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Transverse wave

A transverse wave is a wave in which the oscillations occur perpendicular to the direction of propagation. In mechanical waves, this involves the displacement of the medium's particles perpendicular to the wave's propagation, resulting in oscillations at right angles to the energy transfer path.^[1]^[2] Mechanical transverse waves are characterized by their ability to propagate through solids and on surfaces, but they cannot travel through the bulk of fluids like gases or liquids due to the absence of a restoring force for perpendicular motion.^[1] Common examples include waves on a stretched string, where particles move up and down as the wave travels along the string; surface ripples on water; seismic S-waves, which cause shear deformation in the Earth's crust during earthquakes and travel only through solids; and electromagnetic waves, such as light and radio waves, where the oscillating electric and magnetic fields are perpendicular to each other and to the direction of propagation.^[1]^[3]^[4] In contrast to longitudinal waves, transverse waves exhibit properties like polarization, where the plane of oscillation can be restricted, making them essential in fields such as optics and seismology.^[5]

Fundamentals

Definition

A transverse wave is a type of wave in which the oscillations occur perpendicular to the direction of wave propagation, thereby transferring energy without net displacement in the propagation direction. This includes mechanical transverse waves, where the particles of the medium vibrate perpendicular to the wave's direction, and electromagnetic waves, where the electric and magnetic fields oscillate perpendicular to each other and to the propagation direction.^[6]^[7]^[2] In mechanical transverse waves, the disturbance causes individual particles to vibrate back and forth—such as up and down or side to side—in a plane orthogonal to the forward progress of the wave itself, forming a repeating pattern that advances through the medium over time.^[1]^[8] This perpendicular motion distinguishes transverse waves as a fundamental mode of propagation, enabling phenomena where the wave's energy travels independently of the medium's bulk movement. This perpendicularity of oscillation to propagation contrasts with longitudinal waves, in which particle motion aligns parallel to the wave's direction.^[1]

Key Characteristics

Transverse waves are characterized by several fundamental properties that describe their oscillatory behavior and propagation. The amplitude represents the maximum extent of oscillation, such as the displacement of the medium's particles from their equilibrium position in mechanical waves or the peak field strength in electromagnetic waves, determining the wave's intensity or energy carried.^[9] The wavelength (\lambda) is the spatial distance between consecutive crests or troughs of the wave, providing a measure of its spatial periodicity.^[10] The frequency (f) quantifies the number of oscillations or cycles per unit time, typically measured in hertz (Hz), while the period (T) is the duration of one complete cycle, inversely related to frequency by T = 1/f.^[11] The phase indicates the specific position of a point on the wave relative to a reference point in its cycle, often expressed as the argument of the sinusoidal function describing the wave, such as \phi = kx - \omega t, where it helps determine alignment between different wave components.^[12] A defining feature of transverse waves is the directionality of oscillation, perpendicular to the direction of wave propagation. This perpendicularity distinguishes them from other wave types and allows for motion confined to a plane perpendicular to propagation (linear transverse motion) or more complex paths, such as elliptical or circular trajectories in three dimensions when combining components along the two independent perpendicular axes.^[13]^[14] The speed (v) of a transverse wave depends on the properties of the medium through which it travels (or the vacuum for electromagnetic waves) and relates the other characteristics via the relation v = f \lambda, where the wave speed remains constant for a given medium while frequency and wavelength adjust inversely to maintain this balance.^[11] These properties collectively enable phenomena like polarization, where the orientation of oscillations influences wave behavior.^[9]

