
Notation and Symbols
Source:vignettes/notation-and-symbols/notation-and-symbols.Rmd
notation-and-symbols.RmdIntroduction
This is the landing page for the Physics Primer. It defines the symbols, units, medium numbering, and scattering-angle notation used by the remaining theory pages. A model-specific page may introduce additional symbols, but it should state explicitly whenever it departs from the notation below. Equations and physical interpretation remain on the topical pages rather than being repeated here.
The suggested reading order is:
- this notation guide,
- the acoustic scattering primer,
- scattering boundary conditions,
- numerical methods.
Vectors, positions, and directions
| Symbol | Meaning | Typical units |
|---|---|---|
| \mathbf{x} | field-point position | m |
| r=\lVert\mathbf{x}\rVert | distance from the target origin | m |
| \widehat{\mathbf{x}}=\mathbf{x}/r | observation-direction unit vector | dimensionless |
| \widehat{\mathbf{k}}_i | incident propagation-direction unit vector | dimensionless |
| \widehat{\mathbf{s}} | scattered or receive-direction unit vector | dimensionless |
| \mathbf{n} | unit normal, with orientation stated on the relevant interface | dimensionless |
| \Omega_i=(\theta_i,\phi_i) | incident direction | rad |
| \Omega_s=(\theta_s,\phi_s) | scattered or receive direction | rad |
| \psi=\cos^{-1}(\widehat{\mathbf{s}}\!\cdot\!\widehat{\mathbf{k}}_i) | scattering angle: 0 forward and \pi backward | rad |
Medium indexing
The package theory pages use one exterior-to-interior convention:
| Symbol | Meaning |
|---|---|
1 |
surrounding seawater or ambient exterior fluid |
2 |
first target region encountered from the exterior |
3 |
second target region encountered from the exterior |
4 |
third target region encountered from the exterior |
Examples: an unshelled sphere uses media 1 and
2, an elastic shell with internal fluid uses media
1, 2, and 3, and a
viscous-elastic layered sphere can use media 1,
2, 3, and 4.
Subscripts i and j denote arbitrary media. A subscript
1 always denotes the exterior medium in the Physics Primer
and model-family theory pages.
Shared field variables
| Symbol | Meaning | Typical units |
|---|---|---|
| p_1^{\mathrm{inc}} | incident pressure in seawater | Pa |
| p_1^{\mathrm{sca}} | scattered pressure in seawater | Pa |
| p_1^{\mathrm{tot}} | total exterior pressure, p_1^{\mathrm{inc}} + p_1^{\mathrm{sca}} | Pa |
| p_j | pressure in medium j | Pa |
| \mathbf{u} | elastic displacement vector | m |
| \mathbf{v} | fluid particle velocity | m s^{-1} |
| \rho' | acoustic density perturbation | kg m^{-3} |
| \sigma_{ij} | stress-tensor components | Pa |
| \mathbf{t}=\boldsymbol{\sigma}\mathbf{n} | traction acting on a surface with normal \mathbf{n} | Pa |
| \partial_n=\mathbf{n}\cdot\nabla | normal derivative | m^{-1} acting on the differentiated field |
Frequencies, speeds, and wavenumbers
| Symbol | Meaning | Typical units |
|---|---|---|
| f | acoustic frequency | Hz |
| \omega | angular frequency, 2\pi f | rad s^{-1} |
| c_j | sound speed in medium j | m s^{-1} |
| k_j | acoustic wavenumber in medium j, \omega/c_j | m^{-1} |
| k_{L,j} | longitudinal elastic wavenumber in medium j | m^{-1} |
| k_{T,j} | transverse or shear wavenumber in medium j | m^{-1} |
| \alpha_j | amplitude-attenuation coefficient | Np m^{-1} |
| \widetilde{k}_j | complex acoustic wavenumber | m^{-1} |
| \lambda_a=2\pi/k | acoustic wavelength in a lossless fluid | m |
| a | characteristic radius | m |
| L | characteristic length | m |
| ka | acoustic size based on a chosen radius | dimensionless |
The wavelength is written \lambda_a here to distinguish it from Lamé’s first elastic parameter \lambda. A page using complex sound speed rather than complex wavenumber must state its sign convention explicitly.
