Glossary

Terms used in this book.

A reference list of the physical vocabulary used in Physics Foundations. Inline occurrences in the chapters are auto-tooltipped; this page lists every term in the book’s domain alphabetically.

185 terms from this book.

A

absorption coefficient
The fraction of incident sound energy absorbed by a surface (α = 1 − |R|²). Ranges from 0 (perfect reflection) to 1 (perfect absorption).
acoustic energy density
Energy per unit volume in a sound field: e = p²/(2ρc²) + ½ρv². Sum of potential (pressure) and kinetic (velocity) energy densities.
acoustic impedance
The ratio of acoustic pressure to particle velocity in a propagating wave (Z = p/v). For a plane wave in a medium of density ρ and wave speed c, Z = ρc.
action potential
A brief (~1 ms) all-or-nothing voltage spike propagating along a neuron's axon. The fundamental unit of neural communication.
adiabatic
A process in which no heat is exchanged with the surroundings. Sound propagation in air is adiabatic because compressions/rarefactions happen too fast for heat conduction.
amplitude
The magnitude of a wave's departure from equilibrium. For sound, the size of the pressure fluctuation.
angular frequency
Rate of phase advance in radians per second: ω = 2πf.
auditory nerve
The ~30,000-fibre bundle carrying spike-train information from the cochlea to the cochlear nucleus in the brainstem.

B

basilar membrane
The membrane separating scala media from scala tympani. Its position-dependent stiffness gives different places different natural frequencies.
Bernoulli equation
For steady, inviscid, incompressible flow along a streamline: P + ½ρv² + ρgz = const. Energy conservation per unit volume.
Boltzmann constant
k_B = 1.381×10⁻²³ J/K. Relates temperature to energy at the molecular scale: average kinetic energy per degree of freedom = ½k_BT.
Bond number
Bo = ΔρgL²/γ. Ratio of gravitational to surface-tension forces. Bo ≪ 1: surface tension dominates (small drops, capillary phenomena).
boundary layer
The thin region near a solid surface where viscous effects are significant and velocity transitions from zero (no-slip) to the free-stream value.
Brownian motion
The random motion of a particle suspended in a fluid, driven by molecular collisions. Mathematically: a continuous-time stochastic process with Gaussian independent increments.
Buckingham π theorem
If a physical law involves n variables with k independent dimensions, it can be rewritten in terms of n−k dimensionless groups (π groups).
bulk modulus
The resistance of a material to uniform compression: K = −V(dp/dV). Higher K means stiffer material and faster sound propagation.

C

capacitance
The ability to store charge per unit voltage: C = Q/V. For a parallel plate: C = εA/d. Energy stored = ½CV².
capillary length
Length scale l_c = √(σ/ρg) below which surface tension dominates gravity; ~2.7 mm for water.
capillary number
Ca = μv/γ. Ratio of viscous to surface-tension forces. Governs the shape of menisci and the dynamics of wetting and dewetting.
capillary rise
Height h = 2σ cos θ/(ρgr) a liquid climbs in a narrow tube due to surface tension (Jurin's law).
Carnot
The maximum-efficiency heat engine operating between two reservoirs: η = 1 − T_cold/T_hot. No real engine can exceed Carnot efficiency.
Cauchy stress tensor
Symmetric rank-2 tensor σᵢⱼ giving force per unit area on any internal plane in a deformed continuum.
chemical potential
μ = (∂G/∂N)_{T,P}. The free-energy cost of adding one particle to the system. Drives diffusion, phase transitions, and chemical equilibria (μ equalises at equilibrium).
Clausius-Clapeyron
dP/dT = L/(TΔv). Relates the slope of a phase boundary to the latent heat and volume change. Predicts how boiling point shifts with pressure.
cochlea
The spiral, fluid-filled organ of the inner ear that performs frequency analysis on incoming sound and transduces it into neural signals.
cochlear amplifier
The active feedback process in the cochlea, driven by outer-hair-cell electromotility, that sharpens basilar-membrane tuning beyond passive mechanics.
compressibility
The fractional volume change per unit applied pressure: κ = −(1/V)(dV/dp). The reciprocal of the bulk modulus. Air's high compressibility is why sound exists in it.
contact angle
The angle θ at which a liquid-gas interface meets a solid surface. θ < 90° = wetting (hydrophilic); θ > 90° = non-wetting (hydrophobic). Set by Young's equation.
continuity equation
The local conservation law: ∂ρ/∂t + ∇·(ρv) = 0. Any density change equals the negative divergence of the flux.
control volume
A fixed region in space through which fluid flows; used to derive conservation laws in integral form.
convective derivative
D/Dt = ∂/∂t + U·∇; rate of change following a fluid element moving at velocity U.
Coulomb's law
Force between point charges: F = kq₁q₂/r². The electric field of a point charge falls as 1/r².
critical point
Thermodynamic state (T_c, p_c) above which liquid and vapor are indistinguishable; surface tension vanishes.
CROS
Contralateral Routing of Signal. A hearing-aid configuration for unilateral deafness: a microphone on the dead ear transmits wirelessly to a receiver on the better ear.

