AP Unit 11 Problems
19 learning problems for Unit 11. Draw the situation, name the model and explain why each step follows. These are authored practice, with worked solutions on a separate page.
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Problem 1
A metallic wire carries conventional current from left to right: 0.20 A for 3.0 s, then 0.50 A for 2.0 s, then zero for 4.0 s.
Part a
Construct the current-versus-time graph and find the charge-flow magnitude through a cross section and the number of electrons involved over the full 9.0 s.
Part b
Give the electron drift direction, explain why current is not added as a spatial vector at a bend, and describe electron motion during the zero-current interval.
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Problem 2
Wire A transfers 0.90 C of net charge in 0.30 s. Wire B transfers 1.20 C in 0.80 s. Each is part of an external circuit driven by a maintained battery potential difference.
Part a
Compare their currents and the charge each transfers in the next 2.0 s if its current remains constant. Explain why emf should have units of volts rather than newtons.
Part b
At the same current, a wire is bent into a U shape without adding branches. Compare current through its two legs and state the relation of electron drift to current arrows.
Draw the U-shaped wire and add conventional-current and electron-drift arrows on both legs.
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Problem 3
Build a schematic from this description: a battery connects nodes A and B; between A and B there is one resistor branch and a second branch containing a bulb and switch in series. An ideal voltmeter measures across the bulb. The switch is initially closed.
Part a
Draw the circuit with conventional-current arrows and standard symbols. Identify two complete loops and the component belonging to both. Show how to mark an adjustable resistor.
Part b
Predict branch behavior when the switch opens. Does the resistor branch also stop? Can the open switch have nonzero voltage?
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Problem 4
A 12 V ideal battery, closed switch, 2 Ω feed resistor, and 6 Ω load resistor form one series loop. A student adds an ideal wire across only the 6 Ω load, leaving the feed resistor in the loop, and claims the load will carry more current because the wire is “another source.”
Part a
Draw the changed topology, including the retained feed resistor. Explain and calculate the load voltage and current and the source current after the shunt is added. Relate the result to the definition of a short.
Part b
Consider a separate hypothetical circuit: remove both finite resistors and connect the ideal 12 V source directly to only ideal zero-resistance wire. Why is there no sensible finite steady current? State what real effects must be restored. Explain why changing only a line’s bend differs from adding the shunt in part a.
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Problem 5
Two wires use the same metallic material. Wire A has length L and circular radius a; wire B has length 3L and radius 2a. Both are initially at the same temperature.
Part a
Derive RB/RA. For ρ = 2.0 × 10⁻⁸ Ω·m, L = 1.0 m, and a = 0.10 mm, calculate each resistance and describe the distinction between R and ρ.
Part b
Wire A is heated while its geometry changes negligibly. Predict its typical metallic resistance trend and explain why an ideal constant-resistivity ohmic calculation might give a different prediction.
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Problem 6
A controlled-temperature element gives these readings: (ΔV, I) = (0 V, 0 A), (1 V, 0.040 A), (2 V, 0.080 A), (3 V, 0.120 A). A heated bulb gives (1 V, 0.10 A), (2 V, 0.16 A), (3 V, 0.20 A).
Part a
Plot I versus ΔV for both elements. Determine the fixed element’s resistance and whether each data set supports one constant-R model over the tested range. Explain how changing graph axes alters the slope interpretation.
Part b
Design a check for heating as the cause of the bulb’s changing resistance. Identify measured variables, a temperature-related control, a repeat procedure, and where the thermal energy comes from. Contrast this with the ideal fixed-ρ model.
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Problem 7
A 30 Ω ohmic resistor is connected across a 6.0 V ideal source for 120 s. Assume resistance remains constant.
Part a
Derive the resistor forms of power from P = IΔV, then find current, power, and converted energy.
Part b
Compare power if source voltage doubles with R fixed, and if resistance doubles with source voltage fixed. Create two qualitative graphs: P versus positive V with R fixed, and P versus positive R with V fixed. Label axes and explain each shape.
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Problem 8
Two bulbs have stipulated constant resistances RA = 4 Ω and RB = 8 Ω. They are used with an ideal 12 V supply. Treat power as a qualitative brightness guide for these modeled bulbs.
Part a
Connect them in series. Find each power, rank brightness, and explain the fixed-current comparison.
Part b
Reconnect them in parallel across 12 V. Find each power, rank brightness, and explain why the ranking reverses. State a limitation for real bulbs.
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Problem 9
An ideal 18 V battery supplies a 3 Ω resistor in series with a parallel combination of 6 Ω and 12 Ω. A switch can add another 12 Ω branch in parallel with that combination.
Part a
With the added branch open, find equivalent resistance, source current, branch currents, and voltage drops. Explain the topology behind each equality.
First draw and label the node schematic and branch-current arrows.
Part b
Close the extra 12 Ω branch. Predict and calculate the new equivalent resistance, source current, and original 6 Ω branch current. Why does original branch current change here even though the battery is ideal?
