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Relativistic Time Dilation Calculator

Calculate how moving clocks run slow by finding the Lorentz factor and the dilated time for a given velocity.
As fraction of c (β) or in m/s

Velocity unit

s

Time measured in the moving frame
Lorentz factor γ
2,294157

Dilated time = γ × proper time

Dilated time Δt
2,294157 s
Time gained Δt − Δt₀
1,294157 s
Speed (fraction of c)
0,9
Nopeus
269 813 212,2 m/s
Lorentz factor γ vs v/c (0 to 0.999)
Step by step
  1. 1

    1 − β²

    1 − 0,9² = 0,19
  2. 2

    √(1 − β²)

    √0,19 = 0,43588989
  3. 3

    Lorentz factor γ = 1 ÷ √(1 − β²)

    1 ÷ 0,43588989 = 2,294157
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Relativistic time dilation makes moving clocks run slow. The Lorentz factor γ = 1/√(1 − v²/c²) multiplies the proper time Δt₀ to give the observed time Δt = γ·Δt₀. Enter a velocity (in m/s or as a fraction of light speed) below c to get γ, the dilated time, and the extra time gained.

Kaava
γ = 1 / √(1 − v²/c²), Δt = γ · Δt₀
How this is calculated

Enter the velocity v of the moving object and the proper time Δt₀ (the time interval measured by a clock at rest in the moving frame). The velocity can be given directly in meters per second or as a fraction of the speed of light c = 2.99792458×10⁸ m/s using the unit selector; in the latter case v = β·c where β is the chosen fraction.

The Lorentz factor is γ = 1/√(1 − v²/c²). Because Δt = γ·Δt₀ and γ ≥ 1, the elapsed time observed in a frame relative to which the clock moves is always longer than the proper time — moving clocks tick slow. The time gained is simply Δt − Δt₀, which grows without bound as v approaches c.

The calculator requires v < c (|β| < 1); at or above light speed the square root becomes zero or imaginary and γ diverges, so no finite result is returned. At everyday speeds β is tiny and γ ≈ 1, making dilation negligible, while near β = 0.999 the factor blows up dramatically, as shown in the γ-versus-v/c curve.

Usein kysytyt kysymykset

The Lorentz factor γ = 1/√(1 − v²/c²) quantifies relativistic effects. It equals 1 at rest and increases toward infinity as the speed approaches that of light, scaling time, length, and relativistic mass.

For v ≥ c the term 1 − v²/c² becomes zero or negative, so √(1 − v²/c²) is zero or imaginary and γ is undefined. Massive objects cannot reach c, so the model only applies for v < c.

Longer. Since γ ≥ 1, the dilated time Δt = γ·Δt₀ is always at least the proper time, meaning a moving clock appears to run slow compared with a stationary observer.

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lorentzin kerroin
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APA

TG we-Calculate Editorial Team. (2026). Relativistic Time Dilation Calculator [Online calculator]. TG we-Calculate. https://we-calculate.com/fi/calculator/time-dilation-calculator

Chicago

TG we-Calculate Editorial Team. "Relativistic Time Dilation Calculator." TG we-Calculate. 2026. https://we-calculate.com/fi/calculator/time-dilation-calculator.

IEEE

TG we-Calculate Editorial Team, "Relativistic Time Dilation Calculator," TG we-Calculate, 2026. [Online]. Available: https://we-calculate.com/fi/calculator/time-dilation-calculator

BibTeX

@misc{wecalculate_time_dilation_calculator, title = {Relativistic Time Dilation Calculator}, author = {{TG we-Calculate Editorial Team}}, howpublished = {\url{https://we-calculate.com/fi/calculator/time-dilation-calculator}}, year = {2026}, note = {TG we-Calculate} }

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