AP Physics 2 Quiz: Conservation Of Electric Energy
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Conservation Of Electric EnergyQuestion 1 of 20

A 1.5V1.5\,\text{V} ideal battery charges a capacitor C=2.0μFC=2.0\,\mu\text{F}, then is removed. Define the system as the capacitor only. The capacitor is then connected to an identical uncharged capacitor in parallel. Which statement correctly describes what happens to the electric potential energy stored in the capacitors?

It stays the same because total charge is conserved when the capacitors are connected.
It decreases because some energy must leave the capacitor system during charge redistribution.
It increases because the equivalent capacitance doubles when connected in parallel.
It becomes equal to the battery's power output because the battery set the initial voltage.
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AP Physics 2 Quiz

AP Physics 2 Quiz: Conservation Of Electric Energy

Practice Conservation Of Electric Energy in AP Physics 2 with focused quiz questions that help you check what you know, review explanations, and build confidence with test-style prompts.

What this quiz covers

This quiz focuses on Conservation Of Electric Energy, giving you a quick way to practice the rules, question types, and explanations that matter most for AP Physics 2.

How to use this quiz

Try each quiz question before looking at the correct answer. Use the explanations to review missed ideas, then come back to similar questions until the pattern feels familiar.

All questions

Question 1

A 1.5V1.5\,\text{V} ideal battery charges a capacitor C=2.0μFC=2.0\,\mu\text{F}, then is removed. Define the system as the capacitor only. The capacitor is then connected to an identical uncharged capacitor in parallel. Which statement correctly describes what happens to the electric potential energy stored in the capacitors?

  1. It stays the same because total charge is conserved when the capacitors are connected.
  2. It decreases because some energy must leave the capacitor system during charge redistribution. (correct answer)
  3. It increases because the equivalent capacitance doubles when connected in parallel.
  4. It becomes equal to the battery's power output because the battery set the initial voltage.

Explanation: This problem tests conservation of electric energy. Initially, the charged 2.0μF capacitor stores U₁ = ½(2.0μF)(1.5V)² = 2.25μJ. When connected to an identical uncharged capacitor, charge redistributes until both reach the same voltage. The total charge Q = (2.0μF)(1.5V) = 3.0μC is conserved, giving final voltage Vf = Q/Ctotal = 3.0μC/4.0μF = 0.75V. The final total energy is Uf = ½(4.0μF)(0.75V)² = 1.125μJ, which is half the initial energy. Choice A incorrectly assumes charge conservation implies energy conservation. Choice C wrongly thinks parallel connection increases energy, missing that energy is lost during charge redistribution. The strategy is to recognize that connecting capacitors at different voltages always dissipates energy, even though charge is conserved.

Question 2

A capacitor is charged to voltage V0V_0 and then disconnected from any battery. Define the system as capacitor + external agent. The agent slowly decreases the plate separation, increasing the capacitance by a factor of 3 while keeping charge on the plates constant. Which statement correctly describes the capacitor's stored energy?

  1. It increases by a factor of 3 because capacitance increases at constant charge.
  2. It decreases by a factor of 3 because U=Q22CU=\dfrac{Q^2}{2C} with constant QQ. (correct answer)
  3. It stays the same because energy cannot change without a battery present.
  4. It becomes zero because the electric field must vanish when plates move closer.

Explanation: This problem tests conservation of electric energy. When an isolated capacitor's plate separation decreases by factor of 3, its capacitance increases by factor of 3 (since C ∝ 1/d). With charge Q held constant, the stored energy U = Q²/2C decreases by factor of 3. If initially U₁ = Q²/2C, then finally U₂ = Q²/(2×3C) = U₁/3. Choice A incorrectly claims energy increases, confusing the inverse relationship between C and U at constant charge. Choice C wrongly assumes energy can't change without a battery, missing that the external agent does negative work by allowing attractive force between plates to pull them together. The strategy is to use U = Q²/2C for constant charge situations and remember that increasing capacitance decreases stored energy when charge is fixed.

