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NEET UG · Physics

Electric potential and capacitance

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NEET UG · Physics

Continue studying Electric Potential And Capacitance

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Choose work signs and decide what stays fixed before solving a capacitor change, with original diagrams, worked examples and self-checks. Potential work and capacitor constraints: a NEET decision guide

About 5 min · NEET UG

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Potential work and capacitor constraints: a NEET decision guide

Choose work signs and decide what stays fixed before solving a capacitor change, with original diagrams, worked examples and self-checks.

What you will understand

For NEET UG students: decide the signs of potential-energy change and field work, then choose the quantity that stays fixed when a capacitor changes.

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Quick answer: write the constraint before a formula

For a test charge moved from A to B, ΔV=VB−VA\Delta V=V_B-V_A, ΔU=qΔV\Delta U=q\Delta V and Wfield=−ΔUW_\mathrm{field}=-\Delta U. For a linear capacitor, use Q=CVQ=CV and U=Q2/(2C)=CV2/2U=Q^2/(2C)=CV^2/2. Here QQ is the magnitude of the free charge on either plate and VV is the voltage magnitude between the plates. A connected ideal battery fixes VV; an isolated disconnected capacitor with no leakage fixes QQ. Those are different experiments.

Read the potential drop before the work sign

A uniform rightward electric field is 200 volts per metre. Point A is at 100 volts and point B, 0.20 metre to the right, is at 60 volts, so the potential change from A to B is minus 40 volts. For plus 2 microcoulombs, the potential-energy change is minus 80 microjoules and field work is plus 80 microjoules. For minus 2 microcoulombs, the energy change is plus 80 microjoules and field work minus 80 microjoules. External work equals the energy change only for quasi-static motion with no kinetic-energy change or other work. Diagram is schematic.
A fixed potential drop gives opposite energy changes for opposite test-charge signs.

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A negative charge moves toward lower potential

In a uniform rightward field, A is at 100 V100\,\mathrm V and B, 0.20 m0.20\,\mathrm m to its right, is at 60 V60\,\mathrm V. Thus Ex=−ΔV/Δx=+200 V/mE_x=-\Delta V/\Delta x=+200\,\mathrm{V/m}. Move q=−2 μCq=-2\,\mu\mathrm C from A to B: ΔU=(−2×10−6)(60−100)=+80 μJ\Delta U=(-2\times10^{-6})(60-100)=+80\,\mu\mathrm J, so Wfield=−80 μJW_\mathrm{field}=-80\,\mu\mathrm J. The field points right but the force on this negative charge points left. Quasi-static external work is +80 μJ+80\,\mu\mathrm J if no other force does work and kinetic energy does not change.

Know what changes capacitance

For ideal parallel plates with area AA, gap dd and a linear homogeneous dielectric completely filling that gap, C=Kϵ0A/dC=K\epsilon_0A/d. Neglect fringing. KK is relative permittivity. Capacitance depends on geometry and material in this model, not on whichever QQ and VV happen to be present. Inserting K=2K=2 at unchanged geometry doubles CC; it does not by itself tell you whether QQ or VV doubles.

Compare the disconnected and connected experiments

Two separate ideal capacitors initially have capacitance 2 microfarads, voltage 6 volts, charge magnitude 12 microcoulombs and stored energy 36 microjoules. A homogeneous linear dielectric with relative permittivity K=2 completely fills each gap at unchanged geometry. For the disconnected isolated capacitor, charge stays 12 microcoulombs: capacitance becomes 4 microfarads, voltage 3 volts and energy 18 microjoules. With the ideal 6 volt battery connected, capacitance becomes 4 microfarads, charge 24 microcoulombs and energy 72 microjoules. The battery exchanges energy and charge. No leakage or edge effects are included; drawings are schematic.
Same capacitance change; the battery connection determines the fixed quantity.

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Disconnect first: fixed charge

Initially C0=2 μFC_0=2\,\mu\mathrm F and V0=6 VV_0=6\,\mathrm V, so Q0=C0V0=12 μCQ_0=C_0V_0=12\,\mu\mathrm C and U0=C0V02/2=36 μJU_0=C_0V_0^2/2=36\,\mu\mathrm J. Disconnect the battery, isolate the plates with no leakage, and fully fill the gap with K=2K=2 dielectric at unchanged geometry. Then C=4 μFC=4\,\mu\mathrm F, Q=12 μCQ=12\,\mu\mathrm C, V=Q/C=3 VV=Q/C=3\,\mathrm V and U=Q2/(2C)=18 μJU=Q^2/(2C)=18\,\mu\mathrm J. Fixed QQ makes energy inversely proportional to capacitance. The decreased capacitor energy can be transferred mechanically during insertion; do not claim it disappears.