Comparison with Longitudinal Waves

Transverse waves differ fundamentally from longitudinal waves in the direction of oscillation relative to the direction of wave propagation. In transverse waves, oscillations occur perpendicular to the propagation direction, resulting in crests and troughs, whereas in longitudinal waves, oscillations occur parallel to the propagation direction, producing compressions and rarefactions.^[1]^[7] This distinction arises because mechanical transverse waves require a medium with shear strength to support perpendicular motion, such as solids or taut strings, while longitudinal waves can propagate through media lacking such rigidity, including fluids like air or water. Electromagnetic transverse waves, however, do not require a medium.^[15]^[16] Despite these differences, both transverse and longitudinal waves share core similarities as disturbances that propagate energy without net transport of matter. They exhibit common properties, including wavelength, frequency, amplitude, and speed, which determine their behavior in transmission and interference.^[1]^[7] The following table summarizes key contrasts in oscillation and medium requirements (noting that electromagnetic transverse waves do not require a medium):

Aspect	Transverse Waves (Mechanical)	Longitudinal Waves
Oscillation Direction	Perpendicular to propagation	Parallel to propagation
Oscillation Path	Up-and-down or side-to-side (circular or linear in plane)	Back-and-forth along propagation axis
Medium Requirement	Needs shear strength (e.g., solids, strings)	No shear strength needed (e.g., fluids, gases)
Propagation Capability	Possible in solids; limited in fluids	Possible in solids, fluids, and gases
Occurrence Examples	Vibrations on strings, seismic S-waves	Sound waves in air, seismic P-waves

^[15]^[16]^[1]

Examples in Nature and Technology

Mechanical Transverse Waves

Mechanical transverse waves are disturbances in a medium where particles oscillate perpendicular to the direction of wave propagation, requiring the medium to provide restoring forces that act transversely to the displacement.^[1] These waves necessitate a medium capable of sustaining shear stress, such as solids or tensed strings, where elasticity or tension supplies the perpendicular restoring force; in contrast, fluids without boundaries cannot support pure transverse waves due to the lack of such shear resistance.^[17]^[1] A classic example is the wave on a tensed string, as seen in the vibration of a guitar string, where plucking causes transverse oscillations that propagate along the string's length while the string itself moves up and down perpendicular to that direction.^[18] Another prominent instance occurs during earthquakes with seismic S-waves, which are transverse shear waves that cause ground particles to move horizontally or vertically relative to the wave's propagation path through Earth's solid crust.^[3]^[19] Surface waves on water, such as ripples, exhibit transverse components where water particles primarily move in circular orbits with vertical displacements dominating near the surface, combining with minor longitudinal motion.^[15]^[6] A straightforward experimental demonstration involves securing one end of a long rope or string to a fixed point and shaking the free end up and down to generate traveling transverse waves that propagate along the rope, allowing observation of wave speed variations with tension or linear density.^[20] This setup can also produce standing waves by adjusting the shaking frequency to match the rope's natural resonances, illustrating node and antinode patterns.

Electromagnetic Transverse Waves

Electromagnetic waves consist of oscillating electric and magnetic fields that are perpendicular to each other and to the direction of wave propagation, making them inherently transverse.^[21] These fields vary sinusoidally in phase, with the electric field \mathbf{E} inducing the magnetic field \mathbf{B} and vice versa through mutual interaction, enabling self-propagation without a medium.^[21] In vacuum, all electromagnetic waves travel at the constant speed of light c \approx 3.00 \times 10^8 m/s, determined by the fundamental constants of permittivity \epsilon_0 and permeability \mu_0 of free space.^[21] Prominent examples include visible light, which spans wavelengths from about 400 to 700 nm and is responsible for human vision as well as photosynthesis in plants; radio waves, with wavelengths ranging from millimeters to kilometers used in communication technologies; and X-rays, featuring short wavelengths on the order of 0.01 to 10 nm, employed in medical imaging and material analysis.^[22] Each of these propagates as a transverse wave in vacuum at speed c, carrying energy across the electromagnetic spectrum without requiring a physical medium.^[22] The transverse exclusivity of electromagnetic waves arises from Maxwell's equations, particularly Gauss's laws, which in free space (with no charges or currents) require the divergence of both \mathbf{E} and \mathbf{B} to be zero (\nabla \cdot \mathbf{E} = 0, \nabla \cdot \mathbf{B} = 0).^[21] For plane waves, this implies no longitudinal components along the propagation direction, as such components would produce nonzero divergence, violating the source-free conditions; thus, only transverse oscillations can sustain propagation.^[21] This fundamental constraint ensures that electromagnetic waves maintain their perpendicular field structure throughout propagation.^[21]

