Keep battery work in an energy-derived force
An energy derivative gives mechanical force only after the electrical constraint is stated. The supplied lateral-overlap approximation is C(x)=C0[1+3x/ell], with C0=100 pF and ell=0.1 m. It corresponds to relative permittivity 4 occupying part of a plate area at the same gap. Initial voltage at zero overlap is 10 V.
Learning outcome: Compare fixed charge and fixed voltage at overlap fractions 0,0.5,1. Retain source work, stored-energy change and external work before inferring force. Explain why the same geometric Cprime does not make force independent of the electrical constraint.
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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At half overlap, C=250 pF. With maintained 10 V, source work from zero overlap is 15 nJ, stored-energy increase is 7.5 nJ and external work is −7.5 nJ; pull is 150 nN. With fixed initial charge 1 nC, voltage instead becomes 4 V and the pull is 24 nN.
Open the experimentPredict
At maintained voltage, why is stored-energy change alone insufficient to infer mechanical work?
Experiment
Compare fixed charge and fixed voltage at overlap fractions 0,0.5,1. Retain source work, stored-energy change and external work before inferring force. Explain why the same geometric Cprime does not make force independent of the electrical constraint.
Differentiate capacitance while retaining source work
Worked teaching model · synthetic values · Lateral dielectric overlap of ideal plates length .1 m. C(x)=100 pF[1+3x/.1], corresponding to relative permittivity4 and equal gap. Initial voltage10 V at zero overlap. Slow lossless motion. Bulk-capacitance approximation estimates energy/force; actual edge fields transmit the force and are not resolved. No insertion procedure.
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Energy-derived force under the selected constraint
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: fixed-charge or fixed-voltage energy derivative (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Energy-derived force under the selected constraint
fixed-charge or fixed-voltage energy derivative
| overlap fraction | force toward greater overlap (N) |
|---|---|
| 0 | 1.50000e-7 |
| 0.0125 | 1.50000e-7 |
| 0.025 | 1.50000e-7 |
| 0.0375 | 1.50000e-7 |
| 0.05 | 1.50000e-7 |
| 0.0625 | 1.50000e-7 |
| 0.075 | 1.50000e-7 |
| 0.0875 | 1.50000e-7 |
| 0.1 | 1.50000e-7 |
| 0.1125 | 1.50000e-7 |
| 0.125 | 1.50000e-7 |
| 0.1375 | 1.50000e-7 |
| 0.15 | 1.50000e-7 |
| 0.1625 | 1.50000e-7 |
| 0.175 | 1.50000e-7 |
| 0.1875 | 1.50000e-7 |
| 0.2 | 1.50000e-7 |
| 0.2125 | 1.50000e-7 |
| 0.225 | 1.50000e-7 |
| 0.2375 | 1.50000e-7 |
| 0.25 | 1.50000e-7 |
| 0.2625 | 1.50000e-7 |
| 0.275 | 1.50000e-7 |
| 0.2875 | 1.50000e-7 |
| 0.3 | 1.50000e-7 |
| 0.3125 | 1.50000e-7 |
| 0.325 | 1.50000e-7 |
| 0.3375 | 1.50000e-7 |
| 0.35 | 1.50000e-7 |
| 0.3625 | 1.50000e-7 |
| 0.375 | 1.50000e-7 |
| 0.3875 | 1.50000e-7 |
| 0.4 | 1.50000e-7 |
| 0.4125 | 1.50000e-7 |
| 0.425 | 1.50000e-7 |
| 0.4375 | 1.50000e-7 |
| 0.45 | 1.50000e-7 |
| 0.4625 | 1.50000e-7 |
| 0.475 | 1.50000e-7 |
| 0.4875 | 1.50000e-7 |
| 0.5 | 1.50000e-7 |
| 0.5125 | 1.50000e-7 |
| 0.525 | 1.50000e-7 |
| 0.5375 | 1.50000e-7 |
| 0.55 | 1.50000e-7 |
| 0.5625 | 1.50000e-7 |
| 0.575 | 1.50000e-7 |
| 0.5875 | 1.50000e-7 |
| 0.6 | 1.50000e-7 |
| 0.6125 | 1.50000e-7 |
| 0.625 | 1.50000e-7 |
| 0.6375 | 1.50000e-7 |
| 0.65 | 1.50000e-7 |
| 0.6625 | 1.50000e-7 |
| 0.675 | 1.50000e-7 |
| 0.6875 | 1.50000e-7 |
| 0.7 | 1.50000e-7 |
| 0.7125 | 1.50000e-7 |
| 0.725 | 1.50000e-7 |
| 0.7375 | 1.50000e-7 |
| 0.75 | 1.50000e-7 |
| 0.7625 | 1.50000e-7 |
| 0.775 | 1.50000e-7 |
| 0.7875 | 1.50000e-7 |
| 0.8 | 1.50000e-7 |
| 0.8125 | 1.50000e-7 |
| 0.825 | 1.50000e-7 |
| 0.8375 | 1.50000e-7 |
| 0.85 | 1.50000e-7 |
| 0.8625 | 1.50000e-7 |
| 0.875 | 1.50000e-7 |
| 0.8875 | 1.50000e-7 |
| 0.9 | 1.50000e-7 |
| 0.9125 | 1.50000e-7 |
| 0.925 | 1.50000e-7 |
| 0.9375 | 1.50000e-7 |
| 0.95 | 1.50000e-7 |
| 0.9625 | 1.50000e-7 |
| 0.975 | 1.50000e-7 |
| 0.9875 | 1.50000e-7 |
| 1 | 1.50000e-7 |
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 |
|---|---|---|
| Capacitance | 2.50000e-10 | F |
| Voltage | 10 | V |
| Free plate charge | 2.50000e-9 | C |
| Stored energy | 1.25000e-8 | J |
| Source work from zero overlap | 1.50000e-8 | J |
| External quasistatic work from zero overlap | -7.50000e-9 | J |
| Pull toward increased overlap | 1.50000e-7 | N |
| Energy residual | 0 | J |
At fixed voltage the source contributes work, so differentiating stored energy alone gives the wrong mechanical sign.
The parallel-area approximation gives C=C0[1+(kappa−1)x/ell]. At fixed charge, F=−d(Q²/2C)/dx=Q² Cprime/(2C²). At maintained voltage, source work is V² dC while stored energy rises by V²dC/2, leaving positive mechanical output Fdx=V²dC/2. The external agent work is negative during insertion. Actual edge fields transmit this force; the bulk approximation does not resolve them or authorize handling.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
At fixed voltage the source contributes work, so differentiating stored energy alone gives the wrong mechanical sign.
The parallel-area approximation gives C=C0[1+(kappa−1)x/ell]. At fixed charge, F=−d(Q²/2C)/dx=Q² Cprime/(2C²). At maintained voltage, source work is V² dC while stored energy rises by V²dC/2, leaving positive mechanical output Fdx=V²dC/2. The external agent work is negative during insertion. Actual edge fields transmit this force; the bulk approximation does not resolve them or authorize handling.
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