AP Physics C Electricity and Magnetism Quiz: Circuits With Capacitors And Inductors
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Circuits With Capacitors And InductorsQuestion 1 of 20

An ideal LC circuit has a total electromagnetic energy of 5050 μ\muJ. At a certain instant, the energy stored in the electric field of the capacitor is 3030 μ\muJ. What is the energy stored in the magnetic field of the inductor at that same instant?

8080 μ\muJ
5050 μ\muJ
3030 μ\muJ
2020 μ\muJ
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AP Physics C Electricity and Magnetism Quiz

AP Physics C Electricity and Magnetism Quiz: Circuits With Capacitors And Inductors

Practice Circuits With Capacitors And Inductors in AP Physics C Electricity and Magnetism with focused quiz questions that help you check what you know, review explanations, and build confidence with test-style prompts.

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This quiz focuses on Circuits With Capacitors And Inductors, giving you a quick way to practice the rules, question types, and explanations that matter most for AP Physics C Electricity and Magnetism.

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Question 1

An ideal LC circuit has a total electromagnetic energy of 5050 μ\muJ. At a certain instant, the energy stored in the electric field of the capacitor is 3030 μ\muJ. What is the energy stored in the magnetic field of the inductor at that same instant?

  1. 8080 μ\muJ
  2. 5050 μ\muJ
  3. 3030 μ\muJ
  4. 2020 μ\muJ (correct answer)
Explanation: In an ideal LC circuit, total energy is conserved. The total energy UtotalU_{total} is the sum of the energy in the capacitor UCU_C and the energy in the inductor ULU_L. Therefore, UL=UtotalUC=50μJ30μJ=20μJU_L = U_{total} - U_C = 50 \mu J - 30 \mu J = 20 \mu J.

Question 2

In an oscillating ideal LC circuit, the total energy is constant. At the instant the charge on the capacitor is at its maximum positive value, which of the following statements is true?

  1. The energy stored in the inductor's magnetic field is at its maximum value.
  2. The current flowing through the inductor is at its maximum value.
  3. The current flowing through the inductor is zero. (correct answer)
  4. The energy is equally shared between the capacitor and the inductor.
Explanation: When the charge on the capacitor is maximum, all the energy of the circuit is stored in the capacitor's electric field. Therefore, the energy stored in the inductor is zero. Since inductor energy is given by 12LI2\frac{1}{2}LI^2, the current II must be zero at this instant.

Question 3

In an ideal LC circuit, the charge on the capacitor q(t)q(t) and the current in the inductor I(t)I(t) oscillate sinusoidally. What is the phase difference between the charge oscillations and the current oscillations?

  1. They are in phase (00 radians).
  2. They are out of phase by π/2\pi/2 radians (9090^\circ). (correct answer)
  3. They are out of phase by π\pi radians (180180^\circ).
  4. They are out of phase by π/4\pi/4 radians (4545^\circ).
Explanation: If the charge is given by q(t)=Qmaxcos(ωt)q(t) = Q_{max} \cos(\omega t), the current is I(t)=dq/dt=ωQmaxsin(ωt)I(t) = dq/dt = -\omega Q_{max} \sin(\omega t). The sine and cosine functions are out of phase by π/2\pi/2 radians. The current leads the charge by π/2\pi/2 radians.

Question 4

An LC circuit is oscillating. At the instant when the capacitor stores its maximum energy, the plates of the capacitor are pulled apart, doubling their separation distance. How does the maximum current ImaxI_{max} in the subsequent oscillations compare to its initial value?

  1. It increases because the total energy of the circuit increases. (correct answer)
  2. It decreases because the total energy of the circuit decreases.
  3. It remains the same because the charge on the capacitor is conserved.
  4. It decreases because the capacitance decreases, reducing the stored charge.
Explanation: At the instant of maximum energy in the capacitor, the current is zero, so the capacitor is electrically isolated. Pulling the plates apart does positive work on the system, which increases the stored potential energy UC=Q2/(2C)U_C = Q^2/(2C) because C decreases while Q remains constant. This increased total energy is then conserved. Since the new maximum inductor energy 12LInew,max2\frac{1}{2}LI_{new,max}^2 must equal this new, larger total energy, the new maximum current must be greater than the initial maximum current.

