Keep source potential separate from pair energy
Potential is a scalar source property at a point, with units joules per coulomb. The potential created by several point charges is the signed sum kQ_i/r_i. Multiplying that potential by a newly introduced passive charge gives its interaction energy with those sources. It does not automatically include energy already stored in interactions among the original sources.
Learning outcome: Compare third charges −3,0,+3 nC at one geometry. Retain first-pair energy and third-insertion work separately. Then double L. Explain why removing the third charge leaves nonzero first-pair energy even though the third insertion term vanishes.
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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At a=−1 nC and L=2 m, the dimensionless pair coefficient is 2−2−1/√2=−1/√2. The total is −k×10⁻¹⁸/(2√2)≈−3.17757941 nJ. The first positive pair stores positive energy, but adding the negative charge releases a larger amount.
Open the experimentPredict
In the total energy of three distinct point charges, each unordered pair appears:
Experiment
Compare third charges −3,0,+3 nC at one geometry. Retain first-pair energy and third-insertion work separately. Then double L. Explain why removing the third charge leaves nonzero first-pair energy even though the third insertion term vanishes.
Compare source potential with whole-system pair energy
Worked teaching model · synthetic values · Fixed charges +2 nC at (0,0), +1 nC at (L,0), selected charge at (0,L). Zero potential at infinity. Distinct point-source interaction energy excludes self-energy; external assembly is quasistatic.
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Total energy under uniform dilation
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: unordered pair sum (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Total energy under uniform dilation
unordered pair sum
| side scale (m) | pair energy (J) |
|---|---|
| 1 | -6.35516e-9 |
| 1.05 | -6.05253e-9 |
| 1.1 | -5.77742e-9 |
| 1.15 | -5.52623e-9 |
| 1.2 | -5.29597e-9 |
| 1.25 | -5.08413e-9 |
| 1.3 | -4.88858e-9 |
| 1.35 | -4.70753e-9 |
| 1.4 | -4.5394e-9 |
| 1.45 | -4.38287e-9 |
| 1.5 | -4.23677e-9 |
| 1.55 | -4.1001e-9 |
| 1.6 | -3.97197e-9 |
| 1.65 | -3.85161e-9 |
| 1.7 | -3.73833e-9 |
| 1.75 | -3.63152e-9 |
| 1.8 | -3.53064e-9 |
| 1.85 | -3.43522e-9 |
| 1.9 | -3.34482e-9 |
| 1.95 | -3.25906e-9 |
| 2 | -3.17758e-9 |
| 2.05 | -3.10008e-9 |
| 2.1 | -3.02627e-9 |
| 2.15 | -2.95589e-9 |
| 2.2 | -2.88871e-9 |
| 2.25 | -2.82452e-9 |
| 2.3 | -2.76311e-9 |
| 2.35 | -2.70432e-9 |
| 2.4 | -2.64798e-9 |
| 2.45 | -2.59394e-9 |
| 2.5 | -2.54206e-9 |
| 2.55 | -2.49222e-9 |
| 2.6 | -2.44429e-9 |
| 2.65 | -2.39817e-9 |
| 2.7 | -2.35376e-9 |
| 2.75 | -2.31097e-9 |
| 2.8 | -2.2697e-9 |
| 2.85 | -2.22988e-9 |
| 2.9 | -2.19143e-9 |
| 2.95 | -2.15429e-9 |
| 3 | -2.11839e-9 |
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 |
|---|---|---|
| Potential at third site before insertion | 12.1651 | V |
| Work to add selected third charge | -1.21651e-8 | J |
| First pair interaction energy | 8.98755e-9 | J |
| Total pair interaction energy | -3.17758e-9 | J |
| System total charge | 2 | nC |
| Energy after doubling all separations | -1.58879e-9 | J |
Source potential at a site is not the same object as total interaction energy of all charges.
The three distances are L, L and sqrt(2)L. Sum each pair once. Adding the third charge costs q3 times the potential of the first two, not its own singular self-potential. Negative assembly work means energy is released under the quasistatic external convention. Equal total charge does not determine interaction energy, which also depends on geometry and pair products.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Source potential at a site is not the same object as total interaction energy of all charges.
The three distances are L, L and sqrt(2)L. Sum each pair once. Adding the third charge costs q3 times the potential of the first two, not its own singular self-potential. Negative assembly work means energy is released under the quasistatic external convention. Equal total charge does not determine interaction energy, which also depends on geometry and pair products.
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