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9.3 Conservation of Electric Energy

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Verified for the 2027 examUpdated September 2026Fiveable Content Team
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💡AP Physics C: Electricity and Magnetism Unit 9 Review

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9.3 Conservation of Electric Energy

💡 AP Physics C: Electricity and Magnetism

Conservation of electric energy connects how a charged object moves between two points at different electric potentials to its change in energy. The core relationship is ΔUE=qΔV\Delta U_E = q\Delta V, and because the electrostatic force is conservative, any loss in electric potential energy shows up as a gain in kinetic energy, or the reverse.

The Translation Between Representations question can draw on content from any unit, and the energy reasoning in this topic gives you practice connecting graphs, equations, and verbal explanations of the same scenario.

Energy Conservation for a Charge in a Potential Difference

  • The change in electric potential energy of a charge-field system is ΔUE=qΔV\Delta U_E = q\Delta V, measured in joules.
  • The electrostatic force is conservative, so energy is conserved: UE+KU_E + K stays constant when no nonconservative forces act.
  • A drop in electric potential energy means a gain in kinetic energy, and a rise in potential energy means a loss of kinetic energy.
  • The sign of the charge decides which way it moves "naturally." Positive charges tend toward lower potential, negative charges toward higher potential.
  • Use ΔK=−ΔUE=−qΔV\Delta K = -\Delta U_E = -q\Delta V to find speed changes from a potential difference.
  • Watch units and signs carefully. Coulombs times volts gives joules, and the sign of qq and ΔV\Delta V both matter.

Changes Due to Electric Potential Difference

System Energy Changes

When a charged object moves through an electric field, the energy of the charge-field system changes in a predictable way. The core relationship is:

ΔUE=qΔV\Delta U_{E}=q \Delta V

This says the change in electric potential energy depends on both the charge of the object and the potential difference it moves through.

  • The change in electric potential energy (ΔUE\Delta U_{E}) is measured in joules (J)
  • The charge (qq) is measured in coulombs (C)
  • The electric potential difference (ΔV\Delta V) is measured in volts (V)

For a positive charge:

  • Moving from high to low potential (downhill electrically), the system loses electric potential energy
  • Moving from low to high potential (uphill electrically), the system gains electric potential energy

A 1 coulomb positive charge moving through a potential difference of 5 volts has a change in electric potential energy of 5 joules. Whether that energy is gained or lost depends on whether the charge moves to higher or lower potential.

Conservation of energy ties the change in potential energy to an opposite change in kinetic energy:

  • Decreasing potential energy means increasing kinetic energy (the charge speeds up)
  • Increasing potential energy means decreasing kinetic energy (the charge slows down)

Charged Object Movement

ChargeMotion relative to EPotential changeElectric potential-energy changeKinetic-energy change
Positive charge (proton)With EToward lower VΔUE<0\Delta U_E<0ΔK>0\Delta K>0
Negative charge (electron)Opposite EToward higher VΔUE<0\Delta U_E<0ΔK>0\Delta K>0

How a charged particle moves in an electric field depends on the sign of the charge. The sign sets both the direction of motion and the energy transformation.

Positive charges (like protons) move naturally from high to low potential:

  • They move in the direction of the electric field
  • The field does positive work on the charge
  • Electric potential energy converts to kinetic energy
  • The particle accelerates in the field direction

Negative charges (like electrons) behave the opposite way:

  • They move naturally from low to high potential
  • They move opposite to the electric field direction
  • The field still does positive work on the charge
  • Electric potential energy converts to kinetic energy
  • The particle accelerates opposite to the field direction

The link between potential difference and kinetic energy change comes from the work-energy theorem:

ΔK=12mvf2−12mvi2=−qΔV\Delta K=\frac{1}{2} m v_{f}^{2}-\frac{1}{2} m v_{i}^{2}=-q \Delta V

This lets you calculate how much a charged particle's speed changes as it moves through a potential difference.

Conservation of Energy

Because the electrostatic force is conservative, energy conservation applies cleanly to a charge moving in an electric field. In an isolated system, energy is not created or destroyed, only transformed.

For a charged particle moving in an electric field:

UE+K=constantU_{E}+K=\text{constant}

The sum of electric potential energy and kinetic energy stays the same throughout the motion. As one increases, the other decreases by the same amount.

