equation

Lorentz transformations

Lorentz transformations are the equations that relate space and time coordinates between inertial frames in special relativity.
18 related articles · 2 formulas · 2 who worked here

Description

Imagine a train traveling almost at the speed of light. A passenger on the train and a person on the platform measure the length of the same carriage and the time on the clocks — and get different results! The Lorentz transformations show how these measurements are related so that the speed of light remains the same for both observers. It is as if space and time compress and stretch, adjusting to the motion.

History

In 1892–1904, Hendrik Lorentz developed these equations, independently starting from the FitzGerald length contraction hypothesis, to explain the null result of the Michelson-Morley experiment. In 1905, Henri Poincaré was the first to give the complete mathematical form and showed that they form a group, naming them 'Lorentz transformations'. In the same year, Albert Einstein derived them from two postulates — the constancy of the speed of light and the equivalence of inertial frames.

How it works

They are used in all problems of special relativity to recalculate physical quantities between frames of reference. They allow for the correct description of electrodynamics of moving media, relativistic kinematics, time dilation and length contraction effects. Limits of applicability: only for inertial frames; in the presence of gravity, they are replaced by the more general transformations of general relativity.

Fun fact

GPS satellites move at high speed, and their clocks tick slightly slower than those on Earth. Without taking the Lorentz transformations into account, the navigator would accumulate an error of several kilometers every day!

Concept graph →

Formulas

$$\Gamma = \frac{1}{\sqrt{1 - \beta^2}}$$
Factor relating time dilation and length contraction in relativity.
What is in the formula
ΓvariableLorentz factor — lorentz factor
βvariablespeed in units of c — velocity
\gamma=\frac{1}{\sqrt{1-β^2}} · 2606.27430
\gamma=\frac{1}{\sqrt{1-β^2}} · 2607.16104v1
$$\varepsilon''(\omega) = \frac{\omega_p^2 \gamma \omega}{(\omega_0^2 - \omega^2)^2 + \gamma^2 \omega^2}$$
Describes the frequency-dependent dielectric loss in resonant materials.
What is in the formula
ε''variableImaginary part of the dielectric function (dielectric loss) — dielectric function
ωvariableAngular frequency of the applied electromagnetic field — angular frequency radian per second
ω_0variableResonance angular frequency of the oscillator — angular frequency radian per second
γvariableDamping rate of the oscillator — angular frequency radian per second
ω_pvariablePlasma frequency, related to the density of oscillators — angular frequency radian per second
\frac{\varepsilon''(ν)}{ν}=\frac{sν_0^2\gammaν}{(ν^2-ν_0^2)^2+\gamma^2ν^2}+b(ν) · 2607.14764

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