Question 3

An external agent performs +10 J+10 \text{ J} of work to move a charge at a constant speed from point X to point Y in an electric field. What is the change in the electric potential energy of the charge-field system?

  1. +10 J+10 \text{ J} (correct answer)
  2. 10 J-10 \text{ J}
  3. Zero, because the speed is constant.
  4. The change cannot be determined without knowing the value of the charge.

Explanation: The work-energy theorem states that the net work done on an object equals its change in kinetic energy. Since the charge moves at a constant speed, its kinetic energy does not change, so the net work is zero. The net work is the sum of the work done by the external agent (WextW_{ext}) and the work done by the electric field (WEW_E). So, Wnet=Wext+WE=0W_{net} = W_{ext} + W_E = 0. This means WE=Wext=10 JW_E = -W_{ext} = -10 \text{ J}. The change in potential energy is related to the work done by the conservative electric field by ΔUE=WE\Delta U_E = -W_E. Therefore, ΔUE=(10 J)=+10 J\Delta U_E = -(-10 \text{ J}) = +10 \text{ J}.

Question 4

A capacitor C=2.0μFC=2.0\,\mu\text{F} is charged to V=8.0VV=8.0\,\text{V} by a battery and then disconnected. The plates are pulled farther apart so the capacitance becomes 1.0μF1.0\,\mu\text{F} while charge cannot leave. The system is the capacitor plus field. Which statement correctly describes the stored energy?​​

  1. It decreases because increasing plate separation weakens the electric field.
  2. It increases because U=Q22CU=\dfrac{Q^2}{2C} and CC decreases while QQ stays constant. (correct answer)
  3. It stays the same because the battery was disconnected so no energy can change.
  4. It becomes zero because the voltage must remain fixed at 8.0V8.0\,\text{V}.

Explanation: This question assesses the skill of conservation of electric energy. With the battery disconnected, charge Q is conserved, and increasing plate separation decreases C, so stored energy U = Q²/(2C) increases. This increase comes from mechanical work done pulling the plates apart, redistributing energy into the electric field. Energy is conserved as the external work adds to the system's stored energy without dissipation. Choice A wrongly says it decreases due to weakened field, missing the misconception that energy depends only on field strength without considering capacitance changes. Track where energy goes, not just where charge ends up.

Question 5

A small particle with charge q-q and mass mm is in a circular orbit of radius RR around a large, fixed particle with charge +Q+Q. What is the minimum speed the small particle must be given to escape to an infinite distance away?

  1. kQqmR\sqrt{\frac{kQq}{mR}}
  2. 2kQqmR\sqrt{\frac{2kQq}{mR}} (correct answer)
  3. kQq2mR\sqrt{\frac{kQq}{2mR}}
  4. kQqmR\frac{kQq}{mR}

Explanation: To escape, the particle's total energy must be at least zero. The total energy is the sum of kinetic and potential energy: E=K+UEE = K + U_E. To just escape (vf=0v_f=0 at r=r=\infty), the final total energy is zero. By conservation of energy, the initial total energy must also be zero. The initial potential energy is UE,i=k(+Q)(q)R=kQqRU_{E,i} = k\frac{(+Q)(-q)}{R} = -k\frac{Qq}{R}. The initial kinetic energy is Ki=12mvesc2K_i = \frac{1}{2}mv_{esc}^2. Setting Ei=0E_i=0 gives 12mvesc2kQqR=0\frac{1}{2}mv_{esc}^2 - k\frac{Qq}{R} = 0. Solving for vescv_{esc} yields vesc=2kQqmRv_{esc} = \sqrt{\frac{2kQq}{mR}}. Note that the initial speed for a circular orbit is less than this value.

Question 6

A particle of mass mm and charge +q+q is traveling with an initial speed vv. What magnitude of potential difference must the particle move through to be brought to rest?

