Special Relativity: Dynamics
Terms and Formulae for Relativistic Dynamics
Terms
1
and
p
mv
.
| A 0 = γ(A 0' + (v/c)A 1') | |||
| A 1 = γ(A 1' + (v/c)A 0') | |||
| A 2 = A 2' | |||
| A 3 = A 3' |
Only those vectors for which the result of the above transformation is equal to the transformation of the individual coordinates under the Lorentz transformations are 4-vectors. The velocity 4-vector (γv, γbfv) and the energy-momentum 4-vector (E/c,
are the most common.
Δτ =
|
This is a particularly useful quantity because it is in independent of the frame in which it is measured.
| AƒB = A 0 B 0 - A 1 B 1 - A 2 B 2 - A 3 B 3 |
Note that the minus signs make this inner product different from the usual dot product in 3-space. When defined in this way, the inner product of any two 4-vectors is a constant, independent of frame (that is, it is independent of the frame in which the vectors are written).
Formulae
| Lorentz Transformations for Energy and Momentum |
|
| Formula for Velocity in terms of Energy and Momentum |
|
| Relativistic relationship between mass, energy, and momentum. (Specifically, this equation states that the square of the energy-momentum 4-vector is equal to m 2 c 4 .) The formula reduces to the familiar E = mc 2 when the momentum p is zero. |
|
| Lorentz transformations for force undergoing a boost in the y-direction. |
|
Readers' Notes allow users to add their own analysis and insights to our SparkNotes—and to discuss those ideas with one another. Have a novel take or think we left something out? Add a Readers' Note!
=