Question 5

In an ideal LC circuit, a capacitor with capacitance CC is initially charged to a maximum charge QmaxQ_{max}. The circuit then oscillates. By conservation of energy, what is the maximum energy UL,maxU_{L,max} stored in the inductor during one cycle?

  1. UL,max=Qmax22CU_{L,max} = \frac{Q_{max}^2}{2C} (correct answer)
  2. UL,max=12LQmax2U_{L,max} = \frac{1}{2} L Q_{max}^2
  3. UL,max=Qmax22LU_{L,max} = \frac{Q_{max}^2}{2L}
  4. UL,max=0U_{L,max} = 0
Explanation: The total energy in an ideal LC circuit is conserved. It oscillates between the capacitor's electric field and the inductor's magnetic field. The maximum energy stored in the inductor must equal the maximum energy initially stored in the capacitor, which is UC,max=Qmax22CU_{C,max} = \frac{Q_{max}^2}{2C}.

Question 6

An ideal LC circuit has a capacitor with capacitance CC initially charged to a potential difference VmaxV_{max}. The maximum current is ImaxI_{max}. If the capacitance is changed to 4C4C and the capacitor is again charged to the same initial potential difference VmaxV_{max}, what is the new maximum current?

  1. Imax/2I_{max}/2
  2. ImaxI_{max}
  3. 2Imax2I_{max} (correct answer)
  4. 4Imax4I_{max}
Explanation: By energy conservation, the maximum energy in the capacitor equals the maximum energy in the inductor. Initially, 12CVmax2=12LImax2\frac{1}{2}CV_{max}^2 = \frac{1}{2}LI_{max}^2. With the new capacitance, 12(4C)Vmax2=12LInew,max2\frac{1}{2}(4C)V_{max}^2 = \frac{1}{2}LI_{new,max}^2. This means 4(12CVmax2)=12LInew,max24(\frac{1}{2}CV_{max}^2) = \frac{1}{2}LI_{new,max}^2, so 4(12LImax2)=12LInew,max24(\frac{1}{2}LI_{max}^2) = \frac{1}{2}LI_{new,max}^2. This simplifies to 4Imax2=Inew,max24I_{max}^2 = I_{new,max}^2, so Inew,max=2ImaxI_{new,max} = 2I_{max}.

Question 7

An ideal LC circuit consists of an inductor with inductance LL and a capacitor with capacitance CC. Applying Kirchhoff's loop rule to this circuit results in which of the following differential equations, where qq is the charge on the capacitor and II is the current?

  1. LdIdt+qC=0L\frac{dI}{dt} + \frac{q}{C} = 0 (correct answer)
  2. LdIdtqC=0L\frac{dI}{dt} - \frac{q}{C} = 0
  3. I+Cdqdt=0I + C\frac{dq}{dt} = 0
  4. dIdt+LCq=0\frac{dI}{dt} + LCq = 0
Explanation: According to Kirchhoff's loop rule, the sum of potential differences around a closed loop is zero. The potential difference across the inductor is VL=LdIdtV_L = L\frac{dI}{dt} and across the capacitor is VC=qCV_C = \frac{q}{C}. Therefore, VL+VC=0V_L + V_C = 0, which gives LdIdt+qC=0L\frac{dI}{dt} + \frac{q}{C} = 0.

Question 8

The charge qq on the capacitor in an ideal LC circuit is described by the differential equation Ld2qdt2+qC=0L\frac{d^2q}{dt^2} + \frac{q}{C} = 0. If the capacitor has its maximum charge QmaxQ_{max} at t=0t=0, which of the following is a valid solution for q(t)q(t)? Let ω=1/LC\omega = 1/\sqrt{LC}.

