AP Physics 2 Unit 11 ReviewElectric Circuits

Verified for the 2027 examCompiled by AP educators
Pep mascot
Upgrade your Fiveable account to print any study guide

Download study guides as beautiful PDFs See example

Print or share PDFs with your students

Always prints our latest, updated content

Mark up and annotate as you study

Click below to go to billing portal → update your plan → choose Yearly→ and select "Fiveable Share Plan". Only pay the difference

Plan is open to all students, teachers, parents, etc
Pep mascot
Upgrade your Fiveable account to export vocabulary

Download study guides as beautiful PDFs See example

Print or share PDFs with your students

Always prints our latest, updated content

Mark up and annotate as you study

Plan is open to all students, teachers, parents, etc

AP Physics 2 Unit 11, Electric Circuits, covers 8 topics worth 15-18% of the AP exam, with capacitors and their behavior in circuits as a central focus alongside current, resistance, and power. You'll work through current and resistance, Ohm's Law, and resistivity before moving into series and parallel circuits and full circuit analysis. RC circuits and electrical power round out the unit, and AP Physics 2 ties it all together with conservation of energy as the underlying logic.

unit 11 review

AP Physics 2 Unit 11, Electric Circuits, is about how charge moves through wires, resistors, bulbs, and capacitors, and how energy is transferred along the way. The single biggest idea is conservation, applied twice over. Energy conservation gives you Kirchhoff's loop rule, and charge conservation gives you the junction rule, and together those two principles let you analyze any DC circuit. The unit makes up 15-18% of the AP exam, tied for the largest weight in the course.

What this unit covers

Current, resistance, and Ohm's law

  • Current is the rate at which charge passes through a cross-sectional area of wire, I=Δq/ΔtI = \Delta q / \Delta t. It's not a vector, but it has a direction, defined by the flow of positive charge.
  • Charge moves because of a potential difference, sometimes called electromotive force or emf (ε\varepsilon). No potential difference, no net charge flow. Individual electrons still jiggle around, but their net motion is zero.
  • Resistance measures how strongly an object opposes charge flow. For a uniform resistor, R=ρ/AR = \rho \ell / A. Longer wire means more resistance; thicker wire means less. Resistivity ρ\rho is a property of the material itself, set by its atomic structure.
  • Ohm's law, I=ΔV/RI = \Delta V / R, relates current, potential difference, and resistance. Materials with constant resistance at all currents are called ohmic. A graph of current vs. voltage for an ohmic material is a straight line; for a non-ohmic element like a real light bulb filament, it curves.
  • Resistors convert electrical energy to thermal energy, which can heat up the resistor and its surroundings. That's why resistance can change with temperature.

Circuit behavior and electric power

  • A circuit is a set of loops built from wires, batteries, resistors, lightbulbs, capacitors, switches, ammeters, and voltmeters. Closed circuits let charge flow, open circuits don't, and a short circuit lets charge flow with no change in potential difference (which is how things overheat).
  • Power is the rate of energy transfer in a circuit element, P=IΔVP = I\Delta V, with the derived forms P=I2RP = I^2 R and P=(ΔV)2/RP = (\Delta V)^2 / R.
  • Bulb brightness tracks power. This is the engine behind the classic AP question "what happens to bulb A's brightness when the switch closes?" You answer it by reasoning about how current and voltage redistribute, then comparing power.

Series, parallel, and Kirchhoff's rules

  • In series, charge passing through one element must pass through all of them, so current is the same everywhere and resistances add, Req=R1+R2+R_{eq} = R_1 + R_2 + \dots
  • In parallel, elements share the same potential difference, current splits among branches, and 1/Req=1/Ri1/R_{eq} = \sum 1/R_i. The equivalent resistance of a parallel set is always less than the smallest branch resistance.
  • Kirchhoff's loop rule says the potential differences around any closed loop sum to zero, ΔV=0\sum \Delta V = 0. This is conservation of energy in circuit language. A charge that goes around a loop and comes back to its starting point must return to the same potential.
  • Kirchhoff's junction rule says current in equals current out at any junction, Iin=Iout\sum I_{in} = \sum I_{out}. This is conservation of charge. Charge doesn't pile up at a junction or vanish.
  • You can represent the potential at points around a circuit graphically, climbing through the battery and dropping through each resistor. This picture is worth drawing for tricky loop-rule problems.