Mathematical Description

Wave Equation

The wave equation provides the fundamental mathematical framework for describing the propagation of transverse waves in a one-dimensional medium, such as a taut string. It is a partial differential equation that relates the transverse displacement y(x, t) to its spatial and temporal variations:

\frac{\partial^2 y}{\partial t^2} = v^2 \frac{\partial^2 y}{\partial x^2},

where x is the position along the direction of propagation, t is time, and v is the constant speed of the wave.^[23] This second-order linear equation arises from the physics of wave motion and applies to small-amplitude transverse disturbances where the displacement is perpendicular to the propagation direction.^[24] The derivation begins by applying Newton's second law to an infinitesimal element of the medium, typically a string with uniform linear mass density \mu (mass per unit length) under constant tension T. For a small segment of length \Delta x, the mass is \mu \Delta x, and the net transverse force is the difference in the vertical components of tension at the ends, approximated as T \frac{\partial^2 y}{\partial x^2} \Delta x for small slopes. This force equals mass times transverse acceleration \mu \Delta x \frac{\partial^2 y}{\partial t^2}, yielding the wave equation upon dividing by \Delta x and taking the limit \Delta x \to 0. The wave speed emerges as v = \sqrt{T / \mu}, reflecting how higher tension increases speed while greater mass density decreases it.^[23]/Book%3A_University_Physics_I_-Mechanics_Sound_Oscillations_and_Waves(OpenStax)/16%3A_Waves/16.04%3A_Wave_Speed_on_a_Stretched_String) A common solution to this equation for monochromatic waves is the sinusoidal form y(x, t) = A \sin(kx - \omega t + \phi), where A is the amplitude, k = 2\pi / \lambda is the wave number (\lambda being the wavelength), \omega = 2\pi f is the angular frequency (f being the frequency), and \phi is the phase constant. This traveling wave solution satisfies the equation because the dispersion relation \omega = v k holds, ensuring consistency between spatial and temporal derivatives.^[25]^[26]

Polarization States

Polarization in transverse waves refers to the orientation of the oscillations perpendicular to the direction of propagation. For waves in two or three dimensions, such as electromagnetic waves, the displacement or electric field vector can oscillate in various patterns, leading to different polarization states. These states are determined by the relative amplitudes and phase differences of the components along perpendicular axes.^[27] Linear polarization occurs when the oscillation is confined to a fixed plane, such as vertical or horizontal relative to the propagation direction. In this state, the electric field vector of an electromagnetic wave vibrates back and forth along a straight line, with no phase difference between any perpendicular components. For example, a linearly polarized plane wave propagating in the z-direction can have its electric field along the x-axis, described by \vec{E} = E_0 \hat{x} \cos(kz - \omega t). This is the simplest form of polarization and is commonly produced using polarizers that transmit only one orientation of the field.^[5]^[28] Circular and elliptical polarization arise from the superposition of two perpendicular linear oscillations with a phase difference, typically \pi/2 for circular cases. In circular polarization, the amplitudes of the perpendicular components are equal, and the electric field vector rotates at a constant angular speed, tracing a circle in the plane perpendicular to propagation. The handedness—right-handed or left-handed—is defined by the rotation direction when looking toward the source: clockwise for right-circular and counterclockwise for left-circular. For a right-handed circularly polarized electromagnetic wave propagating in the +z direction, the electric field components are given by

