounters a boundary between two media, part of the wave may be reflected and part may be transmitted. The behavior depends on the properties of the media and the boundary conditions.

  • Fixed End Reflection: If a wave pulse reaches a fixed boundary, it reflects and is inverted.

  • Free End Reflection: If the boundary is free to move, the reflected pulse is not inverted.

Reflection of a wave at fixed and free ends

  • Transmission at a Boundary: When a wave passes from a light string to a heavy string, part of the wave is reflected (inverted) and part is transmitted (upright but reduced in amplitude). The heavier the second medium, the more energy is reflected.

Wave pulse at a boundary between light and heavy strings

Wave Fronts and Huygen's Principle

A wave front is a continuous line or surface representing points of equal phase (e.g., all crests or all troughs). Wave fronts help visualize the propagation of waves in two or three dimensions.

  • Plane Wave: Wave fronts are parallel lines (crests).

  • Circular Wave: Wave fronts are concentric circles.

  • Ray: A line perpendicular to the wave front, indicating the direction of energy propagation.

  • Huygen's Principle: Every point on a wave front acts as a source of secondary spherical wavelets. The new wave front is the tangent to these wavelets.

Huygen's principle for plane and circular waves

  • Rays and Wave Fronts: Rays are always perpendicular to wave fronts, showing the direction of wave travel.

Rays and wave fronts for curved and plane waves

Reflection of a Wave Front: Fermat's Principle of Least Time

Fermat's principle states that the path taken by a ray of light (or any wave) between two points is the one that takes the least time. For reflection, this leads to the law of reflection:

  • Law of Reflection: The angle of incidence equals the angle of reflection ($\theta_i = \theta_r$), both measured from the normal to the surface.

  • Universality: This law applies to both mechanical and electromagnetic waves.

Reflection of wave fronts and rays at a surface

Interference

Interference occurs when two or more waves overlap in space, resulting in a new wave pattern. The principle of superposition governs the resultant displacement.

  • Constructive Interference: Occurs when waves are in phase, resulting in increased amplitude.

  • Destructive Interference: Occurs when waves are out of phase by half a wavelength ($\pi$ radians), resulting in reduced or zero amplitude.

Constructive and destructive interference of waves

Standing Waves

A standing wave is formed by the superposition of two waves of the same frequency and amplitude traveling in opposite directions. The result is a wave pattern that appears stationary, with fixed points of zero displacement (nodes) and maximum displacement (antinodes).

  • Mathematical Form: The sum of a right-traveling and left-traveling wave: $y(x, t) = A \sin(kx - \omega t) + A \sin(kx + \omega t)$ Using trigonometric identities, this simplifies to: $y(x, t) = 2A \sin(kx) \cos(\omega t)$

  • Nodes: Points where $\sin(kx) = 0$, i.e., $kx = n\pi$ ($n = 0, 1, 2, ...$).

  • Antinodes: Points where $\sin(kx)$ is maximum, i.e., $kx = (2n+1)\frac{\pi}{2}$.

  • Boundary Conditions: For a string fixed at both ends, only certain wavelengths are allowed: $\lambda_n = \frac{2L}{n}$, $n = 1, 2, 3, ...$ The corresponding frequencies are $f_n = \frac{nv}{2L}$.

  • Fundamental Frequency: The lowest frequency ($n=1$) is called the fundamental; higher frequencies are harmonics or overtones.

Photographs of standing waves on a string

Refraction of a Wave Front: Fermat's Principle of Least Time

Refraction occurs when a wave passes from one medium into another with a different wave speed, causing the wave to change direction. Fermat's principle leads to the law of refraction (Snell's Law):

  • Law of Refraction (Snell's Law): $\frac{\sin \theta_i}{\sin \theta_r} = \frac{v_1}{v_2}$, where $\theta_i$ is the angle of incidence, $\theta_r$ is the angle of refraction, and $v_1$, $v_2$ are the wave speeds in the respective media.

  • Physical Example: A sound wave traveling from warm air (higher speed) into cold air (lower speed) bends toward the normal.

Diffraction of a Wave Front

Diffraction is the bending of waves around obstacles or through openings. Huygen's principle explains diffraction by considering each point on a wave front as a source of secondary wavelets that spread out in all directions.

Diffraction of a wave at a barrier

Important Equations

  • General wave equation: $y(x, t) = \pm A \sin(kx - \omega t)$

  • Wavenumber: $k = \frac{2\pi}{\lambda}$

  • Wave speed: $v = \frac{\omega}{k}$

  • Law of reflection: $\theta_i = \theta_r$

  • Standing wave: $y(x, t) = 2A \sin(kx) \cos(\omega t)$

  • Law of refraction: $\frac{\sin \theta_i}{\sin \theta_r} = \frac{v_1}{v_2}$

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