  1. mv22q\frac{mv^2}{2q} (correct answer)
  2. mv2q\frac{mv}{2q}
  3. 2qmv2\frac{2q}{mv^2}
  4. 2qmv\frac{2q}{mv}

Explanation: To bring the particle to rest, the change in its kinetic energy must be ΔK=012mv2=12mv2\Delta K = 0 - \frac{1}{2}mv^2 = -\frac{1}{2}mv^2. By the work-energy theorem for conservative forces, ΔK=ΔUE\Delta K = -\Delta U_E. The change in potential energy is ΔUE=qΔV\Delta U_E = q \Delta V. Therefore, 12mv2=qΔV-\frac{1}{2}mv^2 = -q \Delta V. Solving for the magnitude of the potential difference ΔV|\Delta V| gives ΔV=mv22q|\Delta V| = \frac{mv^2}{2q}

Question 7

A proton and an electron are placed at rest at the exact midpoint between two large, parallel, oppositely charged conducting plates. The plates are separated by a distance dd. Which particle has the greater kinetic energy upon striking a plate?

  1. The proton, because it has a greater mass.
  2. The electron, because it has a smaller mass and thus greater acceleration.
  3. They both have the same kinetic energy. (correct answer)
  4. It depends on the separation distance dd between the plates.

Explanation: Let the potential difference between the plates be VV. The potential at the midpoint is V/2V/2 relative to the negative plate. The proton (charge +e+e) moves through a potential difference of V/2V/2 to reach the negative plate. The electron (charge e-e) moves through a potential difference of V/2V/2 to reach the positive plate. The magnitude of the change in potential energy for both is ΔUE=qΔV=e(V/2)|\Delta U_E| = |q \Delta V| = e(V/2). By conservation of energy, the kinetic energy gained by each is equal to this value. Thus, they strike the plates with the same kinetic energy.

Question 8

In a region with a static electric field, a charged particle is moved from point A to point B along two different paths. Path 1 is a straight line, while Path 2 is a curved path that is longer than Path 1. How does the change in the system's electric potential energy for Path 1, ΔU1\Delta U_1, compare to that for Path 2, ΔU2\Delta U_2?

  1. ΔU1>ΔU2\Delta U_1 > \Delta U_2 because Path 2 is longer.
  2. ΔU1<ΔU2\Delta U_1 < \Delta U_2 because the force is averaged over a longer distance.
  3. ΔU1=ΔU2\Delta U_1 = \Delta U_2 because the electrostatic force is a conservative force. (correct answer)
  4. The relationship cannot be determined without knowing the exact shape of Path 2.

Explanation: The electrostatic force is a conservative force. This means the work done by the force, and therefore the change in potential energy, depends only on the initial and final positions of the particle, not on the path taken between them. Since both paths start at A and end at B, the change in electric potential energy is the same for both paths: ΔU1=ΔU2\Delta U_1 = \Delta U_2.

Question 9

A 1.5 V1.5\ \text{V} ideal battery is connected to a parallel combination of C1=2.0 μFC_1=2.0\ \mu\text{F} and C2=6.0 μFC_2=6.0\ \mu\text{F} until steady state. System boundary: both capacitors only. Which statement correctly describes the energy distribution between the capacitors?

  1. C1C_1 stores three times the energy of C2C_2 because it has less charge.
  2. They store equal energy because they are in parallel.
  3. Neither stores energy because the battery provides constant power, not energy.
  4. C2C_2 stores three times the energy of C1C_1 because both have the same voltage. (correct answer)

Explanation: This problem tests conservation of electric energy. In parallel, both capacitors have the same voltage V = 1.5 V but different charges proportional to their capacitances. The energy stored in each is U = ½CV². Since C₂ = 6.0 μF = 3×C₁, we have U₂ = 3U₁. Specifically, U₁ = ½(2.0×10⁻⁶)(1.5)² = 2.25 μJ and U₂ = ½(6.0×10⁻⁶)(1.5)² = 6.75 μJ. Choice B incorrectly relates energy to charge amount, missing that for parallel capacitors at the same voltage, energy is directly proportional to capacitance. The strategy is to remember that for parallel capacitors, U ∝ C when V is constant.

