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

De Broglie Wavelength Calculator

De Broglie wavelength calculator: λ = h/(mv). See why electrons diffract like waves while everyday objects never do, with the exact SI Planck constant.

De Broglie Wavelength Calculator

kg
m/s
De Broglie wavelength
0
Result of λ = h / (mv) using the entered coherent-SI magnitudes.
Model scope
Nonrelativistic momentum p = mv; use relativistic momentum when speed is not small compared with light speed, and do not substitute kinetic energy as momentum.

Background.

In 1924 Louis de Broglie proposed that everything that moves has a wavelength: λ = h/p, Planck's constant over momentum. Three years later Davisson and Germer scattered electrons off a nickel crystal and watched them diffract exactly as X-rays of that predicted wavelength would — matter really does interfere with itself. The proposal earned de Broglie the 1929 Nobel Prize and sits at the foundation of wave mechanics.

This page evaluates the nonrelativistic form λ = h/(mv) from a particle's mass and speed. Planck's constant has been exact by definition since the 2019 SI: h = 6.626 070 15×10⁻³⁴ J·s, so the only uncertainty in the result is the uncertainty in your inputs.

The formula explains a striking asymmetry in nature. An electron at a million metres per second carries so little momentum that its wavelength, 0.73 nm, is larger than an atom — comparable to crystal lattice spacings, which is why electron diffraction and electron microscopy work. A 0.145 kg baseball at 40 m/s has λ ≈ 1.1×10⁻³⁴ m, some twenty orders of magnitude below a proton's radius; no conceivable experiment resolves it, which is why baseballs travel in trajectories rather than interference patterns. Quantum behaviour is not switched off for large objects — it is merely scaled beyond all observability by h's smallness.

The nonrelativistic momentum p = mv underneath this page is accurate to about 1% up to roughly 14% of light speed (electrons of a few keV). Faster than that, relativistic momentum γmv is required — the scope note beside the result marks the boundary.

What is de broglie wavelength calculator?

The de Broglie wavelength is the wavelength of the quantum matter wave associated with any moving particle: λ = h/p, where h is Planck's constant and p the particle's momentum — in this nonrelativistic implementation, p = mv. It is not a metaphor: the wavelength predicts real interference fringes and diffraction angles, confirmed for electrons, neutrons, whole atoms, and molecules as large as C₆₀ and beyond. Because h ≈ 6.6×10⁻³⁴ J·s is so small, only microscopic momenta yield wavelengths large enough to detect.

How to use this calculator.

  1. Enter the particle's mass in kilograms — electron 9.109×10⁻³¹, proton 1.673×10⁻²⁷, neutron 1.675×10⁻²⁷ kg.
  2. Enter its speed in m/s; if you know kinetic energy instead, convert with v = √(2E/m) first — substituting energy for momentum directly is a dimensional error the page cannot catch for you.
  3. Check the relativity boundary before trusting the output: below ≈4×10⁷ m/s (≈14% of c) the nonrelativistic form stays within 1%.
  4. Compare the resulting λ with the feature size that would diffract it — crystal spacings run 0.2–0.5 nm — to judge whether wave behaviour is observable in your setup.
  5. For thermal neutrons or gas atoms, use the thermal speed for a first estimate: room-temperature neutrons near 2,200 m/s give λ ≈ 0.18 nm, matching lattice spacings — the basis of neutron diffraction.

The formula.

λ = h / (mv)

De Broglie's relation λ = h/p unifies two earlier surprises: Einstein's photon momentum p = h/λ (light behaving as particles) read in reverse (particles behaving as waves). With nonrelativistic momentum p = mv the page's form λ = h/(mv) follows. Wavelength shrinks inversely with both mass and speed — double either and the wavelength halves — which is the entire reason quantum effects vanish at everyday scales: h/(mv) with kilogram masses is smaller than any physically meaningful length. The relation is exact in the momentum form; what is approximate here is only p = mv, which understates true momentum as speed climbs (by 1% at 0.14c, by 15% at 0.5c). Electron microscopists exploit the inverse-speed scaling deliberately — accelerating electrons to shrink λ below atomic spacing is what gives a TEM its resolution. The engine divides the exact 2019-SI Planck constant by the mass-speed product in Decimal arithmetic, rounding once to twelve significant digits.

A worked example.

Example

How wavelike is a laboratory electron? Take the electron mass, 9.109×10⁻³¹ kg, moving at a million metres per second — the speed a bench-top gun of a few electron-volts produces. Momentum first: p = mv = 9.109×10⁻³¹ × 1×10⁶ = 9.109×10⁻²⁵ kg·m/s. Then the wavelength: λ = h/p = 6.626×10⁻³⁴ / 9.109×10⁻²⁵ ≈ 7.27×10⁻¹⁰ m — 0.73 nanometres. That number is the punchline: it is three times the spacing between nickel atoms (0.25 nm), so a crystal presents this electron with a diffraction grating matched to its wavelength — precisely the Davisson–Germer configuration that first proved matter waves exist. Scale check the other way: a thrown baseball (0.145 kg, 40 m/s) gives λ = 6.626×10⁻³⁴/5.8 ≈ 1.1×10⁻³⁴ m. The electron diffracts; the baseball, wavelength 10²⁵ times smaller than an atom, simply flies.

particle Mass Kg0
particle Speed Mps1,000,000

Frequently asked questions.

Does a baseball really have a wavelength?
Formally yes — λ = h/p applies to any momentum — but at 0.145 kg and 40 m/s it comes to about 1.1×10⁻³⁴ m, twenty orders of magnitude below a proton's size. No slit, crystal, or instrument can ever be built fine enough to reveal interference at that scale, so classical trajectories describe the ball perfectly. The formula is universal; the observability is not.
When do I need the relativistic version?
When speed stops being small against c = 3×10⁸ m/s. Nonrelativistic p = mv understates momentum by about 1% at 0.14c and the error compounds from there, so the true wavelength λ = h/(γmv) is shorter than this page reports. In practice: electrons beyond a few kilovolts of acceleration — including every electron microscope — need the relativistic form; a 100 keV TEM electron's real wavelength is 3.7 pm, not the 3.9 pm the classical formula suggests.
Why did electrons prove matter waves before anything else?
Because the electron's tiny mass makes its wavelength conveniently large: even modest speeds give λ comparable to crystal lattice spacings (0.2–0.5 nm), and crystals were the ready-made diffraction gratings of the 1920s. Heavier particles need to move absurdly slowly to match — a proton wants speeds a thousandfold lower for the same λ — which is why neutron diffraction waited for reactors producing slow thermal neutrons.
How does kinetic energy enter, since the formula only takes speed?
Through v = √(2E/m). A useful worked shortcut for electrons: accelerating through U volts gives λ ≈ 1.226/√U nanometres nonrelativistically — 150 V yields 0.1 nm, atomic scale. The trap the scope note warns about is substituting energy where momentum belongs: λ = h/E is dimensionally wrong for matter (it happens to work for photons only because E = pc there).
Has matter-wave interference been shown for anything bigger than electrons?
Extensively. Neutron and whole-atom interferometry are standard laboratory tools; C₆₀ buckyballs (720 atomic mass units) showed textbook fringes in 1999, and Vienna experiments have since interfered custom molecules beyond 25,000 amu. Each step up in mass demands slower beams and finer gratings, exactly as λ = h/(mv) dictates — the boundary is technological, with no fundamental cutoff yet observed.

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λ = h / (mv)
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