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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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.
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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.
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Energy limit for hypothetical illuminated trials
- 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.
| frequency (×10¹⁴ Hz) | maximum allowed kinetic energy (eV) |
|---|---|
| 6 | 0.2814 |
| 6.1 | 0.32276 |
| 6.2 | 0.36411 |
| 6.3 | 0.40547 |
| 6.4 | 0.44683 |
| 6.5 | 0.48818 |
| 6.6 | 0.52954 |
| 6.7 | 0.5709 |
| 6.8 | 0.61225 |
| 6.9 | 0.65361 |
| 7 | 0.69497 |
| 7.1 | 0.73632 |
| 7.2 | 0.77768 |
| 7.3 | 0.81904 |
| 7.4 | 0.86039 |
| 7.5 | 0.90175 |
| 7.6 | 0.94311 |
| 7.7 | 0.98446 |
| 7.8 | 1.0258 |
| 7.9 | 1.0672 |
| 8 | 1.1085 |
| 8.1 | 1.1499 |
| 8.2 | 1.1912 |
| 8.3 | 1.2326 |
| 8.4 | 1.274 |
| 8.5 | 1.3153 |
| 8.6 | 1.3567 |
| 8.7 | 1.398 |
| 8.8 | 1.4394 |
| 8.9 | 1.4807 |
| 9 | 1.5221 |
| 9.1 | 1.5635 |
| 9.2 | 1.6048 |
| 9.3 | 1.6462 |
| 9.4 | 1.6875 |
| 9.5 | 1.7289 |
| 9.6 | 1.7702 |
| 9.7 | 1.8116 |
| 9.8 | 1.853 |
| 9.9 | 1.8943 |
| 10 | 1.9357 |
| 10.1 | 1.977 |
| 10.2 | 2.0184 |
| 10.3 | 2.0597 |
| 10.4 | 2.1011 |
| 10.5 | 2.1425 |
| 10.6 | 2.1838 |
| 10.7 | 2.2252 |
| 10.8 | 2.2665 |
| 10.9 | 2.3079 |
| 11 | 2.3492 |
| 11.1 | 2.3906 |
| 11.2 | 2.4319 |
| 11.3 | 2.4733 |
| 11.4 | 2.5147 |
| 11.5 | 2.556 |
| 11.6 | 2.5974 |
| 11.7 | 2.6387 |
| 11.8 | 2.6801 |
| 11.9 | 2.7214 |
| 12 | 2.7628 |
Each plot rescales independently. Compare values and units rather than apparent screen angles. Different panels can represent different quantities and are not silently overlaid.
| Quantity | Value | Unit |
|---|---|---|
| Incident photon energy | 3.3085 | eV |
| Work function | 2.2 | eV |
| Photon energy minus work function | 1.1085 | eV |
| Threshold frequency | 531960000000000 | Hz |
| Incident photon rate | 3773000000 | photons/s |
| Ideal collected-current upper bound | 0.6045 | nA |
| Stopping-potential magnitude under illumination | 1.1085 | V |
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.
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Which comparison would distinguish zero illumination from a below-threshold illuminated surface?
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