Distinguish an exact fit from independent electromagnetic evidence
For an initially zero-current LR circuit, true current is (E/R)[1 − exp(−tR/L)].
Learning outcome: Fit the supplied trace under two different gain assumptions and show why both match. Retain an independent LC calculation and explicitly audit the known-capacitor, clock and unchanged-inductor premises. Submit a critique/revision pair and an unfamiliar changed response in the versioned course project, distinguishing generated evidence from real observation.
Starting recap
Defend source and state boundaries, conserved inventories and independent cross-model evidence.
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Try
True L = 2 H, R = 3 ohm, source 6 V and current gain 1.5 produce a reported asymptote of 3 A and tau = 2/3 s. Assuming unit gain gives apparent R = 2 ohm and L = 4/3 H, exactly fitting the reported trace. A separate known C = 2 F period of 4pi s recovers L = 2 H, then R = 3 ohm and gain 1.5.
Open the experimentPredict
Why does an exact LR current-trace fit fail to prove the sensor gain is one?
Experiment
Fit the supplied trace under two different gain assumptions and show why both match. Retain an independent LC calculation and explicitly audit the known-capacitor, clock and unchanged-inductor premises. Submit a critique/revision pair and an unfamiliar changed response in the versioned course project, distinguishing generated evidence from real observation.
Discriminate a shared current-gain bias
Worked teaching model · synthetic values · Synthetic LR experiment has source 6 V and current sensor gain 1.5. The normalized time constant is unaffected by gain. A separate ideal LC period uses the same linear inductor and an independently known 2 F capacitor. No actual measurement or physical switching is implied.
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Reported LR current
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.
Reported LR current: numerical coordinates
| time (s) | reported current (A) |
|---|---|
| 0 | 0 |
| 0.0444444 | 0.193479 |
| 0.0888889 | 0.37448 |
| 0.133333 | 0.543808 |
| 0.177778 | 0.702215 |
| 0.222222 | 0.850406 |
| 0.266667 | 0.98904 |
| 0.311111 | 1.11873 |
| 0.355556 | 1.24006 |
| 0.4 | 1.35357 |
| 0.444444 | 1.45975 |
| 0.488889 | 1.55908 |
| 0.533333 | 1.65201 |
| 0.577778 | 1.73895 |
| 0.622222 | 1.82028 |
| 0.666667 | 1.89636 |
| 0.711111 | 1.96754 |
| 0.755556 | 2.03413 |
| 0.8 | 2.09642 |
| 0.844444 | 2.15469 |
| 0.888889 | 2.20921 |
| 0.933333 | 2.26021 |
| 0.977778 | 2.30792 |
| 1.02222 | 2.35255 |
| 1.06667 | 2.39431 |
| 1.11111 | 2.43337 |
| 1.15556 | 2.46992 |
| 1.2 | 2.5041 |
| 1.24444 | 2.53609 |
| 1.28889 | 2.566 |
| 1.33333 | 2.59399 |
| 1.37778 | 2.62018 |
| 1.42222 | 2.64467 |
| 1.46667 | 2.66759 |
| 1.51111 | 2.68903 |
| 1.55556 | 2.70908 |
| 1.6 | 2.72785 |
| 1.64444 | 2.7454 |
| 1.68889 | 2.76182 |
| 1.73333 | 2.77718 |
| 1.77778 | 2.79155 |
| 1.82222 | 2.80499 |
| 1.86667 | 2.81757 |
| 1.91111 | 2.82934 |
| 1.95556 | 2.84034 |
| 2 | 2.85064 |
| 2.04444 | 2.86027 |
| 2.08889 | 2.86928 |
| 2.13333 | 2.87771 |
| 2.17778 | 2.8856 |
| 2.22222 | 2.89298 |
| 2.26667 | 2.89988 |
| 2.31111 | 2.90634 |
| 2.35556 | 2.91238 |
| 2.4 | 2.91803 |
| 2.44444 | 2.92332 |
| 2.48889 | 2.92826 |
| 2.53333 | 2.93289 |
| 2.57778 | 2.93722 |
| 2.62222 | 2.94127 |
| 2.66667 | 2.94505 |
Naive model in reported-current units
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.
