Einstein's Photoelectric Equation

Key idea: Apply Einstein’s photoelectric equation Kmax = hf − Φ and the stopping potential relation Kmax = eVs, including graph interpretation (A Level Physics).

  • GCE A-Level H2 Physics 2027
On this page

Learning objectives

  • Use photon energy and momentum and analyse the photoelectric effect.
  • Apply de Broglie wavelength and wave-particle evidence.
  • Interpret wavefunctions, probability density and superposition.
  • Apply uncertainty and infinite-square-well energy quantisation.
  • Analyse atomic energy levels and emission or absorption spectra.
Legacy calculation method

The current 9478 outcome names threshold frequency and photon energy E = hf, but does not explicitly name stopping potential or Einstein’s photoelectric equation. Use this page as supporting method work where your school or an older paper includes it.

1. Definitions (Must Know)

A. Work function, Φ

The work function, Φ, is the minimum energy needed to remove an electron from the metal surface.

B. Einstein’s photoelectric equation

For the most energetic photoelectrons:

Kₘₐₓ = hf-Φ

C. Stopping potential, Vₛ

The stopping potential, Vₛ, is the minimum retarding potential difference needed to reduce the photoelectric current to zero.

It links to maximum kinetic energy:

Kₘₐₓ = eVₛ

2. Key Ideas (What Earns Marks)

  • Threshold frequency: Kₘₐₓ = 0 ⇒ hf₀ = Φ ⇒ f₀ = Φ/h
  • Combine with stopping potential: eVₛ = hf-Φ ⇒ Vₛ = (h/e)f-Φ/e
  • Vₛ vs f is a straight line:
    • gradient: h/e
    • intercept: -Φ/e
Units check

hf and Φ are energies (J). eVₛ is also energy (C·V = J).

3. Detailed Explanations

Monochromatic light ejects electrons from an emitter in an evacuated tube. The electrons travel towards a collector connected to a microammeter. An adjustable retarding supply makes the emitter positive and collector negative; the stopping potential is reached when the photocurrent becomes zero.
Reverse the electrode polarity to oppose the photoelectrons, then increase the retarding potential until even the fastest electrons cannot reach the collector.

How Vₛ is found (I–V curve)

The stopping potential is found by increasing a retarding potential until the photocurrent just falls to zero.

Photoelectric I–V curves (qualitative)

Qualitative photoelectric current–voltage curves showing saturation current, stopping potential, and how intensity vs frequency affects the graph.

Scroll across the graph to read all labels.

Qualitative photoelectric current–voltage curves showing saturation current, stopping potential, and how intensity vs frequency affects the graph.Qualitative photoelectric current–voltage curves showing saturation current, stopping potential, and how intensity vs frequency affects the graph.
Intensity changes the saturation current (how many electrons per second). Frequency changes the stopping potential (how energetic the fastest electrons are).
Open full-size graph
View figure data
Values and uncertainty for Photoelectric I–V curves (qualitative)
SeriesAnode potential, V (V)Anode potential, V uncertaintyPhotocurrent (scaled)Photocurrent uncertainty
Same f, higher intensity-2.50
Same f, higher intensity-20
Same f, higher intensity-1.20
Same f, higher intensity-0.80.25
Same f, higher intensity-0.40.62
Same f, higher intensity00.9
Same f, higher intensity0.41
Same f, higher intensity0.81
Same f, higher intensity1.21
Same f, lower intensity-2.50
Same f, lower intensity-20
Same f, lower intensity-1.20
Same f, lower intensity-0.80.12
Same f, lower intensity-0.40.31
Same f, lower intensity00.45
Same f, lower intensity0.40.5
Same f, lower intensity0.80.5
Same f, lower intensity1.20.5
Higher f (more energetic): larger Vs-2.50
Higher f (more energetic): larger Vs-1.80
Higher f (more energetic): larger Vs-1.40.18
Higher f (more energetic): larger Vs-10.36
Higher f (more energetic): larger Vs-0.60.46
Higher f (more energetic): larger Vs00.5
Higher f (more energetic): larger Vs0.60.5
Higher f (more energetic): larger Vs1.20.5

A. Why only the maximum matters

Electrons come from different depths in the metal and can lose energy in collisions before escaping.