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Problem 10
A battery has emf 12 V and internal resistance 2.0 Ω. Its external loop has a 9.0 Ω load and a total 1.0 Ω of wire resistance. Meters are ideal unless the part asks otherwise.
Part a
Find current, loaded terminal voltage, load voltage, and open-circuit terminal voltage. Explain when wire resistance may be neglected and why it is retained here.
Part b
Draw and label the complete connected meter schematic: an ammeter to measure load current and a voltmeter to measure load voltage. State ideal meter resistances and qualitatively discuss nonideal meter effects.
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Problem 11
A single loop contains an ideal battery and two resistors. Traversing with the measured 2.0 A current, a potential graph reads: before battery 4 V; after battery 16 V; after the first resistor 10 V; after the second resistor back to 4 V. Wires are ideal.
Part a
Find emf and both resistances, construct the signed loop equation, and explain how the graph tests energy conservation.
Part b
For 0.50 C passing through this loop, give the source energy input and conversion in each resistor. Create a quantitative potential-versus-position graph with labeled components and voltage scale if the starting reference becomes 0 V.
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Problem 12
A 15 V ideal battery sends current I0 through a 2 Ω feed resistor to a junction. From that node, currents I1 through 3 Ω and I2 through 6 Ω return to the negative source node. All assumed currents follow source-driven conventional directions.
Part a
A student writes 15 − 2I0 − 3I1 − 6I2 = 0 as a single-loop equation. Explain the path error, write two independent correct loops and one junction equation, and solve the three currents.
Draw and label the source, feed, both return branches and the three assumed current directions before writing equations.
Part b
Write the loop going down the 3 Ω branch and up the 6 Ω branch. Is it independent? Create a labeled qualitative potential-versus-ordered-position graph through the source, feed, and 6 Ω return branch with source negative terminal set to zero; mark the calculated plateau potentials.
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Problem 13
At a steady junction, branch A brings in 4.0 mC every 2.0 ms, branch B brings in 0.50 A, and branch C takes out 1.20 A. The direction of unknown branch D is initially assumed outward.
Part a
Find ID and the charge leaving through D in 5.0 s. State the conservation principle used.
Part b
If a student instead reports ID = 0.80 A outward, find the predicted accumulation rate in the junction region and explain why this is inconsistent with steady conditions.
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Problem 14
A node has measured branch currents 1.4 A inward in A, 0.8 A outward in B, and 1.0 A outward in C. Unknown D is drawn outward. Farther along B, its wire bends 90° and passes through two series resistors without any new junction.
Part a
Solve the signed current in D and redraw its actual direction. Compare both incoming and outgoing totals after correction.
Part b
Find current through both series resistors in B. Explain why neither the bend angle nor the first resistor’s heating reduces the second resistor’s current.
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Problem 15
Capacitors of 2 μF and 6 μF can be connected in series or parallel across a 12 V source. Both initially are uncharged and isolated intermediate nodes start neutral.
Part a
For the series connection, derive Ceq, find each charge and voltage, and explain why equal charge magnitude follows from conservation. Compare Ceq to the smaller capacitor.
Part b
Reconnect the uncharged capacitors in parallel across 12 V. Find Ceq and each plate-charge magnitude, and explain how the equivalent represents the source’s total charge separation.
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Problem 16
An ideal 10 V source charges an initially uncharged 200 μF capacitor through a 5.0 kΩ resistor. A switch later removes the source and allows the capacitor to discharge through the same resistor.
Part a
Find the charging time constant and initial and long-time values of current, capacitor voltage, charge, and stored energy. Explain the initial wire and final open-branch models.
Part b
Sketch charging Q, VC, current magnitude, and energy against time, indicating endpoint behavior and the meaning of one τ. Compare qualitatively if R doubles with all else fixed. Do not use a transient formula.
Part c
After it is fully charged, switch to discharge. State initial current direction and magnitude, describe immediate and long-time changes in charge and energy, and explain the 37% landmark.
Create labeled qualitative discharge graphs of Q, VC, current magnitude and stored energy against time, showing their starting values and zero asymptotes.
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Problem 17
A student tests a resistor with ideal meters and a low-voltage source. I-versus-ΔV data yield best-fit slope 0.020 A/V, with plausible uncertainty bounds 0.019 to 0.021 A/V. At 4.0 V the measured current is 0.080 A. The resistor is a uniform sample 0.10 m long with cross-sectional area 2.0 × 10⁻⁸ m².
Part a
Design a coherent measurement procedure to collect the current–voltage data: identify the connected meters, varied and measured quantities, temperature and geometry controls, repeated readings, and a test of constant R. Then infer resistance and a range from the supplied slope bounds and calculate resistivity.
Part b
At the stated 4.0 V operating point, find power and charge transferred in 30 s. Find converted energy two ways and explain why heating can change later readings.