D

decibel
A logarithmic unit of ratio: 20·log10(amplitude ratio) or 10·log10(power ratio). Used for sound pressure level (SPL) and hearing level (HL).
differential equation
An equation relating an unknown function to its derivatives. ODEs involve one variable; PDEs involve several.
diffusion coefficient
D, in Fick's law J = −D∇c. Measures how fast a species spreads. For a sphere in fluid: D = k_BT/(6πμa) (Stokes-Einstein).
diffusion equation
The parabolic PDE ∂u/∂t = D∇²u describing how a concentration or temperature field spreads out over time. Solutions are Gaussian spreading profiles.
diffusivity
The constant D in the diffusion equation u_t = D∇²u; sets how quickly spatial gradients are smoothed.
dimensionless number
A ratio of physical quantities that has no units. Characterises the relative importance of different physical effects (e.g. Re, Ma, Q).
directivity
Angular dependence of a source's radiated field; D(θ) = 1 on-axis, with nulls and sidelobes off-axis.
dispersion
The dependence of wave speed on frequency. In a dispersive medium, different frequency components travel at different speeds, distorting the waveform.
dispersion relation
The relation between frequency ω and wavenumber k for a wave. Non-dispersive: ω = ck. Dispersive: ω(k) is nonlinear.
divergence
A scalar measuring how much a vector field spreads from a point: ∇·v = ∂vₓ/∂x + ∂vᵧ/∂y + ∂v_z/∂z. Positive = source; negative = sink.
divergence theorem
Relates a volume integral of a divergence to a surface integral: ∫∫∫(∇·F)dV = ∮(F·n̂)dA. Converts between flux through a surface and source strength inside.
dynamic viscosity
Coefficient μ relating shear stress to velocity gradient in a Newtonian fluid: τ = μ(du/dy).

E

ear canal
The tube about 25 mm long running from the pinna to the eardrum. Its closed-tube resonance amplifies frequencies near 3 kHz.
eardrum
The tympanic membrane: a thin sheet at the inner end of the ear canal that vibrates in response to pressure waves and drives the ossicular chain.
electromotility
The voltage-driven length change of outer hair cells, mediated by prestin. Generates the active gain of the cochlear amplifier.
endocochlear potential
The +80 mV potential of the endolymph in scala media relative to perilymph. Powers hair-cell transduction by driving K⁺ through open MET channels.
endolymph
The fluid in scala media; high in K⁺, low in Na⁺. Held at +80 mV (the endocochlear potential) relative to perilymph.
enthalpy
H = U + PV. The heat content at constant pressure: ΔH = Q_p for isobaric processes. The natural potential for constant-pressure chemistry and engineering.
entropy
A measure of the number of microstates consistent with a macrostate: S = k_B ln Ω. Thermodynamically: dS = δQ_rev/T. Always increases in isolated systems.
equation of state
A relation among state variables (P, V, T, n) that closes the thermodynamic description. Ideal gas: PV = nRT. Real gases: van der Waals, Redlich-Kwong, etc.
equipartition
Each quadratic degree of freedom in thermal equilibrium carries average energy ½k_BT. Gives heat capacities for ideal gases and harmonic solids.
Euler equation
Newton's second law for an inviscid fluid: ρ Dv/Dt = −∇p. The momentum equation of ideal fluid mechanics.