So emitted electrons have a range of kinetic energies. The equation uses Kₘₐₓ for the most energetic electrons (often those that escape with minimal loss).

B. From Kₘₐₓ to stopping potential

Stopping potential is defined so that even the most energetic electrons are just stopped:

Kₘₐₓ = eVₛ

Combine with Einstein’s equation:

eVₛ = hf-Φ

4. Common Mistakes

  • Treating Φ as a “force” (it is an energy).
  • Using Vₛ when the question is about a different potential in the circuit.
  • Using f₀ formula but forgetting to use the same units (Hz, J, J·s).

5. Exam Tips

  • If asked for a “threshold wavelength”, use f = c/λ: f₀ = Φ/h ⇒ λ₀ = c/f₀ = hc/Φ
  • If given a Vₛ vs f graph, read:
    • gradient → h/e,
    • x-intercept → f₀.

6. Worked Examples

Modelled example 1

Find Kₘₐₓ

Core

Problem

Light of frequency 8.0 × 10¹⁴ Hz illuminates a metal with work function 2.4 × 10⁻¹⁹ J. Using h = 6.63 × 10⁻³⁴ J s, find Kₘₐₓ.
Study the worked solution
  1. Check the energy balance

    Method

    One photon supplies energy hf; the work function is the minimum removal energy.

    Reason

    Only the remaining energy can become maximum electron kinetic energy.

    Working

    Kₘₐₓ = hf-Φ
  2. Calculate photon energy

    Method

    Multiply Planck’s constant by frequency.

    Reason

    J s multiplied by s⁻¹ gives joules.

    Working

    hf = (6.63 × 10⁻³⁴)(8.0 × 10¹⁴) = 5.304 × 10⁻¹⁹ J
  3. Subtract the work function

    Method

    Use unrounded energy before the final rounding.

    Reason

    The emitted electron retains the surplus.

    Working

    Kₘₐₓ = 5.304 × 10⁻¹⁹-2.4 × 10⁻¹⁹ = 2.9 × 10⁻¹⁹ J

Guided practice 2

Find stopping potential

About 4 min

Problem

Using the preceding unrounded Kₘₐₓ result and e = 1.60 × 10⁻¹⁹ C, find the stopping potential.

Try this before viewing the solution

Hints

Hint 1: match energy to electric work
At the stopping condition, Kₘₐₓ = eVₛ.
View solution step by step
  1. Select relation

    Method

    Set maximum kinetic energy equal to electric stopping work.

    Reason

    The fastest photoelectrons are just prevented from reaching the collector.

    Working

    Kₘₐₓ = eVₛ
  2. Calculate

    Method

    Divide by the elementary charge.

    Reason

    One joule per coulomb is one volt.

    Working

    Vₛ = (2.9 × 10⁻¹⁹)/(1.60 × 10⁻¹⁹) = 1.8 V

Common misconception 3

Find threshold frequency

Find and correct the mistake

Learner claim

A metal has Φ = 3.0 × 10⁻¹⁹ J. A learner says threshold frequency depends on light intensity because stronger light supplies more energy. Diagnose the claim and calculate f₀.

Try this before viewing the solution

Condition at threshold

View solution step by step
  1. State threshold condition

    Method

    At threshold, the most energetic emitted electron has zero kinetic energy.

    Reason

    One photon just supplies the removal energy.

    Working

    0 = hf₀-Φ
  2. Separate intensity

    Method

    Intensity changes photon arrival rate, not energy per photon.

    Reason

    Photon energy is hf, controlled by frequency.

    Working

    E_γ = hf
  3. Calculate

    Method

    Divide the work function by h.

