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In ], a '''four-vector''' is a ] in a four-dimensional real ], whose components transform like the space and time coordinates (''ct'', ''x'', ''y'', ''z'') under spatial rotations and ''boosts'' (a change by a constant velocity to another ]). The set of all such rotations and boosts, called ] and described by 4×4 matrices, forms the Lorentz group. | In ], a '''four-vector''' is a ] in a four-dimensional real ], whose components transform like the space and time coordinates (''ct'', ''x'', ''y'', ''z'') under spatial rotations and ''boosts'' (a change by a constant velocity to another ]). The set of all such rotations and boosts, called ] and described by 4×4 matrices, forms the Lorentz group. | ||
Examples of four-vectors include the coordinates (''ct'', ''x'', ''y'', ''z'') themselves, the four-current (''c''&rho, '''J''') formed from charge density ρ and current density '''J''', the electromagnetic four-potential (φ, '''A''') formed from the scalar potential φ and vector potential '''A''', and the four-momentum (''E''/''c'', '''p''') formed from the (relativistic) energy ''E'' and momentum '''p'''. The ] (''c'') is often used to ensure that the first coordinate (''time-like'', labeled by index 0) has the same units as the following three coordinates (''space-like'', labeled by indices 1,..,3). | Examples of four-vectors include the coordinates (''ct'', ''x'', ''y'', ''z'') themselves, the four-current (''c''ρ, '''J''') formed from charge density ρ and current density '''J''', the electromagnetic four-potential (φ, '''A''') formed from the scalar potential φ and vector potential '''A''', and the four-momentum (''E''/''c'', '''p''') formed from the (relativistic) energy ''E'' and momentum '''p'''. The ] (''c'') is often used to ensure that the first coordinate (''time-like'', labeled by index 0) has the same units as the following three coordinates (''space-like'', labeled by indices 1,..,3). | ||
The ] between four-vectors ''a'' and ''b'' is defined as follows: | The ] between four-vectors ''a'' and ''b'' is defined as follows: |
Revision as of 11:18, 14 June 2003
In relativity, a four-vector is a vector in a four-dimensional real vector space, whose components transform like the space and time coordinates (ct, x, y, z) under spatial rotations and boosts (a change by a constant velocity to another inertial reference frame). The set of all such rotations and boosts, called Lorentz transformations and described by 4×4 matrices, forms the Lorentz group.
Examples of four-vectors include the coordinates (ct, x, y, z) themselves, the four-current (cρ, J) formed from charge density ρ and current density J, the electromagnetic four-potential (φ, A) formed from the scalar potential φ and vector potential A, and the four-momentum (E/c, p) formed from the (relativistic) energy E and momentum p. The speed of light (c) is often used to ensure that the first coordinate (time-like, labeled by index 0) has the same units as the following three coordinates (space-like, labeled by indices 1,..,3).
The scalar product between four-vectors a and b is defined as follows:
Strictly speaking, this is not a proper inner product, since its value can be negative. Like the ordinary dot product of three-vectors, however, the result of this scalar product is a scalar: it is invariant under any Lorentz transformation. (This property is sometimes use to define the Lorentz group.) The 4×4 matrix in the above definition is called the metric tensor, sometimes denoted by g; its sign is a matter of convention, and some authors multiply it by -1.
The laws of physics are also postulated to be invariant under Lorentz transformations. An object in an inertial reference frame will perceive the universe as if the universe were Lorentz-transformed so that the perceiving object is stationary.
See also: four-velocity, four-acceleration, four-momentum, four-force.