  1. q(t)=Qmaxsin(ωt)q(t) = Q_{max} \sin(\omega t)
  2. q(t)=Qmaxeωtq(t) = Q_{max} e^{-\omega t}
  3. q(t)=Qmax(1cos(ωt))q(t) = Q_{max} (1 - \cos(\omega t))
  4. q(t)=Qmaxcos(ωt)q(t) = Q_{max} \cos(\omega t) (correct answer)
Explanation: The given differential equation is for simple harmonic motion. The general solution is q(t)=Acos(ωt)+Bsin(ωt)q(t) = A\cos(\omega t) + B\sin(\omega t). The initial condition q(0)=Qmaxq(0) = Q_{max} gives A=QmaxA=Q_{max}. At t=0t=0, the charge is maximum, so the current I=dq/dtI = dq/dt must be zero. I(0)=Aωsin(0)+Bωcos(0)=Bω=0I(0) = -A\omega\sin(0) + B\omega\cos(0) = B\omega = 0, which implies B=0B=0. Thus, q(t)=Qmaxcos(ωt)q(t) = Q_{max} \cos(\omega t).

Question 9

In an ideal LC circuit, the capacitor is fully charged at t=0t=0. The period of oscillation for the charge is TT. At which of the following times is the energy stored in the capacitor first equal to the energy stored in the inductor?

  1. t=T/8t = T/8 (correct answer)
  2. t=T/4t = T/4
  3. t=T/2t = T/2
  4. t=Tt = T
Explanation: Let q(t)=Qmaxcos(ωt)q(t) = Q_{max} \cos(\omega t). The energy in the capacitor is UC=q22C=Utotalcos2(ωt)U_C = \frac{q^2}{2C} = U_{total} \cos^2(\omega t). The energy is split equally when UC=UL=Utotal/2U_C = U_L = U_{total}/2. This occurs when cos2(ωt)=1/2\cos^2(\omega t) = 1/2, or cos(ωt)=±1/2\cos(\omega t) = \pm 1/\sqrt{2}. The first positive time this occurs is when ωt=π/4\omega t = \pi/4. Since ω=2π/T\omega = 2\pi/T, we have (2π/T)t=π/4(2\pi/T)t = \pi/4, which gives t=T/8t = T/8.

Question 10

An inductor with inductance L=2.0L=2.0 H and a capacitor with capacitance CC are connected in an ideal LC circuit. The charge on the capacitor oscillates with a period of π\pi seconds. What is the value of the capacitance CC?

  1. 0.1250.125 F (correct answer)
  2. 0.250.25 F
  3. 0.500.50 F
  4. 2.02.0 F
Explanation: The period of an LC circuit is T=2πLCT = 2\pi\sqrt{LC}. We are given T=πT = \pi s and L=2.0L = 2.0 H. Plugging these values in: π=2π(2.0)C\pi = 2\pi\sqrt{(2.0)C}. Dividing by 2π2\pi gives 1/2=2C1/2 = \sqrt{2C}. Squaring both sides gives 1/4=2C1/4 = 2C, so C=1/8=0.125C = 1/8 = 0.125 F.

Question 11

The behavior of the charge qq in an ideal LC circuit is described by the differential equation d2qdt2+2500q=0\frac{d^2q}{dt^2} + 2500q = 0, where qq is in coulombs and tt is in seconds. What is the angular frequency of the oscillation?

  1. 25002500 rad/s
  2. 2500/π\sqrt{2500/\pi} rad/s
  3. 5050 rad/s (correct answer)
  4. 2525 rad/s
Explanation: The standard form of the differential equation for simple harmonic motion, which applies to an LC circuit, is d2qdt2+ω2q=0\frac{d^2q}{dt^2} + \omega^2 q = 0. By comparing the given equation to this standard form, we can identify that ω2=2500\omega^2 = 2500 s2^{-2}. Taking the square root gives the angular frequency ω=50\omega = 50 rad/s.

