Physics · Glossary

What is Four-vectors?

Definition 6.1 University Physics — Year 3 · Chapter 6 — Covariant Electromagnetism

A four-vector is a quadruple aμ=(a0,a)a^\mu = (a^0, \vect a), μ=0,1,2,3\mu = 0, 1, 2, 3, whose components mix under a boost exactly as (ct,r)(ct, \vect r) do:

a0=γ(a0βa1),a1=γ(a1βa0),a2,3=a2,3a'^0 = \gamma(a^0 - \beta a^1) , \qquad a'^1 = \gamma(a^1 - \beta a^0) , \qquad a'^{2,3} = a^{2,3}

for a boost at βc\beta c along xx. Any two four-vectors give the invariant scalar product ab=a0b0aba\cdot b = a^0b^0 - \vect a\cdot\vect b, the same number in every frame — the pattern behind c2t2x2c^2t^2 - x^2 and E2p2c2E^2 - p^2c^2. Position (ct,r)(ct, \vect r) and four-momentum (E/c,p)(E/c, \vect p) are the two we have; electromagnetism now supplies three more: current, potential, and wave-vector.

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