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  1. Home
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  4. /Lorentz Factor Calculator

Lorentz Factor Calculator

Last updated: March 18, 2026

Calculator

Results

Lorentz Factor (γ)

1.3423847

β = v/c

0.6671281904

Velocity

200,000,000

m/s

β²

0.4450600224

1/γ

0.74494294

γ − 1

0.3423847

Moving Clock Rate

0.74494294

Time Dilation Increase

34.2385

%

Length Contraction

25.5057

%

Results

Lorentz Factor (γ)

1.3423847

β = v/c

0.6671281904

Velocity

200,000,000

m/s

β²

0.4450600224

1/γ

0.74494294

γ − 1

0.3423847

Moving Clock Rate

0.74494294

Time Dilation Increase

34.2385

%

Length Contraction

25.5057

%

The Lorentz Factor Calculator computes the central quantity of special relativity — the Lorentz factor $$\gamma = \frac{1}{\sqrt{1 - \beta^2}} = \frac{1}{\sqrt{1 - v^2/c^2}}$$ along with all the derived relativistic effects: time dilation percentage, length contraction percentage, and the kinetic energy factor. The Lorentz factor γ appears in virtually every equation of special relativity and determines the magnitude of all relativistic effects.

At rest (v = 0), γ = 1 and there are no relativistic effects. As velocity increases toward c, γ grows from 1 toward infinity, and relativistic effects become increasingly pronounced. This calculator provides a comprehensive overview of how γ and its related quantities vary with velocity, making it an essential reference tool for physics students and researchers.

Visual Analysis

How It Works

The Lorentz factor is defined as:

$$\gamma = \frac{1}{\sqrt{1 - \beta^2}}$$

where $$\beta = v/c$$ is the velocity expressed as a fraction of the speed of light. The Lorentz factor appears throughout special relativity:

  • Time dilation: $$t = \gamma t_0$$ — moving clocks run slow by factor γ. The percentage shown is $$(\gamma - 1) \times 100\%$$.
  • Length contraction: $$L = L_0/\gamma$$ — moving objects are shortened by factor 1/γ. The percentage is $$(1 - 1/\gamma) \times 100\%$$.
  • Relativistic momentum: $$p = \gamma m_0 v$$.
  • Relativistic energy: $$E = \gamma m_0 c^2$$, with kinetic energy $$KE = (\gamma - 1)m_0 c^2$$.
  • Lorentz transformation: $$x' = \gamma(x - vt)$$, $$t' = \gamma(t - vx/c^2)$$.

Behavior of γ at notable velocities:

β (v/c)γTime DilationLength Contraction
0.0011.0000005~0.00005%~0.00005%
0.11.005040.5%0.5%
0.51.154715.5%13.4%
0.8662.0100%50%
0.92.294129%56.4%
0.997.089609%85.9%
0.99922.372137%95.5%
0.999970.716971%98.6%

The γ − 1 value is particularly useful because it directly gives the kinetic energy as a multiple of rest energy: $$KE = (\gamma - 1) m_0 c^2$$. When γ − 1 = 1, the kinetic energy equals the rest energy. For ultra-relativistic particles (γ ≫ 1), almost all the energy is kinetic.

For very small velocities, computing γ directly from $$1/\sqrt{1-\beta^2}$$ can suffer from floating-point precision loss. In such cases, the Taylor expansion $$\gamma \approx 1 + \beta^2/2 + 3\beta^4/8$$ gives better numerical precision.

Understanding Your Results

The Lorentz factor γ is the master parameter of special relativity. γ = 1 means no relativistic effects; γ = 2 means time runs at half speed and lengths are halved; γ = 10 means time runs at 1/10 speed and lengths shrink to 10% of their rest values. The time dilation percentage shows how much extra time a stationary observer measures (e.g., 100% means double the proper time). The length contraction percentage shows how much shorter a moving object appears (e.g., 50% means half the rest length).

Worked Examples

International Space Station Orbital Speed

Inputs

velocity7660
input modevelocity

Results

gamma1.000000000327
beta0.00002555
velocity ms7660
one over gamma0.999999999673
gamma minus 13.27e-10
time dilation pct3.27e-8
length contraction pct3.27e-8
beta squared6.53e-10

At ISS orbital velocity (7.66 km/s), γ exceeds 1 by only 3.3 × 10⁻¹⁰ — astronauts age about 0.01 seconds less per year than people on Earth (ignoring gravitational effects).

Ultra-Relativistic Particle (γ = 1000)

Inputs

beta input0.9999995
input modebeta

Results

gamma1000
beta0.9999995
velocity ms299792308
one over gamma0.001
gamma minus 1999
time dilation pct99900
length contraction pct99.9
beta squared0.999999

At γ = 1000, time dilates by a factor of 1000 — one second of proper time corresponds to ~17 minutes for a stationary observer. Length contracts to 0.1% of rest length.

Frequently Asked Questions

The Lorentz factor $$\gamma = 1/\sqrt{1 - v^2/c^2}$$ is a dimensionless quantity that appears in all equations of special relativity. It ranges from 1 (at rest) to infinity (at the speed of light) and determines the magnitude of time dilation, length contraction, and the relationship between energy and momentum.

Beta $$\beta = v/c$$ is the velocity expressed as a fraction of the speed of light. It ranges from 0 (at rest) to 1 (at light speed, for massless particles). Using β simplifies many relativistic formulas and makes it easy to compare velocities to c. The Lorentz factor is $$\gamma = (1 - \beta^2)^{-1/2}$$.

Setting $$\gamma = 2$$ and solving: $$2 = 1/\sqrt{1-\beta^2}$$ gives $$\beta = \sqrt{3}/2 \approx 0.866$$. At about 86.6% of the speed of light, time runs at half speed, lengths contract by half, and momentum is double the classical value.

Time dilation: $$t = \gamma t_0$$ (multiply proper time by γ). Length contraction: $$L = L_0/\gamma$$ (divide proper length by γ). Time stretches by factor γ while length shrinks by factor 1/γ. Both effects have the same underlying cause: the geometry of Minkowski spacetime.

The quantity $$\gamma - 1$$ is the kinetic energy factor: $$KE = (\gamma - 1)m_0c^2$$. When $$\gamma - 1 = 1$$, the kinetic energy equals the rest energy. For a proton, this occurs at about 0.866c. The LHC achieves $$\gamma - 1 \approx 7000$$ for protons.

No. Since $$0 \leq \beta < 1$$ for massive particles, the term $$1 - \beta^2$$ is between 0 and 1, so its square root is also between 0 and 1, and the reciprocal $$\gamma$$ is always ≥ 1. A γ < 1 would require $$v > c$$, which is physically impossible for massive objects.

Sources & Methodology

Lorentz, H.A. (1904). Electromagnetic Phenomena in a System Moving with Any Velocity Less Than That of Light. Proceedings of the Royal Netherlands Academy. Einstein, A. (1905). On the Electrodynamics of Moving Bodies. Annalen der Physik. Taylor, E.F. & Wheeler, J.A. (1992). Spacetime Physics, 2nd Ed. W.H. Freeman.
R

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