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.
A 1.5V ideal battery charges a capacitor C=2.0μF, 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?
AP Physics 2 Quiz
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.
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.
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.
A 1.5V ideal battery charges a capacitor C=2.0μF, 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?
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.
A capacitor is charged to voltage V0 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?
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.
An external agent performs +10 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?
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 (Wext) and the work done by the electric field (WE). So, Wnet=Wext+WE=0. This means WE=−Wext=−10 J. The change in potential energy is related to the work done by the conservative electric field by ΔUE=−WE. Therefore, ΔUE=−(−10 J)=+10 J.
A capacitor C=2.0μF is charged to V=8.0V by a battery and then disconnected. The plates are pulled farther apart so the capacitance becomes 1.0μF while charge cannot leave. The system is the capacitor plus field. Which statement correctly describes the stored energy?
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.
A small particle with charge −q and mass m is in a circular orbit of radius R around a large, fixed particle with charge +Q. What is the minimum speed the small particle must be given to escape to an infinite distance away?
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+UE. To just escape (vf=0 at r=∞), 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=kR(+Q)(−q)=−kRQq. The initial kinetic energy is Ki=21mvesc2. Setting Ei=0 gives 21mvesc2−kRQq=0. Solving for vesc yields vesc=mR2kQq. Note that the initial speed for a circular orbit is less than this value.
A particle of mass m and charge +q is traveling with an initial speed v. What magnitude of potential difference must the particle move through to be brought to rest?
Explanation: To bring the particle to rest, the change in its kinetic energy must be ΔK=0−21mv2=−21mv2. By the work-energy theorem for conservative forces, ΔK=−ΔUE. The change in potential energy is ΔUE=qΔV. Therefore, −21mv2=−qΔV. Solving for the magnitude of the potential difference ∣ΔV∣ gives ∣ΔV∣=2qmv2
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 d. Which particle has the greater kinetic energy upon striking a plate?
Explanation: Let the potential difference between the plates be V. The potential at the midpoint is V/2 relative to the negative plate. The proton (charge +e) moves through a potential difference of V/2 to reach the negative plate. The electron (charge −e) moves through a potential difference of V/2 to reach the positive plate. The magnitude of the change in potential energy for both is ∣ΔUE∣=∣qΔV∣=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.
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, compare to that for Path 2, ΔU2?
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.
A 1.5 V ideal battery is connected to a parallel combination of C1=2.0 μF and C2=6.0 μF until steady state. System boundary: both capacitors only. Which statement correctly describes the energy distribution between the capacitors?
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.
An electron is released from rest very close to the negative plate of a parallel-plate capacitor with a potential difference of V between the plates. What is the kinetic energy of the electron just as it reaches the positive plate?
Explanation: The electron moves from the negative plate (lower potential) to the positive plate (higher potential). The potential difference it moves through is +ΔV. The charge of the electron is q=−e. The change in kinetic energy is ΔK=−ΔUE=−qΔV=−(−e)(V)=eV. Since it starts from rest, its final kinetic energy is eV.
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. What is the change in the kinetic energy of the electron?
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. The change in potential energy is given by ΔUE=qΔV. For an electron, q=−e=−1.6×10−19 C. Thus, ΔUE=(−1.6×10−19 C)(+100 V)=−1.6×10−17 J. The change in kinetic energy is then ΔK=−(−1.6×10−17 J)=+1.6×10−17 J. The positive sign indicates an increase in kinetic energy.
A proton with an initial kinetic energy of K0 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?
Explanation: For a positive charge like a proton, electric potential energy is given by UE=qV. As the proton moves to a region of increasing electric potential (V increases), its electric potential energy UE also increases. By the law of conservation of energy, the total energy (K+UE) must remain constant. Therefore, if UE increases, the kinetic energy K must decrease.
An electron and a proton are both accelerated from rest through the same potential difference, ∣ΔV∣. Which of the following correctly compares the final kinetic energy K and final speed v of the two particles?
Explanation: The change in kinetic energy is given by ΔK=−qΔV. 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∣=e∣ΔV∣. Thus, their final kinetic energies are equal, Ke=Kp. Since kinetic energy is K=21mv2, 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>vp
A charge of +2.0 C is moved from a point with an electric potential of 50 V to a point with an electric potential of 20 V. What is the work done by the electric field on the charge?
Explanation: The work done by the electric field is equal to the negative of the change in electric potential energy: WE=−ΔUE. The change in potential energy is ΔUE=qΔV=q(Vf−Vi). Here, q=+2.0 C, Vi=50 V, and Vf=20 V. So, ΔUE=(2.0 C)(20 V−50 V)=−60 J. Therefore, the work done by the field is WE=−(−60 J)=+60 J.
A small, positively charged particle is fired from a great distance with an initial speed vi directly toward a large, fixed, positively charged nucleus. The particle slows down due to repulsion and reaches a distance of closest approach, rmin.
If the experiment is repeated with a new particle of the same mass and charge, but with an initial speed of 2vi, what is the new distance of closest approach?
Explanation: By conservation of energy, the initial kinetic energy is converted into electric potential energy at the closest approach. 21mvi2=krminQq. When the initial speed is doubled, the initial kinetic energy becomes 21m(2vi)2=4×21mvi2. For this quadrupled energy to equal the potential energy at closest approach, we need 4×krminQq=krnewQq, which gives rnew=rmin/4.
A particle of charge +q and mass m is released from rest at a point A where the electric potential is VA. It then accelerates to a point B where the potential is VB. Which expression represents the speed of the particle at point B?
Explanation: From the conservation of energy, the gain in kinetic energy equals the loss in potential energy. Kf−Ki=−(UE,f−UE,i). Since the particle starts from rest, Ki=0. So, 21mvf2=−(qVB−qVA)=q(VA−VB). Solving for the final speed vf gives vf=m2q(VA−VB). Note that for a positive charge to accelerate from rest, it must move to a region of lower potential, so VA>VB, making the term under the square root positive.
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?
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.
A proton is released from rest at x=4.0 m in a region where the electric potential is described by the function V(x)=(10 V/m2)x2. What is the kinetic energy of the proton when it reaches the position x=2.0 m?
Explanation: The initial potential at xi=4.0 m is Vi=(10)(4.0)2=160 V. The final potential at xf=2.0 m is Vf=(10)(2.0)2=40 V. The change in potential is ΔV=Vf−Vi=40 V−160 V=−120 V. The change in kinetic energy is ΔK=−ΔUE=−qΔV. For a proton, q=+e. So, ΔK=−(+e)(−120 V)=+120 eV. Since it started from rest, its final kinetic energy is 120 eV.
Two identical positive charges are released from rest at the same location in a uniform electric field. Charge 1 travels a distance d1. Charge 2 travels a distance d2=2d1 along the same line. How does the kinetic energy gained by charge 2, K2, compare to the kinetic energy gained by charge 1, K1?
Explanation: The kinetic energy gained is equal to the work done by the electric field, K=WE=FEd. In a uniform electric field, the force FE=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, d. Since charge 2 travels twice the distance of charge 1 (d2=2d1), the work done on it is twice as large, and it gains twice the kinetic energy: K2=2K1.
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?
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.