    Reason

    The quotient has units s⁻¹.

    Working

    f₀ = (3.0 × 10⁻¹⁹)/(6.63 × 10⁻³⁴) = 4.5 × 10¹⁴ Hz

Examiner practice 4

Find h and Φ from two data points

5 marks

Examination question

For one metal, Vₛ = 0.40 V at 5.0 × 10¹⁴ Hz and Vₛ = 1.20 V at 7.0 × 10¹⁴ Hz. From Vₛ = (h/e)f-Φ/e, find h and Φ. Use e = 1.60 × 10⁻¹⁹ C. [5 marks]

Try this before viewing the solution

View solution step by step
  1. Find gradient

    1 mark

    Method

    Use changes in stopping potential and frequency.

    Reason

    The two points define the line’s gradient.

    Working

    m = (1.20-0.40)/((7.0-5.0) × 10¹⁴) = 4.0 × 10⁻¹⁵ V s
  2. Interpret gradient

    1 mark

    Method

    Set m = h/e.

    Reason

    This follows from the coefficient of f.

    Working

    h = me
  3. Calculate h

    1 mark

    Method

    Multiply by the elementary charge.

    Reason

    V s times C gives J s.

    Working

    h = (4.0 × 10⁻¹⁵)(1.60 × 10⁻¹⁹) = 6.4 × 10⁻³⁴ J s
  4. Find work function

    2 marks

    Method

    Substitute either point into Φ = hf-eVₛ.

    Reason

    The intercept energy is the photon energy not retained as kinetic energy.

    Working

    Φ = (6.4 × 10⁻³⁴)(5.0 × 10¹⁴)-(1.60 × 10⁻¹⁹)(0.40) = 2.56 × 10⁻¹⁹ J

Challenge 5

Threshold wavelength from work function (eV form)

Minimal support

Independent transfer

A metal has work function 2.5 eV. Using hc = 1240 eV·nm, find its threshold wavelength and state what happens for longer-wavelength light.

Try this before viewing the solution

Hints

Hint 1: use the threshold equality
Orient with hc/λ₀ = Φ and remember that longer wavelength means lower photon energy.
View solution step by step
  1. Rearrange

    Method

    Use the photon-energy form at threshold.

    Reason

    E = hc/λ equals the work function when Kₘₐₓ = 0.

    Working

    λ₀ = hc/Φ
  2. Calculate

    Method

    Keep eV and nm units paired.

    Reason

    The supplied hc avoids an unnecessary joule conversion.

    Working

    λ₀ = 1240/2.5 = 496 nm ≈ 5.0 × 10² nm
  3. Interpret boundary

    Method

    Longer wavelengths do not eject electrons in this model.

    Reason

    Their lower-frequency photons have E < Φ.

    Working

    λ > λ₀ ⇒ f < f₀

7. Mind Stretchers

Mind stretcher 1: Explain the straight-line graphExtension

Explain why a plot of Vₛ against f is a straight line.

Show Answer

From eVₛ = hf-Φ: Vₛ = (h/e)f-Φ/e

This is of the form y = mx + c, so the graph is a straight line with constant gradient h/e.

Mind stretcher 2: Meaning of the interceptsExtension

In Vₛ = (h/e)f-Φ/e, what do the x-intercept and y-intercept represent physically?

Show Answer

The x-intercept occurs when Vₛ = 0, so f = f₀ = Φ/h (the threshold frequency).

The y-intercept is -Φ/e, a negative voltage value; it encodes the work function (how much energy per electron must be supplied before any kinetic energy remains).

8. Optional (Enrichment)

A. Threshold wavelength

Sometimes the threshold is quoted as a wavelength λ₀: λ₀ = hc/Φ

Use this only if the question explicitly gives wavelength instead of frequency.

Continue with the next resource in this course.

Course and syllabus information
Course
GCE A-Level H2 Physics
Edition
GCE A-Level H2 Physics 2027