E_x = A \cos(kz - \omega t), \quad E_y = A \sin(kz - \omega t),

where A is the amplitude. Left-handed polarization reverses the y-component sign: E_y = -A \sin(kz - \omega t). These can be conceptually represented using Jones vectors, such as \begin{pmatrix} 1 \\ i \end{pmatrix} for left-circular and \begin{pmatrix} 1 \\ -i \end{pmatrix} for right-circular (normalized). Elliptical polarization is a generalization where the amplitudes differ (A ≠ B) or the phase difference is not exactly \pi/2, resulting in the field tracing an ellipse; for instance, unequal A and B in the above equations produce an ellipse tilted along the major axis.^[27]^[28]^[5] In electromagnetic waves, particularly light, polarization states are crucial because natural light from most sources is unpolarized, meaning it consists of a random mixture of all possible orientations with no fixed phase relationships. However, interactions with matter can select or alter these states; for example, polarizers transmit linear polarization, while birefringent materials like quarter-wave plates convert linear to circular polarization by introducing the necessary phase shift. These effects are fundamental in optics, enabling applications such as reducing glare in sunglasses or analyzing molecular structures in spectroscopy.^[27]^[28]

Superposition Principle

The superposition principle governs the behavior of transverse waves in linear media, stating that the total displacement at any point is the vector sum of the displacements from each individual wave, provided the medium responds linearly to the applied forces.^[29] For transverse waves, where displacements occur perpendicular to the direction of propagation, this vector addition applies in the plane of oscillation, assuming the waves are polarized in the same direction as relevant to their polarization states.^[30] This principle leads to interference patterns when transverse waves overlap. Constructive interference occurs when the waves are in phase, meaning their phase difference is an integer multiple of $2\pi, resulting in maxima where the amplitudes add to produce a displacement up to twice that of a single wave.^[29] Destructive interference happens when the waves are out of phase by an odd multiple of \pi, causing minima where the amplitudes cancel, potentially reducing the displacement to zero.^[30] A mathematical illustration of superposition for two identical transverse waves with amplitude A, wave number k, angular frequency \omega, and phase difference \delta is given by:

y_1 = A \sin(kx - \omega t)

y_2 = A \sin(kx - \omega t + \delta)

The resultant displacement y is:

y = y_1 + y_2 = 2A \cos\left(\frac{\delta}{2}\right) \sin\left(kx - \omega t + \frac{\delta}{2}\right)

Here, the amplitude of the resultant wave is $2A \cos(\delta/2), which reaches a maximum of $2A for \delta = 0 (constructive) and zero for \delta = \pi (destructive).^[29] In applications to transverse waves, such as electromagnetic waves, the superposition principle produces observable interference fringes in light, as seen in Young's double-slit experiment where coherent light waves from two slits interfere to form alternating bright and dark bands on a screen due to path length differences causing phase shifts.^[30] Analogously, though sound waves are longitudinal, the principle similarly yields beats when frequencies differ slightly, a phenomenon that parallels intensity modulations in superposed transverse waves like light.^[29]

