Infer an unknown charge from spatial force data
A single force reading can fit many explanations: a larger source charge, a shorter separation or a sensor offset. To distinguish them, keep the probe charge fixed and compare several known separations. For point charges in vacuum, the magnitude is F=k|Qq|/r², where r is center-to-center separation and k=8.99×10⁹ N m²/C². Like signs repel and opposite signs attract along their line of separation.
Learning outcome: Capture source=3 at offsets 0 and 2 µN. Compare fitted charge, intercept and the nearest-reading estimate that ignores bias. Propose a separate check that could expose a wrong distance origin.
Starting recap
Use signed charge, vector components, inverse-square ratios and energy conservation. Distinguish potential from potential energy and name the system boundary.
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Try
Ignoring the stipulated reading errors, a +3 nC source and +2 nC probe at 0.10 m repel with 5.394 µN. At 0.20 m the force is 1.3485 µN. A +1 µN offset changes those readings to 6.394 and 2.3485 µN: their ratio is no longer four, although the inverse-square slope is unchanged.
Open the experimentPredict
Will adding the same 2 µN to every reading alter the fitted charge when an intercept is allowed?
Experiment
Capture source=3 at offsets 0 and 2 µN. Compare fitted charge, intercept and the nearest-reading estimate that ignores bias. Propose a separate check that could expose a wrong distance origin.
Infer charge without mistaking offset for inverse-square force
Worked teaching model · synthetic values · Positive 2 nC probe held at 0.10, 0.15, 0.20 and 0.25 m from an isolated positive point source. Outward force is positive. Original synthetic errors [0.10,−0.10,−0.10,0.10] µN. Fit signed force versus inverse squared separation, allowing an intercept. No hazardous apparatus is requested.
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Axes rescale with settings; compare numerical values, not screen angles or apparent lengths. Solid/points show the selected model relationship or observations; the dashed comparison is explained below.
| Quantity | Value | Unit |
|---|---|---|
| Fitted charge | 3.0608 | nC |
| Fitted sensor intercept | 0.94932 | µN |
| Largest force residual | 0.13319 | µN |
| Single nearest-reading inferred charge ignoring offset | 3.6118 | nC |
Accessible plot coordinates
| inverse squared separation (m⁻²) | signed outward force (µN) |
|---|---|
| 100 | 6.494 |
| 44.444 | 3.2973 |
| 25 | 2.2485 |
| 16 | 1.963 |
| inverse squared separation (m⁻²) | signed outward force (µN) |
|---|---|
| 100 | 6.4526 |
| 44.444 | 3.3952 |
| 25 | 2.3251 |
| 16 | 1.8299 |
A constant offset changes the intercept, not the fitted inverse-square slope.
The small fixed synthetic errors still affect the inferred slope. Agreement with this model does not prove isolation of a real source; position error and unwanted fields remain alternative explanations. Points are ordered by measurement radius, so this profile is a data connection, not a time trace.
A constant offset changes the intercept, not the fitted inverse-square slope.
The small fixed synthetic errors still affect the inferred slope. Agreement with this model does not prove isolation of a real source; position error and unwanted fields remain alternative explanations. Points are ordered by measurement radius, so this profile is a data connection, not a time trace.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
Understand
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Public practice checks a specific claim. It does not establish independent mastery.
Why does a small residual not prove that the point-charge model or the distance calibration is correct?
Continue
Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.
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