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IB · E · extended response

A photoelectric threshold measured with stopping voltage

Nuclear and quantum physics · Original GioPhysics question with a detailed, mark-by-mark answer guide.

Demand
discriminating
Marks
6
Topics
1
Answer
Complete
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.

extended response6 marks

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).

  1. (a)

    Estimate Planck's constant and the work function from the graph; find maximum electron kinetic energy at 8.0×10¹⁴ Hz.

    3 marks
  2. (b)

    Predict the effect of doubling intensity at fixed frequency above threshold, and of using intense light below threshold.

    3 marks
Ready to self-mark?Reveal the detailed answer guide
Answer overview(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.
01

(a)

3 marks

Estimate Planck's constant and the work function from the graph; find maximum electron kinetic energy at 8.0×10¹⁴ Hz.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 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. 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. 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.

02

(b)

3 marks

Predict the effect of doubling intensity at fixed frequency above threshold, and of using intense light below threshold.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 1

    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.

  2. 2

    Stopping potential depends on the maximum energy per emitted electron, so it does not double with intensity.

  3. 3

    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.

Complete marking guidance

Use these worked steps alongside the part-by-part answers. They explain the method and mark allocation; they do not add extra marks.

  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.

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