Glossary

Terms used in this book.

A reference list of the mathematical and physical vocabulary used in Math Foundations. Inline occurrences in the chapters are auto-tooltipped.

313 terms from this book.

A

adaptive step size
Automatically adjusting the integration step h based on local error estimates. Smaller steps where the solution changes fast.
aliasing
The artefact that occurs when a signal is sampled below the Nyquist rate: high frequencies masquerade as lower ones, folding back into the baseband.
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.
ansatz
An educated guess for the form of a solution, with unknown parameters to be determined by substitution into the equation.
anti-aliasing filter
An analog low-pass filter applied before sampling to remove content above the Nyquist frequency.
antiderivative
A function F whose derivative equals f: F′(x) = f(x). The indefinite integral ∫f(x)dx = F(x) + C.
argument
The phase angle of a complex number: arg(z) = atan2(b, a) for z = a + bi. Represents the phase shift when z is a phasor.
attractor
A set in state space toward which trajectories converge as t → ∞. Can be a fixed point, a closed loop (limit cycle), or a fractal "strange" set.
autocorrelation
The correlation of a signal with a time-shifted copy of itself: R(τ) = ⟨x(t)x(t+τ)⟩. Its Fourier transform is the power spectral density (Wiener-Khinchin).

B

band-limited
A signal containing no frequency content above some maximum frequency B. Such signals can be perfectly reconstructed from samples at rate ≥ 2B.
basis
A minimal spanning set for a vector space: every vector can be written uniquely as a linear combination of basis vectors. An n-dimensional space has exactly n basis vectors.
Bayes
Bayes' theorem: P(M|S) = P(S|M)·P(M)/P(S). The posterior over hypotheses given data combines likelihood with prior.
Bayes' theorem
P(M|S) = P(S|M)·P(M)/P(S). The brain's posterior over hypotheses given sensory data combines the likelihood with the prior.
Bayesian updating
Applying Bayes' rule sequentially: each posterior becomes the next prior. The foundation of online estimation and Kalman filtering.
Bernoulli distribution
Two outcomes: 1 with probability p, 0 with probability 1−p. A single coin toss. Building block of the binomial.
Bessel function
Solutions to Bessel's differential equation, arising in problems with cylindrical symmetry. J_n(x) are finite at the origin; Y_n(x) diverge there.
bifurcation
A qualitative change in a system's long-term behaviour as a parameter crosses a critical value — a fixed point losing stability, or a cycle splitting in two (period-doubling).
binomial distribution
The number of successes in n independent Bernoulli(p) trials. Pr(X=k) = C(n,k)pᵏ(1−p)^{n−k}.
binomial series
The Taylor expansion of (1+x)ᵖ for general p: 1 + px + p(p−1)x²/2! + … Converges for |x| < 1.
bisection method
A root-finding algorithm that repeatedly halves an interval [a,b] where f changes sign. Guaranteed convergence but only linear (one bit per step).
Bode plot
A log-frequency plot of transfer-function magnitude and phase; the standard visualisation of filter response.
boundary-value problem
A differential equation with conditions specified at two or more spatial points, rather than at an initial time.
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).
butterfly
The elementary operation of the FFT: combining two partial DFT values with a twiddle factor. The building block of Cooley-Tukey.