Keep the battery connected: fixed voltage

Start with a separate identical 2 μF2\,\mu\mathrm F capacitor across the ideal 6 V6\,\mathrm V battery. Keep the battery attached while fully inserting K=2K=2 at unchanged geometry. CC again becomes 4 μF4\,\mu\mathrm F, but V=6 VV=6\,\mathrm V stays fixed, so Q=24 μCQ=24\,\mu\mathrm C and U=CV2/2=72 μJU=CV^2/2=72\,\mu\mathrm J. This is twice the initial stored energy. The battery supplies extra charge: ΔQ=12 μC\Delta Q=12\,\mu\mathrm C, with electrical work VΔQ=72 μJV\Delta Q=72\,\mu\mathrm J. Only 36 μJ36\,\mu\mathrm J is the capacitor-energy increase; the rest is accounted for by mechanical transfer and any dissipation in the actual insertion process. Capacitor energy alone is not conserved.

Common mistakes: identify the omitted condition

Wrong: “Dielectric always decreases capacitor energy.” Correct: it decreases energy for the isolated fixed-charge experiment but increases it at fixed voltage. Wrong: “Connected means charge stays fixed.” Correct: charge can flow through the battery leads. Wrong: use E=ΔV/dE=\Delta V/d without signs for an arbitrary direction. Correct: the field component is −dV/dx-dV/dx; a magnitude formula needs the appropriate direction and uniform-field assumption. Wrong: external work always equals qΔVq\Delta V. Correct: if kinetic energy changes and only electric and external work act, Wext=ΔK+ΔUW_\mathrm{ext}=\Delta K+\Delta U.

Try it: one charge, two signs

Move q=+3 μCq=+3\,\mu\mathrm C from A at 20 V20\,\mathrm V to B at −10 V-10\,\mathrm V. Find ΔU\Delta U and work by the field. What would quasi-static external work be if there is no other work?

Reveal the answer

ΔV=−30 V\Delta V=-30\,\mathrm V, hence ΔU=−90 μJ\Delta U=-90\,\mu\mathrm J and Wfield=+90 μJW_\mathrm{field}=+90\,\mu\mathrm J. With no kinetic-energy change and no other work, Wext=−90 μJW_\mathrm{ext}=-90\,\mu\mathrm J: the external agent removes energy. Reversing the charge sign would reverse all three work/energy signs, not the source potential difference.

Try it: double the gap after disconnecting

A vacuum parallel-plate capacitor is initially 3 μF3\,\mu\mathrm F at 4 V4\,\mathrm V. Disconnect and isolate it with no leakage, then double the plate gap while retaining the plate area. Neglect fringing. Find its new capacitance, charge, voltage and stored energy.

Reveal the answer

Initially Q=12 μCQ=12\,\mu\mathrm C and U=24 μJU=24\,\mu\mathrm J. Since C∝1/dC\propto1/d, the new C=1.5 μFC=1.5\,\mu\mathrm F. Charge remains 12 μC12\,\mu\mathrm C, so V=8 VV=8\,\mathrm V and U=48 μJU=48\,\mu\mathrm J. Separating attracted plates requires positive external work in the quasi-static ideal model. The fixed-voltage result would be a different experiment.

NEET recall: make a constraint table

Rebuild three rows from memory: connected battery → fixed voltage; disconnected and isolated with no leakage → fixed charge; full homogeneous dielectric at unchanged geometry → capacitance multiplied by KK. Then derive the remaining quantities with Q=CVQ=CV and one energy expression. Use the diagram only after you have predicted whether voltage, charge and energy rise or fall.

Come back tomorrow: solve the other experiment

Re-solve the gap-doubling self-check while keeping the ideal 4 V4\,\mathrm V battery connected. Predict the changes first. The result is C=1.5 μFC=1.5\,\mu\mathrm F, Q=6 μCQ=6\,\mu\mathrm C and U=12 μJU=12\,\mu\mathrm J. Explain why these differ from the disconnected answers. Continue with broad chapter practice below; these links are not a dedicated dielectric set or a promise of every JEE question format.

Sources and review

Technical review: Codex (automated). Primary textbook sources checked on 23 October 2026. Numerical examples, self-checks and diagrams are original. Human subject review is not claimed.

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