Separate geometric slope from a parallel stray capacitance
Capacitance measured at one gap cannot by itself separate geometric capacitance from an added parallel stray term. The synthetic family is C=S/d+Cs, with d in independently exact millimetres, C in picofarads and S in pF mm. Gain is stipulated calibrated. Two distinct gaps fit its two parameters; a third gap is reserved for validation.
Learning outcome: Freeze the third-gap prediction after fitting only the first two records. Compare several stray values without changing S. Propagate reading bounds, then derive the direct third-prediction formula in terms of C1,C2 to avoid treating correlated parameter intervals as independent.
Starting recap
Review charge conservation, conductor equipotential conditions, definite field integrals and energy derivatives under a stated electrical constraint. Convert capacitance and charge units before interpreting small energies.
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For S=20 pF mm and Cs=4 pF, the first two readings are 24 and14 pF. Their fitted parameters predict the third reading 32/3≈10.666667 pF at3 mm. The separate compatible intervals are S=20±0.4 pF mm and Cs=4±0.3 pF, not probabilistic confidence intervals.
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Which record is fresh validation of the stated two-parameter fit?
Experiment
Freeze the third-gap prediction after fitting only the first two records. Compare several stray values without changing S. Propagate reading bounds, then derive the direct third-prediction formula in terms of C1,C2 to avoid treating correlated parameter intervals as independent.
Separate geometric capacitance from a parallel stray term
Worked teaching model · synthetic values · Synthetic indicated capacitance C=S/d+Cstray at independently exact gaps1 and2 mm; reserve3 mm for validation. Gain is stipulated calibrated. Two readings identify S and stray within this model, not a gap-zero error or arbitrary dielectric geometry. Independent reading-error bounds ±.1 pF; all units are explicit.
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Inverse-gap calibration with a withheld third gap
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: model fitted only to first two gaps (solid).2: fresh third observation (open-circle marked location). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Inverse-gap calibration with a withheld third gap
model fitted only to first two gaps
| gap (mm) | indicated capacitance (pF) |
|---|---|
| 1 | 24 |
| 1.025 | 23.5122 |
| 1.05 | 23.04762 |
| 1.075 | 22.60465 |
| 1.1 | 22.18182 |
| 1.125 | 21.77778 |
| 1.15 | 21.3913 |
| 1.175 | 21.02128 |
| 1.2 | 20.66667 |
| 1.225 | 20.32653 |
| 1.25 | 20 |
| 1.275 | 19.68627 |
| 1.3 | 19.38462 |
| 1.325 | 19.09434 |
| 1.35 | 18.81481 |
| 1.375 | 18.54545 |
| 1.4 | 18.28571 |
| 1.425 | 18.03509 |
| 1.45 | 17.7931 |
| 1.475 | 17.55932 |
| 1.5 | 17.33333 |
| 1.525 | 17.11475 |
| 1.55 | 16.90323 |
| 1.575 | 16.69841 |
| 1.6 | 16.5 |
| 1.625 | 16.30769 |
| 1.65 | 16.12121 |
| 1.675 | 15.9403 |
| 1.7 | 15.76471 |
| 1.725 | 15.5942 |
| 1.75 | 15.42857 |
| 1.775 | 15.26761 |
| 1.8 | 15.11111 |
| 1.825 | 14.9589 |
| 1.85 | 14.81081 |
| 1.875 | 14.66667 |
| 1.9 | 14.52632 |
| 1.925 | 14.38961 |
| 1.95 | 14.25641 |
| 1.975 | 14.12658 |
| 2 | 14 |
| 2.025 | 13.87654 |
| 2.05 | 13.7561 |
| 2.075 | 13.63855 |
| 2.1 | 13.52381 |
| 2.125 | 13.41176 |
| 2.15 | 13.30233 |
| 2.175 | 13.1954 |
| 2.2 | 13.09091 |
| 2.225 | 12.98876 |
| 2.25 | 12.88889 |
| 2.275 | 12.79121 |
| 2.3 | 12.69565 |
| 2.325 | 12.60215 |
| 2.35 | 12.51064 |
| 2.375 | 12.42105 |
| 2.4 | 12.33333 |
| 2.425 | 12.24742 |
| 2.45 | 12.16327 |
| 2.475 | 12.08081 |
| 2.5 | 12 |
| 2.525 | 11.92079 |
| 2.55 | 11.84314 |
| 2.575 | 11.76699 |
| 2.6 | 11.69231 |
| 2.625 | 11.61905 |
| 2.65 | 11.54717 |
| 2.675 | 11.47664 |
| 2.7 | 11.40741 |
| 2.725 | 11.33945 |
| 2.75 | 11.27273 |
| 2.775 | 11.20721 |
| 2.8 | 11.14286 |
| 2.825 | 11.07965 |
| 2.85 | 11.01754 |
| 2.875 | 10.95652 |
| 2.9 | 10.89655 |
| 2.925 | 10.83761 |
| 2.95 | 10.77966 |
| 2.975 | 10.72269 |
| 3 | 10.66667 |
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.
fresh third observation
| gap (mm) | indicated capacitance (pF) |
|---|---|
| 3 | 10.66667 |
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 |
|---|---|---|
| First capacitance reading at 1 mm | 24 | pF |
| Second capacitance reading at 2 mm | 14 | pF |
| Inferred geometry coefficient | 20 | pF mm |
| Inferred constant stray | 4 | pF |
| Fresh withheld reading at 3 mm | 10.66667 | pF |
| Prediction from the first two readings | 10.66667 | pF |
| Withheld observed minus predicted | 0 | pF |
| Geometry coefficient lower bound | 19.6 | pF mm |
| Geometry coefficient upper bound | 20.4 | pF mm |
| Stray lower bound | 3.7 | pF |
| Stray upper bound | 4.3 | pF |
| Inferred area | 0.002261947 | m² |
Two exact-gap readings separate a geometric slope from a constant parallel stray term; a third gap tests that fitted family.
At gaps1 and2 mm, C1=S+Cs and C2=S/2+Cs, so S=2(C1−C2), Cs=2C2−C1. Independent ±0.1 pF errors give S bound±0.4 pF mm and Cs bound±0.3 pF by absolute coefficient sums; these individual intervals are correlated and must not be treated as an independent rectangle for further inference. A gap-zero error or gain error requires a new model and independent information, not relabeling Cs as proof.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Two exact-gap readings separate a geometric slope from a constant parallel stray term; a third gap tests that fitted family.
At gaps1 and2 mm, C1=S+Cs and C2=S/2+Cs, so S=2(C1−C2), Cs=2C2−C1. Independent ±0.1 pF errors give S bound±0.4 pF mm and Cs bound±0.3 pF by absolute coefficient sums; these individual intervals are correlated and must not be treated as an independent rectangle for further inference. A gap-zero error or gain error requires a new model and independent information, not relabeling Cs as proof.
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