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SCIENCE · INVESTIGATE AND EXPLAIN

Reconcile field pressure with source and separating work

For vacuum parallel plates in the no-fringe approximation, field energy density is ε0E²/2 and attractive pressure has the same numerical value in SI. The plates have area 0.01 m², initial gap 0.001 m and initial voltage 10 V. We change the gap slowly while declaring either fixed initial charge or maintained voltage; these are different mechanical experiments.

Learning outcome: Compare final gap ratios 0.5,1,1.5,2 under both constraints. Retain field, force, stored-energy change and source/external work separately. Verify the exact no-change state and explain why the sign of stored-energy change alone cannot establish force direction under maintained voltage.

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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Try

Let U0=ε0A(10 V)²/(2d0). Doubling the gap at fixed initial charge doubles stored energy, leaves attraction fixed and requires external work +U0. Doubling it at maintained voltage halves stored energy, returns U0 to the source and requires external work +U0/2. Attraction in the latter case is one quarter of its initial value.

Open the experiment

Predict

When the gap doubles at maintained voltage, how does ideal attraction change?

Experiment

Compare final gap ratios 0.5,1,1.5,2 under both constraints. Retain field, force, stored-energy change and source/external work separately. Verify the exact no-change state and explain why the sign of stored-energy change alone cannot establish force direction under maintained voltage.

Reconcile field stress with fixed-charge or fixed-voltage work

Worked teaching model · synthetic values · Ideal vacuum parallel plates area .01 m², initial gap .001 m and initial voltage10 V. Quasistatic change to the selected gap, with either fixed initial free charge or maintained10 V. No fringe, elastic, pull-in, breakdown or radiative model. External work is positive for increasing gap, negative for compression, and zero for unchanged gap; source work depends on the constraint. No capacitor handling.

Reset keeps your prediction, captures and practice history.

Electrostatic attraction under the selected constraint

attractive force (N)gap ratio to initial021.76839e-50

Unlike graph quantities rescale independently; read units and values, not screen angles. 1: field-energy stress (solid). Joined curves show the supplied model, not additional observations.

Equivalent numerical coordinates for Electrostatic attraction under the selected constraint

field-energy stress

gap ratio to initialattractive force (N)
0.51.76839e-5
0.518751.64286e-5
0.53751.53024e-5
0.556251.42882e-5
0.5751.33716e-5
0.593751.25404e-5
0.61251.17843e-5
0.631251.10947e-5
0.651.04638e-5
0.668759.88530e-6
0.68759.35346e-6
0.706258.86341e-6
0.7258.41088e-6
0.743757.99215e-6
0.76257.60393e-6
0.781257.24332e-6
0.86.90777e-6
0.818756.59500e-6
0.83756.30301e-6
0.856256.02999e-6
0.8755.77433e-6
0.893755.53459e-6
0.91255.30948e-6
0.931255.09783e-6
0.954.89858e-6
0.968754.71079e-6
0.98754.53360e-6
1.006254.36622e-6
1.0254.20794e-6
1.043754.05812e-6
1.06253.91615e-6
1.081253.78151e-6
1.13.65369e-6
1.118753.53225e-6
1.13753.41676e-6
1.156253.30685e-6
1.1753.20215e-6
1.193753.10235e-6
1.21253.00714e-6
1.231252.91625e-6
1.252.82942e-6
1.268752.74641e-6
1.28752.66700e-6
1.306252.59099e-6
1.3252.51817e-6
1.343752.44839e-6
1.36252.38147e-6
1.381252.31725e-6
1.42.25560e-6
1.418752.19637e-6
1.43752.13945e-6
1.456252.08471e-6
1.4752.03205e-6
1.493751.98135e-6
1.51251.93253e-6
1.531251.88550e-6
1.551.84015e-6
1.568751.79643e-6
1.58751.75424e-6
1.606251.71353e-6
1.6251.67421e-6
1.643751.63624e-6
1.66251.59954e-6
1.681251.56406e-6
1.71.52975e-6
1.718751.49655e-6
1.73751.46443e-6
1.756251.43333e-6
1.7751.40320e-6
1.793751.37402e-6
1.81251.34574e-6
1.831251.31832e-6
1.851.29174e-6
1.868751.26595e-6
1.88751.24092e-6
1.906251.21663e-6
1.9251.19304e-6
1.943751.17014e-6
1.96251.14788e-6
1.981251.12626e-6
21.10524e-6

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.

