Mistake Master
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CED objectives

Kirchhoff's Loop Rule

▶︎  Watch it animatedinteractive step-through · ~3 min · optional ⚙︎  Open the appletLoop Rule Lab · pick a direction to walk the loop, commit a sign to every term, and read the terminal voltages against the EMFs

The loop rule states that the potential changes around any closed walk sum to zero, which is energy conservation per unit charge. Signs are assigned from the traversal direction: a resistor crossed along its current arrow contributes $-IR$ and crossed against it contributes $+IR$, while a battery contributes $+\varepsilon$ when entered at its negative plate and $-\varepsilon$ when entered at its positive plate, in both cases without reference to which way current flows. A real source carries internal resistance $r$, so its terminal voltage is $\varepsilon - Ir$ while discharging and $\varepsilon + Ir$ while being charged.

Three errors dominate. Assigning signs by component type, making every battery positive and every resistor negative, which breaks as soon as two sources oppose or a guessed current runs backward. Using the EMF as the terminal voltage under load, so a measured battery reading below its label looks like a defective battery rather than $\varepsilon - Ir$. And reasoning locally after a change: closing a switch or swapping a resistor alters $R_{\text{eq}}$, the source current and every node potential, so the entire circuit must be re-solved before any element is called brighter or dimmer.

one closed walk, four crossings, each priced where you stand 12 V +12 3 Ω −3I 6 V −6 1 Ω −1I walk this way +12 − 3I − 6 − 1I = 0, so I = 1.5 A signs by component type give +12 − 3I + 6 − 1I
The second battery is crossed positive plate first, so it contributes minus six volts. Nothing about it being a battery makes its term positive.
V(terminal) = EMF − Ir, with I positive while discharging I V EMF = 9.0 V at I = 0 2.0 A: terminals read 8.0 V discharging: below the label charging: above the label a flat line at 9.0 V is the terminal-equals-EMF error: it has r = 0
The line crosses the EMF only at zero current. Loading pulls the terminals down by Ir, and reversing the current to charge the cell pushes them above the printed value.

The work

3 ways in · any order
Lesson
Kirchhoff's Loop Rule

Prices every loop crossing from the traversal direction, replaces the sign-by-component-type shortcut, puts internal resistance into the terminal voltage in both the discharging and charging cases, and drills re-solving a circuit after a switch closes.

Skill check · 10 scenarios
Diagnostic
10-item topic check

Ten items spanning the failure modes of this topic: assigning loop signs by component type, cancelling or adding opposing EMFs, treating a battery's terminal voltage as its EMF under load, and predicting a bulb's brightness from its own branch instead of re-solving the circuit. 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