Home / IBDP Physics- E.2 Quantum physics- IB Style Questions For HL Paper 2

IBDP Physics- E.2 Quantum physics- IB Style Questions For HL Paper 2 -FA 2025

Question

(a) Explain why Compton scattering provides stronger evidence for the particle nature of light than does the photoelectric effect.
A photon with wavelength \(6.40\times10^{-12}\,m\) and energy \(0.194\,MeV\) strikes an electron that is initially at rest. After the interaction, the photon is scattered through an angle \(\theta\) and emerges with a wavelength of \(7.47\times10^{-12}\,m\). The electron recoils as a result of the collision.
(b) Explain why the wavelength of the photon after scattering is greater than the wavelength of the incident photon.
(c) (i) Show that the energy of the scattered photon is approximately \(0.17\,MeV\).
(ii) Calculate the kinetic energy of the recoiling electron.
(iii) For an electron, \(\frac{h}{m_{e}c}=2.43\times10^{-12}\,m\). Determine the value of \(\theta\).

Most-appropriate topic codes (IB Physics):

Topic E.2: Quantum physics (Compton scattering) — part (a), (b), (c)
▶️ Answer/Explanation
Detailed solution

(a)
In Compton scattering, a photon collides with an electron and the interaction can be treated as a particle-like collision in which momentum is exchanged. The measurable change in the photon’s wavelength (and hence momentum) is direct evidence of photon momentum.
The photoelectric effect shows that light energy is quantized, but it does not as directly demonstrate a momentum-exchange “collision” between light and a particle.

(b)
During the scattering, the photon transfers some of its energy to the electron (the electron gains kinetic energy). The scattered photon therefore has lower energy than the incident photon. Since \(E=\frac{hc}{\lambda}\), a decrease in photon energy implies an increase in wavelength, so the scattered wavelength is longer.

(c)
(i)
Using \(E=\frac{hc}{\lambda}\) and \(hc \approx 1.24\times10^{-6}\,eV\,m\):
\(E_s=\frac{1.24\times10^{-6}}{7.47\times10^{-12}}\,eV \approx 1.66\times10^{5}\,eV = 0.166\,MeV \approx 0.17\,MeV.\)

(ii)
By energy conservation (electron initially at rest):
\(K_e = E_i – E_s = 0.194\,MeV – 0.166\,MeV = 0.028\,MeV.\)

(iii)
Compton shift: \(\Delta\lambda=\lambda_s-\lambda_i=\frac{h}{m_ec}(1-\cos\theta)\).
\(\Delta\lambda=(7.47-6.40)\times10^{-12}\,m = 1.07\times10^{-12}\,m.\)
\(1.07\times10^{-12} = (2.43\times10^{-12})(1-\cos\theta)\)
\(1-\cos\theta = \frac{1.07}{2.43}\approx 0.44\)
\(\cos\theta \approx 0.56 \Rightarrow \theta \approx 56^\circ\) (about \(0.98\,rad\)).

Scroll to Top