Dawn of Modern Physics
Classical physics treated light purely as a wave. In 1900 Planck showed that radiation is emitted and absorbed in discrete packets of energy, and modern physics began. The PMDC MDCAT 2026 syllabus reduces this whole chapter to a single subtopic — "Quantum Theory and Radiation" — with one learning outcome: explain the particle model of light in terms of photons with energy.
Quantum Theory and Radiation
Quantum theory says that electromagnetic radiation is not a continuous stream of energy. It comes in indivisible packets called quanta, and a single quantum of light is called a photon. This is the particle model of light.
Planck's quantum hypothesis (1900)
Planck proposed that radiation is emitted and absorbed only in discrete packets, each carrying an energy fixed by the frequency of the radiation:
E = hf = hc/λ
where h = 6.626 × 10−34 J s is Planck's constant, c = 3.0 × 108 m s−1, f is the frequency and λ the wavelength. This one equation is the foundation of quantum theory and is the most-tested relation in the chapter.
The photon
A photon is one quantum of electromagnetic radiation — the "particle" of light. Its properties:
- Energy E = hf = hc/λ. Energy is directly proportional to frequency and inversely proportional to wavelength, so gamma rays carry far more energy per photon than radio waves.
- Zero rest mass, no electric charge, and it always travels at the speed of light c in vacuum.
- It carries momentum p = E/c = h/λ, which is why a beam of light exerts a small radiation pressure.
- Energy is quantised: a source cannot emit half a photon. If a source emits n photons per second, the beam power is P = nhf.
Photon energy in joules and electron volts
MDCAT numericals quote photon energies in either joules or electron volts, where 1 eV = 1.602 × 10−19 J. A shortcut worth memorising:
hc = 1240 eV nm → E (in eV) = 1240 / λ (in nm)
- Worked example 1. Green light of wavelength 500 nm: E = 1240/500 = 2.48 eV, i.e. 2.48 × 1.602 × 10−19 = 3.97 × 10−19 J.
- Worked example 2. A photon of frequency 6.0 × 1014 Hz: E = hf = (6.626 × 10−34)(6.0 × 1014) = 3.98 × 10−19 J ≈ 2.48 eV — the same photon, since λ = c/f = 500 nm.
Light behaves sometimes as a wave (interference, diffraction, refraction) and sometimes as a stream of particles (photons carrying energy hf and momentum h/λ). The two pictures are complementary, not contradictory — the experiment you perform decides which face of light appears.
Worked MCQs
Five MCQs that capture the high-yield testing patterns for this chapter. Read the explanation even when you get the answer right — it's where the deeper concept lives.
Q1. The energy of a photon of wavelength 620 nm is approximately:
Using hc = 1240 eV nm, E = 1240/620 = 2.0 eV. In joules that is 2.0 × 1.602 × 10−19 = 3.2 × 10−19 J.
Q2. If the frequency of a monochromatic source is doubled, the energy carried by each photon:
E = hf, so photon energy is directly proportional to frequency. Equivalently, doubling the frequency halves the wavelength and E = hc/λ doubles.
Q3. The momentum of a photon of wavelength λ is given by:
A photon has zero rest mass but carries momentum p = E/c = (hc/λ)/c = h/λ. Note hc/λ is the photon's energy, not its momentum — a favourite distractor.
Q4. Increasing the intensity of a monochromatic light beam increases:
Beam power P = nhf. For fixed frequency, more intensity simply means a larger n. Photon energy hf and photon speed c are both unchanged.
Q5. The energy of a photon of frequency 5.0 × 1014 Hz is closest to:
E = hf = (6.626 × 10−34)(5.0 × 1014) = 3.31 × 10−19 J, which is about 2.07 eV.
Quick Recap
- A photon is one quantum of electromagnetic radiation — the particle of light.
- Planck: E = hf = hc/λ, with h = 6.626 × 10−34 J s.
- Photon momentum p = E/c = h/λ; rest mass is zero and speed is always c in vacuum.
- Intensity → number of photons per second; frequency → energy of each photon.
- Beam power P = nhf for n photons per second.
- Useful conversions: hc = 1240 eV nm and 1 eV = 1.602 × 10−19 J.
- Light is complementary: wave behaviour in interference/diffraction, particle behaviour as photons.