Compton Scattering: A Shallow-Angle Comparison
1 · Predict
At small scattering angles, a photon barely changes direction. Does its wavelength shift also become vanishingly small as the angle approaches zero?
- Yes — as θ → 0°, (1 − cos θ) → 0, so the wavelength shift vanishes for a photon that barely scatters.
- The shift stays roughly constant even at small angles.
- The shift actually grows larger at small angles.
2 · Set Up
- Open the compton-45 preset and press Reset. The incident X-ray wavelength is 0.08 nm; the scattering angle is fixed at 45°.
- Enable the wavelength-shift readout.
- Set the scattering angle for each trial (small angles) and record the wavelength shift.
3 · Collect Data
| Scattering angle θ (°) | Wavelength shift Δλ (pm) |
|---|---|
| 15 | |
| 30 | |
| 45 |
Plot Δλ (y-axis) against scattering angle θ (x-axis) for your three trials.
4 · Analyze
- For one trial, compute Δλ = (h/(m_ec))(1 − cos θ). Compare to the table. Confirm the shift shrinks as θ decreases.
- Explain why a nearly-undeflected photon (small θ) transfers very little momentum to the electron, and therefore loses very little energy — hence the tiny wavelength shift.
5 · Extend
- Unlike this experiment's incident wavelength (0.08 nm, different from compton-90's 0.05 nm), the wavelength SHIFT Δλ at any given angle would be identical between the two experiments. Explain why the Compton formula makes the shift independent of the incoming photon's wavelength.
- At very small angles, Δλ becomes hard to measure experimentally against the (much larger) incident wavelength. Explain why Compton scattering experiments typically use short-wavelength X-rays rather than visible light, where an already-tiny picometer-scale shift would be even less noticeable.
The Physics Behind This Experiment
Compton Shift at Small Angles
As θ → 0°, (1 − cos θ) → 0, so Δλ → 0: a photon that barely changes direction barely loses energy, consistent with momentum conservation for a nearly-undisturbed collision.