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SCIENCE · INVESTIGATE AND EXPLAIN

Distinguish photon energy, count rate and missing stopping evidence

In the photoelectric effect, an absorbed photon can transfer energy to an electron. The maximum emitted-electron kinetic energy is Kmax=hf−φ when the photon exceeds the surface work function φ. A retarding potential of magnitude Vs stops the fastest electrons when eVs=Kmax. Work function is a material/surface property, not energy accumulated indefinitely by one electron from a dim classical wave.

Learning outcome: At frequency control 8 compare powers 0, 1 and 2 nW; then compare frequency controls 4 and 8 at 2 nW. Retain missing values as missing and distinguish a count-rate change from a kinetic-energy change.

Starting recap

Use scientific notation, signed energy differences and vector momentum. Distinguish a stipulated quantum or nuclear model from actual apparatus and label optional numerical extensions.

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Try

For f=8×10¹⁴ Hz, P=2 nW and φ=2.2 eV, photon energy≈3.30853 eV, Kmax≈1.10853 eV and stopping magnitude≈1.10853 V. Photon rate≈3.77298×10⁹/s gives ideal upper current≈0.604497 nA.

Open the experiment

Predict

Does doubling power at unchanged above-threshold frequency double the stopping potential?

Experiment

At frequency control 8 compare powers 0, 1 and 2 nW; then compare frequency controls 4 and 8 at 2 nW. Retain missing values as missing and distinguish a count-rate change from a kinetic-energy change.

Separate a threshold limit from an illuminated current

Worked teaching model · synthetic values · Hypothetical clean surface work function 2.20 eV. Ideal one-photon/one-electron upper bound with complete collection above threshold; actual yield can be lower. Zero incident power produces no emitted electrons and no measured stopping voltage. No tube, high-voltage or radiation activity.

Reset keeps your prediction, captures and practice history.

Energy limit for hypothetical illuminated trials

0122.76280frequency (×10¹⁴ Hz)maximum allowed kinetic energy (eV)
  • 1: above-threshold energy line — solid line
Accessible coordinates for this panel

These tables sample up to 82 displayed coordinates per series, including both endpoints. Fine curves may contain additional calculated points between table entries; use the ledger for exact analytic minima, frequencies or other named evidence. Values are synthetic, not instrument readings.

above-threshold energy line
frequency (×10¹⁴ Hz)maximum allowed kinetic energy (eV)
60.2814
6.10.32276
6.20.36411
6.30.40547
6.40.44683
6.50.48818
6.60.52954
6.70.5709
6.80.61225
6.90.65361
70.69497
7.10.73632
7.20.77768
7.30.81904
7.40.86039
7.50.90175
7.60.94311
7.70.98446
7.81.0258
7.91.0672
81.1085
8.11.1499
8.21.1912
8.31.2326
8.41.274
8.51.3153
8.61.3567
8.71.398
8.81.4394
8.91.4807
91.5221
9.11.5635
9.21.6048
9.31.6462
9.41.6875
9.51.7289
9.61.7702
9.71.8116
9.81.853
9.91.8943
101.9357
10.11.977
10.22.0184
10.32.0597
10.42.1011
10.52.1425
10.62.1838
10.72.2252
10.82.2665
10.92.3079
112.3492
11.12.3906
11.22.4319
11.32.4733
11.42.5147
11.52.556
11.62.5974
11.72.6387
11.82.6801
11.92.7214
122.7628

Each plot rescales independently. Compare values and units rather than apparent screen angles. Different panels can represent different quantities and are not silently overlaid.

Calculated evidence ledger — original synthetic model
QuantityValueUnit
Incident photon energy3.3085eV
Work function2.2eV
Photon energy minus work function1.1085eV
Threshold frequency531960000000000Hz
Incident photon rate3773000000photons/s
Ideal collected-current upper bound0.6045nA
Stopping-potential magnitude under illumination1.1085V

Above threshold, frequency fixes the maximum energy while power affects the upper-bound event rate.

eVs=Kmax=hf−φ applies to the stopping magnitude when illuminated photoelectrons exist. The plotted line is a hypothetical frequency series, not measured points at the selected power; it does not fabricate a measured zero-power voltage. Actual collection/yield can be smaller than the one-electron-per-photon upper bound. At exact threshold the model has zero excess kinetic energy and assigns no positive collected current.