F

far field
The region far enough from a source (r ≫ λ and r ≫ source size) that the wavefronts are effectively planar and pressure falls as 1/r.
Faraday's law
A changing magnetic flux through a loop induces an EMF: ε = −dΦ_B/dt. Foundation of generators, transformers, and electromagnetic induction.
Fick's law
The flux of a diffusing species is proportional to its concentration gradient: J = −D∇c. The diffusion analogue of Fourier's law for heat.
Fourier transform
A mathematical operation that decomposes a signal into its sinusoidal components. Time-domain ↔ frequency-domain pair.
frequency
The number of oscillation cycles per second, measured in hertz (Hz). For sound, this is what the brain perceives as pitch.
frequency selectivity
The ability to resolve individual frequency components in a complex sound. Determined by cochlear mechanics and the sharpness of basilar-membrane tuning.

G

Gauss's law
Maxwell equation ∇·E = ρ/ε₀; electric flux through any closed surface equals enclosed charge / ε₀.
Gibbs free energy
G = H − TS. The thermodynamic potential minimised at constant T and P. ΔG < 0 for a spontaneous process; ΔG = 0 at equilibrium.
Green's function
The response of a linear system to a unit impulse. Fully characterises propagation from source to receiver in any linear medium.
group velocity
The speed at which a wave packet's envelope (and its energy) travels: v_g = dω/dk. The physically meaningful propagation speed for a signal.

H

half-life
The time for a decaying quantity to reach half its initial value; related to time constant by T½ = τ ln 2.
Hamiltonian
The operator Ĥ = −(ℏ²/2m)∇² + V representing total energy; its eigenvalues are the allowed energies.
harmonic
An integer multiple of the fundamental frequency. The nth harmonic has frequency nf₁. Harmonics are the building blocks of periodic signals.
heat capacity
The energy required to raise a system's temperature by 1 K. C_V (constant volume) and C_P (constant pressure) differ by nR for an ideal gas.
heat equation
The parabolic PDE ∂u/∂t = α∇²u describing thermal conduction (or any diffusive process). Solutions smooth out discontinuities instantly.
Helmholtz free energy
F = U − TS. The thermodynamic potential minimised at constant T and V. Work obtainable equals −ΔF.
heterogeneous nucleation
Bubble formation at pre-existing weak points: surface crevices, impurities, dissolved gas pockets. The dominant mechanism in all practical cavitation scenarios.
homogeneous nucleation
Spontaneous formation of a vapour cavity in a pure liquid with no pre-existing defects. Requires enormous negative pressures (rarely achieved in practice).
Hooke's law
The linear relation between stress and strain for small deformations: σ = Eε (1-D) or σ_ij = C_ijkl ε_kl (general). Valid below the elastic limit.
HRTF
Head-Related Transfer Function. The frequency-dependent filter the head, pinnae, and torso apply between a sound source in space and the eardrum.
hydrogen bond
A strong (~20 kJ/mol) directional interaction between a hydrogen bonded to an electronegative atom (O, N, F) and a nearby lone pair. Dominates water's anomalous properties.
hydrophilic
Tending to attract water; contact angle < 90°. Hydrophilic surfaces wet easily.
hydrophobic
Tending to repel water; contact angle > 90°. Hydrophobic crevices trap gas pockets that serve as nuclei.