C

catastrophic cancellation
Severe loss of significant digits when subtracting two nearly-equal floating-point numbers.
Cauchy–Schwarz inequality
For any vectors u, v in an inner-product space: |⟨u,v⟩| ≤ ‖u‖·‖v‖, with equality iff u and v are parallel. The most-used inequality in functional analysis.
central limit theorem
The sum of many independent random variables (with finite variance) converges to a Gaussian distribution regardless of the individual distributions.
centred difference
The finite-difference approximation [f(x+h)−f(x−h)]/(2h). Second-order accurate: error is O(h²).
CFL condition
The stability bound for explicit finite-difference schemes: the Courant number C = c·Δt/Δx must satisfy C ≤ 1. Numerical signal speed must not exceed physical signal speed.
chain rule
The derivative of a composition: d/dx[f(g(x))] = f′(g(x))·g′(x). The single most-used differentiation technique.
characteristic curve
Curve in (x,t) space along which information propagates; for the wave equation, lines x ± ct = const.
characteristic polynomial
det(A − λI) = 0: a polynomial in λ whose roots are the eigenvalues of A. Degree n for an n×n matrix.
completeness
An orthogonal set is complete if any function can be expanded in it with no leftover residual. Makes Fourier and modal expansions exact.
complex conjugate
For z = a + bi, its conjugate is z* = a − bi. The product z·z* = |z|² is always real and non-negative.
complex plane
The plane with real part horizontal and imaginary part vertical. Phasors, eigenvalues, and impedances all live here.
composition
Applying one function to the output of another: h(x) = f(g(x)). Differentiated by the chain rule.
conjugate prior
A prior distribution that, when combined with a specific likelihood via Bayes' theorem, yields a posterior of the same distributional family. Simplifies sequential updating.
constructive interference
When two waves combine in phase, doubling amplitude. Aligned phasors sum to twice their individual magnitude.
continuity equation
The local conservation law: ∂ρ/∂t + ∇·(ρv) = 0. Any density change equals the negative divergence of the flux.
continuous
A function with no jumps, holes, or breaks: lim_{x→a} f(x) = f(a) for every point a in its domain.
convergence
A sequence or series approaches a definite value as n grows. For a Taylor series, convergence holds within the radius of convergence.
convolution
A mathematical operation combining two signals: the output at time t is the weighted sum of one signal across all times, weighted by the other shifted to t.
convolution theorem
Convolution in the time domain corresponds to multiplication in the frequency domain: F{f*g} = F{f}·F{g}. The computational basis for fast filtering via FFT.
Cooley-Tukey
The divide-and-conquer FFT algorithm that computes a length-N DFT in O(N log N) operations by recursively splitting into even- and odd-indexed sub-transforms.
cosine
For a point at angle θ on the unit circle, its horizontal coordinate, cos θ. Equal to sine shifted by a quarter turn: cos θ = sin(θ + π/2).
Courant number
The dimensionless ratio C = c·Δt/Δx in a finite-difference discretisation of the wave equation. The CFL condition requires C ≤ 1 for stability.
covariance
A measure of joint variability between two random variables: Cov(X,Y) = E[(X−μ_X)(Y−μ_Y)]. Zero for independent variables; sign indicates direction of association.
Crank-Nicolson
A second-order implicit finite-difference scheme for parabolic PDEs that averages the spatial operator between the current and next time step. Unconditionally stable.
critically damped
A damped oscillator with γ = ω₀: returns to equilibrium as fast as possible without oscillating. The design target for many engineered systems.
cumulative distribution
F(x) = P(X ≤ x). The integral of the PDF from −∞ to x. Monotonically non-decreasing from 0 to 1.
curl
A vector measuring local rotation of a field: ∇×v. Its magnitude gives the rotation rate; its direction is the axis of rotation (right-hand rule).

D

d-prime
d′ = (μ_signal − μ_noise)/σ. A bias-free measure of detection sensitivity in signal detection theory. Higher d′ = easier to tell signal from noise.
d'Alembert's solution
The general solution to the 1-D wave equation: u(x,t) = f(x−ct) + g(x+ct). Any disturbance splits into two pulses traveling in opposite directions.
damped natural frequency
The oscillation frequency of a damped system: ω_d = √(ω₀² − γ²), slightly lower than the undamped natural frequency.
damped oscillation
Oscillation with energy loss (friction, viscosity, radiation). Amplitude decays exponentially; the system eventually returns to equilibrium.
damping rate
The coefficient γ controlling exponential energy loss in a damped oscillator. Sets the decay envelope e^{−γt}.
de Moivre's theorem
(cos θ + i sin θ)ⁿ = cos(nθ) + i sin(nθ). A consequence of Euler's formula; simplifies trigonometric identities and nth-root extraction.
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).
degenerate
Two or more modes sharing the same eigenfrequency, typically due to domain symmetry (e.g. a square cavity).
del
The vector differential operator ∇ = (∂/∂x, ∂/∂y, ∂/∂z). Applied to a scalar gives gradient; dot with a vector gives divergence; cross gives curl.
derivative
The instantaneous rate of change of a function: f′(x) = lim_{h→0} [f(x+h)−f(x)]/h. Geometrically, the slope of the tangent line.
destructive interference
When two waves combine with opposite phase, reducing or cancelling amplitude. Phasors 180° apart sum to zero.
determinant
A scalar encoding the signed volume scaling of a linear map. det(A) = 0 means the map is singular (collapses a dimension).
deterministic chaos
Long-term unpredictable behaviour produced by a deterministic system with no randomness, arising from sensitive dependence on initial conditions. Bounded, aperiodic, and exponentially sensitive to its starting point.
DFT
Discrete Fourier Transform. Maps N samples in the time domain to N complex coefficients in the frequency domain. Computed efficiently via the FFT in O(N log N).
diagonalisation
Writing a matrix as A = PDP⁻¹ where D is diagonal (eigenvalues) and P holds eigenvectors. Makes computing Aⁿ and e^{At} trivial.
differential equation
An equation relating an unknown function to its derivatives. ODEs involve one variable; PDEs involve several.
differential operator
A linear map that acts on functions by differentiation, e.g. L = d²/dt² + 2γ d/dt + ω₀².
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).
Dirac delta
A generalised function that is zero everywhere except at the origin, with unit integral: ∫δ(x)dx = 1. The identity element for convolution.
directional derivative
The rate of change of a function along a specified direction û: D_û f = ∇f · û. The gradient gives the maximum directional derivative.
Dirichlet boundary
A boundary condition specifying the value of the solution on the boundary: u|∂Ω = g. Physically: a fixed displacement, a grounded conductor, a clamped edge.
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.
domain of dependence
The set of initial-data points that can influence the solution at a given (x,t). For the wave equation: the backward characteristic cone.
Dormand-Prince
An adaptive-step embedded Runge-Kutta pair (orders 4 and 5) that estimates local error by comparing two solutions. The default integrator in most scientific computing libraries.
dot product
The sum of componentwise products: u·v = Σuₖvₖ. Gives lengths, angles, and projections of vectors.

