Learn

Learning preferences

Make learning more comfortable. Changes apply immediately.

Enlarges page content, including diagrams and their labels. You can also use your browser’s zoom.

Choose the colours that are easiest for you to distinguish. Applies to lesson diagrams and lab plots. Labels, shapes, hatching and line patterns also distinguish meanings. Source photographs and raw image brightness stay unchanged; mask-only views are available for image overlays.

ExampleComparisonSample link

Saved in this browser on this device. Preferences are separate from progress backups.

SCIENCE · INVESTIGATE AND EXPLAIN

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.

All lessons are open directly. Your saved experiments remain when you leave and return.

Try

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.

Open the experiment

Predict

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.

Reset keeps your prediction, captures and practice history.

Single-electron energy levels

0 eV-13.6 eVEnergy increases upward; dashed line is ionization zero.
Discrete level labels and energies
LevelEnergy (eV)
n=1-13.6
n=2 final-3.4
n=3 initial-1.5111
n=4-0.85
Ionization boundary0

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
Initial atomic energy-1.5111eV
Final atomic energy-3.4eV
Atomic energy change-1.8889eV
Ionization energy from initial level1.5111eV
Transition photon energy1.8889eV
Transition photon wavelength656.39nm
Transition photon frequency456730000000000Hz

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.

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

Understand

Begin with evidence

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.

Connect the model

The supplied hydrogen model uses En=−13.6/n² eV for n=1–4. It is intentionally separate from the slightly rounded-constant Bohr calculation. Use one consistent energy packet for a numerical inference rather than mixing its rounded levels with another model’s extra digits. The continuum begins at zero energy, so ionization from n requires at least 13.6/n² eV; excess energy can become electron kinetic energy.

Interpret the ledger

The workbench omits photon frequency and wavelength when initial and final levels are the same. That state change has zero energy difference and is not an emitted zero-frequency spectral line. A permitted energy gap also does not establish that the upper state is populated, how often a transition occurs, or the observed line intensity.

Test the boundary

Emission lines and absorption lines can correspond to the same energy gaps. Reverse the endpoints to preserve photon energy while changing whether energy enters or leaves the atom. Do not replace the diagram with a continuous thermal spectrum, and do not transfer this hydrogen formula unchanged to a many-electron atom.

Worked original case

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.

Predict, compare and retain evidence

Will reversing a pair of levels change the photon wavelength? 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.

Changed-case practice

Find the photon energy for 4→2 and the minimum energy to ionize from n=4. Explain why they differ.

Check the reasoning after your attempt

E4=−0.85 eV and E2=−3.4 eV, so the emitted photon has 2.55 eV. Ionization to zero needs 0.85 eV. The endpoints differ.

Use more than one line to compare candidate sources

Different elements have different allowed level structures, producing characteristic sets of emission and absorption frequencies. Observing a matched energy gap can support a candidate identity, but one shared line, unresolved blends, absent excitation or unknown instrument response can leave alternatives. An absorption spectrum tests what a foreground material removes from a broadband source; emission tests what an excited source adds.

Predict and check with fictional libraries: candidate A has allowed lines at 2.0 and 3.0 eV, candidate B at 2.0 and 4.0 eV. A 2.0 eV line alone does not distinguish them. Observed 2.0 and 3.0 eV emission supports A over B under the declared complete-library and response assumptions. A 3.0 eV absorption feature supplies the reverse transition test if the lower state is populated. Absence of the 4.0 eV line alone does not prove B absent without an excitation and sensitivity premise. These are original hypothetical spectra, not empirical element identifications. (Current clause 15.3.A.4.)

Reflect and source-check

Why can an energetically allowed line still be absent from an observed spectrum?

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.

Clause-level source/action reconciliation checked 31 October 2026 against the linked current framework and Fall 2026 clarification. Added packets are original virtual comparisons; no new practical or learner-completion claim.

Apply

For hydrogen En=−13.6/n² eV, the 3→2 emitted photon energy is:

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

Why can an energetically allowed line still be absent from an observed spectrum?

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

Skipping retains experiments and awards no mastery.

Save a science backup or import one

Science work is stored locally in this browser, separately from mathematics and AI. It does not sync automatically. Use this science-only backup; this checkout's older all-subject export does not include science.

A legacy file is available only when the complete snapshot fits the 36 MB limit. For larger snapshots, prepare a complete file set below; never discard notebooks to make a smaller file.

Matching imported notebook drafts replace their current drafts. Omitted lessons and known first attempts remain. Export your current work first if you want to retain both drafts.

Complete file sets and course backups

A file set can hold more work than one science file. Keep its manifest and every part together. Each file is limited to 36 MB. This format needs this version of LearnAI or a compatible newer version; older versions can use only the legacy single-file backup above.

The set includes every saved science course and global continuation at this moment. Later edits need a new export. A conflicting tab exports its own visible work, which may differ from saved work in another tab.

0 file(s) selected. File order and filenames do not determine identity. Missing, changed or conflicting parts block the entire restore; no good part is applied by itself.

Science storage: loading. No account or remote computation is required.