Difference between revisions of "4-vectors"
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| Line 26: | Line 26: | ||
| + | Using the Lorentz transformations and the index notation, | ||
| + | <center><math> | ||
| + | \begin{cases} | ||
| + | t'=\gamma (t-vz/c^2) \\ | ||
| + | |||
| + | x'=x' \\ | ||
| + | |||
| + | y'=y' \\ | ||
| + | |||
| + | z'=\gamma (z-vt) | ||
| + | \end{cases} | ||
| + | </math></center> | ||
| + | |||
| + | |||
| + | <center><math>\begin{bmatrix} | ||
| + | x_0' \\ | ||
| + | x_1' \\ | ||
| + | x_2 '\\ | ||
| + | x_3' | ||
| + | \end{bmatrix}= | ||
| + | \begin{bmatrix} | ||
| + | \gamma (x_0-vx_3/c^2) \\ | ||
| + | x_1 \\ | ||
| + | x_2 \\ | ||
| + | \gamma (x_3-vx_0) | ||
| + | \end{bmatrix}</math></center> | ||
---- | ---- | ||