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
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.
- Enter the particle's mass in kilograms — electron 9.109×10⁻³¹, proton 1.673×10⁻²⁷, neutron 1.675×10⁻²⁷ kg.
- 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.
- Check the relativity boundary before trusting the output: below ≈4×10⁷ m/s (≈14% of c) the nonrelativistic form stays within 1%.
- 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.
- 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.
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.
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.
Frequently asked questions.
Does a baseball really have a wavelength?
When do I need the relativistic version?
Why did electrons prove matter waves before anything else?
How does kinetic energy enter, since the formula only takes speed?
Has matter-wave interference been shown for anything bigger than electrons?
References& sources.
How this page was produced
- Published by
- Quanta Calculator
- Primary sources
- 3 cited below
- Method
- λ = h / (mv)
- Published
- Last verified
Built with AI assistance and verified by automated tests against the cited sources — every worked example on this page is computed by the same code that runs the calculator. How we build and check calculators.
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