Travel-time tomography
Builds on Seismic tomographyFermat's principleEikonal equationRadon transform
Definition
Let be the wave speed on a region and let be the slowness. For a source and a receiver , the travel time is Here is arc length, and is the ray from to , a path that makes the travel time stationary by Fermat's principle. Travel-time tomography is the seismic tomography that estimates from the observed travel times of many source-receiver pairs. In linearised form, for a reference slowness with rays , it solves the following equations for the slowness perturbation : Here are the travel times in .
Remarks
The linearisation keeps the reference rays, because by Fermat's principle the first-order change of the path does not change the time. Example: two unit square cells side by side with slownesses ; a horizontal ray through both has time , and a vertical ray through cell has time . Times and give and , so both cells are determined. Non-example of a well-posed set-up: with only the horizontal ray, only the sum is known, so the data do not determine the model. For a constant reference speed the rays are straight lines, and the data are samples of the Radon transform (in two dimensions) of . Travel times in a general medium solve the eikonal equation , which is used to compute rays and times.
Reading path
To understand this page from the ground up, read these 8 pages in order. The foundations come first.
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- no evidence level
- Calculus of variations concept
- Eikonal equation concept
- Euler–Lagrange equation concept
- Geodesic concept
- Radon transform concept
- Seismic tomography concept
- Fermat's principle statement
- Travel-time tomography definition
Further reading
About this page
| Tag | J9W1CBXYS9 |
|---|---|
| URI | m2://J9W1CBXYS9 |
| Kind | definition |
| Writing | W0 stub |
| MSC | 86A22, 86A15, 44A12 |
| Defines | Travel-time tomography |
| Uses | Seismic tomography, Fermat's principle, Eikonal equation, Radon transform |
| Changed | 3 November 2026 |
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