Question 10

An electron is released from rest very close to the negative plate of a parallel-plate capacitor with a potential difference of VV between the plates. What is the kinetic energy of the electron just as it reaches the positive plate?

  1. eVeV (correct answer)
  2. eV-eV
  3. Zero, as the energy is stored as potential energy.
  4. It depends on the distance between the plates.

Explanation: The electron moves from the negative plate (lower potential) to the positive plate (higher potential). The potential difference it moves through is +ΔV+\Delta V. The charge of the electron is q=eq=-e. The change in kinetic energy is ΔK=ΔUE=qΔV=(e)(V)=eV\Delta K = -\Delta U_E = -q \Delta V = -(-e)(V) = eV. Since it starts from rest, its final kinetic energy is eVeV.

Question 11

An electron is released from rest in a region of space where there is a uniform electric field. It moves through a potential difference of +100 V+100 \text{ V}. What is the change in the kinetic energy of the electron?

  1. It increases by 1.6×1017 J1.6 \times 10^{-17} \text{ J}. (correct answer)
  2. It decreases by 1.6×1017 J1.6 \times 10^{-17} \text{ J}.
  3. It increases by 100 J100 \text{ J}.
  4. It decreases by 100 J100 \text{ J}.

Explanation: According to the conservation of energy, the change in kinetic energy is equal to the negative of the change in electric potential energy, ΔK=ΔUE\Delta K = -\Delta U_E. The change in potential energy is given by ΔUE=qΔV\Delta U_E = q \Delta V. For an electron, q=e=1.6×1019 Cq = -e = -1.6 \times 10^{-19} \text{ C}. Thus, ΔUE=(1.6×1019 C)(+100 V)=1.6×1017 J\Delta U_E = (-1.6 \times 10^{-19} \text{ C})(+100 \text{ V}) = -1.6 \times 10^{-17} \text{ J}. The change in kinetic energy is then ΔK=(1.6×1017 J)=+1.6×1017 J\Delta K = -(-1.6 \times 10^{-17} \text{ J}) = +1.6 \times 10^{-17} \text{ J}. The positive sign indicates an increase in kinetic energy.

Question 12

A proton with an initial kinetic energy of K0K_0 travels directly toward a region of increasing electric potential. Assuming the electric force is the only force acting on the proton, how does its kinetic energy change as it enters this region?

  1. The kinetic energy increases because the electric field does positive work on the proton.
  2. The kinetic energy decreases because the proton's electric potential energy increases. (correct answer)
  3. The kinetic energy remains constant because the electric field is conservative.
  4. The change in kinetic energy cannot be determined without knowing the path taken.

Explanation: For a positive charge like a proton, electric potential energy is given by UE=qVU_E = qV. As the proton moves to a region of increasing electric potential (VV increases), its electric potential energy UEU_E also increases. By the law of conservation of energy, the total energy (K+UEK + U_E) must remain constant. Therefore, if UEU_E increases, the kinetic energy KK must decrease.

Question 13

An electron and a proton are both accelerated from rest through the same potential difference, ΔV|\Delta V|. Which of the following correctly compares the final kinetic energy KK and final speed vv of the two particles?

  1. Ke>KpK_e > K_p and ve>vpv_e > v_p
  2. Ke<KpK_e < K_p and ve<vpv_e < v_p
  3. Ke=KpK_e = K_p and ve>vpv_e > v_p (correct answer)
  4. Ke=KpK_e = K_p and ve<vpv_e < v_p

Explanation: The change in kinetic energy is given by ΔK=qΔV\Delta K = -q \Delta V. Since the electron and proton have charges of the same magnitude (e) and are accelerated through the same potential difference, the magnitude of their change in kinetic energy will be the same: ΔK=eΔV|\Delta K| = e|\Delta V|. Thus, their final kinetic energies are equal, Ke=KpK_e = K_p. Since kinetic energy is K=12mv2K = \frac{1}{2}mv^2, the particle with the smaller mass will have the greater final speed. The electron's mass is much smaller than the proton's mass, so ve>vpv_e > v_p

Question 14

A charge of +2.0 C+2.0 \text{ C} is moved from a point with an electric potential of 50 V50 \text{ V} to a point with an electric potential of 20 V20 \text{ V}. What is the work done by the electric field on the charge?