Question 12

In an ideal LC circuit with inductance L=4.0L = 4.0 H and capacitance C=9.0C = 9.0 F, the maximum current observed is Imax=0.5I_{max} = 0.5 A. What is the maximum charge QmaxQ_{max} stored on the capacitor?

  1. 1.51.5 C
  2. 3.03.0 C (correct answer)
  3. 6.06.0 C
  4. 1818 C
Explanation: By conservation of energy, the maximum energy in the inductor equals the maximum energy in the capacitor: 12LImax2=12Qmax2C\frac{1}{2}LI_{max}^2 = \frac{1}{2}\frac{Q_{max}^2}{C}. Solving for QmaxQ_{max} gives Qmax=ImaxLC=(0.5 A)(4.0 H)(9.0 F)=(0.5 A)36 s2=(0.5 A)(6 s)=3.0Q_{max} = I_{max}\sqrt{LC} = (0.5 \text{ A})\sqrt{(4.0 \text{ H})(9.0 \text{ F})} = (0.5 \text{ A})\sqrt{36 \text{ s}^2} = (0.5 \text{ A})(6 \text{ s}) = 3.0 C.

Question 13

An LC circuit oscillates with a natural frequency ff. If the inductance is doubled and the capacitance is increased to eight times its original value, what is the new frequency of oscillation?

  1. f/16f/16
  2. 16f16f
  3. f/4f/4 (correct answer)
  4. 4f4f
Explanation: The natural frequency of an LC circuit is given by f=12πLCf = \frac{1}{2\pi\sqrt{LC}}. Let Lnew=2LL_{new} = 2L and Cnew=8CC_{new} = 8C. The new frequency is fnew=12π(2L)(8C)=12π16LC=14(12πLC)=f4f_{new} = \frac{1}{2\pi\sqrt{(2L)(8C)}} = \frac{1}{2\pi\sqrt{16LC}} = \frac{1}{4} \left( \frac{1}{2\pi\sqrt{LC}} \right) = \frac{f}{4}.

Question 14

Which of the following statements provides the best description of the energy transformations in an ideal LC circuit?

  1. Energy is continuously dissipated as thermal energy due to the resistance of the inductor and connecting wires.
  2. The circuit's total energy oscillates between a maximum value and zero with a frequency determined by L and C.
  3. Energy is transformed back and forth between the electric field of the capacitor and the magnetic field of the inductor. (correct answer)
  4. A constant source of energy, such as a battery, must be present to sustain the oscillations in the circuit.
Explanation: In an ideal LC circuit with no resistance, the total electromagnetic energy is conserved. This energy oscillates between being stored as electric potential energy in the capacitor's electric field and as magnetic potential energy in the inductor's magnetic field.

Question 15

In an ideal LC circuit, which of the following quantities oscillate sinusoidally with time?

  1. Charge on the capacitor, current in the inductor, and total energy in the circuit.
  2. Energy in the capacitor and energy in the inductor only.
  3. Total energy in the circuit only.
  4. Charge on the capacitor and current in the inductor only. (correct answer)
Explanation: In an ideal LC circuit, the charge on the capacitor and the current in the inductor vary sinusoidally as energy is transferred between the two components. The total energy of the circuit is conserved and remains constant, so it does not oscillate. While the individual energies of the capacitor and inductor do oscillate, their functional form is proportional to cos2\cos^2 or sin2\sin^2, which is not a simple sinusoid, and they oscillate at twice the frequency of the charge and current.

Question 16

An LC circuit consists of a 1010 mH inductor and a 1010 μ\muF capacitor. The capacitor is initially charged to a maximum charge of 1010 mC. What is the maximum current in the circuit?