Capacitors and RC circuits

  • Capacitors store charge and energy. A group of capacitors can be replaced with one equivalent capacitance CeqC_{eq}, but the rules are flipped relative to resistors. In series, 1/Ceq=1/Ci1/C_{eq} = \sum 1/C_i, and the result is smaller than the smallest capacitor. In parallel, capacitances add.
  • The time constant τ=ReqCeq\tau = R_{eq} C_{eq} sets how fast a capacitor charges or discharges. For a charging capacitor, τ\tau is the time to reach about 63% of its final charge. For a discharging one, it's the time to fall to about 37% of its starting value.
  • The limiting cases matter most. At the instant a switch closes, an uncharged capacitor acts like a plain wire (no potential difference across it). After a long time, a fully charged capacitor acts like a break in the circuit (no current through its branch). Most RC questions hinge on these two snapshots.

Unit 11, Electric Circuits at a glance

TopicCore ideaKey equationWatch out for
Current and resistanceCurrent is charge flow rate driven by a potential differenceI=Δq/ΔtI = \Delta q / \Delta tCurrent has a direction but isn't a vector
Resistivity and Ohm's lawResistance depends on material and geometry; ohmic means constant RR=ρ/AR = \rho \ell / A, I=ΔV/RI = \Delta V / RReal bulbs are non-ohmic; R changes with temperature
Electric powerPower sets the rate of energy transfer and bulb brightnessP=IΔV=I2R=(ΔV)2/RP = I\Delta V = I^2 R = (\Delta V)^2/RPick the form whose variables you actually know
Series and parallelSeries shares current; parallel shares voltageReq,s=RiR_{eq,s} = \sum R_i; 1/Req,p=1/Ri1/R_{eq,p} = \sum 1/R_iParallel ReqR_{eq} is smaller than every branch
Kirchhoff's loop rulePotential differences around a closed loop sum to zeroΔV=0\sum \Delta V = 0It's just conservation of energy
Kirchhoff's junction ruleCurrent in equals current out at every junctionIin=Iout\sum I_{in} = \sum I_{out}It's just conservation of charge
Capacitor combinationsEquivalent capacitance rules are the reverse of resistor rulesCeq,p=CiC_{eq,p} = \sum C_i; 1/Ceq,s=1/Ci1/C_{eq,s} = \sum 1/C_iDon't apply resistor rules to capacitors
RC circuitsThe time constant sets charging and discharging speedτ=ReqCeq\tau = R_{eq} C_{eq}At t=0t=0 capacitor acts like a wire; at tt \to \infty like a gap

Why Unit 11, Electric Circuits matters in AP Physics 2

Circuits are where conservation laws stop being abstract and start predicting things you can measure with a multimeter. The whole unit is two old ideas wearing new clothes. Conservation of energy becomes the loop rule, and conservation of charge becomes the junction rule. AP Physics 2 also leans hard on this unit for experimental design, because circuits are easy to build, modify, and measure in a lab.

  • This is one of the heaviest-weighted units on the exam at 15-18%, and circuit reasoning shows up in both multiple-choice and free-response.
  • Energy transfer through power (P=IΔVP = I\Delta V) connects circuits to the course-wide theme of tracking where energy goes, from chemical energy in a battery to thermal energy in a resistor.
  • Circuit analysis is the course's best training ground for the "design an experiment" skill, like determining a material's resistivity from measurements of length, area, and resistance.

How this unit connects across the course

  • Everything here builds directly on electric potential and capacitance from Electric Force, Field, and Potential (Unit 10). The potential difference that drives current is the same ΔV\Delta V you learned there, and ΔUE=qΔV\Delta U_E = q\Delta V carries straight over into the loop rule.
  • Resistors converting electrical energy into thermal energy is an energy-transfer story you already told in Thermodynamics (Unit 9). Power dissipated in a resistor is heat flowing into the environment.
  • Current-carrying wires are the source of magnetic fields in Magnetism and Electromagnetism (Unit 12), and induced emfs from changing magnetic flux drive currents in circuits. You can't do Unit 12 without fluency in current, emf, and resistance from this unit.
  • The idea of charge as discrete carriers moving in response to fields foreshadows the particle-level picture in Modern Physics (Unit 15).

