Explore high-speed motion with precise energy estimates today. Switch inputs, solve for speed or mass. Built for students, engineers, and curious space thinkers everywhere.
Relativistic kinetic energy is computed from the Lorentz factor: γ = 1 / √(1 − β²), where β = v/c.
The kinetic energy is: K = (γ − 1) m c². This reduces to classical K ≈ ½mv² when v ≪ c.
If solving for speed from energy, use γ = 1 + K/(mc²) and v = c √(1 − 1/γ²).
| Case | Mass | Speed | β | γ | K (J) | K (MeV) |
|---|---|---|---|---|---|---|
| Electron, 0.50c | 9.109e-31 kg | 0.50 × c | 0.50 | 1.1547 | 1.27e-14 | 0.079 |
| Proton, 0.90c | 1.673e-27 kg | 0.90 × c | 0.90 | 2.2942 | 1.95e-10 | 1216 |
| 1 kg object, 1000 m/s | 1 kg | 1000 m/s | 3.34e-6 | 1.0000 | 5.00e+5 | 3.12e+18 |
Classical kinetic energy (½mv²) becomes inaccurate as speeds approach light speed. Relativistic kinetic energy grows with the Lorentz factor, so near‑light motion demands rapidly increasing energy. This explains why particle beams need huge energy for small speed gains at high β.
Enter mass (kg, g, or u) and speed (m/s, km/s, or as β = v/c), or switch modes to solve for speed from energy. The calculator converts to SI internally, then reports energy in J, kJ, and MJ, plus eV, MeV, and GeV for particle work.
γ rises slowly at first, then steeply: 0.50c → γ≈1.155, 0.90c → γ≈2.294, 0.99c → γ≈7.09, 0.999c → γ≈22.37. Since KE = (γ − 1)mc², kinetic energy tracks γ − 1 directly.
The outputs show KE, β, γ, and rest energy mc². A quick consistency check is KE/(mc²) = γ − 1. At 0.90c, γ − 1 ≈ 1.294, so the kinetic energy is about 129% of the rest energy.
An electron has rest energy about 0.511 MeV, so at 0.99c KE ≈ (7.09 − 1)×0.511 ≈ 3.1 MeV. A proton has rest energy about 938 MeV, giving KE ≈ (7.09 − 1)×938 ≈ 5.7 GeV. These estimates help sanity‑check accelerator or cosmic‑ray problems.
For everyday motion, β is tiny and γ≈1. A 1 kg object at 1000 m/s has β≈3.3×10⁻⁶, so relativistic KE≈5×10⁵ J, essentially the same as ½mv². The difference becomes noticeable only when v is a significant fraction of c.
Physics requires 0 ≤ v < c. As β → 1, γ can become very large, so outputs may jump quickly with small input changes. Entering β directly helps reduce unit mistakes.
Use CSV to collect multiple runs in a spreadsheet and compare how KE changes with β. Use PDF to save a clean record of a single scenario for homework, lab notes, or documentation. Exported rows include KE, β, γ, mc², and unit conversions for quick auditing. This supports consistent comparisons across runs easily.
Total energy is E = γmc². Relativistic kinetic energy is KE = E − mc² = (γ − 1)mc². The calculator reports kinetic energy and also shows the rest energy mc².
Because γ = 1/√(1 − β²) diverges as β → 1. Each extra increment in speed demands a much larger increase in energy, which is why v cannot reach c for massive objects.
If β is small (for example, below about 0.01), then γ is extremely close to 1 and relativistic kinetic energy matches the classical value to a very good approximation.
Yes. The tool uses γ = 1 + KE/(mc²) and then solves v = c√(1 − 1/γ²). This is useful when energy is reported in MeV/GeV and you want the corresponding speed.
In particle physics, energies are commonly quoted in electronvolts. Converting Joules to eV, MeV, and GeV makes it easy to compare your result with accelerator beam energies, decay energies, and rest energies of common particles.
You can use kilograms directly, or choose atomic mass units for particle-scale problems. For reference checks, an electron’s rest energy is about 0.511 MeV and a proton’s is about 938 MeV.
The calculator will flag invalid inputs because the formulas require v < c. If you are working with near-light speeds, enter a fraction of c (β) to avoid unit mistakes and reduce rounding issues.
Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.