Infer a photon from an energy-level difference, not a level label
A single-electron energy diagram assigns an energy to each stationary state. A transition emits a photon when the final state has lower energy, and absorbs a photon when it has higher energy. Conservation gives photon energy |Ef−Ei|=hf=hc/λ. The magnitude of one level relative to zero is not generally the energy of a transition between two bound states.
Learning outcome: Capture 3→2, 2→3 and 2→2. Predict emission, absorption or no energy-changing event before checking. Compare the ionization threshold from each initial state with the bound-to-bound gap.
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 n=3→2, ΔE=−1.88889 eV, so the emitted photon has λ≈656.387 nm. Reversing 2→3 requires absorption of the same photon energy. Ionizing from n=3 needs 1.51111 eV, a different process.
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Will reversing a pair of levels change the photon wavelength?
Experiment
Capture 3→2, 2→3 and 2→2. Predict emission, absorption or no energy-changing event before checking. Compare the ionization threshold from each initial state with the bound-to-bound gap.
Infer photon energy from a signed level change
Worked teaching model · synthetic values · Stipulated hydrogen levels En=−13.6/n² eV, zero at ionization. If initial=final there is no transition photon and no finite wavelength is assigned. Occupation, rates, selection rules and line strengths are not modeled; only single-electron energy diagrams.
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Single-electron energy levels
| Level | Energy (eV) |
|---|---|
| n=1 | -13.6 |
| n=2 final | -3.4 |
| n=3 initial | -1.5111 |
| n=4 | -0.85 |
| Ionization boundary | 0 |
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 |
|---|---|---|
| Initial atomic energy | -1.5111 | eV |
| Final atomic energy | -3.4 | eV |
| Atomic energy change | -1.8889 | eV |
| Ionization energy from initial level | 1.5111 | eV |
| Transition photon energy | 1.8889 | eV |
| Transition photon wavelength | 656.39 | nm |
| Transition photon frequency | 456730000000000 | Hz |
The atom loses energy and emits a photon matching the level gap.
Negative total energy means bound relative to the chosen ionization zero, not negative photon energy. Emission and reverse absorption share the same frequency when both starting states are available. The diagram is single-electron hydrogen with rounded 13.6 eV ground binding. Ionization is a transition to the continuum, not another finite line forced between equal levels; intensity and populations are outside this model.
The atom loses energy and emits a photon matching the level gap.
Negative total energy means bound relative to the chosen ionization zero, not negative photon energy. Emission and reverse absorption share the same frequency when both starting states are available. The diagram is single-electron hydrogen with rounded 13.6 eV ground binding. Ionization is a transition to the continuum, not another finite line forced between equal levels; intensity and populations are outside this model.
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Why can an energetically allowed line still be absent from an observed spectrum?
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