Above threshold, frequency fixes the maximum energy while power affects the upper-bound event rate.

eVs=Kmax=hf−φ applies to the stopping magnitude when illuminated photoelectrons exist. The plotted line is a hypothetical frequency series, not measured points at the selected power; it does not fabricate a measured zero-power voltage. Actual collection/yield can be smaller than the one-electron-per-photon upper bound. At exact threshold the model has zero excess kinetic energy and assigns no positive collected current.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

Begin with evidence

In the photoelectric effect, an absorbed photon can transfer energy to an electron. The maximum emitted-electron kinetic energy is Kmax=hf−φ when the photon exceeds the surface work function φ. A retarding potential of magnitude Vs stops the fastest electrons when eVs=Kmax. Work function is a material/surface property, not energy accumulated indefinitely by one electron from a dim classical wave.

Connect the model

At fixed above-threshold frequency, increasing light power increases incident photon rate P/(hf). It does not increase each photon’s energy or the ideal maximum electron energy. The ledger’s eP/(hf) is an ideal upper current assuming every photon produces a collected electron, not a guaranteed real yield. Reflection, emission probabilities and collection geometry can lower an actual current.

Interpret the ledger

Frequency below threshold yields no photoemission in the single-photon model, regardless of increased low-level intensity. With zero light power there is no emitted population to stop even if the selected frequency would be energetic enough. The interface therefore omits a measured stopping potential in those cases rather than inventing a zero-voltage observation. The plotted above-threshold line is a theoretical relation, not measured data at the selected power.

Test the boundary

A calibration of Vs against f gives slope h/e and intercept −φ/e only for appropriate above-threshold observations. A missing current is ambiguous: it can indicate no light, insufficient photon energy, collection failure or a different surface. Use contrasting controls to separate these possibilities before assigning a work function. All controls are virtual; no vacuum tube, wiring or ultraviolet exposure is requested.

Worked original case

For f=8×10¹⁴ Hz, P=2 nW and φ=2.2 eV, photon energy≈3.30853 eV, Kmax≈1.10853 eV and stopping magnitude≈1.10853 V. Photon rate≈3.77298×10⁹/s gives ideal upper current≈0.604497 nA.

Predict, compare and retain evidence

Does doubling power at unchanged above-threshold frequency double the stopping potential? At frequency control 8 compare powers 0, 1 and 2 nW; then compare frequency controls 4 and 8 at 2 nW. Retain missing values as missing and distinguish a count-rate change from a kinetic-energy change.

Changed-case practice

A supplied above-threshold calibration has Vs=0.4 V at 6×10¹⁴ Hz and 1.2 V at 8×10¹⁴ Hz. Infer slope and extrapolated threshold; explain why a dark reading is not another point on that line.

Check the reasoning after your attempt

Slope is 4×10⁻¹⁵ V s, and extrapolated zero is 5×10¹⁴ Hz. No electrons exist to define a stopping cutoff in darkness; zero current does not measure Vs=0.

Reflect and source-check

Which comparison would distinguish zero illumination from a below-threshold illuminated surface?

Original prose and supplied numerical evidence; checked 30 October 2026 against the current AP Physics 2 framework, fall 2026 clarifications and OpenStax. Virtual-only: no physical source, exposure or apparatus is requested. Public examples and model captures are not independent mastery or supervised laboratory participation.

Apply

At fixed above-threshold frequency, doubling incident light power ideally changes maximum electron kinetic energy by:

Public practice checks a specific claim. It does not establish independent mastery.

Which comparison would distinguish zero illumination from a below-threshold illuminated surface?

Continue

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