  1. +60 J+60 \text{ J} (correct answer)
  2. 60 J-60 \text{ J}
  3. +140 J+140 \text{ J}
  4. 140 J-140 \text{ J}

Explanation: The work done by the electric field is equal to the negative of the change in electric potential energy: WE=ΔUEW_E = -\Delta U_E. The change in potential energy is ΔUE=qΔV=q(VfVi)\Delta U_E = q \Delta V = q(V_f - V_i). Here, q=+2.0 Cq = +2.0 \text{ C}, Vi=50 VV_i = 50 \text{ V}, and Vf=20 VV_f = 20 \text{ V}. So, ΔUE=(2.0 C)(20 V50 V)=60 J\Delta U_E = (2.0 \text{ C})(20 \text{ V} - 50 \text{ V}) = -60 \text{ J}. Therefore, the work done by the field is WE=(60 J)=+60 JW_E = -(-60 \text{ J}) = +60 \text{ J}.

Question 15

A small, positively charged particle is fired from a great distance with an initial speed viv_i directly toward a large, fixed, positively charged nucleus. The particle slows down due to repulsion and reaches a distance of closest approach, rminr_{min}.

If the experiment is repeated with a new particle of the same mass and charge, but with an initial speed of 2vi2v_i, what is the new distance of closest approach?

  1. rmin/4r_{min}/4 (correct answer)
  2. rmin/2r_{min}/2
  3. 2rmin2r_{min}
  4. 4rmin4r_{min}

Explanation: By conservation of energy, the initial kinetic energy is converted into electric potential energy at the closest approach. 12mvi2=kQqrmin\frac{1}{2}mv_i^2 = k\frac{Qq}{r_{min}}. When the initial speed is doubled, the initial kinetic energy becomes 12m(2vi)2=4×12mvi2\frac{1}{2}m(2v_i)^2 = 4 \times \frac{1}{2}mv_i^2. For this quadrupled energy to equal the potential energy at closest approach, we need 4×kQqrmin=kQqrnew4 \times k\frac{Qq}{r_{min}} = k\frac{Qq}{r_{new}}, which gives rnew=rmin/4r_{new} = r_{min}/4.

Question 16

A particle of charge +q+q and mass mm is released from rest at a point A where the electric potential is VAV_A. It then accelerates to a point B where the potential is VBV_B. Which expression represents the speed of the particle at point B?

  1. 2q(VBVA)m\sqrt{\frac{2q(V_B - V_A)}{m}}
  2. 2q(VAVB)m\sqrt{\frac{2q(V_A - V_B)}{m}} (correct answer)
  3. 2q(VAVB)m\frac{2q(V_A - V_B)}{m}
  4. q(VAVB)2m\frac{q(V_A - V_B)}{2m}

Explanation: From the conservation of energy, the gain in kinetic energy equals the loss in potential energy. KfKi=(UE,fUE,i)K_f - K_i = -(U_{E,f} - U_{E,i}). Since the particle starts from rest, Ki=0K_i = 0. So, 12mvf2=(qVBqVA)=q(VAVB)\frac{1}{2}mv_f^2 = -(qV_B - qV_A) = q(V_A - V_B). Solving for the final speed vfv_f gives vf=2q(VAVB)mv_f = \sqrt{\frac{2q(V_A - V_B)}{m}}. Note that for a positive charge to accelerate from rest, it must move to a region of lower potential, so VA>VBV_A > V_B, making the term under the square root positive.

Question 17

Three identical positive point charges are held at the vertices of an equilateral triangle. When the charges are released simultaneously from rest, they fly apart. Which of the following best describes the energy of the system of three charges as their separation increases?