E

eigenfunction
A function that a linear operator merely multiplies by a scalar: L[f] = λf. Modes of vibration are eigenfunctions of the wave operator.
eigenmode
A natural vibration pattern of a bounded system, corresponding to a specific eigenfrequency. Each eigenmode shape satisfies the boundary conditions.
eigenstate
An eigenfunction of a linear operator, interpreted as a state of the system. Energy eigenstates form a complete basis for any wavefunction.
eigenvalue
A scalar λ such that Av = λv for some nonzero vector v. The eigenvalues of a matrix determine its stretching/shrinking along principal directions.
eigenvector
A nonzero vector v satisfying Av = λv. Points along a direction that the linear map A merely scales (by λ) without rotating.
elliptic PDE
A PDE with no time evolution (like Laplace's equation). Boundary data determines the interior solution globally.
equilibrium
A state where all rates of change are zero; the system remains there unless disturbed.
Euler's formula
e^{iθ} = cos θ + i sin θ. Connects the exponential function to trigonometry; the foundation of phasor analysis and Fourier theory.
expectation
The probability-weighted average of a random variable: E[X] = ∫x·f(x)dx (continuous) or Σx·P(x) (discrete). Also called the mean or first moment.
explicit method
A numerical scheme computing the next value directly from known current values. Simple but stability-limited.
exponential
The function eˣ, the unique function equal to its own derivative. Basis of growth, decay, oscillation (via Euler's formula), and phasor analysis.
exponential decay
The solution x(t) = x₀e^{−αt} of dx/dt = −αx. The generic loss process: decay rate proportional to what remains.
exponential distribution
f(t) = λe^{−λt} for t ≥ 0. The distribution of inter-arrival times in a Poisson process. Memoryless: P(T > s+t | T > s) = P(T > t).
exponential function
The function eˣ, the unique function equal to its own derivative. Solution to dx/dt = x. Basis of growth, decay, and phasor analysis.

F

false alarm rate
The probability of reporting 'signal present' when only noise is present; one axis of the ROC curve.
Feigenbaum constant
The universal ratio δ ≈ 4.6692 at which successive period-doubling bifurcations accumulate, identical for every smooth unimodal map. Evidence that the route to chaos is universal.
FFT
Fast Fourier Transform. An O(N log N) algorithm for computing the DFT, versus the naive O(N²). Enables real-time spectral analysis.
finite difference
Approximation of a derivative by a difference quotient on a grid: f′(x) ≈ [f(x+h)−f(x−h)]/(2h) (centred, second-order).
fixed point
A value x* such that f(x*) = x*. Iterative methods converge when the mapping is contractive near the fixed point (|f′(x*)| < 1).
flux
The flow of a vector field through a surface: ∫∫F·dA. Measures how much of the field passes through the area.
forcing
An external drive applied to a system. The particular solution responds to forcing; the homogeneous solution decays away.
forward Euler
The simplest ODE integrator: y_{n+1} = y_n + h·f(t_n, y_n). First-order accurate; conditionally stable. Useful pedagogically but rarely in production.
Fourier coefficient
The complex amplitude cₙ of the n-th harmonic in a Fourier series. Extracted by projection: cₙ = (1/T)∫f(t)e^{−inω₀t}dt.
Fourier series
Decomposition of a periodic signal into a sum of sinusoids at multiples of its fundamental frequency.
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.
fundamental frequency
The lowest frequency in a periodic signal's Fourier series: f₁ = 1/T where T is the period. All other harmonics are integer multiples.
fundamental theorem of calculus
Links differentiation and integration: d/dx ∫ₐˣ f(t)dt = f(x), and ∫ₐᵇ f(x)dx = F(b)−F(a) where F′ = f.
FWHM
Full Width at Half Maximum — the frequency (or other) interval where a peak exceeds half its peak value.

G

Gauss-Seidel
An iterative method for solving Ax = b that updates each variable using the latest available values of other variables. Converges for diagonally-dominant or symmetric positive-definite A.
Gaussian distribution
The normal distribution: f(x) = (1/σ√2π)exp(−(x−μ)²/2σ²). The Central Limit Theorem makes it ubiquitous for sums of independent random variables.
Gaussian elimination
The standard algorithm for solving Ax = b: reduce to upper-triangular form by row operations, then back-substitute.
general solution
The full family of solutions to a differential equation, containing as many free constants as the order.
Gibbs phenomenon
The ~9% overshoot that persists at a discontinuity when a function is represented by a truncated Fourier series, no matter how many terms are included.
gradient
The vector of partial derivatives ∇φ = (∂φ/∂x, ∂φ/∂y, ∂φ/∂z). Points in the direction of steepest increase; its magnitude is the rate of increase.
Gram-Schmidt
An algorithm that converts any linearly independent set into an orthonormal basis by sequential projection and normalisation.
Green's function
The response of a linear system to a unit impulse. Fully characterises propagation from source to receiver in any linear medium.