Energy and Power Transmission

In transverse waves, energy is transported through the medium via oscillatory motion, divided equally between kinetic and potential forms on average. For a sinusoidal transverse wave propagating along a stretched string, the kinetic energy arises from the transverse velocity of string elements, while the potential energy stems from the stretching of the string beyond its equilibrium length. These energies fluctuate over each cycle, but their time-averaged total per unit length, known as the average energy density u, is given by u = \frac{1}{2} \mu \omega^2 A^2, where \mu is the linear mass density of the string, \omega is the angular frequency, and A is the amplitude.^[31] This equality between average kinetic and potential energies holds because, at any point, the maximum kinetic energy occurs when potential is zero, and vice versa, leading to equipartition over the wave period.^[31] The power transmitted by such a wave, representing the rate of energy flow past a point on the string, is the product of the energy density and the wave speed v. The time-averaged power P for a sinusoidal wave is thus P = \frac{1}{2} \mu v \omega^2 A^2.^[31] This formula quantifies how energy propagates along the string at speed v = \sqrt{T/\mu}, where T is the tension, without any net displacement of the medium's mass.^[31] Electromagnetic transverse waves, such as light, carry energy through oscillating electric and magnetic fields in vacuum or media. The instantaneous energy flux is described by the Poynting vector \mathbf{S} = \frac{1}{\mu_0} \mathbf{E} \times \mathbf{B}, where \mathbf{E} and \mathbf{B} are the electric and magnetic field vectors, and \mu_0 is the permeability of free space; its magnitude points in the direction of propagation and gives the power per unit area./University_Physics_II_-Thermodynamics_Electricity_and_Magnetism(OpenStax)/16%3A_Electromagnetic_Waves/16.04%3A_Energy_Carried_by_Electromagnetic_Waves) For a plane sinusoidal wave, the time-averaged intensity I, or power per unit area, simplifies to I = \frac{1}{2} c \epsilon_0 E_0^2, where c is the speed of light, \epsilon_0 is the permittivity of free space, and E_0 is the electric field amplitude (with B_0 = E_0 / c)./University_Physics_II_-Thermodynamics_Electricity_and_Magnetism(OpenStax)/16%3A_Electromagnetic_Waves/16.04%3A_Energy_Carried_by_Electromagnetic_Waves) This intensity measures the radiant energy flow, analogous to power in mechanical waves. In both mechanical and electromagnetic transverse waves, energy propagation occurs without net transport of matter; particles or field disturbances oscillate locally around equilibrium positions while the wave pattern advances, transferring energy from one region to another.^[31]/University_Physics_II_-Thermodynamics_Electricity_and_Magnetism(OpenStax)/16%3A_Electromagnetic_Waves/16.04%3A_Energy_Carried_by_Electromagnetic_Waves)

Applications and Phenomena

Wave Propagation in Media

When a transverse wave encounters an interface between two media, part of the wave is reflected back into the first medium, while the remainder is transmitted into the second medium. The law of reflection states that the angle of incidence equals the angle of reflection, ensuring that the reflected wave's direction lies in the plane defined by the incident wave and the normal to the interface. This behavior arises from the boundary conditions that maintain continuity of the wave's displacement and the transverse component of the wave's momentum across the boundary. For oblique incidence, the transmitted wave refracts according to Snell's law, which relates the angles of incidence and refraction to the wave speeds in the respective media:

n_1 \sin \theta_1 = n_2 \sin \theta_2,

where n_1 and n_2 are the refractive indices (inversely proportional to the phase velocities) of the first and second media, \theta_1 is the angle of incidence, and \theta_2 is the angle of refraction. This law ensures phase matching along the interface, preventing discontinuities in the wave front. In mechanical transverse waves on strings with different linear densities but the same tension, an analogous refraction occurs, bending the wave path toward the normal when entering a denser medium.^[32]^[33] At such boundaries, the amplitudes of the reflected and transmitted waves depend on the impedance mismatch between the media. For mechanical transverse waves on strings, the impedance is defined as Z = T / v, where T is tension and v is wave speed. For a wave incident from medium 1 to medium 2, the reflection coefficient r (ratio of reflected to incident displacement amplitude) is r = (Z_1 - Z_2)/(Z_1 + Z_2), while the transmission coefficient t = 2 Z_1 / (Z_1 + Z_2).^[34] For electromagnetic waves, the intrinsic impedance is \eta = \sqrt{\mu / \varepsilon}, where \mu is permeability and \varepsilon is permittivity, and the coefficients for the electric field amplitude are r = (\eta_2 - \eta_1)/(\eta_2 + \eta_1), t = 2 \eta_2 / (\eta_2 + \eta_1).^[35] These coefficients determine the energy partitioning, with no net energy loss at ideal boundaries. The boundary conditions for transverse waves on joined strings specifically require continuity of transverse displacement (to avoid breaking) and continuity of the transverse force, which equates to the tension times the slope (T \partial y / \partial x) being equal on both sides. If tensions differ, the slopes adjust accordingly to balance forces.^[33]^[36] In dispersive media, the propagation speed of transverse waves varies with frequency, causing different frequency components of a wave packet to travel at different velocities. This frequency-dependent phase velocity v_p(\omega) leads to dispersion, where a initially narrow pulse spreads out over distance as its components separate. For electromagnetic transverse waves in dielectrics, dispersion arises from the frequency dependence of the refractive index n(\omega), often modeled by the Sellmeier equation based on atomic resonances. In non-ideal media, this effect limits signal integrity in applications like optical fibers, where pulse broadening can degrade information transmission.^[37] Attenuation in transverse wave propagation occurs through energy loss mechanisms such as absorption, where wave energy converts to heat via material damping, or scattering, where inhomogeneities redirect energy away from the primary propagation direction. In absorbing media, the wave amplitude decays exponentially as e^{-\alpha z}, with attenuation coefficient \alpha increasing with frequency due to resonant interactions. For electromagnetic transverse waves, intrinsic absorption follows the imaginary part of the dielectric constant, while scattering dominates in turbid media like biological tissues. In mechanical contexts, such as transverse waves in viscoelastic solids, attenuation results from internal friction, broadening wave pulses and reducing peak amplitudes over distance. These losses distinguish real media from ideal non-dispersive, lossless cases.^[38]