Key equations and processes

  • I=Δq/ΔtI = \Delta q / \Delta t defines current as the rate of charge flow through a cross section.
  • R=ρ/AR = \rho \ell / A gives resistance from resistivity, length, and cross-sectional area. Use it whenever a problem changes a wire's geometry.
  • I=ΔV/RI = \Delta V / R (Ohm's law) relates the three core circuit quantities for ohmic elements.
  • P=IΔV=I2R=(ΔV)2/RP = I\Delta V = I^2 R = (\Delta V)^2 / R gives the rate of energy transfer. Use the version matching the quantities you know, and use it to rank bulb brightness.
  • ΔUE=qΔV\Delta U_E = q\Delta V converts potential difference into energy change for a moving charge.
  • ΔV=0\sum \Delta V = 0 (loop rule) is the bookkeeping equation for any closed loop. Walk the loop, add gains through batteries and drops through resistors, set the total to zero.
  • Iin=Iout\sum I_{in} = \sum I_{out} (junction rule) splits and recombines currents at junctions.
  • Req=RiR_{eq} = \sum R_i in series and 1/Req=1/Ri1/R_{eq} = \sum 1/R_i in parallel collapse resistor networks into one equivalent resistor.
  • Ceq=CiC_{eq} = \sum C_i in parallel and 1/Ceq=1/Ci1/C_{eq} = \sum 1/C_i in series do the same for capacitors, with the rules reversed.
  • τ=ReqCeq\tau = R_{eq} C_{eq} sets the charging and discharging timescale of an RC circuit. After one time constant, a charging capacitor reaches about 63% of its final charge.

Unit 11, Electric Circuits on the AP exam

At 15-18% of the exam, circuits content carries as much weight as any unit in AP Physics 2, so expect it across multiple-choice and free-response. The exam rarely asks you to just plug into V=IRV = IR. Instead it asks you to reason about change. A switch closes, a bulb burns out, a resistor is added in parallel, and you have to predict and justify what happens to current, potential difference, and brightness elsewhere in the circuit.

  • Qualitative ranking tasks are everywhere. Rank bulbs by brightness, rank currents through branches, or predict whether an ammeter reading increases, decreases, or stays the same when the circuit changes. Justify with the loop rule, junction rule, and power equations, not vibes.
  • Free-response questions in this course include experimental design. A classic setup asks you to design a procedure to measure resistivity or to determine whether a circuit element is ohmic, including what to measure, what to graph, and how the slope gives the answer.
  • Quantitative analysis shows up as multi-loop circuits where you apply Kirchhoff's rules, reduce networks to equivalent resistance or capacitance, and solve for an unknown current or voltage.
  • RC circuit questions usually test the limiting cases (right after the switch closes vs. a long time later) and the meaning of the time constant, often with a graph of charge or current versus time to interpret.

Essential questions

  • How do conservation of energy and conservation of charge completely determine the behavior of a circuit?
  • Why does adding a resistor in parallel decrease total resistance while adding one in series increases it?
  • What physical properties of a material and an object decide how strongly it resists current?
  • How does a capacitor's behavior in a circuit change over time, and what controls how fast that change happens?

Key terms to know

  • Current: The rate at which charge passes through a cross-sectional area of a wire, measured in amperes.
  • Electromotive force (emf): The potential difference a source like a battery provides to drive charge through a circuit.
  • Resistance: A measure of how strongly an object opposes the flow of electric charge, measured in ohms.
  • Resistivity: A fundamental material property, set by atomic structure, that quantifies how much the material opposes charge flow.
  • Ohmic material: A material whose resistance stays constant for all currents, giving a linear current-voltage graph.
  • Short circuit: A path where charge flows with no change in potential difference, bypassing other circuit elements.
  • Equivalent resistance: The single resistance that could replace a network of resistors without changing the circuit's behavior.
  • Equivalent capacitance: The single capacitance that could replace a group of capacitors, with combination rules opposite to those for resistors.
  • Kirchhoff's loop rule: The sum of potential differences around any closed loop is zero, a consequence of energy conservation.
  • Kirchhoff's junction rule: Total current entering a junction equals total current leaving it, a consequence of charge conservation.
  • Electric power: The rate at which energy is transferred or dissipated by a circuit element, given by P=IΔVP = I\Delta V.
  • Time constant (τ\tau): The product ReqCeqR_{eq}C_{eq}, the time for a charging capacitor to reach about 63% of its final charge.
  • Ammeter: A meter placed in series to measure current; an ideal one has zero resistance.
  • Voltmeter: A meter placed in parallel to measure potential difference; an ideal one has infinite resistance.