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.
Hann window
A raised-cosine window w(n) = ½[1 − cos(2πn/N)] used to reduce spectral leakage in DFT analysis.
harmonic
An integer multiple of the fundamental frequency. The nth harmonic has frequency nf₁. Harmonics are the building blocks of periodic signals.
harmonic function
A function satisfying Laplace's equation ∇²u = 0. Its value at any interior point equals the average on a surrounding sphere (the mean-value property).
heat equation
The parabolic PDE ∂u/∂t = α∇²u describing thermal conduction (or any diffusive process). Solutions smooth out discontinuities instantly.
Helmholtz decomposition
Any vector field splits into an irrotational part (gradient of a scalar) plus a solenoidal part (curl of a vector).
Helmholtz equation
The time-independent wave equation: ∇²u + k²u = 0. Arises from separating the time dependence out of the wave equation for steady-state oscillations.
Hermitian
A complex matrix or operator equal to its own conjugate transpose (A† = A). Hermitian operators have real eigenvalues and orthogonal eigenvectors forming a complete basis.
Hilbert space
A complete inner-product space — the infinite-dimensional generalisation of Euclidean space. The natural setting for Fourier analysis, quantum mechanics, and PDE solutions.
homogeneous
A differential equation with zero forcing (RHS = 0). Solutions obey superposition and can be freely added.
hyperbolic PDE
A PDE with finite propagation speed (like the wave equation). Information travels along characteristics.

I

i.i.d.
Independent and identically distributed. Random variables that share the same distribution and carry no information about each other. The standard simplifying assumption.
identity matrix
The square matrix I with 1s on the diagonal and 0s elsewhere. The "do nothing" transformation: Iv = v for all v.
imaginary unit
The number i satisfying i² = −1. Extends the reals to the complex plane and enables phasor algebra.
implicit method
A numerical scheme whose update depends on the (unknown) future value. Requires solving an equation at each step but is unconditionally stable.
impulse response
A system's output when given a single, brief impulse as input. Fully characterises any linear time-invariant system.
initial condition
The value(s) of the solution and its derivatives at the starting time: y(0) = y₀, y′(0) = v₀. Picks out a unique solution from the general family.
inner product
A generalisation of the dot product to abstract vector spaces: ⟨f, g⟩ = ∫f*(x)g(x)dx for functions. Defines orthogonality, norms, and projections.
integral
The signed area under a curve: ∫f(x)dx. The Fundamental Theorem connects it to the antiderivative. Extends to line, surface, and volume integrals.
integration by parts
∫u dv = uv − ∫v du. Derived from the product rule; converts one integral into another (hopefully simpler) one.
inter-arrival time
The random waiting time between consecutive events in a Poisson process; exponentially distributed with mean 1/λ.
inverse Fourier transform
Recovers a time-domain signal from its frequency-domain representation: f(t) = (1/2π)∫F(ω)e^{iωt}dω. The inverse of the forward transform.
inverse function
A function f⁻¹ that undoes f: f⁻¹(f(x)) = x. Exists when f is one-to-one. Its graph is the reflection of f across y = x.
inverse rule
If y = f(x) and x = f⁻¹(y), then dx/dy = 1/(dy/dx). The slope of an inverse function is the reciprocal of the original.
irreversible
A process that cannot be undone by reversing time; the heat equation loses information as high-k modes decay.
irrotational
A vector field with zero curl everywhere (∇×v = 0). Such a field can be written as the gradient of a scalar potential: v = ∇φ.

J

Jacobi iteration
The simplest relaxation method: replace each interior grid value by the average of its neighbours. Trivially parallel but slow to converge.
Jacobian
The matrix of all first-order partial derivatives of a vector-valued function. Locally approximates a nonlinear map as a linear one; its determinant gives the volume scaling factor.

