Mistake Master

Capacitors

A capacitor stores $+Q$ and $-Q$ on two conductors, and $C = Q/V$ is fixed by geometry alone: $C = \varepsilon_0 A/d$ for parallel plates, with no $Q$ and no $V$ in it. The charge collects on the facing inner surfaces, the field is $\sigma/\varepsilon_0$ in the gap and zero outside, and no charge crosses the gap. Series capacitors share $Q$ and add reciprocally; parallel capacitors share $V$ and add directly, the mirror of the resistor rules. The stored energy is $Q^2/2C = \tfrac12 QV = \tfrac12 CV^2$, three forms of one quantity that stop agreeing about the DIRECTION of a change as soon as the capacitor is altered.

The errors cluster. Reading $C = Q/V$ as a recipe, so that more charge means more capacitance. Adding series capacitances directly, or handing series capacitors equal voltages instead of equal charge. Using the full gap field to compute the force on a plate, which double-counts, or using half of it for a charge placed in the gap. Painting charge on both faces of each plate. Running a steady current through the insulating gap. And the largest one: quoting an energy change from a formula whose variable is not the one the wiring holds fixed, which reverses the sign of the answer.

first question of every capacitor problem: what is clamped? BATTERY ATTACHED DISCONNECTED V is clamped by the emf Q is stranded on the plates use U = CV² / 2 use U = Q² / 2C Q = CV floats with C V = Q / C floats against C pull the plates apart, C halves: pull the plates apart, C halves: U HALVES U DOUBLES picking the wrong column reverses the direction of the answer
Same physical action, opposite energy changes, both correct. The formula is not a preference: it is chosen by whichever variable the circuit is holding still.
where the charge sits, and which field belongs to which question + + + + + E = sigma / eps0 for anything IN the gap E = 0 E = 0 force ON a plate uses the OTHER plate's field: F = Q² / 2 eps0 A NOT charge on the outer faces, and NOT QE with the full gap field
The two charges pin each other to the facing surfaces, which is why the field lives only in the gap. A plate cannot push on itself, so its force uses half the gap field.

The work

Lesson live · diagnostic and drills coming soon
Lesson
Capacitors

Establishes capacitance as geometry, locates the charge on the facing surfaces, mirrors the series and parallel rules against resistors, and drills the habit of choosing the energy formula from whichever variable the wiring holds fixed.

Skill check · 10 scenarios
Diagnostic
10-item topic check

Ten items spanning the failure modes of this topic: making capacitance track the charge or voltage applied, swapping the series and parallel rules, using the full gap field for the force on a plate, coating both faces of a plate with charge, running current across the gap, and quoting an energy change from the formula the wiring did not clamp. Take it cold to find which one is yours, or after the lesson to confirm it is not.

Not yet available · 10 items
Targeted Practice
Drill a single misconception

Pick one of the failure modes you missed and drill it on its own. The round is adaptive: two correct in a row clears it for now and moves you to the next. Two in a row is a checkpoint, not proof: if the error resurfaces later, the misconception comes back.

Unlocks from the diagnostic, which is not published yet