Quantum Photoelectric & Line Spectra Explorer
Move between photoelectric observations, stopping-potential graphs, and spectral-line transitions to keep quantum evidence and equations aligned.
Learning goals
- Use photon energy and momentum and analyse the photoelectric effect.
- Analyse atomic energy levels and emission or absorption spectra.
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Move frequency across threshold, then change intensity to see what changes and what stays fixed.
Photoelectric effect
Photon rate: medium
- Photon
- Electron
- Threshold
Stopping potential graph
Adjust frequency first: emission only begins when photon energy reaches the work function.
Emission: yesKEmax: 0.88 eVhf: 2.98 eVVs: 0.88 V
- Frequencysets photon energyhf = 2.98 eV
- Intensitysets electron rateKEmax unchanged
- Surfacesets the thresholdf0 = 5.08 × 10¹⁴ Hz
Change one variable at a time and watch the model respond.
Try this: move frequency below and above threshold, then increase intensity.
Explore
Results
Live readouts
Photoelectron current
Current appears only when frequency is at or above threshold.
Current calculation
Try a preset, then compare the animation with the readouts.
Caesium-like surface emits photoelectrons at the current frequency.
Practice
Exam formula box
E = hf
hf = Φ + KEmax
KEmax = hf - Φ when hf > Φ
eVs = KEmax
ΔE = hf = hc / λ for line spectra.
Worked example
If a caesium-like surface has Φ = 2.10 eV and the photon energy is 2.98 eV, then KEmax = 0.88 eV. The stopping potential is therefore about0.88 V.
Common misconceptions
- Intensity does not increase photon energy; frequency does.
- Bright low-frequency light still cannot eject electrons below threshold.
- Stopping potential measures maximum kinetic energy per unit charge, not emission rate.
- Line spectra are not continuous rainbows; they come from discrete energy transitions.
Exam idea
Use E = hf and Kmax = hf - Φ. Intensity changes how many photons arrive each second, so above threshold it changes emission rate/current, not the maximum kinetic energy or stopping potential.
Observation logCompare what changed0 saved
Change one variable, save another reading, then compare the evidence.
Scroll sideways to compare readings.
Fair-test check
Study lensDistinguish intensity effects from frequency effects in photoelectric emission.
Try this
Keep the evidence chain tight: observation first, then photon explanation, then equation only where it genuinely adds information.
Learn to
- Distinguish intensity effects from frequency effects in photoelectric emission.
- Use threshold frequency and stopping potential as evidence for photon-energy quantisation.
- Interpret emission and absorption spectra using the energy-level relation ΔE = hf = hc/λ.
Exam transfer
Governing idea
Photoelectric emission obeys hf = φ + Kₘₐₓ and eVₛ = Kₘₐₓ; spectral photons satisfy ΔE = hf.
Model boundary
Surfaces have a single ideal work function and energy levels are simplified. Contact potentials, surface contamination, and line broadening are omitted.
Avoid this trap
Above threshold, greater intensity emits more electrons but does not raise their maximum kinetic energy at fixed frequency.
How to explore
Link photoelectric observations, stopping-potential graphs, and line spectra without mixing photon energy with intensity.
Predict the outcome, change one variable at a time, then interpret the result. Completion records participation only and does not award mastery.
About this activity
Move between photoelectric observations, stopping-potential graphs, and spectral-line transitions to keep quantum evidence and equations aligned. A text explanation and no-JavaScript route remain available.
How this activity affects progress
Course and syllabus information
- Course
- GCE A-Level H2 Physics
- Edition
- GCE A-Level H2 Physics 2027