Common mix-ups

  • Resistor and capacitor combination rules are opposites. Resistances add in series; capacitances add in parallel. If you memorize one set, remember the other is flipped.
  • Adding a parallel branch lowers total resistance, which means total current from the battery goes up, not down. More paths means easier flow, even though you added a component.
  • "Same current in series, same voltage in parallel" is the rule for identifying connections, not the other way around. Two resistors carrying the same current aren't automatically in series unless every charge through one must pass through the other.
  • A capacitor acts like a wire only at the first instant after the switch closes. After a long time it acts like an open gap. Mixing up these two limits flips your answer on most RC questions.

Frequently Asked Questions

What topics are covered in AP Physics 2 Unit 11?

AP Physics 2 Unit 11 covers 8 topics built around capacitors and circuit analysis: Current and Resistance, Electric Power, Resistance/Resistivity/Ohm's Law, Series and Parallel Circuits, Analysis of Circuits, Capacitors in Circuits, RC Circuits, and Electrical Power in Circuits. Together they connect conservation of energy to real circuit behavior. See the full topic breakdown at AP Physics 2 Unit 11.

How much of the AP Physics 2 exam is Unit 11?

Unit 11 makes up 15-18% of the AP Physics 2 exam, making it one of the heavier-weighted units. It covers electric circuits topics including capacitors, series and parallel circuits, Ohm's Law, RC circuits, and electrical power. Expect multiple MCQ questions and at least one FRQ that draws from this material.

What's on the AP Physics 2 Unit 11 progress check (MCQ and FRQ)?

The AP Physics 2 Unit 11 progress check includes both MCQ and FRQ parts drawn from all 8 unit topics. MCQ questions test current and resistance, Ohm's Law, and series and parallel circuits. The FRQ portion typically asks you to analyze a circuit, work with capacitors, or explain RC circuit behavior quantitatively and conceptually. Practice with questions matched to every progress check topic at AP Physics 2 Unit 11.

How do I practice AP Physics 2 Unit 11 FRQs?

The best way to practice AP Physics 2 Unit 11 FRQs is to focus on the three highest-yield topics: Analysis of Circuits, Capacitors in Circuits, and RC Circuits. FRQs from this unit typically ask you to derive current or voltage using Kirchhoff's rules, explain how adding a capacitor changes circuit behavior, or sketch and interpret RC charging/discharging graphs. Start by writing out full solutions, not just plugging numbers. Show your reasoning for each step, since College Board awards points for justification. Find FRQ-style practice sets at AP Physics 2 Unit 11.

Where can I find AP Physics 2 Unit 11 practice questions?

You can find AP Physics 2 Unit 11 practice questions, including MCQ and practice test sets, at AP Physics 2 Unit 11. The page organizes practice by topic, so you can drill series and parallel circuits separately from capacitors or RC circuits before taking a full unit practice test. For the best results, mix MCQ drills with at least one timed FRQ attempt per study session.

How should I study AP Physics 2 Unit 11?

Start AP Physics 2 Unit 11 by building a solid foundation in current and resistance and Ohm's Law before moving to series and parallel circuits, since later topics like RC circuits and capacitors stack directly on those ideas. Here's a practical study sequence: 1. **Topics 11.1-11.3** (Current, Resistance, Ohm's Law): Practice drawing V-I graphs and using R = V/I in multiple forms. 2. **Topic 11.4** (Series and Parallel Circuits): Redraw every circuit you see. Label current paths and voltage drops before calculating anything. 3. **Topics 11.5 and 11.8** (Analysis and Electrical Power): Apply Kirchhoff's rules to multi-loop circuits. Connect power dissipation to real components like light bulbs. 4. **Topics 11.6 and 11.7** (Capacitors and RC Circuits): Understand charging and discharging curves conceptually first, then work through the math. After each topic, do a short MCQ check, then finish with a timed FRQ. Find topic-by-topic practice at AP Physics 2 Unit 11.