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
- Radians per unit time. Related to the ordinary frequency (cycles per unit time) by .
- Dispersion relation
- An algebraic relation between and (or ) 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, . Distinct from the phase velocity . 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, . For the systems in this book these are complex exponentials. See Chapter 1.
- Linearity
- Superposition: if and are solutions, so is . 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, .
- 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 is a solution, so is .
- Translation invariance
- The infinite system looks the same after a discrete (or continuous) shift in space. This is what makes a useful building block for waves.