Formula and Method for Compton Scattering
Compton scattering describes what happens when a photon collides with a free (or loosely bound) electron: the photon transfers part of its energy and momentum to the electron and scatters off at an angle θ with a longer wavelength — and therefore lower energy — than it had going in. Applying conservation of energy and momentum to this photon-electron collision gives the Compton scattering formula: Δλ = λ' − λ = (h / mₑc)(1 − cos θ), where h is Planck's constant, mₑ is the electron's rest mass, c is the speed of light, and θ is the angle between the incoming and scattered photon directions. This calculator applies that formula to find the wavelength shift, the scattered wavelength, and how the lost photon energy splits off as kinetic energy for the recoiling electron.
How the calculation works
Enter the incident photon's wavelength λ and the scattering angle θ. The calculator first evaluates the Compton wavelength of the electron, λ_C = h / (mₑc) ≈ 2.42631 pm, a fixed quantity built from fundamental constants. The wavelength shift is Δλ = λ_C(1 − cos θ), which is added to the incident wavelength to get the scattered wavelength, λ' = λ + Δλ. Photon energy follows from E = hc/λ (and E' = hc/λ' for the scattered photon); by conservation of energy, the kinetic energy transferred to the recoiling electron is KE = E − E'.
Common mistakes
- Ignoring the scale: the Compton shift is at most a few picometers, so it's negligible next to visible light (~500 nm) but significant for X-rays and gamma rays (~10-100 pm), which is why Compton's original 1923 experiment used X-rays.
- Mixing degrees and radians: θ in the formula is an angle, not a slope — this calculator takes θ in degrees (0° to 180°) and converts to radians internally before applying cos θ.
- Confusing scattering mechanisms: Compton scattering is inelastic (the photon loses energy), unlike classical Thomson scattering, which is elastic and only valid when the photon energy is much smaller than the electron's rest-mass energy (511 keV).
Real-world applications
- Compton scattering is one of the three dominant photon-matter interactions (with the photoelectric effect and pair production) and is a core input to radiation shielding design and medical dosimetry calculations.
- Compton cameras used in gamma-ray astronomy and nuclear medicine imaging (such as SPECT) reconstruct where a gamma photon came from by measuring its scattering angle and energy loss in a detector.
- The 1923 experiment that confirmed this effect — for which Arthur Compton won the 1927 Nobel Prize in Physics — was direct evidence that light carries momentum as discrete photons, not just as a wave.