For example the rule describing Newton's force of gravity between two chunks of matter is the same whether they are in this galaxy or another (translational invariance in space). It is also the same today as it was a million years ago (translational invariance in time). The law does not work differently depending on whether one chunk is east or north of the other one (rotational invariance). Nor does the law have to be changed depending on whether you measure the force between the two chunks in a railroad station, or do the same experiment with the two chunks on a uniformly moving train (principle of relativity).— David Mermin: It's About Time - Understanding Einstein's Relativity, Chapter 1
Another example of a physical invariant is the speed of light under a Lorentz transformation and time under a Galilean transformation. Such spacetime transformations represent shifts between the reference frames of different observers, and so by Noether's theorem invariance under a transformation represents a fundamental conservation law. For example, invariance under translation leads to conservation of momentum, and invariance in time leads to conservation of energy.
Quantities can be invariant under some common transformations but not under others. For example, the velocity of a particle is invariant when switching from rectangular coordinates to curvilinear coordinates, but is not invariant when transforming between frames of reference that are moving with respect to each other. Other quantities, like the speed of light, are always invariant.
Invariants are important in modern theoretical physics, and many theories are expressed in terms of their symmetries and invariants. Noether's theorem states that every differentiable symmetry of the action of a physical system has a corresponding conservation law.
- General covariance
- Physical constant
- Eigenvalues and eigenvectors
- Weyl transformation
- Casimir operator
- Killing form
- Charge (physics)