Infer a decay time separately from a voltage offset
A discharge trace can appear to approach a nonzero voltage because of a fixed instrument offset. The supplied true signal is 8exp(−t/2) V, but the indicated signal is Aexp(−t/τ)+o with A equal to instrument gain times true initial voltage. We deliberately keep the source generator visible for teaching while asking which parameters the observations alone identify.
Learning outcome: Compare offsets −1,0,+1 V at one gain and show which differences remain invariant. Then change gain and check that inferred τ remains the same while fitted amplitude changes. Freeze a third-second prediction and propose an independent reference to distinguish gain from initial voltage.
Starting recap
Use charge continuity, energy per charge, consistent SI units and an explicit circuit topology. Exponential responses are supplied algebraic models; initial state, source constraint and measurement loading must be declared.
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With gain1.1 and offset .5 V, the indicated amplitude is 8.8 V, but differences retain decay factor exp(−.5)≈.606531 and recover τ=2 s. The fit gives offset .5 V and amplitude8.8 V, not independent proof of gain1.1 or true initial8 V.
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The exponential trace alone identifies amplitude A as:
Experiment
Compare offsets −1,0,+1 V at one gain and show which differences remain invariant. Then change gain and check that inferred τ remains the same while fitted amplitude changes. Freeze a third-second prediction and propose an independent reference to distinguish gain from initial voltage.
Infer a decay time without mistaking voltage offset for leakage
Worked teaching model · synthetic values · Synthetic discharge true V=8 exp(−t/2) V at exact t=0,1,2 s, indicated V=gain times true V plus offset. Three samples fit one exponential with constant offset. Gain and true initial voltage are not separately identifiable without an independent reference.
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A common gain and offset can conceal a true discharge
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: offset exponential (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for A common gain and offset can conceal a true discharge
offset exponential
| time (s) | indicated voltage (V) |
|---|---|
| 0 | 9.3 |
| 0.15 | 8.66414 |
| 0.3 | 8.07423 |
| 0.45 | 7.52694 |
| 0.6 | 7.0192 |
| 0.75 | 6.54815 |
| 0.9 | 6.11113 |
| 1.05 | 5.70569 |
| 1.2 | 5.32954 |
| 1.35 | 4.98058 |
| 1.5 | 4.65683 |
| 1.65 | 4.35647 |
| 1.8 | 4.07781 |
| 1.95 | 3.81929 |
| 2.1 | 3.57945 |
| 2.25 | 3.35694 |
| 2.4 | 3.15051 |
| 2.55 | 2.95899 |
| 2.7 | 2.78131 |
| 2.85 | 2.61647 |
| 3 | 2.46355 |
| 3.15 | 2.32167 |
| 3.3 | 2.19004 |
| 3.45 | 2.06792 |
| 3.6 | 1.95463 |
| 3.75 | 1.84952 |
| 3.9 | 1.75201 |
| 4.05 | 1.66155 |
| 4.2 | 1.57762 |
| 4.35 | 1.49975 |
| 4.5 | 1.42751 |
| 4.65 | 1.36049 |
| 4.8 | 1.29832 |
| 4.95 | 1.24063 |
| 5.1 | 1.18712 |
| 5.25 | 1.13747 |
| 5.4 | 1.09141 |
| 5.55 | 1.04868 |
| 5.7 | 1.00903 |
| 5.85 | 0.972249 |
| 6 | 0.938126 |
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 |
|---|---|---|
| Indication at zero seconds | 9.3 | V |
| Indication at one second | 5.83747 | V |
| Indication at two seconds | 3.73734 | V |
| Successive difference ratio | 0.606531 | ratio |
| Recovered time constant | 2 | s |
| Recovered indicated exponential amplitude | 8.8 | V |
| Recovered offset | 0.5 | V |
| Predicted indication at three seconds | 2.46355 | V |
Differences remove a fixed offset; their ratio determines the decay factor under the single-exponential hypothesis.
With equally spaced times Delta t=1 s, successive differences have ratio exp(−Delta t/tau). The natural logarithm reverses the exponential: tau=−Delta t/ln(ratio). The fitted amplitude is gain times true initial voltage, so those two factors cannot be separated by this trace alone. A changed time constant might arise from capacitance, resistance or parallel leakage; an independent static resistance or capacitance reference is needed.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Differences remove a fixed offset; their ratio determines the decay factor under the single-exponential hypothesis.
With equally spaced times Delta t=1 s, successive differences have ratio exp(−Delta t/tau). The natural logarithm reverses the exponential: tau=−Delta t/ln(ratio). The fitted amplitude is gain times true initial voltage, so those two factors cannot be separated by this trace alone. A changed time constant might arise from capacitance, resistance or parallel leakage; an independent static resistance or capacitance reference is needed.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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Which independent observation could reject this model rather than merely refit its parameters?
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