  1. The total kinetic energy increases, and the total electric potential energy increases.
  2. The total kinetic energy decreases, and the total electric potential energy increases.
  3. The total kinetic energy increases, and the total electric potential energy decreases. (correct answer)
  4. The total kinetic energy decreases, and the total electric potential energy decreases.

Explanation: The system is isolated, so its total energy is conserved. The total energy is the sum of the total kinetic energy and the total electric potential energy. Initially, the charges are at rest, so the kinetic energy is zero, and the potential energy is positive due to repulsion. As they fly apart, their speeds increase, so the total kinetic energy increases. Because total energy must be conserved, the increase in kinetic energy must be accompanied by a decrease in electric potential energy.

Question 18

A proton is released from rest at x=4.0 mx = 4.0\text{ m} in a region where the electric potential is described by the function V(x)=(10 V/m2)x2V(x) = (10\text{ V/m}^2)x^2. What is the kinetic energy of the proton when it reaches the position x=2.0 mx = 2.0\text{ m}?

  1. 120 eV120 \text{ eV} (correct answer)
  2. 160 eV160 \text{ eV}
  3. 200 eV200 \text{ eV}
  4. 400 eV400 \text{ eV}

Explanation: The initial potential at xi=4.0 mx_i = 4.0\text{ m} is Vi=(10)(4.0)2=160 VV_i = (10)(4.0)^2 = 160 \text{ V}. The final potential at xf=2.0 mx_f = 2.0\text{ m} is Vf=(10)(2.0)2=40 VV_f = (10)(2.0)^2 = 40 \text{ V}. The change in potential is ΔV=VfVi=40 V160 V=120 V\Delta V = V_f - V_i = 40 \text{ V} - 160 \text{ V} = -120 \text{ V}. The change in kinetic energy is ΔK=ΔUE=qΔV\Delta K = -\Delta U_E = -q \Delta V. For a proton, q=+eq = +e. So, ΔK=(+e)(120 V)=+120 eV\Delta K = -(+e)(-120 \text{ V}) = +120 \text{ eV}. Since it started from rest, its final kinetic energy is 120 eV120 \text{ eV}.

Question 19

Two identical positive charges are released from rest at the same location in a uniform electric field. Charge 1 travels a distance d1d_1. Charge 2 travels a distance d2=2d1d_2 = 2d_1 along the same line. How does the kinetic energy gained by charge 2, K2K_2, compare to the kinetic energy gained by charge 1, K1K_1?

  1. K2=4K1K_2 = 4K_1
  2. K2=2K1K_2 = 2K_1 (correct answer)
  3. K2=K1K_2 = K_1
  4. K2=K1/2K_2 = K_1/2

Explanation: The kinetic energy gained is equal to the work done by the electric field, K=WE=FEdK = W_E = F_E d. In a uniform electric field, the force FE=qEF_E = qE is constant. Since the charges are identical, the force on each is the same. The work done is directly proportional to the distance traveled, dd. Since charge 2 travels twice the distance of charge 1 (d2=2d1d_2 = 2d_1), the work done on it is twice as large, and it gains twice the kinetic energy: K2=2K1K_2 = 2K_1.

Question 20

An electron is moving in a region of space where the electric potential creates a 'potential well,' which is a local minimum of potential energy. If the electron's total energy is less than the potential energy of the surrounding regions ('hills'), what is the most likely behavior of the electron?

  1. It will be trapped in the well, oscillating back and forth. (correct answer)
  2. It will escape from the well with a constant velocity.
  3. It will move to the point of lowest potential energy and come to rest.
  4. Its total energy will gradually decrease until it stops.

Explanation: This situation is analogous to a ball rolling in a valley. The electron's total energy is conserved. Since its total energy is less than the potential energy required to 'climb the hills,' it cannot escape the well. It will move back and forth, with its kinetic energy converting into potential energy as it moves away from the minimum, and potential energy converting back into kinetic energy as it moves toward the minimum. This constitutes oscillatory motion.