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Terms as they are used in this book. Cross-references point into the chapters where the idea is introduced.

Absorptive amplitude
The imaginary part of a complex driven-oscillator amplitude. It is largest at resonance and measures the part of the response in phase with the driving force’s power input. See Chapter 2.
Angular frequency ω\omega
Radians per unit time. Related to the ordinary frequency ν\nu (cycles per unit time) by ω=2πν\omega = 2\pi\nu.
Dispersion relation
An algebraic relation between ω\omega and kk (or k2k^2) that a traveling or standing wave in a given medium must satisfy. It depends on the infinite system, not on the boundary conditions. See Chapter 5.
Elastic amplitude
The real part of a complex driven-oscillator amplitude; the part of the displacement in phase with the driving force.
Group velocity
The velocity of the envelope of a wave packet, vg=dω/dkv_g = d\omega/dk. Distinct from the phase velocity vφ=ω/kv_\varphi = \omega/k. See Chapter 10.
Impedance
For a traveling wave, the ratio of the driving force (or voltage) to the resulting velocity (or current). Continuity of force and displacement at a junction is conveniently expressed in terms of impedances. See Chapter 8.
Irreducible solution
A solution of a linear, time-translation-invariant equation that merely rescales under a shift of the time origin, z(t+a)=h(a)z(t)z(t+a)=h(a)z(t). For the systems in this book these are complex exponentials. See Chapter 1.
Linearity
Superposition: if x1x_1 and x2x_2 are solutions, so is Ax1+Bx2A x_1 + B x_2. Small oscillations of a conservative system about a stable equilibrium are linear.
Local interactions
Each degree of freedom couples only to its neighbors, not to distant parts of the system. Together with linearity and translation invariance, this produces waves.
Normal mode
A motion in which every coordinate oscillates at a single frequency. In a linear system the general free motion is a superposition of normal modes. See Chapter 3.
Phase velocity
The velocity of a surface of constant phase, vφ=ω/kv_\varphi = \omega/k.
Polarization
The pattern of the two (or more) transverse components of a wave, for example linear or circular. See Chapter 12.
Time translation invariance
The equations of motion do not change if the origin of time is shifted. If x(t)x(t) is a solution, so is x(t+a)x(t+a).
Translation invariance
The infinite system looks the same after a discrete (or continuous) shift in space. This is what makes eikxe^{ikx} a useful building block for waves.