I

ideal gas
A model gas of non-interacting point particles obeying PV = nRT. Valid at low density and high temperature where intermolecular forces are negligible.
impedance
The ratio of a driving quantity to a flow quantity. In acoustics: pressure/velocity. A measure of how strongly a medium resists being moved by a wave.
impedance mismatch
A difference in acoustic impedance between two media at a boundary. The greater the mismatch, the more energy is reflected and the less is transmitted.
isothermal
Process at constant temperature; Newton's (incorrect) assumption for sound gave c ≈ 280 m/s in air.

K

kinematic viscosity
Ratio ν = μ/ρ with units m²/s; a momentum diffusivity setting the Reynolds number Re = UL/ν.
Knudsen number
Kn = λ/L. Ratio of mean free path to characteristic length. Kn ≪ 1: continuum (Navier-Stokes valid). Kn ≫ 1: free-molecular regime.

L

laminar
Smooth, layered flow in which fluid parcels follow parallel streamlines without mixing. Occurs at low Reynolds number.
Laplace pressure
The pressure difference across a curved interface: ΔP = γ(1/R₁ + 1/R₂). For a sphere of radius R: ΔP = 2γ/R. Drives capillary rise and bubble stability.
latent heat
The energy absorbed or released during a phase transition at constant temperature. Latent heat of vaporisation for water: 2260 kJ/kg.
Lennard-Jones
A model pair potential V(r) = 4ε[(σ/r)¹² − (σ/r)⁶] combining short-range Pauli repulsion (r⁻¹²) with long-range van der Waals attraction (r⁻⁶).
linear mass density
Mass per unit length μ of a string; enters the 1-D wave speed as c = √(T/μ).
linearisation
Replacing a function by its first-order Taylor approximation near a point: f(x) ≈ f(x₀) + f′(x₀)(x−x₀). Valid when |x−x₀| is small.
London dispersion
The universal van der Waals attraction between any two atoms/molecules, arising from correlated fluctuations of their electron clouds. Falls as r⁻⁶.
lubrication theory
Thin-film limit of Navier-Stokes for flow between closely spaced surfaces; gives the cochlear long-wave equation.

M

Mach number
The ratio of flow speed to the local speed of sound: M = v/c. M < 1 is subsonic; M > 1 is supersonic.
malleus
The first middle-ear ossicle (the "hammer"); attached to the eardrum on one side and the incus on the other.
material derivative
The time derivative following a fluid element: D/Dt = ∂/∂t + v·∇. Accounts for both local change and advection by the flow.
Maxwell-Boltzmann
The probability distribution of molecular speeds in a gas at thermal equilibrium: f(v) ∝ v²exp(−mv²/2k_BT). Peak speed = √(2k_BT/m).
mean free path
The average distance a molecule travels between collisions: λ = 1/(√2·n·σ). In air at STP: λ ≈ 68 nm.
MEMS
Microelectromechanical Systems. Micron-scale devices integrating mechanical and electrical components on a chip. Used in accelerometers, microphones, pressure sensors.
meniscus
Curved liquid surface at a container wall or inside a capillary, shaped by adhesion and surface tension.
MET channel
Mechanoelectrical Transduction channel. A mechanically-gated ion channel on stereocilia that opens when the bundle is deflected toward the tall edge.
metastable
A thermodynamic state that is locally stable but not the global equilibrium. A superheated liquid or tensile liquid is metastable with respect to the vapour phase.
microbubble
Free gas bubble small enough to remain suspended (< 100 μm); a common cavitation nucleus.
modulus
The magnitude of a complex number: |z| = √(a² + b²) for z = a + bi. Represents the amplitude when z is a phasor.
monopole
A point source that radiates sound equally in all directions (omnidirectional). The simplest acoustic source; its field falls as 1/r.

