concept

proper time

Proper time is the time measured by a clock following a specific worldline in spacetime, invariant under Lorentz transformations.
19 related articles · 5 formulas · 2 who worked here

Description

Proper time is an invariant quantity that does not depend on the reference frame. It equals the time measured by a clock moving with the object. For a stationary observer, the time of such an object runs slower, and the effect is stronger the higher the speed or the closer a massive body. In everyday life, the slowing is imperceptible, but it is detected by precise atomic clocks.

History

The concept of local time appeared in the works of Hendrik Lorentz (1895) and Henri Poincaré (1900) as an auxiliary quantity for electrodynamics. In 1905, Albert Einstein gave it fundamental status in special relativity, and Hermann Minkowski geometrized it as world line length in 1908. In 1915, in general relativity, proper time became the basis for describing gravity. Experimental confirmations were obtained in the Hafele–Keating experiments with atomic clocks (1971).

How it works

In special relativity, proper time τ is related to coordinate time t by dτ = dt √(1 – v²/c²). As v → c, proper time slows sharply. In general relativity, the metric tensor is used: dτ² = –g₀₀ dt², for example, in the exterior Schwarzschild solution g₀₀ = –(1 – rₛ/r), and as r → rₛ (event horizon), proper time tends to zero. Time dilation for moving particles is confirmed by the lifetime of muons in the atmosphere.

In practice

Without correction for the difference in proper time between GPS satellites and ground clocks, navigation error would accumulate to 10 km per day.

Fun fact

An astronaut who spends six months on the International Space Station ages 0.005 seconds less than his peers on Earth.

Concept graph →

Formulas

$$\tau = \int_{0}^{\infty} C(t) \, dt$$
The correlation time equals the integral of the autocorrelation function.
What is in the formula
\tauvariableintegral autocorrelation time — autocorrelation time second
C(t)variableautocorrelation function — autocorrelation function
tvariabletime lag — time second
\int_{0}^{\infty}operatorintegration from zero to infinity — definite integral
τ_{γ}=\int_{0}^{\infty}c_{γ}(t)dt · 2606.31185
$$t_E = \frac{\theta_E}{\mu}$$
Time to cross the Einstein radius at relative proper motion.
What is in the formula
t_EvariableEinstein crossing time — time second
\theta_EvariableAngular radius of the Einstein ring — einstein radius angle radian
\muvariableRelative proper motion between lens and source — angular velocity radian per second
t_{\rme}=θ_{\rme}/μ · 2607.04594v1
$$d\tau = \frac{dr}{\sqrt{f(r)}}$$
Increment of proper time for radial motion in curved spacetime.
What is in the formula
τvariableProper time — proper time second
rvariableRadial coordinate — radial coordinate metre
f(r)variableMetric function — metric function
doperatorInfinitesimal change — differential
dτ=\frac{dr^2}{σ^2f(r)} · 2607.14626
$$f(r) = 1 - \frac{2GM}{c^2 r} + \frac{G k_e Q^2}{c^4 r^2}$$
Describes spacetime around a charged non-rotating mass.
What is in the formula
rvariableRadial coordinate from the center — radial distance metre
f(r)variableMetric function determining spacetime geometry — metric function
GconstantNewtonian constant of gravitation — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared
cconstantSpeed of light in vacuum — speed of light = 299792458 metre per second
k_econstantElectrostatic force constant in Coulomb's law — coulomb constant = 8.9875517923e9 newton metre squared per coulomb squared
f(r)=1-\frac{2gm}{c^2r}+\frac{gk_eq^2}{c^4r^2} · 2605.10587v1
$$\frac{D^2 \xi^\mu}{d\tau^2} = -R^\mu{}_{\nu\rho\sigma} u^\nu u^\rho \xi^\sigma$$
Gravitational waves cause relative acceleration between test masses.
What is in the formula
ξ^μvariabledeviation vector between two nearby geodesics — geodesic deviation vector metre
τvariableproper time along the geodesic — proper time second
u^νvariablefour-velocity of the geodesic — four velocity
u^ρvariablefour-velocity of the geodesic (repeated index) — four velocity
ξ^σvariabledeviation vector (repeated index) — geodesic deviation vector metre
D^2/dτ^2operatorsecond covariant derivative along the geodesic — covariant second derivative

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