Interference and Diffraction

Interference in transverse waves arises from the superposition principle, where waves from multiple sources or paths combine to produce regions of constructive and destructive interference. In Young's double-slit experiment, monochromatic light passes through two closely spaced slits separated by distance d, creating two coherent sources that produce an interference pattern on a distant screen. The path difference \delta between waves from the two slits to a point on the screen at angle \theta is given by \delta = d \sin \theta. Constructive interference, resulting in bright fringes, occurs when this path difference is an integer multiple of the wavelength: m\lambda = \delta, where m = 0, 1, 2, \dots. Destructive interference, producing dark fringes, happens when \delta = (m + 1/2)\lambda. This pattern demonstrates the wave nature of light, a transverse electromagnetic wave, with fringe spacing depending on wavelength, slit separation, and distance to the screen.^[39] Diffraction refers to the bending and spreading of transverse waves around obstacles or through apertures, also explained by the Huygens-Fresnel principle, which posits that every point on a wavefront acts as a source of secondary spherical wavelets that interfere with each other. For a single slit of width a illuminated by monochromatic light, the diffraction pattern consists of a central bright maximum flanked by minima. The condition for minima is derived from the path differences across the slit, yielding \sin \theta = m \lambda / a, where m = \pm 1, \pm 2, \dots, leading to destructive interference at those angles. The intensity distribution follows a sinc-squared function, with the central maximum's width inversely proportional to a. In transverse waves like electromagnetic radiation, polarization plays a key role in diffraction; for instance, the electric field orientation relative to the slit or obstacle affects the amplitude and pattern, as the wave's transverse nature couples the field components to the geometry.^[40]^[41] Polarization effects are particularly evident in diffraction gratings used in spectrometers, where multiple slits enhance angular dispersion. The grating equation d (\sin \theta_i + \sin \theta_m) = m \lambda determines diffraction orders, but efficiency varies with polarization: for grooves parallel to the electric field (TE mode), diffraction is stronger than for perpendicular (TM mode), leading to polarization-dependent spectral resolution and blaze angles optimized for specific orientations. This is crucial in applications like astronomical spectroscopy, where unpolarized light from stars requires accounting for instrumental polarization to avoid biases in measurements.^[42] A vivid example of interference in transverse waves is the colorful patterns on soap bubbles, resulting from thin-film interference. Light reflects from both the inner and outer surfaces of the soap film's water-air interfaces, with a path difference of $2nt \cos \theta (where n is the refractive index, t the thickness, and \theta the incidence angle), plus a \pi phase shift at one interface. Constructive interference for reflected light occurs for wavelengths satisfying $2 n t \cos \theta = (m + 1/2) \lambda, producing iridescent colors that shift as the film thins or drains.^[43]^[44] X-ray diffraction in crystals provides another key phenomenon, exploiting the transverse wave properties of X-rays to probe atomic structures. X-rays scatter off successive atomic planes in a crystal lattice, interfering constructively when the path difference satisfies Bragg's law: $2d \sin \theta = m \lambda, where d is the interplanar spacing. This produces discrete diffraction spots or rings, enabling determination of crystal symmetries and lattice parameters, as in the analysis of minerals or proteins. The transverse polarization of X-rays influences scattering intensities, with certain orientations enhancing or suppressing reflections based on atomic electron distributions.^[45]