N

Navier-Stokes
The fundamental equations of viscous fluid motion: ρ(Dv/Dt) = −∇P + μ∇²v + f. Newton's second law for a continuum with viscosity μ.
negative pressure
A liquid under tension (P < 0): molecules are pulled apart but remain cohesive. The metastable state that precedes cavitation inception.
Nernst equation
Equilibrium potential for an ion across a membrane: E = (RT/zF) ln(c_out/c_in). Sets cochlear potentials.
no-slip condition
Boundary condition requiring fluid velocity to equal zero at a solid wall; creates the boundary layer.
nucleation
The formation of a new phase (vapour bubble, crystal) from a metastable parent phase. Requires overcoming a free-energy barrier set by surface tension.
nucleation site
Preexisting weakness (crevice, free gas, impurity) in a liquid that initiates bubble formation at practical tensions.

O

Ohnesorge number
Oh = μ/√(ρσL). Ratio of viscous to inertio-capillary forces. Classifies droplet behaviour: low Oh = oscillatory breakup; high Oh = viscous breakup.
ossicles
The three smallest bones in the body — malleus, incus, stapes — transmitting motion from the eardrum to the oval window of the cochlea.
outer hair cell
Active mechanical element of the organ of Corti. ~12,000 of them; they shorten and lengthen with voltage, sharpening basilar-membrane tuning.
oval window
A membrane-covered opening at the base of scala vestibuli, where the stapes footplate drives the cochlear fluid.

P

P-wave
Primary (longitudinal) elastic wave; particles oscillate along propagation direction. Speed c_P = √((K+4G/3)/ρ).
particle velocity
The oscillatory velocity of a fluid element as a sound wave passes through it. Related to pressure by Z = p/v in a plane wave.
Peclet number
Pe = vL/D. Ratio of advective to diffusive transport. Pe ≫ 1: convection dominates. Pe ≪ 1: diffusion dominates.
perilymph
The fluid in scala vestibuli and scala tympani; ionic composition resembles extracellular fluid (high Na⁺, low K⁺).
phase transition
A transformation between distinct states of matter (solid, liquid, gas) or order parameters. First-order transitions have latent heat; second-order transitions are continuous.
phase velocity
The speed at which a single-frequency wave's phase fronts travel: v_p = ω/k. May exceed c in dispersive media without violating causality.
piezoelectric
A material that generates voltage when mechanically stressed (and deforms when voltage is applied). Basis of ultrasound transducers, quartz oscillators, MEMS sensors.
plane wave
A wave whose phase fronts are infinite parallel planes; idealisation of a wave from a distant source, valid locally near the listener.
Poisson's ratio
ν = −ε_transverse/ε_axial. The ratio of lateral contraction to axial extension under uniaxial stress. Ranges from −1 to 0.5; most materials: 0.2–0.4.
polytropic
A process in which PVⁿ = const for some exponent n. For gas in a bubble: n = 1 (isothermal) to γ (adiabatic) depending on thermal exchange rate.
polytropic exponent
Effective exponent κ (1 ≤ κ ≤ γ) for bubble gas compression; interpolates between isothermal and adiabatic.
prestin
The membrane protein in outer hair cells that changes conformation with voltage, producing the cell's electromotility.

