Overview
Benchmarked Partially validated Experimental
The transition-matrix method (TMM) represents a target
by the linear map from incident modal coefficients to scattered modal
coefficients. Its retained state can support more than a monostatic
target-strength curve.
Core idea
Choose a basis matched to the supported geometry, solve the boundary problem for the coefficient map, and optionally retain its frequency-wise blocks for angular scattering, orientation averages, and diagnostics (Waterman 1969, 2009).
Best for
- Supported single-target canonical geometries requiring retained angular products
- Bistatic slices, scattering grids, and orientation post-processing from one solved state
- Cross-checking geometry-specific modal families within a transition-matrix representation
Supports
- Sphere, oblate-spheroid, prolate-spheroid, and guarded finite-cylinder branches
- Supported fixed-rigid, pressure-release, penetrable, and spherical-shell boundaries
- Optional retained T-matrix blocks for branch-specific post-processing
Main assumptions
- A single target represented by one of the documented geometry-specific bases
- Homogeneous-region or supported concentric spherical-shell material structure
- Post-processing uses the documented body-fixed angular convention
- Validation and retained-state support differ by geometry and boundary branch
Validation status
- Benchmarked against
SPHMS,PSMS, andFCMSon the currently supported canonical shape branches. - Validated against external BEMPP far-field checks for sphere, oblate, and prolate pressure-release cases.
- Retained prolate angular products are also checked against the exact general-angle spheroidal solution.
- TMM is partially validated because the sphere, oblate, and prolate branches have external checks, but retained general-angle cylinder products remain outside the validated public scope.
- TMM is currently marked experimental because the retained-state workflow and branch matrix are still guarded while shape-specific support continues to be tightened.
Family pages
- Implementation: branch matrix, retained-state workflows, output, and validation
- Theory: coefficient maps, boundary operators, and geometry-matched bases
References
Waterman, P. C. 1969. “New Formulation of
Acoustic Scattering.” The Journal
of the Acoustical Society of America 45 (6): 1417–29. https://doi.org/10.1121/1.1911619.
Waterman, P. C. 2009. “T -Matrix Methods in Acoustic
Scattering.” The Journal of the Acoustical Society of
America 125 (1): 42–51. https://doi.org/10.1121/1.3035839.