L

L'Hôpital's rule
For indeterminate limits 0/0 or ∞/∞: lim f/g = lim f'/g' when the latter exists. Resolves ambiguous limiting ratios.
Laplace equation
The elliptic PDE ∇²φ = 0. Governs equilibrium fields: steady-state temperature, electrostatic potential, incompressible potential flow.
Laplace transform
An integral transform F(s) = ∫₀^∞ f(t)e^{−st} dt that converts ODEs with initial conditions into algebraic equations. The s-domain generalises the Fourier domain to complex frequencies.
Laplacian
The divergence of the gradient: ∇²φ = ∂²φ/∂x² + ∂²φ/∂y² + ∂²φ/∂z². Measures how a function deviates from its local average.
law of large numbers
The sample mean converges to the true mean as sample size grows: (1/n)Σxᵢ → E[X]. The mathematical basis for empirical measurement.
leapfrog scheme
A time-centred finite-difference scheme: y_{n+1} = y_{n−1} + 2h·f(t_n, y_n). Second-order accurate and energy-conserving for Hamiltonian systems.
least-squares
Finding x that minimises ‖Ax − b‖² for an overdetermined system; solved via the normal equations AᵀAx = Aᵀb.
Legendre polynomial
Orthogonal polynomial P_ℓ(cos θ) solving the angular part of Laplace's equation in spherical coordinates.
level set
The set of points where a scalar field takes a constant value; contour lines in 2-D, isosurfaces in 3-D.
likelihood
In Bayesian inference, P(S|M): how probable the observed sensory input is given that hypothesis M is true.
likelihood ratio
The ratio f₁(x)/f₀(x) of probability densities under two hypotheses. The optimal statistic for distinguishing signal from noise.
limit
The value a function approaches as its input approaches some point. The foundation of derivatives and integrals.
limit cycle
An isolated closed trajectory in state space toward which neighbouring trajectories spiral. Represents self-sustained periodic oscillation in a nonlinear system.
linear combination
A sum of vectors each multiplied by a scalar: c₁v₁ + c₂v₂ + … Any vector is a linear combination of basis vectors.
linear independence
Vectors {v₁,…,vₙ} are linearly independent if no nontrivial combination c₁v₁+…+cₙvₙ = 0. Independent vectors span an n-dimensional subspace.
linear time-invariant
A system whose output obeys superposition (linear) and whose behaviour does not change over time (time-invariant). Sinusoids are its eigenfunctions.
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.
linearity
The property that an operation distributes over addition and commutes with scalar multiplication: L(af + bg) = aL(f) + bL(g).
logarithm
The inverse of the exponential: ln(y) = x means eˣ = y. Its derivative is 1/x, making it the antiderivative of 1/x.
logistic map
The quadratic recurrence x_{n+1} = r x_n (1 − x_n), the simplest system exhibiting the full period-doubling route to chaos as r increases toward 4.
Lorentzian
The function 1/[(ω−ω₀)² + Γ²]; the spectral shape of a damped resonance, universal near any isolated pole.
LTI system
Linear Time-Invariant system. Fully characterised by its impulse response; output = input * h(t) (convolution).
Lyapunov exponent
The average exponential rate λ at which nearby trajectories separate: |Δ(t)| ≈ |Δ(0)| e^{λt}. A positive largest Lyapunov exponent is the quantitative signature of chaos.

M

Maclaurin series
A Taylor series expanded about x = 0. The standard expansions of eˣ, sin x, cos x are all Maclaurin series.
marginal likelihood
The total probability of the data P(D) = Σ P(D|H)P(H); normalises the posterior in Bayes' theorem.
matrix
A rectangular array of numbers representing a linear transformation. An m×n matrix maps n-vectors to m-vectors.
matrix inverse
A⁻¹ satisfying A·A⁻¹ = I. Exists iff det(A) ≠ 0. Solving Ax = b becomes x = A⁻¹b (though direct inversion is rarely the best numerical method).
maximum principle
A harmonic function on a bounded region attains its maximum and minimum on the boundary, never in the interior (unless constant).
method of characteristics
A PDE-solving technique that reduces the PDE to ODEs along curves (characteristics) in the (x,t) plane. Natural for hyperbolic equations.
mode shape
The spatial pattern X_n(x) of a single standing-wave mode; a sinusoidal eigenfunction of the spatial operator.
modulus
The magnitude of a complex number: |z| = √(a² + b²) for z = a + bi. Represents the amplitude when z is a phasor.
Monte Carlo
A class of algorithms that use random sampling to estimate numerical quantities — integrals, expectations, probabilities — that are hard to compute deterministically.
multigrid
A numerical method that accelerates convergence of iterative solvers by solving the residual equation on successively coarser grids, then interpolating corrections back up.

N

natural frequency
The frequency at which an undamped system oscillates freely: ω₀ = √(k/m) for a mass-spring. The intrinsic resonance of the system.
natural logarithm
The logarithm to base e, written ln x. Inverse of eˣ, and the base in which log laws carry no extra constant (d/dx ln x = 1/x).
Neumann boundary
A boundary condition specifying the normal derivative on the boundary: ∂u/∂n|∂Ω = h. Physically: a specified flux, a free end, a perfectly reflecting wall.
Newton's method
An iterative root-finding algorithm: x_{n+1} = x_n − f(x_n)/f′(x_n). Converges quadratically near a simple root when started sufficiently close.
nodal line
A curve on a vibrating surface where the displacement is always zero; separates regions oscillating in antiphase.
norm
The length of a vector: ‖v‖ = √(v·v). Generalises Pythagoras to n dimensions.
normal mode
A pattern of motion in which all parts of a system oscillate at the same frequency and in a fixed phase relationship. The building blocks of any vibration.
Nyquist frequency
Half the sample rate: fₛ/2. The maximum frequency representable without aliasing in a sampled signal.
Nyquist plot
A parametric plot of a complex transfer function in the complex plane as frequency sweeps; used for stability analysis.
Nyquist rate
The minimum sampling rate (2× the highest frequency present) required to perfectly reconstruct a band-limited signal from its samples.