R

radiation pressure
A steady force per unit area exerted by a sound wave on an absorbing or reflecting surface. Proportional to the time-averaged energy density.
random walk
A stochastic process consisting of successive random steps. In the simplest form: ±1 steps with equal probability. The mean displacement grows as √N.
Rankine-Hugoniot
Jump conditions for mass, momentum, and energy across a shock discontinuity in a compressible flow.
rate of change
How quickly a quantity varies with respect to another variable. The derivative gives the instantaneous rate of change.
Rayleigh-Plesset
The ODE governing spherical bubble dynamics: RR̈ + (3/2)Ṙ² = (1/ρ)[p_B − p_∞ − ...]. Foundation of all cavitation bubble models.
reflection
When a wave hits a boundary between two media, part of its energy turns back into the first medium. R = (Z2 − Z1)/(Z1 + Z2).
reflection coefficient
The ratio of reflected to incident wave amplitude at a boundary: R = (Z2 − Z1)/(Z1 + Z2). Ranges from −1 (soft boundary) to +1 (rigid boundary).
resonance
The condition where a driving frequency matches a system's natural frequency, producing maximum response amplitude.
resting potential
The membrane voltage of a cell at rest, typically −60 to −70 mV for neurons. Set by the balance of K⁺ leak and Na⁺/K⁺-ATPase activity.
restoring force
Force directed toward equilibrium, proportional to displacement for small perturbations (F = −kx).
Reynolds number
Re = ρvL/μ. The ratio of inertial to viscous forces. Re ≪ 1: Stokes flow (viscosity dominates). Re ≫ 1: inertia dominates, turbulence possible.
ribbon synapse
A specialised presynaptic structure in inner hair cells that releases vesicles continuously at high rates with sub-millisecond precision.
root-mean-square
The square root of the time-averaged square of a signal: f_rms = √((1/T)∫f²dt). For a sinusoid, amplitude/√2.

S

S-wave
Secondary (shear) elastic wave; particles oscillate perpendicular to propagation. Cannot propagate in fluids.
scala media
The middle cochlear chamber, filled with endolymph; contains the organ of Corti.
scalar field
A function assigning a single number to each point in space (temperature, pressure, potential). Visualised as contour maps.
scaling law
A power-law relationship between quantities that holds across scales. Often derivable from dimensional analysis without solving the full equations.
shear modulus
G = τ/γ. The ratio of shear stress to shear strain. Measures resistance to shape change at constant volume. Related to E by G = E/2(1+ν).
shear stress
The component of stress acting tangentially to a surface: τ = F_tangential/A. In a Newtonian fluid: τ = μ(dv/dy).
shock wave
A thin region of abrupt pressure, density and temperature change propagating supersonically. Nonlinear steepening of a large-amplitude wave into a discontinuity.
sonoluminescence
Light emission from a collapsing cavitation bubble, caused by extreme heating of the gas during the final stage of inertial collapse.
specific heat ratio
γ = cₚ/cᵥ; ratio of heat capacities. For diatomic air γ = 1.4; enters sound speed as c = √(γRT/M).
spectrum
The frequency-domain representation of a signal: the set of amplitudes and phases at each frequency component.
speed of sound
The propagation speed of small-amplitude pressure disturbances. ≈343 m/s in air at room temperature, ≈1480 m/s in water.
spinodal
The thermodynamic limit of metastability beyond which a phase becomes absolutely unstable. On the P-V diagram: where (∂P/∂V)_T = 0.
standing wave
A wave pattern formed by superposition of two waves traveling in opposite directions. Characterised by fixed nodes (zero amplitude) and antinodes (maximum amplitude).
steady state
The long-time behaviour of a driven system after transients have died away. For a sinusoidally driven linear system, it oscillates at the driving frequency.
stereocilia
Actin-filled rod-like protrusions on hair cells, arranged in a graded staircase with tip links connecting neighbours.
Stokes flow
Fluid flow at Re ≪ 1 where inertia is negligible and the Navier-Stokes equations reduce to ∇P = μ∇²v. Reversible, linear, dominated by viscosity.
Stokes-Einstein
D = k_BT/(6πμa). Relates the diffusion coefficient of a spherical particle of radius a to temperature and fluid viscosity.
strain
The fractional deformation of a material: ε = ΔL/L for linear strain. Dimensionless; linked to stress via the constitutive law (e.g. Hooke's law).
stress
Force per unit area within a material (σ = F/A). A tensor quantity: normal stresses (tension/compression) and shear stresses act on different faces of an element.
stria vascularis
Metabolically active epithelium on the lateral wall of scala media that maintains the endocochlear potential.
superposition
The principle that solutions of a linear equation can be added to give new solutions. The foundation of Fourier methods and modal analysis.
surface tension
The energy per unit area (or force per unit length) at a liquid interface, arising from the cohesive deficit of surface molecules. Units: N/m or J/m².
surfactant
A molecule with a hydrophilic head and hydrophobic tail that accumulates at interfaces, lowering surface tension. Critical in lung mechanics and microfluidics.

