Use an independent field to challenge a potential fit
Separate an exact fit from an identifiable, independently tested source claim.
Learning outcome: Vary gain and offset separately. Retain fitted charge, fitted offset and the independent field residual. Construct a same-instrument third-potential prediction and explain why it cannot by itself identify gain. Propose a controlled alternative test for a wrong source radius.
Starting recap
Keep source normalization, potential reference, signed energy and evidence independence explicit.
All lessons are open directly. Your saved experiments remain when you leave and return.
Try
With true Q = 2 nC, gain g = 1.05 and offset C = 1 V, the two-point potential fit returns Qfit = 2.10 nC and Cfit = 1 V. It predicts approximately 6.67292 N/C at z = 1 m, while the independent supplied field is 6.35516 N/C. The residual is approximately 0.317758 N/C.
Open the experimentPredict
Which new observation most directly challenges the hidden shared-gain bias in this stated ring fit?
Experiment
Vary gain and offset separately. Retain fitted charge, fitted offset and the independent field residual. Construct a same-instrument third-potential prediction and explain why it cannot by itself identify gain. Propose a controlled alternative test for a wrong source radius.
Challenge a shared-gain potential inference
Worked teaching model · synthetic values · Synthetic ring R = 1 m,Q = 2 nC. Indicated potentials at z = 1 and 2 m share gain and offset. A fit assumes correct gain and solves Q plus offset. Separate field record at z = 1 is stipulated independently calibrated; this is a conditional inference, not an actual calibration claim.
Reset keeps your prediction, captures and practice history.
Potential readout with common gain and offset
Axes rescale independently. Curves join sampled coordinates; a joining segment is not additional measured evidence. Read physical units rather than screen angles or apparent slopes.
Potential readout with common gain and offset: numerical coordinates
| axial z (m) | indicated potential (V) |
|---|---|
| 0 | 19.8739 |
| 0.05 | 19.8503 |
| 0.1 | 19.7802 |
| 0.15 | 19.665 |
| 0.2 | 19.5073 |
| 0.25 | 19.3103 |
| 0.3 | 19.0779 |
| 0.35 | 18.8142 |
| 0.4 | 18.5239 |
| 0.45 | 18.2115 |
| 0.5 | 17.8813 |
| 0.55 | 17.5376 |
| 0.6 | 17.1842 |
| 0.65 | 16.8247 |
| 0.7 | 16.4621 |
| 0.75 | 16.0991 |
| 0.8 | 15.738 |
| 0.85 | 15.3807 |
| 0.9 | 15.0288 |
| 0.95 | 14.6835 |
| 1 | 14.3458 |
| 1.05 | 14.0165 |
| 1.1 | 13.6959 |
| 1.15 | 13.3846 |
| 1.2 | 13.0827 |
| 1.25 | 12.7904 |
| 1.3 | 12.5076 |
| 1.35 | 12.2342 |
| 1.4 | 11.9702 |
| 1.45 | 11.7153 |
| 1.5 | 11.4693 |
| 1.55 | 11.232 |
| 1.6 | 11.0031 |
| 1.65 | 10.7824 |
| 1.7 | 10.5694 |
| 1.75 | 10.3641 |
| 1.8 | 10.166 |
| 1.85 | 9.97484 |
| 1.9 | 9.79043 |
| 1.95 | 9.61246 |
| 2 | 9.44065 |
| 2.05 | 9.27475 |
| 2.1 | 9.11451 |
| 2.15 | 8.95969 |
| 2.2 | 8.81006 |
| 2.25 | 8.6654 |
| 2.3 | 8.5255 |
| 2.35 | 8.39016 |
| 2.4 | 8.25918 |
| 2.45 | 8.13237 |
| 2.5 | 8.00958 |
| 2.55 | 7.89061 |
| 2.6 | 7.77532 |
| 2.65 | 7.66355 |
| 2.7 | 7.55516 |
| 2.75 | 7.45001 |
| 2.8 | 7.34797 |
| 2.85 | 7.2489 |
| 2.9 | 7.1527 |
| 2.95 | 7.05925 |
| 3 | 6.96844 |
| Quantity | Value | Unit |
|---|---|---|
| Indicated potential at z = 1 m | 14.3458 | V |
| Indicated potential at z = 2 m | 9.44065 | V |
| Inferred charge under assumed unit gain | 2.1 | nC |
| Inferred additive offset | 1 | V |
| Field predicted from fitted charge | 6.67292 | N/C |
| Stipulated independent field | 6.35516 | N/C |
| Predicted minus independent field | 0.317758 | N/C |
Two readings fit two unknowns exactly, even when an unmodeled common gain biases the inferred charge.
Subtract readings to remove offset, not gain: Qfit = gain times true Q. The fitted offset remains the supplied offset for this exact ring packet. A third reading from the same faulty instrument can remain consistent. An independently calibrated field record tests the charge inference only under the shared source-geometry assumption.
Derive before checking. Retain contrasting captures and explain one assumption that could fail; calculated evidence is not actual laboratory work.
Two readings fit two unknowns exactly, even when an unmodeled common gain biases the inferred charge.
Subtract readings to remove offset, not gain: Qfit = gain times true Q. The fitted offset remains the supplied offset for this exact ring packet. A third reading from the same faulty instrument can remain consistent. An independently calibrated field record tests the charge inference only under the shared source-geometry assumption.
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 reference, source geometry or evidence-independence assumption limits your inference?
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.