Acoustic material properties
| Symbol | Meaning | Typical units |
|---|---|---|
| \rho_j | equilibrium mass density in medium j | kg m^{-3} |
| c_j | compressional sound speed in medium j | m s^{-1} |
| \kappa_j | adiabatic compressibility of a fluid | Pa^{-1} |
| K_j | bulk modulus | Pa |
| Z_j | plane-wave acoustic impedance | Pa s m^{-1} |
| \eta_j | dynamic or shear viscosity | Pa s |
| \zeta_j | bulk viscosity | Pa s |
Compressibility \kappa and bulk modulus K are distinct symbols.
Elastic material properties
| Symbol | Meaning | Typical units |
|---|---|---|
| E_j | Young’s modulus | Pa |
| \nu_j | Poisson ratio | dimensionless |
| K_j | bulk modulus | Pa |
| G_j or \mu_j | shear modulus (\mu_j is Lamé’s second parameter) | Pa |
| \lambda_j | Lamé’s first parameter | Pa |
| c_{L,j} | longitudinal wave speed | m s^{-1} |
| c_{T,j} | transverse or shear-wave speed | m s^{-1} |
Material contrasts
| Symbol | Meaning | Typical units |
|---|---|---|
| g_{ij} | density contrast, \rho_i / \rho_j | dimensionless |
| h_{ij} | sound-speed contrast, c_i / c_j | dimensionless |
| \gamma_{\rho,ij} | density perturbation, (\rho_i-\rho_j)/\rho_i | dimensionless |
| \gamma_{\kappa,ij} | compressibility perturbation, (\kappa_i-\kappa_j)/\kappa_j | dimensionless |
For example, g_{21} and h_{21} compare the first target region with the exterior medium. The symbols g_{32} and h_{32} compare the next region with the first.
Scattering quantities
| Symbol | Meaning | Typical units |
|---|---|---|
| p_0 | incident plane-wave pressure amplitude | Pa |
| f(\Omega_s\mid\Omega_i) | far-field scattering amplitude | m |
| \mathrm{d}\sigma/\mathrm{d}\Omega | differential scattering cross-section | m^2 sr^{-1} |
| f_{\mathrm{bs}} | backscattering amplitude | m |
| \sigma_{\mathrm{bs}} | backscattering cross-section | m^2 |
| \sigma_s | total scattering cross-section | m^2 |
| \sigma_a | absorption cross-section | m^2 |
| \sigma_e | extinction cross-section | m^2 |
| \mathrm{TS} | monostatic target strength | dB re 1 m^2 |
| \mathrm{TS}(\Omega_s\mid\Omega_i) | directional or bistatic target-strength notation | dB |
| F or \mathcal{F} | dimensionless form function | dimensionless |
Angles and directions
| Symbol | Meaning | Typical units |
|---|---|---|
| \theta_i, \phi_i | incident polar and azimuthal angles | rad |
| \theta_s, \phi_s | scattered or receive polar and azimuthal angles | rad |
| \psi | angle between incident propagation and receive directions | rad |
| \theta | body or target orientation angle when a page uses a 2D axisymmetric reduction | rad |
| \beta | local body-tilt angle along a segmented or curved centerline | rad |
Incident direction, target orientation, and receive direction are independent quantities. A monostatic geometry fixes the receive direction opposite the incident propagation direction. A bistatic geometry does not.
Basis and special-function notation
| Symbol | Meaning |
|---|---|
| J_m, Y_m, H_m^{(1)} | cylindrical Bessel, Neumann, and outgoing Hankel functions |
| j_n, y_n, h_n^{(1)} | spherical Bessel, Neumann, and outgoing Hankel functions |
| P_n | Legendre polynomial |
| P_n^m | associated Legendre function |
| S_{mn} | angular spheroidal wave function |
| R_{mn}^{(q)} | radial spheroidal wave function of kind q |
| prime ' | derivative with respect to the function’s complete argument unless stated otherwise |
Normalizations for spheroidal functions and dimensionless form functions are given on the topical page where they are used.
Coordinate-specific notation
Some theory pages use geometry-matched coordinates that introduce additional symbols:
| Geometry | Symbols | Meaning |
|---|---|---|
| sphere | (r,\theta,\phi) | ordinary spherical coordinates |
| cylinder | (r,\phi,z) | ordinary cylindrical coordinates |
| prolate spheroid | (\xi,\eta,\phi) | prolate spheroidal coordinates |
| oblate spheroid | (\xi,\eta,\phi) or r(\theta) | oblate geometry in a spheroidal or spherical representation |
When a page uses scale factors such as h_\xi, h_\eta, or h_\phi, those are coordinate metric coefficients, not sound-speed contrasts. The contrast notation always keeps the medium subscripts explicitly: h_{21}, h_{32}, and so on.