T

tangent line
The straight line that touches a curve at a single point and matches its slope there. Its slope equals the derivative at that point.
Taylor expansion
An expansion of a smooth function f near a base point x0 as an infinite sum f(x0) + f′(x0)(x−x0) + ½f″(x0)(x−x0)² + … . Truncating gives a polynomial approximation of any required order.
tensile strength
The maximum negative pressure a liquid can sustain before rupturing into vapour. Theoretical: ~GPa for pure water; practical: ~MPa due to pre-existing nuclei.
tensor
A multilinear map that transforms under coordinate changes according to specific rules. Scalars are rank-0, vectors rank-1, stress/strain are rank-2 tensors.
thermal diffusivity
Coefficient α = k/(ρcₚ) governing heat conduction rate; determines whether bubble oscillation is isothermal or adiabatic.
tip link
A molecular thread connecting the top of one stereocilium to the side of its taller neighbour. Stretching opens the MET channel.
tonotopy
Spatial organisation in which neighbouring elements respond to neighbouring frequencies. Preserved from cochlea through brainstem to cortex.
transfer function
The frequency-domain ratio of output to input phasor: H(ω) = Y(ω)/X(ω). Fully characterises a linear system's frequency response.
traveling wave
A wave propagating along the basilar membrane from base to apex, growing in amplitude until reaching its characteristic-frequency place, then dying abruptly.
turbulence
Chaotic, three-dimensional fluid motion characterised by eddies at many scales, enhanced mixing, and energy cascade from large to small scales.

V

van der Waals
Weak intermolecular forces (dipole-dipole, dipole-induced, London dispersion) that fall as r⁻⁶. Responsible for condensation, surface adhesion, and deviations from ideal-gas behaviour.
variance
The expected squared deviation from the mean: Var(X) = E[(X−μ)²]. Measures the spread of a distribution; its square root is the standard deviation.
viscoelastic
A material exhibiting both viscous (time-dependent, dissipative) and elastic (instantaneous, recoverable) response to deformation. Characterised by a complex modulus.
viscous damping
Energy loss from viscous shear at the bubble wall; term −4μṘ/R in the Rayleigh-Plesset equation.
von Kármán vortex street
Alternating pattern of vortices shed behind a bluff body in a flow; source of aeolian tones.

W

wave equation
A second-order PDE describing how a disturbance propagates. For pressure in air: ∂²p/∂t² = c²∇²p.
wavenumber
The spatial frequency of a wave: k = 2π/λ. Higher k means shorter wavelength and more rapid spatial oscillation.
Weber number
We = ρv²L/γ. Ratio of inertial to surface-tension forces. Governs droplet breakup, jet instability, and splash dynamics.
wetting
The tendency of a liquid to spread on a solid surface. Determined by the balance of solid-liquid, solid-gas, and liquid-gas surface energies (Young's equation).
WKB approximation
A method for solving wave equations with slowly-varying coefficients. Gives A(x)·exp(i·∫κ(x)dx) for position-dependent wavenumber κ.

Y

Young-Laplace
The equation relating pressure jump across a curved interface to surface tension and curvature: ΔP = γ(1/R₁ + 1/R₂). Governs bubble equilibrium size.
Young's modulus
E = σ/ε for uniaxial stress. The stiffness of a material: how much stress is needed to produce a given strain. Units: Pa.