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Problem 18
A 12 V ideal source fixes node A at 12 V and node D at 0 V. Left path A→B→D has R1 = 2 Ω and R2 = 4 Ω. Right path A→C→D has R3 = 4 Ω and R4 = 2 Ω. A bridge resistor R5 = 4 Ω joins B to C. Assume currents I1 A→B, I2 B→D, I3 A→C, I4 C→D, and I5 B→C.
Part a
Draw the node schematic and write two independent junction equations and three independent loop equations. Explain why the left pair and right pair cannot be treated as simple series groups before solving.
Part b
Solve the branch currents and node potentials VB and VC. Verify one unused loop and the source-power balance.
Part c
Where would ideal meters measure bridge current and VB − VC? Describe qualitatively how a finite-resistance voltmeter across B–C could disturb the bridge.
Draw the two meter connections on the bridge schematic.
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Problem 19
A 12 V ideal source feeds R1 = 2.0 kΩ from source-positive node A to node B. Between B and source-negative node D there are parallel R2 = 4.0 kΩ and C = 100 μF branches. The capacitor starts uncharged. Later a switch disconnects R1 and the source, leaving C to discharge only through R2.
Part a
For the initial charging instant and long-time charging state, find VB, currents through R1 and R2 and C, final capacitor charge, and final energy. Explain why long-time capacitor voltage is not 12 V.
Draw the initial wire-equivalent and long-time open-branch equivalent schematics, keeping R2 connected in both.
Part b
After disconnecting the source and R1, find the discharge time constant and initial current magnitude through R2. Sketch VC and current magnitude during discharge. State initial stored energy and the total energy eventually converted in R2.
Part c
Plan a hands-on check of the discharge time constant without exponential fitting. Name measured variables, controls, repetitions, and sampling uncertainty. A sample trial gives (t in s, VC in V): (0,8.0), (0.20,4.9), (0.30,3.8), (0.40,3.0), (0.50,2.3), (0.60,1.8), (0.80,1.1). Each voltage has uncertainty ±0.1 V and each sample time ±0.02 s. Create a quantitative plot of VC/VC,0 versus time with scales and uncertainty; read an approximate τ from the 37% landmark and explain its precision.
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More chapter problems
Try these problems before opening the solutions. Show the physical model, your calculation or sketch, and the reason your conclusion follows.
What starts the net current?
A metal resistor is connected into a closed loop with a maintained battery potential difference. Its temperature and resistance are approximately fixed.
(a) Which explanation connects the source to charge motion correctly?
Worked solution and rubric →Revisit the explanation →Revisit the explanation →Read the relevant lesson →
Can two equal wires resist differently?
At a common controlled temperature, uniform wires A and B each have L = 0.50 m and cross-sectional area 2.0 × 10⁻⁷ m². Data are A: (V,I) = (0,0), (1.0,0.25), (2.0,0.50), (3.0,0.75), with V in volts and I in amperes. B has (0,0), (1.0,0.125), (2.0,0.250), (3.0,0.375). Both are approximately ohmic over this tested range.
(a) Construct both quantitative I-versus-V graphs on common axes, find their slopes and resistances, and infer both resistivities. Explain what higher resistivity says about opposition to charge motion and how atomic/molecular structure can cause a difference at equal geometry. State what the graph cannot uniquely tell you microscopically.
(b) A third wire uses material A at the same temperature but has twice the length and twice the area. Predict its R and ρ, and explain why changing the object’s dimensions does not force a change in the material coefficient.
(c) The actual A wire is then heated while geometry changes negligibly. Predict the typical metallic trend of ρ, R and the I-versus-V slope. Contrast it explicitly with the stated temperature-independent ideal ohmic model, and explain whether one linear I–V graph at fixed temperature proves that idealization across temperatures.
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Worked solution and rubric →Revisit the explanation →Revisit the explanation →Read the relevant lesson →
What does ideal mean in the circuit model?
A battery of emf 12.0 V supplies a 10.0 Ω load through an unbranched loop. First use an ideal battery and ideal wires. Then compare a discharging nonideal battery with r = 1.0 Ω and total series wire resistance R_wire = 1.0 Ω. Load resistance remains constant. All stated voltage measurements are by ideal voltmeters.
(a) State the resistance assumptions for both an ideal battery and ideal wires. Draw the ideal circuit and calculate current, terminal voltage, load voltage and wire voltage drop. Explain how finite current is compatible with zero ideal-wire voltage drop.
(b) Draw the nonideal series model with the internal resistor inside the battery boundary and identify the two terminal-measurement nodes and the two load-measurement nodes. Find current and both measured voltages. Write a closed-loop voltage check and verify source power equals the sum of all three resistive powers.
(c) In another trial keep the 10.0 Ω load but reduce r and total wire resistance to 0.010 Ω each. Calculate the fractional current overestimate from using the ideal model, relative to the true nonideal current. Then explain why the same neglect argument fails if the finite load is removed and the battery is connected directly across its wires.
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Worked solution and rubric →Revisit the explanation →Revisit the explanation →Read the relevant lesson →