Mechanics of particles and systems Definition
Galilean transformation
Builds on Orthogonal matrixAffine mapInertial frame of reference
Definition
Let , let , and let be a orthogonal matrix. The Galilean transformation with these data is the map given by Here is a time coordinate and a space coordinate. When , and is the identity, is called a Galilean boost with velocity .
Remarks
Each Galilean transformation is an affine map, and the Galilean transformations form a group under composition. It maps inertial frames to inertial frames: in terms of the new time , a free motion becomes , again of constant velocity. Example: under the boost with velocity , a particle with constant velocity gets velocity ; this is the Galilean rule for adding velocities. Non-example: the map with is not Galilean, since it is not affine in ; it describes an accelerating frame. A Lorentz transformation is not Galilean either, since it changes the time coordinate by an amount that depends on . Some texts require , that is, they leave out reflections.
Reading path
To understand this page from the ground up, read these 10 pages in order. The foundations come first.
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- no evidence level
- Affine map concept
- Euclidean space object
- Identity matrix object
- Matrix definition
- Ordinary differential equation concept
- Classical mechanics concept
- Transpose definition
- Inertial frame of reference concept
- Orthogonal matrix definition
- Galilean transformation definition
Further reading
About this page
| Tag | 80FXZ0XV7J |
|---|---|
| URI | m2://80FXZ0XV7J |
| Kind | definition |
| Writing | W0 stub |
| MSC | 70A05, 70G65 |
| Defines | Galilean transformation |
| Uses | Orthogonal matrix, Affine map, Inertial frame of reference |
| Changed | 3 November 2026 |
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