Naive model in reported-current units: numerical coordinates
| time (s) | predicted reported current (A) |
|---|---|
| 0 | 0 |
| 0.0444444 | 0.193479 |
| 0.0888889 | 0.37448 |
| 0.133333 | 0.543808 |
| 0.177778 | 0.702215 |
| 0.222222 | 0.850406 |
| 0.266667 | 0.98904 |
| 0.311111 | 1.11873 |
| 0.355556 | 1.24006 |
| 0.4 | 1.35357 |
| 0.444444 | 1.45975 |
| 0.488889 | 1.55908 |
| 0.533333 | 1.65201 |
| 0.577778 | 1.73895 |
| 0.622222 | 1.82028 |
| 0.666667 | 1.89636 |
| 0.711111 | 1.96754 |
| 0.755556 | 2.03413 |
| 0.8 | 2.09642 |
| 0.844444 | 2.15469 |
| 0.888889 | 2.20921 |
| 0.933333 | 2.26021 |
| 0.977778 | 2.30792 |
| 1.02222 | 2.35255 |
| 1.06667 | 2.39431 |
| 1.11111 | 2.43337 |
| 1.15556 | 2.46992 |
| 1.2 | 2.5041 |
| 1.24444 | 2.53609 |
| 1.28889 | 2.566 |
| 1.33333 | 2.59399 |
| 1.37778 | 2.62018 |
| 1.42222 | 2.64467 |
| 1.46667 | 2.66759 |
| 1.51111 | 2.68903 |
| 1.55556 | 2.70908 |
| 1.6 | 2.72785 |
| 1.64444 | 2.7454 |
| 1.68889 | 2.76182 |
| 1.73333 | 2.77718 |
| 1.77778 | 2.79155 |
| 1.82222 | 2.80499 |
| 1.86667 | 2.81757 |
| 1.91111 | 2.82934 |
| 1.95556 | 2.84034 |
| 2 | 2.85064 |
| 2.04444 | 2.86027 |
| 2.08889 | 2.86928 |
| 2.13333 | 2.87771 |
| 2.17778 | 2.8856 |
| 2.22222 | 2.89298 |
| 2.26667 | 2.89988 |
| 2.31111 | 2.90634 |
| 2.35556 | 2.91238 |
| 2.4 | 2.91803 |
| 2.44444 | 2.92332 |
| 2.48889 | 2.92826 |
| 2.53333 | 2.93289 |
| 2.57778 | 2.93722 |
| 2.62222 | 2.94127 |
| 2.66667 | 2.94505 |
| Quantity | Value | Unit |
|---|---|---|
| Observed asymptotic current | 3 | A reported |
| Observed normalized time constant | 0.666667 | s |
| Naive resistance assuming unit gain | 2 | ohm |
| Naive inductance assuming unit gain | 1.33333 | H |
| Independent LC period | 12.5664 | s |
| Period-based inductance | 2 | H |
| Cross-record resistance | 3 | ohm |
| Recovered current gain | 1.5 | ratio |
A biased model can fit the entire current trace exactly; an independent constitutive and timing record tests the hidden calibration assumption.
The LR trace determines L/R and gE/R, not L, R and gain separately. Assuming gain one rescales L and R by the same factor, preserving every point in the trace. An independent known-C LC period yields L, then the LR time constant yields R and the amplitude yields gain. If the capacitor or clock shares an unknown bias, this claimed independence must be reconsidered.
Derive before checking. Retain contrasting captures and explain one assumption that could fail; calculated evidence is not actual laboratory work.
A biased model can fit the entire current trace exactly; an independent constitutive and timing record tests the hidden calibration assumption.
The LR trace determines L/R and gE/R, not L, R and gain separately. Assuming gain one rescales L and R by the same factor, preserving every point in the trace. An independent known-C LC period yields L, then the LR time constant yields R and the amplitude yields gain. If the capacitor or clock shares an unknown bias, this claimed independence must be reconsidered.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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Public practice checks a specific claim. It does not establish independent mastery.
Which orientation, initial state, symmetry or independent calibration assumption would change this induction inference?
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