Audited 31 Jul 2026·Last updated 15 Sept 2026·3 citations·Tier 2·0 uses

Electron Speed Calculator

Electron speed calculator: kinetic energy in eV to relativistic speed via γ = 1 + K/(mₑc²), v = c√(1 − 1/γ²) — exact at any energy.

Electron Speed Calculator

eV
Relativistic electron speed
5,930,099.2476
Result of γ = 1 + K/(m_ec²); v = c sqrt(1 - 1/γ²) using the entered coherent-SI magnitudes.
Model scope
Single free electron kinetic-energy conversion; fields, potential losses, binding energy, scattering, radiation, and velocity direction are outside it.

Background.

How fast is an electron with 100 eV of kinetic energy? Questions of this shape come up everywhere electrons are accelerated — vacuum tubes, electron guns, microscopes, X-ray sources, accelerators — and the honest answer must be relativistic, because electrons are so light that modest energies push them toward the speed of light. This page converts kinetic energy in electron volts to speed using the exact relations γ = 1 + K/(mₑc²) and v = c√(1 − 1/γ²).

The electron's rest energy mₑc² = 511 keV is the natural yardstick. Kinetic energy far below it (a few eV to a few keV) leaves γ barely above 1 and the classical v = √(2K/m) nearly right. Kinetic energy comparable to 511 keV bends the curve decisively: at K = 511 keV (γ = 2), speed is 86.6% of c, not the 141% the classical formula would absurdly claim. Beyond that, speed saturates — a 1 GeV electron moves at 99.999987% of c, gaining energy almost entirely as momentum and inertia rather than speed.

Using the exact formula everywhere costs nothing and removes the judgment call of “is my energy small enough to go classical?”. The crossover where the classical error reaches 1% sits near 7 keV — well inside the range of ordinary laboratory equipment: an electron microscope at 100–300 keV is thoroughly relativistic, and even an old CRT's 25 keV beam is off by 3.6% classically.

The conversion treats one free electron and its kinetic energy alone. How the electron got that energy — through what fields, with what losses — and what it subsequently hits are separate questions, as the scope note beside the result records.

What is electron speed calculator?

This is the exact special-relativity conversion from an electron's kinetic energy to its speed. Kinetic energy defines the Lorentz factor, γ = 1 + K/(mₑc²) — total energy over rest energy — and the factor fixes speed through v = c√(1 − 1/γ²). The electron rest energy mₑc² is 511 keV (8.187×10⁻¹⁴ J). Because the formula is exact, it is equally valid for a 1 eV photoelectron and a multi-GeV beam electron; it reduces smoothly to the classical √(2K/m) when K ≪ 511 keV.

How to use this calculator.

  1. Enter the electron's kinetic energy in electron volts — for an electron accelerated from rest through U volts, that is numerically U.
  2. Read the speed in m/s; dividing by c = 2.998×10⁸ gives the fraction of light speed, often the more informative number.
  3. Judge the regime from that fraction: below ≈0.1c classical formulas would have been fine; above it, the relativistic treatment you just used was necessary.
  4. For momentum — what electron optics and diffraction actually respond to — compute p = γmₑv with the same γ rather than mₑv.
  5. Do not extrapolate to other particles by scaling: a proton's rest energy is 938 MeV, so its classical-to-relativistic crossover sits three orders of magnitude higher in energy.

The formula.

γ = 1 + K/(m_ec²); v = c sqrt(1 - 1/γ²)

Relativity assigns a moving particle total energy E = γmₑc², so kinetic energy — total minus rest — is K = (γ − 1)mₑc². Solving for the Lorentz factor gives γ = 1 + K/(mₑc²): with K in eV and the rest energy 511 keV, the fraction is immediate. The factor's definition γ = 1/√(1 − v²/c²) then inverts to v = c√(1 − 1/γ²). The structure explains the saturation: as K grows, 1/γ² collapses toward zero and v creeps asymptotically toward c but never reaches it — the energy pours into γ (inertia and momentum) instead. Expanding for small K recovers ½mₑv² exactly, so there is no seam between regimes. Precision matters near the extremes: at high γ the subtraction 1 − 1/γ² loses digits in ordinary floating point, so the engine carries the whole chain — γ, the quotient, the root — in Decimal arithmetic and rounds once to twelve significant digits.

A worked example.

Example

Give an electron 100 eV — the gain from a 100 V gun, typical of electron-diffraction bench kits. First the Lorentz factor. The rest energy is 511,000 eV, so γ = 1 + 100/511,000 = 1.000 1957 — barely above one, which already announces a mildly relativistic particle at most. Then the speed: 1/γ² = 0.999 609, so v = c√(1 − 0.999 609) = c√(0.000 391) = c × 0.019 78 ≈ 5.93×10⁶ m/s — the engine's 5,930,099 m/s, just under 2% of light speed. Perspective on that “slow” result: it is nearly 6,000 km/s — Nairobi to London in one second — from a bench-top voltage, courtesy of the electron's minuscule inertia. The classical shortcut √(2K/m) here gives 5,930,970 m/s, only 0.015% high; but scale the energy up and the gap explodes — at 511 keV the classical formula exceeds light speed while the exact result is 0.866c. Same arithmetic, no seam: that is why the page always computes relativistically.

kinetic Energy Ev100

Frequently asked questions.

At what energy does an electron become ‘relativistic’?
There is no switch, only growing error in the classical formula: 0.1% high at about 700 eV, 1% at 7 keV, 3.6% at a CRT's 25 keV, and nonsense (v > c) beyond 511 keV. The practical rule is to compare kinetic energy with the 511 keV rest energy — within a few percent of it, relativity is mandatory — or simply to use the exact formula everywhere, as this page does, and never ask.
Why can't the electron reach the speed of light?
Because v = c√(1 − 1/γ²) reaches c only when γ becomes infinite, and γ grows in direct proportion to the energy supplied — an infinite energy bill. What acceleration actually buys at high energy is momentum and inertia: from 1 GeV to 10 GeV an electron's speed changes only in the seventh decimal of c, while its momentum grows tenfold. Accelerator physics is bookkeeping in energy and momentum, not speed.
Is 100 eV a lot for an electron?
Chemically, yes — it is several times any bond energy and seven times hydrogen's 13.6 eV ionisation energy, so a 100 eV electron ionises whatever it strikes; this is the working regime of electron-impact ion sources and old vacuum-tube physics. Relativistically, no — it is 0.02% of the rest energy, hence the modest 2% of c. The two senses of ‘energetic’ part company because chemistry's scale is eV while relativity's is half a million eV.
Does this apply to protons or ions?
The relations γ = 1 + K/(mc²) and v = c√(1 − 1/γ²) hold for any particle, but this page bakes in the electron's rest energy. A proton at the same kinetic energy is far slower and far less relativistic — its rest energy is 938 MeV, 1,836 times the electron's, so 100 eV moves it at only 138 km/s and classical mechanics remains excellent up to tens of MeV. For other species, substitute the appropriate rest energy before reusing the formulas.
What does the speed imply for electron microscopy?
Speed itself is not the goal — wavelength is. The de Broglie wavelength runs through momentum p = γmₑv, which this page's γ makes available: a 100 keV TEM electron (γ = 1.196, v = 0.548c) has λ = 3.70 pm, noticeably shorter than the 3.88 pm a classical calculation gives. Ignoring relativity in lens design at those voltages would misfocus the instrument — one of the quieter places special relativity does daily engineering work.

How this page was produced

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Method
γ = 1 + K/(m_ec²); v = c sqrt(1 - 1/γ²)
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