Calculated quantities under the declared measurement model
QuantityValueUnit
Final gap0.0015m
Final capacitance5.89463e-11F
Final voltage10V
Final free plate charge5.89463e-10C
Final gap field6666.667N/C
Attractive force magnitude1.96488e-6N
Field pressure0.0001964876Pa
Stored-energy change-1.47366e-9J
Source work during gap change-2.94731e-9J
External work during gap change1.47366e-9J
Energy residual0J

A fixed-charge gap change keeps the ideal field and attraction constant; fixed voltage gives a different force and source-energy account.

Vacuum energy density is epsilon0 E²/2, and the attractive pressure has the same numerical value in SI. At fixed Q, E=Q/(epsilon0 A) is constant and external work increases stored energy linearly with gap. At fixed V, C falls as1/d; the source work V DeltaQ is negative during separation, while external work is positive. Compression reverses both work signs; unchanged gap gives zero work. In both cases DeltaU=Wsource+Wexternal. Do not infer elastic stability, pull-in or breakdown from this rigid-plate energy model.

Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.

A fixed-charge gap change keeps the ideal field and attraction constant; fixed voltage gives a different force and source-energy account.

Vacuum energy density is epsilon0 E²/2, and the attractive pressure has the same numerical value in SI. At fixed Q, E=Q/(epsilon0 A) is constant and external work increases stored energy linearly with gap. At fixed V, C falls as1/d; the source work V DeltaQ is negative during separation, while external work is positive. Compression reverses both work signs; unchanged gap gives zero work. In both cases DeltaU=Wsource+Wexternal. Do not infer elastic stability, pull-in or breakdown from this rigid-plate energy model.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

State conductor and source constraints

For vacuum parallel plates in the no-fringe approximation, field energy density is ε0E²/2 and attractive pressure has the same numerical value in SI. The plates have area 0.01 m², initial gap 0.001 m and initial voltage 10 V. We change the gap slowly while declaring either fixed initial charge or maintained voltage; these are different mechanical experiments.

Derive charge, voltage and energy

At fixed Q, E=Q/(ε0A) stays constant and U=Q²d/(2ε0A), so external separating force is the constant Q²/(2ε0A). At fixed V, C=ε0A/d and E=V/d; attraction is ε0AV²/(2d²). Stored energy decreases when the gap grows, but that does not mean the plates spontaneously repel.

Check evidence and excluded mechanisms

The fixed-voltage source takes back charge during separation, so source work VΔQ is negative. External work is positive when the gap increases, negative when it decreases, and zero when unchanged. The complete account is ΔU=Wsource+Wexternal. The rigid-plate model contains no spring, elastic instability, pull-in, fringe or breakdown law. Its small mathematical forces and energies are not a physical handling or design recommendation.

Worked original case

Let U0=ε0A(10 V)²/(2d0). Doubling the gap at fixed initial charge doubles stored energy, leaves attraction fixed and requires external work +U0. Doubling it at maintained voltage halves stored energy, returns U0 to the source and requires external work +U0/2. Attraction in the latter case is one quarter of its initial value.

Investigation

Compare final gap ratios 0.5,1,1.5,2 under both constraints. Retain field, force, stored-energy change and source/external work separately. Verify the exact no-change state and explain why the sign of stored-energy change alone cannot establish force direction under maintained voltage.

Changed-case practice

Try the changed case before feedback

When the gap doubles at fixed initial charge, find the final-to-initial voltage ratio.

This practice is public and unsaved. A matching number does not verify understanding. Retain your explanation, assumptions and changed-case evidence in the separate course workspace.

Sources and boundaries

Original derivations and synthetic numerical packets checked 30 October 2026 against the primary explanation. No charged-capacitor handling, high-voltage apparatus, material safety limit or practical certification is requested. Preserve first predictions, independent critique, revision and newly assigned work separately from public practice feedback.

Apply

When the gap doubles at maintained voltage, how does ideal attraction change?

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Which geometry, calibration or source assumption could fail while an exact arithmetic fit remains possible?

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