Require both curl equations for a vacuum wave
Perpendicular sinusoidal arrows do not automatically form a valid electromagnetic wave. Test the candidate Ey=E0 cos(kx−omega t) and Bz=B0 cos(kx−omega t), with E0=2 V/m and k=π per metre. Controls propose phase speed a times c and signed magnetic amplitude bE0/c. These proposals include deliberately inconsistent choices.
Learning outcome: Compare the valid pair with a Faraday-only pair and with reversed magnetic sign. Predict each residual before inspecting the plots. Explain which violation could be interpreted as requiring a current and which cannot be repaired by an electric-current term.
Starting recap
Review flux integrals, linear differential equations, initial conditions, complex numbers and vector derivatives. Keep source constraints, RMS conventions and calibration roles explicit.
All lessons are open directly. Your saved experiments remain when you leave and return.
Try
At a=1 and b=1, both residuals are zero and cB0=E0. At a=0.5 and b=2, their product is one, so Faraday passes, but b−a=1.5 leaves a nonzero Ampère–Maxwell residual. Matching one derivative relation is therefore an insufficient validation test.
Open the experimentPredict
For a=0.5 and b=2, which statement follows?
Experiment
Compare the valid pair with a Faraday-only pair and with reversed magnetic sign. Predict each residual before inspecting the plots. Explain which violation could be interpreted as requiring a current and which cannot be repaired by an electric-current term.
Test wave amplitude and speed against both curl laws
Worked teaching model · synthetic values · Candidate Ey=2 cos(kx−omega t) V/m,Bz=(b*2/c)cos(kx−omega t) T,k=pi per m,omega=a c k. Source-free vacuum claim must satisfy both curl laws, not just perpendicular arrows. Teaching c3e8,mu0=4pi e−7,epsilon0=1/(mu0 c²) are mutually consistent.
Reset keeps your prediction, captures and practice history.
Candidate fields at zero time, with explicit constraint audit
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: candidate Ey (solid).2: candidate cBz (dashed). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Candidate fields at zero time, with explicit constraint audit
candidate Ey
| x (m) | E and cB on common electric-field scale (V/m) |
|---|---|
| 0 | 2 |
| 0.025 | 1.993835 |
| 0.05 | 1.975377 |
| 0.075 | 1.94474 |
| 0.1 | 1.902113 |
| 0.125 | 1.847759 |
| 0.15 | 1.782013 |
| 0.175 | 1.70528 |
| 0.2 | 1.618034 |
| 0.225 | 1.520812 |
| 0.25 | 1.414214 |
| 0.275 | 1.298896 |
| 0.3 | 1.175571 |
| 0.325 | 1.044997 |
| 0.35 | 0.907981 |
| 0.375 | 0.7653669 |
| 0.4 | 0.618034 |
| 0.425 | 0.4668907 |
| 0.45 | 0.3128689 |
| 0.475 | 0.1569182 |
| 0.5 | 1.22465e-16 |
| 0.525 | -0.1569182 |
| 0.55 | -0.3128689 |
| 0.575 | -0.4668907 |
| 0.6 | -0.618034 |
| 0.625 | -0.7653669 |
| 0.65 | -0.907981 |
| 0.675 | -1.044997 |
| 0.7 | -1.175571 |
| 0.725 | -1.298896 |
| 0.75 | -1.414214 |
| 0.775 | -1.520812 |
| 0.8 | -1.618034 |
| 0.825 | -1.70528 |
| 0.85 | -1.782013 |
| 0.875 | -1.847759 |
| 0.9 | -1.902113 |
| 0.925 | -1.94474 |
| 0.95 | -1.975377 |
| 0.975 | -1.993835 |
| 1 | -2 |
| 1.025 | -1.993835 |
| 1.05 | -1.975377 |
| 1.075 | -1.94474 |
| 1.1 | -1.902113 |
| 1.125 | -1.847759 |
| 1.15 | -1.782013 |
| 1.175 | -1.70528 |
| 1.2 | -1.618034 |
| 1.225 | -1.520812 |
| 1.25 | -1.414214 |
| 1.275 | -1.298896 |
| 1.3 | -1.175571 |
| 1.325 | -1.044997 |
| 1.35 | -0.907981 |
| 1.375 | -0.7653669 |
| 1.4 | -0.618034 |
| 1.425 | -0.4668907 |
| 1.45 | -0.3128689 |
| 1.475 | -0.1569182 |
| 1.5 | -3.67394e-16 |
| 1.525 | 0.1569182 |
| 1.55 | 0.3128689 |
| 1.575 | 0.4668907 |
| 1.6 | 0.618034 |
| 1.625 | 0.7653669 |
| 1.65 | 0.907981 |
| 1.675 | 1.044997 |
| 1.7 | 1.175571 |
| 1.725 | 1.298896 |
| 1.75 | 1.414214 |
| 1.775 | 1.520812 |
