This calculator works out the de Broglie wavelength of a moving particle, the wave-like property every piece of matter carries alongside its familiar particle behaviour. You choose a particle type, electron, proton, neutron or alpha particle, or enter a custom mass, then enter a velocity in metres per second, with preset speeds available for common cases such as a thermal electron, a Bohr-model electron or a thermal neutron. Using the relation lambda equals h divided by mass times velocity, the calculator returns the wavelength in nanometres and picometres, the particle's momentum in kilogram metres per second, and its kinetic energy in electron volts. A breakdown panel shows the mass, velocity and momentum used, plus a check on what fraction of the speed of light your velocity represents, confirming whether the non-relativistic approximation still applies. A comparison table also shows how the wavelength changes across a range of velocities for the same particle, so you can see wavelength shrink as speed rises. This suits physics students working through wave-particle duality problems, and anyone curious why electrons show measurable diffraction, the basis of electron microscopy, while thrown balls never do. The formula used is the standard non-relativistic one, accurate for speeds well below light speed; above roughly ten percent of light speed, a relativistic calculation gives a shorter, more accurate wavelength than shown here.
| Velocity (m/s) | Momentum (kg m/s) | Wavelength (nm) | Wavelength (pm) |
|---|
In 1924, French physicist Louis de Broglie proposed that all matter has wave-like properties, not just light. He suggested that any moving particle has an associated wavelength, now called the de Broglie wavelength, given by lambda = h / p, where h is Planck's constant and p is the particle's momentum. This idea extended wave-particle duality (already established for light) to matter, and was confirmed experimentally in 1927 when electron diffraction patterns were observed, exactly as de Broglie's equation predicted.
The wavelength is calculated as:
lambda = h / p = h / (m x v)
This calculator uses the non-relativistic form p = m x v, which is accurate for velocities well below the speed of light (roughly under 10% of c, or about 3 x 10⁷ m/s). At higher speeds, momentum must be calculated relativistically, and this simple form under-estimates momentum, giving a wavelength that is too long.
| Particle | Rest Mass (kg) | Notes |
|---|---|---|
| Electron | 9.1093837015 x 10⁻³¹ | Lightest common charged particle; shows large, easily measured wavelengths |
| Proton | 1.67262192369 x 10⁻²⁷ | About 1,836 times heavier than an electron |
| Neutron | 1.67492749804 x 10⁻²⁷ | Slightly heavier than a proton; used in neutron diffraction studies |
| Alpha particle (helium-4 nucleus) | 6.6446573357 x 10⁻²⁷ | Two protons and two neutrons bound together |
Because electrons have a much smaller mass than atoms or everyday objects, they can be accelerated to speeds where their de Broglie wavelength is comparable to atomic spacings (roughly 0.01 to 1 nanometre). This is the basis of electron microscopy, which achieves far higher resolution than light microscopy because the electron wavelength is thousands of times shorter than visible light wavelengths (400 to 700 nm). Electron diffraction, first demonstrated by Davisson and Germer in 1927, provided the first direct experimental proof of de Broglie's hypothesis.
An electron (mass 9.10938 x 10⁻³¹ kg) travelling at 1,000,000 m/s has momentum p = m x v = 9.10938 x 10⁻³¹ x 1,000,000 = 9.10938 x 10⁻²⁵ kg m/s. Its de Broglie wavelength is lambda = h / p = 6.62607015 x 10⁻³⁴ / 9.10938 x 10⁻²⁵ ≈ 7.274 x 10⁻¹⁰ m, or about 0.727 nm (727.4 pm). Its kinetic energy is 1/2 x m x v² ≈ 4.555 x 10⁻¹⁹ J, or about 2.84 eV.
This calculator uses the classical (non-relativistic) momentum formula p = m x v. For particles travelling at a significant fraction of the speed of light (typically above about 10% of c), relativistic momentum must be used instead, and the wavelength calculated here will be slightly longer than the true relativistic value. For most textbook problems involving electrons, protons and neutrons at laboratory speeds, the non-relativistic approximation is accurate to within a fraction of a percent.
Sources: CODATA 2018 recommended values for physical constants (physics.nist.gov/cuu/Constants). De Broglie, L. (1924), original hypothesis on wave-particle duality. Davisson, C. and Germer, L. (1927), experimental confirmation of electron diffraction, Physical Review.
This calculator uses the standard non-relativistic de Broglie relation (lambda = h / (m x v)), suitable for typical physics coursework involving electrons, protons, neutrons and similar particles at speeds well below the speed of light. For particles approaching relativistic speeds, a relativistic momentum calculation is required for an accurate result.
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