Historical Development

The concept of transverse waves emerged within the broader development of wave theories for light and other phenomena, beginning with early attempts to explain propagation without relying on particle models. In 1678, Christiaan Huygens proposed a wave theory of light in his unpublished manuscript Traité de la Lumière, later published in 1690, describing light as longitudinal pressure waves propagating through an elastic ether similar to sound waves.^[46] This idea faced significant rejection in the late 17th and 18th centuries, primarily due to Isaac Newton's influential corpuscular theory, which better aligned with observed rectilinear propagation and refraction at the time.^[46] However, the longitudinal nature of Huygens' model struggled to account for later discoveries like polarization, as such waves in a solid-like ether could not easily support the observed transverse restrictions without invoking problematic shear properties in the medium.^[47] The revival of the wave theory in the early 19th century, driven by Thomas Young and Augustin-Jean Fresnel, marked a pivotal shift toward recognizing light as transverse waves. Young's double-slit interference experiments in 1801 demonstrated wave superposition, but it was Fresnel's work on diffraction and polarization from 1815 to 1819 that provided compelling evidence for transverse vibrations. In a 1818 memoir to the French Academy of Sciences, Fresnel explained polarization phenomena—such as the inability of certain light orientations to pass through polarizing crystals—by modeling light waves as transverse oscillations perpendicular to the direction of propagation, with the ether possessing the necessary elasticity for such motions.^[48] This transverse hypothesis resolved inconsistencies in longitudinal models and was experimentally confirmed through predictions like the diffraction patterns observed by François Arago in 1818.^[48] James Clerk Maxwell's unification of electricity, magnetism, and optics in the 1860s solidified the transverse wave nature of light within electromagnetism. In his 1865 paper "A Dynamical Theory of the Electromagnetic Field," Maxwell derived equations showing that electric and magnetic fields oscillate perpendicular to each other and to the propagation direction, forming self-sustaining transverse waves traveling at the speed of light through vacuum, without needing an ether for propagation. This theoretical framework predicted electromagnetic waves across the spectrum, later verified by Heinrich Hertz's experiments in 1887, establishing transverse electromagnetic waves as a cornerstone of classical physics.^[49] In the 20th century, the understanding of transverse waves extended to quantum mechanics and geophysics. Albert Einstein's 1905 explanation of the photoelectric effect introduced light quanta, or photons, as discrete packets of electromagnetic energy inheriting the transverse polarization properties of classical waves.^[50] Concurrently, in seismology, Richard Dixon Oldham's analysis of earthquake records in 1906 classified secondary (S) waves as transverse shear waves, distinct from primary (P) longitudinal waves, providing early evidence for Earth's layered interior as S-waves failed to traverse the liquid outer core.^[51] These advancements maintained a classical foundation while integrating transverse wave concepts into quantum electrodynamics, where photons exhibit two transverse polarization states.^[50]