  1. 0.10.1 A
  2. 1.01.0 A (correct answer)
  3. 1010 A
  4. 100100 A
Explanation: The maximum current ImaxI_{max} is related to the maximum charge QmaxQ_{max} by Imax=ωQmaxI_{max} = \omega Q_{max}. The angular frequency is ω=1/LC=1/(10×103 H)(10×106 F)=1/104 s2=100\omega = 1/\sqrt{LC} = 1/\sqrt{(10 \times 10^{-3} \text{ H})(10 \times 10^{-6} \text{ F})} = 1/\sqrt{10^{-4} \text{ s}^2} = 100 rad/s. Therefore, Imax=(100 rad/s)(10×103 C)=1.0I_{max} = (100 \text{ rad/s})(10 \times 10^{-3} \text{ C}) = 1.0 A.

Question 17

An ideal LC circuit consists of a capacitor with capacitance CC and an inductor with inductance LL. What is the angular frequency ω\omega of the electromagnetic oscillations in the circuit?

  1. ω=1LC\omega = \frac{1}{\sqrt{LC}} (correct answer)
  2. ω=LC\omega = \sqrt{\frac{L}{C}}
  3. ω=CL\omega = \sqrt{\frac{C}{L}}
  4. ω=LC\omega = \sqrt{LC}
Explanation: The differential equation for an ideal LC circuit is Ld2qdt2+1Cq=0L\frac{d^2q}{dt^2} + \frac{1}{C}q = 0, which is the equation for simple harmonic motion, d2qdt2+ω2q=0\frac{d^2q}{dt^2} + \omega^2 q = 0. Comparing these gives ω2=1LC\omega^2 = \frac{1}{LC}, so the angular frequency is ω=1LC\omega = \frac{1}{\sqrt{LC}}.

Question 18

An ideal LC circuit contains an inductor of inductance LL and a capacitor of capacitance CC. What is the period TT of the oscillations in this circuit?

  1. T=LC2πT = \frac{\sqrt{LC}}{2\pi}
  2. T=12πLCT = \frac{1}{2\pi\sqrt{LC}}
  3. T=2πLCT = 2\pi\sqrt{\frac{L}{C}}
  4. T=2πLCT = 2\pi\sqrt{LC} (correct answer)
Explanation: The angular frequency of an LC circuit is ω=1LC\omega = \frac{1}{\sqrt{LC}}. The period TT is related to the angular frequency by T=2πωT = \frac{2\pi}{\omega}. Substituting the expression for ω\omega gives T=2πLCT = 2\pi\sqrt{LC}.

Question 19

An LC circuit has an oscillation period of TT. If the inductance LL is quadrupled while the capacitance CC remains the same, what is the new period of oscillation?

  1. T/2T/2
  2. 2T2T (correct answer)
  3. 4T4T
  4. TT
Explanation: The period of an LC circuit is given by T=2πLCT = 2\pi\sqrt{LC}. If the inductance becomes 4L4L, the new period TnewT_{new} will be Tnew=2π(4L)C=2(2πLC)=2TT_{new} = 2\pi\sqrt{(4L)C} = 2(2\pi\sqrt{LC}) = 2T.

Question 20

In an ideal LC circuit, the charge on the capacitor is given by q(t)=Qmaxcos(ωt)q(t) = Q_{max} \cos(\omega t). Which expression represents the current I(t)I(t) in the circuit, assuming I=dq/dtI = dq/dt?

  1. I(t)=ωQmaxsin(ωt)I(t) = -\omega Q_{max} \sin(\omega t) (correct answer)
  2. I(t)=ωQmaxsin(ωt)I(t) = \omega Q_{max} \sin(\omega t)
  3. I(t)=ωQmaxcos(ωt)I(t) = \omega Q_{max} \cos(\omega t)
  4. I(t)=Qmaxωsin(ωt)I(t) = -\frac{Q_{max}}{\omega} \sin(\omega t)
Explanation: Current is the time derivative of charge, I(t)=dqdtI(t) = \frac{dq}{dt}. Taking the derivative of the given expression for charge gives I(t)=ddt(Qmaxcos(ωt))=ωQmaxsin(ωt)I(t) = \frac{d}{dt}(Q_{max} \cos(\omega t)) = -\omega Q_{max} \sin(\omega t).