O

optimisation
Finding the input that maximises or minimises a function. At an optimum, the derivative is zero (necessary condition for smooth functions).
order of accuracy
The power of h in the leading truncation-error term. A p-th order method has error O(hᵖ); halving h divides error by 2ᵖ.
ordinary differential equation
An equation relating a function to its derivatives with respect to a single independent variable. Order = highest derivative present.
orthogonality
Two vectors are orthogonal when their inner product is zero: ⟨u,v⟩ = 0. Generalises perpendicularity to abstract spaces; the basis of Fourier decomposition.
orthonormal basis
A basis whose vectors are mutually perpendicular and unit-length: ⟨eᵢ, eⱼ⟩ = δᵢⱼ. Makes projections trivial: component = ⟨v, eᵢ⟩.
overdamped
A damped oscillator with γ > ω₀: returns to equilibrium without oscillating but slower than critical damping. Two real decay rates.

P

parabolic PDE
A PDE with diffusive character (like the heat equation). Disturbances smooth out over time at all speeds.
Parseval's theorem
Total energy in the time domain equals total energy in the frequency domain: ∫|f(t)|²dt = ∫|F(ω)|²dω. Energy is preserved by the Fourier transform.
partial derivative
The derivative of a multivariable function with respect to one variable, holding the others fixed: ∂f/∂x.
partial differential equation
An equation involving partial derivatives of an unknown function of two or more variables. Classification: elliptic, parabolic, or hyperbolic.
partial fractions
Decomposing a rational function into simpler fractions that each integrate to logarithms or arctangents.
particular solution
A single solution of a non-homogeneous equation matching the forcing. Added to the homogeneous solution for the full answer.
period-doubling
A bifurcation in which a stable cycle of period T is replaced by a stable cycle of period 2T. An infinite cascade of period-doublings, accumulating geometrically, is one universal route to chaos.
phase portrait
A plot of trajectories in the (position, velocity) plane for a dynamical system. Reveals fixed points, limit cycles, and qualitative behaviour at a glance.
phasor
A complex number Ae^{iφ} representing a sinusoidal signal's amplitude A and phase φ. Converts differential equations into algebraic ones by replacing d/dt with iω.
pivot
The diagonal entry used to eliminate entries below it in Gaussian elimination; must be non-zero.
Plancherel theorem
The Fourier transform preserves the L² inner product (up to a 2π factor); generalises Parseval's identity.
Planck constant
Fundamental quantum of action ℏ ≈ 1.055×10⁻³⁴ J·s; sets the scale at which quantum effects become significant.
Poisson distribution
Distribution of event counts: P(k) = (λT)^k e^{−λT}/k!, with mean = variance = λT.
Poisson process
A stochastic process in which events occur independently at a constant average rate λ. The number of events in any interval is Poisson-distributed with mean λt.
polar form
Writing a complex number as z = re^{iθ} with modulus r = |z| and argument θ. Multiplication becomes scaling and rotation.
polynomial
A function built from powers of x with constant coefficients: aₙxⁿ + … + a₁x + a₀. Degree n means the highest power is n.
positive definite
A matrix A for which vᵀAv > 0 for all nonzero v. Ensures a quadratic form has a unique minimum.
posterior
In Bayesian inference, P(M|S): the probability of hypothesis M given sensory input S. What the brain perceives.
power spectral density
The squared magnitude of a signal's Fourier transform per unit time; gives power per unit frequency.
power spectrum
The distribution of signal power across frequency: |F(ω)|². Its integral equals the total signal energy (Parseval's theorem).
precision
The reciprocal of variance (1/σ²); in Bayesian updating, precisions add when combining prior and data.
prior
In Bayesian inference, P(M): the probability of a hypothesis before any sensory input. Shaped by context, expectation, and learned experience.
probability density function
A function f(x) ≥ 0 whose integral over any interval gives the probability of the random variable falling in that interval. ∫f(x)dx = 1 over the full domain.
product rule
The derivative of a product: (fg)' = f'g + fg'. Each factor is differentiated in turn while the other holds still.
projection
The component of one vector along another: proj_u(v) = (⟨v,u⟩/⟨u,u⟩)u. Fourier coefficients are projections onto sinusoidal basis functions.

Q

quadratic convergence
Error at each step is proportional to the previous error squared. Digits of accuracy double per iteration. Newton's method achieves this near a simple root.
quantisation condition
The constraint (e.g. kL = nπ) that selects a discrete set of allowed wavenumbers from boundary conditions.
quotient rule
The derivative of a ratio: (f/g)' = (f'g − fg')/g². A consequence of the product and chain rules.