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Jul 13, 2022 · The superposition of most waves produces a combination of constructive and destructive interference and can vary from place to place and time ...
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https://openstax.org/books/university-physics-volume-1/pages/16-4-energy-and-power-of-a-wave
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16.4 Energy and Power of a Wave - University Physics Volume 1
Sep 19, 2016 · Begin with the equation of the time-averaged power of a sinusoidal wave on a string: P = 1 2 μ A 2 ω 2 v . P = 1 2 μ A 2 ω 2 v . The amplitude ...
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[PDF] Refraction and Snell's law - MIT OpenCourseWare
Refraction involves a change in the direction of wave propagation due to a change in propagation speed. It involves the oblique incidence of waves on media ...
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[PDF] Traveling Waves and Boundary Interactions - MIT OpenCourseWare
1. Continuity: The string must be continuous across the interface (Eq. (21)). This means the displacement y(x, t) when approaching the interface from the left ...
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[PDF] Lecture 9: Reflection, Transmission and Impedance
Now we have the boundary conditions. What is the solution? 2 Reflection and transmission. Suppose we have some incoming traveling wave. Before it hits the ...
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Waves, Superposition, Dispersion - UMD Physics
May 7, 2024 · This is important to understand: the frequency (and period) are determined by the source of the wave, and the wavelength comes from properties ...Missing: key characteristics
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[PDF] Chapter 7. Electromagnetic Wave Propagation
This chapter covers electromagnetic waves, starting with plane waves, then nonuniform systems, guided waves, and finally resonant cavities and energy ...
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27.3 Young's Double Slit Experiment – College Physics
destructive interference for a double slit: the path length difference must be a half-integral multiple of the wavelength. incoherent: waves have random phase ...
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[PDF] Lecture 36 – Diffraction - Purdue Physics
Huygens-Fresnel Principle Huygens: – Every point on a wave front acts as a point source of secondary spherical waves that have the same phase as the original ...
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[PDF] Chapter 36 - NJIT
single-slit diffraction pattern with slit width a. • The diffraction minima are labeled by the integer m d. = ±1, ±2, … (“d” for. “diffraction”). • Figure (b) ...<|control11|><|separator|>
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Measurement of the instrumental polarization of a high resolution ...
Diffraction grating spectrometers exhibit a complex dependance on the polarization state of incident light. We have characterized the polarization ...
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Interference Phenomena in Soap Bubbles: Interactive Java Tutorial
Jun 14, 2018 · A good example of interference is the thin film of a soap bubble, which reflects a spectrum of beautiful colors when illuminated by natural ...
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[PDF] Chapter 7: Basics of X-ray Diffraction
In X-ray diffraction work we normally distinguish between single crystal and polycrystalline or powder applications. The single crystal sample is a perfect ...
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Light through the ages: Ancient Greece to Maxwell - MacTutor
The wave theory by Huygens and Hooke was a development of Descartes' ideas where now they proposed that light be a wave through the plenum, while Newton ...
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A Very Brief History of Light | SpringerLink
Dec 14, 2016 · In 1821, Fresnel published a paper in which he claimed that light is a transverse wave. Young had independently reached the same conclusion. ...<|control11|><|separator|>
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July 1816: Fresnel's Evidence for the Wave Theory of Light
Jul 1, 2016 · The wave theory was making a comeback, thanks in part to the work of a French civil engineer named Augustin-Jean Fresnel.
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'…a paper …I hold to be great guns': a commentary on Maxwell ...
Apr 13, 2015 · Maxwell's great paper of 1865 established his dynamical theory of the electromagnetic field. The origins of the paper lay in his earlier papers of 1856.
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The dual nature of light as reflected in the Nobel archives
Dec 2, 1999 · Albert Einstein in 1905 drew the conclusion that light sometimes behaves as particles ... The photon is the field quantum (particle) acting ...
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[PDF] History of Seismology - Institute of Geophysics and Planetary Physics
In 1900 R.D. Oldham, using measurements of the. 1897 Assam earthquake, classified the preliminary tremors into two phases, which he identified with longitudinal ...