Account for charge across an object and its reservoir
Charge accounting begins by choosing recipients and drawing the system boundary. In this packet A, B and a reservoir start neutral. Moving n electrons from A to B leaves A with +ne and gives B −ne. If the reservoir then supplies another m electrons to B, the three final charges are +ne, −(n+m)e and +me. Their total is zero even though the A+B subsystem now has negative charge. Charge has crossed that smaller boundary; it has not been created.
Learning outcome: Hold the first transfer at four electrons and compare reservoir transfers zero, two and six. Retain both subsystem and full-system totals. Draw a separate neutral-polarization picture with no net transferred charge, and explain why an attraction observation would not uniquely identify net sign.
Starting recap
Use signed charge, common coordinate axes, SI units, vector components and algebraic ratios. Separate a source field from probe force and a fitted parameter from independently tested evidence.
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Move four electrons A→B and two reservoir→B. The final ledger in units e is A +4, B −6, reservoir +2. The A+B charge is −2e=−3.204353268×10⁻¹⁹ C; the complete ledger remains zero.
Open the experimentPredict
After electrons enter B from an external reservoir, which conservation statement is valid?
Experiment
Hold the first transfer at four electrons and compare reservoir transfers zero, two and six. Retain both subsystem and full-system totals. Draw a separate neutral-polarization picture with no net transferred charge, and explain why an attraction observation would not uniquely identify net sign.
Close an electron and reservoir charge ledger
Worked teaching model · synthetic values · Three initially neutral recipients A, B and reservoir R. Only specified electron transfers occur; positive ionic nuclei remain fixed. Elementary charge e=1.602176634e−19 C. No actual charging or grounding activity.
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Include the recipient that exchanges charge
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: signed recipient ledger (open markers). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Include the recipient that exchanges charge
signed recipient ledger
| recipient index (1 A, 2 B, 3 reservoir) | net charge / e |
|---|---|
| 1 | 4 |
| 2 | -6 |
| 3 | 2 |
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 |
|---|---|---|
| A net charge | 6.40871e-19 | C |
| B net charge | -9.61306e-19 | C |
| Reservoir net charge | 3.20435e-19 | C |
| A plus B net charge | -3.20435e-19 | C |
| Whole closed system net charge | 0 | C |
| Transferred electrons counted | 6 | count |
A subsystem can gain charge while the full recipient ledger conserves it.
Removing electrons leaves positive net charge; adding electrons gives negative charge. Electron count is integer here, not a continuous fraction. Neutral polarization separates bound or mobile charge within an object without changing its total. Grounding in a different model exchanges charge with a reservoir; it does not destroy charge or always mean zero object charge.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
A subsystem can gain charge while the full recipient ledger conserves it.
Removing electrons leaves positive net charge; adding electrons gives negative charge. Electron count is integer here, not a continuous fraction. Neutral polarization separates bound or mobile charge within an object without changing its total. Grounding in a different model exchanges charge with a reservoir; it does not destroy charge or always mean zero object charge.
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Which independent observation could reject this model rather than merely refit its parameters?
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