R

radian
The natural measure of angle: the arc length subtended on a circle of radius 1. A full turn is 2π radians (360°). Radians are the unit in which d/dθ sin θ = cos θ.
radius of convergence
The distance from the expansion point within which a power series converges absolutely. Beyond it, the series diverges.
radix-2
FFT variant requiring N to be a power of 2; splits the DFT into even- and odd-indexed halves at each level.
random variable
A quantity determined by a random process. Described by its distribution (PMF for discrete, PDF for continuous).
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.
rate of change
How quickly a quantity varies with respect to another variable. The derivative gives the instantaneous rate of change.
Rayleigh quotient
For a matrix A and vector v: R(v) = vᵀAv/vᵀv. Bounded by the eigenvalues of A; iterating on power-method iterates converges to the dominant eigenvalue.
reactance
The imaginary part X of a complex impedance Z = R + iX; stores energy without dissipating it.
region of influence
The set of spacetime points that can be affected by a given initial-data point; forward-opening wedge bounded by characteristics.
restoring force
Force directed toward equilibrium, proportional to displacement for small perturbations (F = −kx).
Riemann sum
An approximation of a definite integral as a finite sum of rectangle areas. Converges to the integral as the partition refines.
Robin boundary
A boundary condition that is a linear combination of Dirichlet and Neumann: αu + β∂u/∂n = g. Models imperfect absorption or impedance boundaries.
ROC curve
Receiver Operating Characteristic: a plot of true-positive rate vs. false-positive rate as the detection threshold varies. Area under the curve measures discriminability.
root-mean-square
The square root of the time-averaged square of a signal: f_rms = √((1/T)∫f²dt). For a sinusoid, amplitude/√2.
Runge-Kutta
A family of single-step ODE solvers that evaluate the derivative at multiple trial points per step to achieve high-order accuracy. RK4 (the "classic" method) is fourth-order.

S

sample rate
Samples per second f_s when digitising a signal; must exceed 2× the maximum frequency to avoid aliasing.
sampling theorem
Shannon's theorem: a band-limited signal with maximum frequency B is completely determined by samples taken at rate ≥ 2B (the Nyquist rate).
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.
secant method
A root-finding algorithm like Newton's method but replacing the derivative with a finite-difference approximation from the two most recent iterates. Superlinear convergence (order ≈1.618).
self-adjoint
A linear operator that equals its own adjoint. For real matrices: A = Aᵀ (symmetric). For differential operators: ⟨f, Lg⟩ = ⟨Lf, g⟩. Guarantees real eigenvalues and orthogonal eigenfunctions.
sensitive dependence on initial conditions
The hallmark of chaos: two trajectories that start arbitrarily close together separate exponentially fast, at a rate set by the largest Lyapunov exponent. Small uncertainties are amplified until prediction fails.
separation constant
The shared constant that both sides of a separated PDE must equal; becomes the eigenvalue of the spatial problem.
separation of variables
A PDE-solving technique that assumes the solution factors as u(x,t) = X(x)·T(t), reducing one PDE to two ODEs. Works when the operator and domain allow it.
signal detection theory
A framework for analysing decisions under uncertainty: the observer must decide whether a noisy observation came from a signal-present or signal-absent distribution.
simple harmonic motion
Oscillation governed by ẍ = −ω₀²x. Solution: x(t) = A cos(ω₀t + φ). The linearised dynamics near any stable equilibrium.
sinc function
sinc(x) = sin(πx)/(πx). The Fourier transform of a rectangular pulse and the ideal interpolation kernel for band-limited reconstruction.
sine
For a point at angle θ on the unit circle, its vertical coordinate, sin θ. Periodic with period 2π; the building block of oscillations and Fourier series.
singular matrix
A square matrix with determinant zero. Not invertible; its columns are linearly dependent.
sinusoid
A function of the form A sin(ωt + φ) or equivalently A cos(ωt + φ). The basic periodic waveform; all Fourier components are sinusoids.
slope
The ratio of vertical to horizontal change along a line or curve. For a curve, the slope at a point is the derivative there.
slope field
A plot showing the local slope f(t,x) at every point; solutions are curves threading tangentially through the field.
solenoidal
A vector field with zero divergence everywhere (∇·v = 0). Incompressible fluid flow is solenoidal; such fields can be written as the curl of a vector potential.
Sommerfeld radiation condition
The boundary condition at infinity for an unbounded Helmholtz problem: φ at large r must look like an outgoing spherical wave (~e^{ikr}/r), not incoming.
sparse matrix
A matrix with mostly zero entries; the 5-point Laplacian stencil on an N×N grid has only 5 non-zeros per row.
spectral leakage
Energy spreading from a signal's true frequency into adjacent DFT bins when the analysis window does not contain an integer number of cycles. Mitigated by window functions.
spectral method
A PDE-solving technique that expands the solution in a global basis (Fourier, Chebyshev) and solves for the coefficients. Exponential convergence for smooth problems.
spectral radius
The largest absolute eigenvalue of an iteration matrix; must be < 1 for convergence of iterative methods.
spectral theorem
A self-adjoint linear operator has a complete orthonormal basis of eigenvectors with real eigenvalues. The reason mode expansions and separation of variables work.
spectrum
The frequency-domain representation of a signal: the set of amplitudes and phases at each frequency component.
spherical harmonic
Eigenfunction Y_ℓm(θ,φ) of the angular Laplacian on the sphere; the angular modes in spherical geometry.
stable spiral
A fixed point with complex eigenvalues having negative real part; trajectories spiral inward.
standard deviation
The square root of variance: σ = √Var(X). Measures spread in the same units as the variable. ≈68% of a Gaussian falls within ±1σ of the mean.
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.
stencil
The pattern of grid points used in a finite-difference formula. The 5-point stencil approximates the 2-D Laplacian.
stiff system
An ODE system with widely separated time scales. Explicit methods are forced into tiny steps; implicit methods are required.
stochastic process
A family of random variables indexed by time or space. Brownian motion and Poisson processes are the two canonical examples.
Stokes theorem
Relates a surface integral of curl to a line integral around the boundary: ∫∫(∇×F)·dA = ∮F·dr. Generalises Green's theorem to 3-D.
strange attractor
An attractor with fractal (non-integer) dimension on which the motion is chaotic. Trajectories are confined to it yet never repeat and never cross — the Lorenz butterfly is the canonical example.
Strouhal number
Dimensionless St = fd/U relating vortex-shedding frequency to flow speed and body size; St ≈ 0.2.
Sturm–Liouville theorem
For a self-adjoint differential operator on a bounded interval with appropriate boundary conditions, there is a countably infinite sequence of real eigenvalues and a complete orthonormal basis of eigenfunctions.
substitution
An integration technique mirroring the chain rule: replace a composite integrand with a simpler variable u = g(x).
successive over-relaxation
An acceleration of Gauss-Seidel using an over-relaxation factor ω > 1. Optimal ω reduces iteration count from O(N²) to O(N).
superposition
The principle that solutions of a linear equation can be added to give new solutions. The foundation of Fourier methods and modal analysis.
symmetric matrix
A matrix equal to its transpose: A = Aᵀ. The spectral theorem guarantees real eigenvalues and orthogonal eigenvectors.

