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CED objectives

Resistor-Capacitor (RC) Circuits

▶︎  Watch it animatedinteractive step-through · ~3 min · optional ⚙︎  Open the appletRC Lab · a clock counting in time constants, a resistor laid across the block, and the two combination rules the wrong way round

Capacitors combine the opposite way from resistors: capacitances add in parallel and their reciprocals add in series, so a series combination is smaller than its smallest member, and series capacitors carry equal magnitudes of charge. At the instant a switch closes, an uncharged capacitor has no potential difference across it and behaves like a plain wire, so the current in its branch is at its largest and is found by replacing the capacitor with a wire. After a long time no current flows in that branch, so it is treated as open and the capacitor's potential difference is whatever appears across the two points it bridges. The crossing has time constant $\tau = RC$.

Four errors dominate. Reusing the resistor combining rules for capacitors, which inverts every equivalent capacitance. Treating a capacitor as an open switch from the moment the circuit closes, which puts the initial current at zero when it is at its maximum. Charging every capacitor up to the source emf regardless of where it sits, when it reads only the potential difference at its own terminals. And reading $\tau$ as a finishing time, or scaling the speed backward so a larger resistor is expected to fill the capacitor faster.

two easy moments, two ordinary resistor circuits R wire t = 0, uncharged: ΔV = Q/C = 0 so it acts as a WIRE the current is at its LARGEST here, not zero R gap t → long: no charge arriving so the branch is OPEN read ΔV across the two points it bridges: often NOT ε “capacitors block DC” is the right-hand panel applied to the left-hand one
Neither panel contains a capacitor. Choosing which substitution to make is the whole of the analysis at those two moments.
τ is not a finishing time Q t final τ about 63% of the final charge effectively finished around here larger R or larger C makes τ BIGGER, so everything takes longer: less current to move more charge
One time constant is a landmark on the curve, not its end. The curve is still visibly rising when the first one has passed.

The work

3 ways in · any order
Lesson
Resistor-Capacitor (RC) Circuits

Reverses the combining rules for capacitors, replaces the capacitor with a wire at the switching instant and a gap long afterward, and reads the time constant as a landmark rather than a finishing time.

Skill check · 10 scenarios
Diagnostic
10-item topic check

Ten items spanning the failure modes of this topic: copying the resistor combining rules, zeroing the current at the switching instant, charging every capacitor to the source emf, and treating one time constant as the end of the process. Take it cold to find which one is yours, or after the lesson to confirm it is not.

Not started · 10 items · ~15 min
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.

Take the diagnostic to identify your misconceptions