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IB Diploma Physics · topic E.2

Quantum physics

Connect the ideas, make your working visible, and test the result. Use the hints when you need a starting point; open the full solution after your attempt.

Extra challenging questions

Work through the linked stages and explain what each result means.

Extra challenging · 01

Same light energy, different photon counts

A source emits monochromatic pulses of equal energy 6.626×10⁻⁶ J at two frequencies: 5.0×10¹⁴ Hz and 1.0×10¹⁵ Hz. Use h = 6.626×10⁻³⁴ J s and c = 3.0×10⁸ m s⁻¹. The graph provides photon energy as a function of frequency. Supplied model: Use photon energy E = hf, wavelength λ = c/f and photon count N = Epulse/Ephoton. Supplied data (Frequency / 10¹⁴ Hz; Photon energy / 10⁻¹⁹ J): (0, 0), (5, 3.313), (10, 6.626). (a) Calculate each wavelength, photon energy and photon count. Identify the approximate spectral region of each pulse. [3 marks] (b) Explain why interference supports a wave model while photon-counting detection needs a particle-like model. Evaluate the claim that all electromagnetic radiation has identical biological effects. [3 marks]

Explore the question data

Photon-energy model

Supplied question data. Read the labelled axes and use the observations to test the physical model.

Vertical axis (y): Photon energy / 10⁻¹⁹ J

Photon-energy modelSupplied question data. Read the labelled axes and use the observations to test the physical model. Horizontal axis: Frequency / 10¹⁴ Hz. Vertical axis: Photon energy / 10⁻¹⁹ J. Exact values are available in the data table below.01.6573.3134.976.62602.557.510xy

Horizontal axis (x): Frequency / 10¹⁴ Hz

Reading 1Frequency / 10¹⁴ Hz: 0Photon energy / 10⁻¹⁹ J: 0
Read the exact data as a table
Photon-energy model — supplied values
Frequency / 10¹⁴ HzPhoton energy / 10⁻¹⁹ J
00
53.313
106.626

These are the supplied values, not a worked answer. Lines join the supplied values; they are not a fitted model.

Show a hint

Begin with part (a): Calculate each wavelength, photon energy and photon count. Identify the approximate spectral region of each pulse.

Reveal the worked solution
  1. Use λ = c/f: the lower frequency has wavelength 6.0×10⁻⁷ m and the higher 3.0×10⁻⁷ m.
  2. Ephoton = hf gives 3.313×10⁻¹⁹ and 6.626×10⁻¹⁹ J. Dividing equal total pulse energy by these values gives 2.0×10¹³ and 1.0×10¹³ photons.
  3. 600 nm is visible light and 300 nm is ultraviolet. Both propagate at c in vacuum; the higher-frequency pulse contains fewer photons for the same total energy.
  4. Spatial interference patterns follow phase and superposition, which a simple stream of classical particles does not explain.
  5. Localized detector events with frequency-dependent energy are described by photons. These are complementary descriptions of quantum light rather than literal tiny balls riding classical waves.
  6. Absorption, penetration, dose and photon energy depend on wavelength and material. Ultraviolet can cause photochemical damage; exposure assessment cannot be inferred from vacuum speed alone.

Answer (a) 600 nm, 3.313×10⁻¹⁹ J, 2.0×10¹³ photons; 300 nm, 6.626×10⁻¹⁹ J, 1.0×10¹³ photons. (b) Different models describe different observations; common vacuum speed does not imply identical interaction or hazard.

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Extra challenging · 02

A photoelectric threshold measured with stopping voltage

A metal's stopping-potential measurements against incident-light frequency are supplied. Use electron charge e = 1.60×10⁻¹⁹ C and Kmax = eVs. The stopping-potential fit extrapolates to Vs = 0 at 5.0×10¹⁴ Hz. Assume one-photon photoemission and no contact-potential correction. Supplied data (Frequency / 10¹⁴ Hz; Stopping potential / V): (5, 0), (6, 0.414), (7, 0.828), (8, 1.242). (a) Estimate Planck's constant and the work function from the graph; find maximum electron kinetic energy at 8.0×10¹⁴ Hz. [3 marks] (b) Predict the effect of doubling intensity at fixed frequency above threshold, and of using intense light below threshold. [3 marks]

Explore the question data

Photoelectric stopping potential

Supplied question data. Read the labelled axes and use the observations to test the physical model.

Vertical axis (y): Stopping potential / V

Photoelectric stopping potentialSupplied question data. Read the labelled axes and use the observations to test the physical model. Horizontal axis: Frequency / 10¹⁴ Hz. Vertical axis: Stopping potential / V. Exact values are available in the data table below.00.31050.6210.93151.24202468xy

Horizontal axis (x): Frequency / 10¹⁴ Hz

Reading 1Frequency / 10¹⁴ Hz: 5Stopping potential / V: 0
Read the exact data as a table
Photoelectric stopping potential — supplied values
Frequency / 10¹⁴ HzStopping potential / V
50
60.414
70.828
81.242

These are the supplied values, not a worked answer. No fitted trend is drawn.

Show a hint

Begin with part (a): Estimate Planck's constant and the work function from the graph; find maximum electron kinetic energy at 8.0×10¹⁴ Hz.

Reveal the worked solution
  1. Einstein's relation gives Vs = (h/e)f−φ/e. Graph slope is 0.414/(1.0×10¹⁴) = 4.14×10⁻¹⁵ V s.
  2. Thus h = e×slope = 6.624×10⁻³⁴ J s. At threshold, φ = hf0 = 3.312×10⁻¹⁹ J, or 2.07 eV.
  3. At 8.0×10¹⁴ Hz, Kmax = eVs = (1.60×10⁻¹⁹)(1.242)≈1.987×10⁻¹⁹ J. The graph intercept is an energy-per-charge condition, not a delay.
  4. At fixed frequency, each photon carries the same hf. Doubling intensity supplies more photons per second, which can increase photocurrent if collection and material conditions remain unchanged.
  5. Stopping potential depends on the maximum energy per emitted electron, so it does not double with intensity.
  6. Below threshold each photon lacks the work-function energy. Increasing photon arrival rate does not fix that within the stated single-photon model; multiphoton regimes are outside this approximation.

Answer (a) h≈6.624×10⁻³⁴ J s; work function≈3.312×10⁻¹⁹ J = 2.07 eV; Kmax≈1.987×10⁻¹⁹ J = 1.242 eV. (b) Above threshold, emission rate can rise without changing Kmax; below threshold the ideal one-photon model predicts no photoemission.

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