Students will be able to:
A photon is a mass‑less quantum of electromagnetic radiation. Its energy is directly proportional to its frequency:
E = h ν
6.626 × 10⁻³⁴ J sEven though a photon has no rest mass, it carries linear momentum:
p = h/λ = E/c
2.998 × 10⁸ m s⁻¹1 eV = 1.602 × 10⁻¹⁹ J. Converting between joules and eV is useful when dealing with atomic‑scale processes.
In the photo‑electric effect a photon can liberate an electron from a metal only if its energy exceeds the metal’s work function (ϕ). The minimum frequency required is called the threshold frequency (ν0); the corresponding wavelength is the threshold wavelength (λ0).
ν0 = ϕ / h
λ0 = c / ν0 = hc / ϕ
When photons are absorbed or reflected they transfer momentum to a surface, producing a pressure:
P = I / c (absorbing surface)
P = 2I / c (reflecting surface)
| Observation | Interpretation |
|---|---|
| Current appears instantly when light shines on a metal. | Energy is delivered in discrete packets (photons) rather than by a wave‑like heating process. |
| No current if the light frequency is below a certain value, no matter how intense. | A minimum photon energy (the work function) is required → defines ν0 and λ0. |
| Maximum kinetic energy of emitted electrons increases linearly with frequency. | Kmax = h(ν – ν0) – quantitative confirmation of the photon model. |
Problem: The work function of sodium is 2.28 eV. Calculate the threshold frequency (ν0) and threshold wavelength (λ0) for sodium.
Solution:
ϕ = 2.28 eV × 1.602 × 10⁻¹⁹ J eV⁻¹ = 3.65 × 10⁻¹⁹ J.
ν0 = ϕ / h = (3.65 × 10⁻¹⁹ J) / (6.626 × 10⁻³⁴ J s) ≈ 5.5 × 10¹⁴ Hz.
λ0 = c / ν0 = (2.998 × 10⁸ m s⁻¹) / (5.5 × 10¹⁴ Hz) ≈ 5.5 × 10⁻⁷ m = 550 nm.
Thus visible light with wavelength shorter than 550 nm (e.g., blue or ultraviolet) can cause photo‑emission from sodium, whereas longer wavelengths cannot.
| Region | λ (nm) | E (J) | E (eV) |
|---|---|---|---|
| Radio | 10⁶ – 10⁹ | 10⁻²⁸ – 10⁻²⁴ | 10⁻⁹ – 10⁻⁵ |
| Microwave | 1 mm – 1 cm | 10⁻²⁴ – 10⁻²² | 10⁻⁵ – 10⁻³ |
| Infrared | 700 – 10⁴ | 10⁻²² – 10⁻²⁰ | 10⁻³ – 0.1 |
| Visible | 400 – 700 | 2.8 × 10⁻¹⁹ – 5.0 × 10⁻¹⁹ | 1.8 – 3.1 |
| Ultraviolet | 10 – 400 | 5 × 10⁻¹⁹ – 2 × 10⁻¹⁷ | 3 – 124 |
| X‑ray | 0.01 – 10 | 2 × 10⁻¹⁶ – 2 × 10⁻¹⁴ | 124 – 12 400 |
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