T

tangent
The ratio tan θ = sin θ / cos θ, the slope of the radius to the point at angle θ on the unit circle. Diverges where cos θ = 0.
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.
Taylor polynomial
A polynomial of degree N matching a function and its first N derivatives at a base point. The finite truncation of a Taylor series.
Taylor series
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.
time constant
τ = 1/α: the time for an exponentially decaying quantity to fall to 1/e ≈ 37% of its initial value.
time-harmonic
Oscillating at a single frequency; a field of the form φ(r)e^{−iωt}, reducing the wave equation to Helmholtz.
total differential
The first-order change in a multivariate function: df = (∂f/∂x)dx + (∂f/∂y)dy + … Measures response to simultaneous small changes.
trace
The sum of diagonal elements of a matrix: tr(A) = Σaᵢᵢ. Equals the sum of eigenvalues. Invariant under change of basis.
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.
transient
The component of a system's response that decays over time after a perturbation, leaving only the steady state.
transpose
The matrix Aᵀ formed by swapping rows and columns: (Aᵀ)ᵢⱼ = Aⱼᵢ. A symmetric matrix satisfies Aᵀ = A.
truncation error
The error introduced by replacing a continuous operator with a discrete approximation. For a p-th order method: error ∝ hᵖ as h → 0.
twiddle factor
The complex exponential weight W_N^k = e^{−2πik/N} appearing in the DFT. Pre-computing twiddle factors is a key optimisation in FFT implementations.

U

uncertainty principle
A signal cannot be simultaneously narrow in time and narrow in frequency. Time-bandwidth product has a minimum, saturated by the Gaussian.
underdamped
A damped oscillator with γ < ω₀: oscillates with exponentially decaying amplitude. The most common regime for musical and biological systems.
uniform distribution
Constant probability density on an interval [a,b]. The default when only bounds are known and no value is preferred.
unit circle
The circle |z| = 1 in the complex plane. e^{iθ} traces it as θ varies. Phasors of unit amplitude live on it.
unitary
A transformation preserving inner products (and norms); time evolution under the Schrödinger equation is unitary.
unstable node
A fixed point with two real positive eigenvalues; trajectories diverge from it monotonically.

V

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.
vector
An ordered tuple of numbers representing magnitude and direction. The fundamental object of linear algebra.
vector field
A function assigning a vector to each point in space (velocity, electric field, force). Visualised as arrow fields or streamlines.
velocity potential
A scalar field φ such that v = ∇φ. Exists when the flow is irrotational. Central to linearised acoustics.
von Neumann stability analysis
Substituting a Fourier mode into a finite-difference scheme and checking whether its amplitude grows. The standard stability test for PDE schemes.

W

wave equation
A second-order PDE describing how a disturbance propagates. For pressure in air: ∂²p/∂t² = c²∇²p.
wavefunction
Complex-valued function Ψ(r,t) in quantum mechanics whose squared magnitude gives the probability density of position.
wavenumber
The spatial frequency of a wave: k = 2π/λ. Higher k means shorter wavelength and more rapid spatial oscillation.
wavevector
Vector k pointing in propagation direction with magnitude 2π/λ; encodes spatial periodicity and direction.
well-posed problem
A PDE problem (in Hadamard's sense) where a solution exists, is unique, and depends continuously on the data. Ill-posed problems require regularisation.
Wiener process
The continuous-time limit of a random walk: a Gaussian process with independent increments, continuous paths, and variance growing linearly with time. The mathematical model of Brownian motion.
window function
A tapering function (Hann, Hamming, Blackman, etc.) multiplied with a signal segment before DFT to reduce spectral leakage at the cost of frequency resolution.
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.