(455) HL Compton scattering [IB Physics HL]
Compton Scattering
Compton scattering demonstrates the wave-particle duality of photons.
Photons possess momentum without mass, represented by the equation: λ = H / P.
Key Experiment Overview
Named after Arthur Compton (1923) who investigated the scattering of photons by stationary electrons.
Light collides with an electron, causing it to move and altering the photon's wavelength.
Initial wavelength (BB_i) decreases while final wavelength (BB_f) increases, indicating a shift to a higher wavelength.
Significance of Observation
The increase in wavelength cannot be explained solely by wave theory, providing evidence for the particle nature of light.
Experiment Components
Incident photon with initial wavelength λ_i collides with a stationary electron.
After the collision, the photon is scattered at an angle θ resulting in a final wavelength λ_f.
Important Equation
Change in wavelength: Δλ = λ_f - λ_i = H / (m_e * c) * (1 - cos(θ))
H = Planck's constant (6.63 x 10^-34 J·s)
m_e = mass of the electron (9.11 x 10^-31 kg)
c = speed of light (3 x 10^8 m/s)
θ = scattering angle (in degrees)
Cosine Analysis
For θ = 0°: Δλ = 0 (no change in wavelength if angle is zero).
Example Calculation
Given: Incident wavelength (λ_i), scattered at θ = 90°
Rearranging the equation gives: λ_f = H / (m_e * c) * (1 - cos(θ)) + λ_i
With θ = 90°, cos(90°) = 0 ⇒ λ_f = H / (m_e * c) + λ_i.
Calculation Steps
Substitute constants into H / (m_e * c).
Ensure units are consistent (usually in meters or nanometers).
Perform calculations to find λ_f.
Conclusion of Example
λ_f determined to be approximately 5.5259 x 10^-12 m or 0.055 nanometers.
Wavelength increased from 0.31 nanometers to 0.055 nanometers, consistent with expectation.