| 1.8 | 1.618034 |
| 1.825 | 1.70528 |
| 1.85 | 1.782013 |
| 1.875 | 1.847759 |
| 1.9 | 1.902113 |
| 1.925 | 1.94474 |
| 1.95 | 1.975377 |
| 1.975 | 1.993835 |
| 2 | 2 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
candidate cBz
| x (m) | E and cB on common electric-field scale (V/m) |
|---|---|
| 0 | 2 |
| 0.025 | 1.993835 |
| 0.05 | 1.975377 |
| 0.075 | 1.94474 |
| 0.1 | 1.902113 |
| 0.125 | 1.847759 |
| 0.15 | 1.782013 |
| 0.175 | 1.70528 |
| 0.2 | 1.618034 |
| 0.225 | 1.520812 |
| 0.25 | 1.414214 |
| 0.275 | 1.298896 |
| 0.3 | 1.175571 |
| 0.325 | 1.044997 |
| 0.35 | 0.907981 |
| 0.375 | 0.7653669 |
| 0.4 | 0.618034 |
| 0.425 | 0.4668907 |
| 0.45 | 0.3128689 |
| 0.475 | 0.1569182 |
| 0.5 | 1.22465e-16 |
| 0.525 | -0.1569182 |
| 0.55 | -0.3128689 |
| 0.575 | -0.4668907 |
| 0.6 | -0.618034 |
| 0.625 | -0.7653669 |
| 0.65 | -0.907981 |
| 0.675 | -1.044997 |
| 0.7 | -1.175571 |
| 0.725 | -1.298896 |
| 0.75 | -1.414214 |
| 0.775 | -1.520812 |
| 0.8 | -1.618034 |
| 0.825 | -1.70528 |
| 0.85 | -1.782013 |
| 0.875 | -1.847759 |
| 0.9 | -1.902113 |
| 0.925 | -1.94474 |
| 0.95 | -1.975377 |
| 0.975 | -1.993835 |
| 1 | -2 |
| 1.025 | -1.993835 |
| 1.05 | -1.975377 |
| 1.075 | -1.94474 |
| 1.1 | -1.902113 |
| 1.125 | -1.847759 |
| 1.15 | -1.782013 |
| 1.175 | -1.70528 |
| 1.2 | -1.618034 |
| 1.225 | -1.520812 |
| 1.25 | -1.414214 |
| 1.275 | -1.298896 |
| 1.3 | -1.175571 |
| 1.325 | -1.044997 |
| 1.35 | -0.907981 |
| 1.375 | -0.7653669 |
| 1.4 | -0.618034 |
| 1.425 | -0.4668907 |
| 1.45 | -0.3128689 |
| 1.475 | -0.1569182 |
| 1.5 | -3.67394e-16 |
| 1.525 | 0.1569182 |
| 1.55 | 0.3128689 |
| 1.575 | 0.4668907 |
| 1.6 | 0.618034 |
| 1.625 | 0.7653669 |
| 1.65 | 0.907981 |
| 1.675 | 1.044997 |
| 1.7 | 1.175571 |
| 1.725 | 1.298896 |
| 1.75 | 1.414214 |
| 1.775 | 1.520812 |
| 1.8 | 1.618034 |
| 1.825 | 1.70528 |
| 1.85 | 1.782013 |
| 1.875 | 1.847759 |
| 1.9 | 1.902113 |
| 1.925 | 1.94474 |
| 1.95 | 1.975377 |
| 1.975 | 1.993835 |
| 2 | 2 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
| Quantity | Value | Unit |
|---|---|---|
| Proposed angular frequency | 9.42478e+8 | rad/s |
| Proposed signed magnetic amplitude | 6.66667e-9 | T |
| Faraday sine-coefficient residual | 0 | V/m² |
| Ampere-Maxwell sine-coefficient residual | 0 | T/m |
| Source-free vacuum curl constraints satisfied | 1 | flag |
| Electric divergence | 0 | V/m² |
| Magnetic divergence | 0 | T/m |
Both curl constraints hold with E/B=c and phase speed c for this traveling vacuum wave.
For phase kx−omega t, curl E has z component −kE0 sin(phase), while −dB/dt is −omega B0 sin(phase). Their equality requires kE0=omega B0. The source-free Ampere-Maxwell equation independently requires kB0=mu0 epsilon0 omega E0. With consistent constants both imply speed c and B0=E0/c for +x propagation. A current could modify Ampere, but cannot repair a Faraday violation of this candidate field pair.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Both curl constraints hold with E/B=c and phase speed c for this traveling vacuum wave.
For phase kx−omega t, curl E has z component −kE0 sin(phase), while −dB/dt is −omega B0 sin(phase). Their equality requires kE0=omega B0. The source-free Ampere-Maxwell equation independently requires kB0=mu0 epsilon0 omega E0. With consistent constants both imply speed c and B0=E0/c for +x propagation. A current could modify Ampere, but cannot repair a Faraday violation of this candidate field pair.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
Understand
Apply
Public practice checks a specific claim. It does not establish independent mastery.
Which source, initial-state, calibration or field-law premise makes the result conditional, and what unused evidence would challenge it?
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.