  • When electric potential energy decreases, kinetic energy increases
  • When electric potential energy increases, kinetic energy decreases
  • The magnitude of the change is identical for both forms of energy

In real setups, some energy can convert to thermal energy through resistance or friction. Even then, the total energy of the system (including thermal energy) stays constant, so conservation still holds.

Setting Up Charge Energy Problems Without Sign Errors

Problem Solving: A reliable approach for energy problems in this topic:

  1. Identify the charge qq (with its sign) and the potential difference ΔV\Delta V between start and end points.
  2. Find the change in potential energy with ΔUE=qΔV\Delta U_E = q\Delta V.
  3. Apply conservation of energy: ΔK=−ΔUE\Delta K = -\Delta U_E.
  4. If the charge starts from rest, the final kinetic energy equals ΔK\Delta K, so 12mvf2=−qΔV\tfrac{1}{2}mv_f^2 = -q\Delta V.
  5. Solve for the unknown (speed, energy, or potential difference) and check units.

Free Response: For the Translation Between Representations question, you may be asked to build an energy diagram for a charge moving through a region with an electric field and then connect it to an equipotential or field map. Show the trade-off between UEU_E and KK clearly, and justify why your energy diagram matches the field or equipotential picture. Tie your reasoning back to ΔUE=qΔV\Delta U_E = q\Delta V and energy conservation.

Common Trap: Sign errors are the biggest issue here. Keep the sign of the charge attached to qq and the sign of ΔV\Delta V attached to the potential difference. Decide direction of motion from the physics (positive charges fall toward lower potential, negative charges toward higher potential) rather than guessing from the math alone.

Practice Problem 1: Electron Acceleration

An electron (charge = -1.6 × 10^-19 C, mass = 9.11 × 10^-31 kg) accelerates from rest through a potential difference of 100 V. What is the final speed of the electron?

Solution

Use the relationship between potential difference and kinetic energy change:

ΔK=−qΔV\Delta K = -q \Delta V

Since the electron starts from rest, its initial kinetic energy is zero, so the final kinetic energy equals the change in kinetic energy:

Kf=ΔK=−qΔVK_f = \Delta K = -q \Delta V

For an electron with charge q = -1.6 × 10^-19 C moving through a potential difference of ΔV = 100 V:

Kf=−(−1.6×10−19 C)(100 V)=1.6×10−17 JK_f = -(-1.6 × 10^{-19} \text{ C})(100 \text{ V}) = 1.6 × 10^{-17} \text{ J}

Now find the final speed using the kinetic energy formula:

Kf=12mvf2K_f = \frac{1}{2}mv_f^2

Rearranging to solve for v_f:

vf=2Kfm=2(1.6×10−17 J)9.11×10−31 kg=5.92×106 m/sv_f = \sqrt{\frac{2K_f}{m}} = \sqrt{\frac{2(1.6 × 10^{-17} \text{ J})}{9.11 × 10^{-31} \text{ kg}}} = 5.92 × 10^6 \text{ m/s}

The electron's final speed is approximately 5.92 × 10^6 m/s.

Practice Problem 2: Conservation of Energy in an Electric Field

A proton (charge = 1.6 × 10^-19 C, mass = 1.67 × 10^-27 kg) is released from rest in a uniform electric field. After moving 5 cm, the proton has gained 8.0 × 10^-18 J of kinetic energy. What is the electric potential difference between the starting and ending points?

Solution

By conservation of energy, the decrease in electric potential energy equals the increase in kinetic energy:

−ΔUE=ΔK-\Delta U_E = \Delta K

Since the change in electric potential energy is related to the potential difference by:

ΔUE=qΔV\Delta U_E = q\Delta V

We can write:

−qΔV=ΔK-q\Delta V = \Delta K

Rearranging to solve for the potential difference:

ΔV=−ΔKq\Delta V = -\frac{\Delta K}{q}

Substituting the given values:

ΔV=−8.0×10−18 J1.6×10−19 C=−50 V\Delta V = -\frac{8.0 × 10^{-18} \text{ J}}{1.6 × 10^{-19} \text{ C}} = -50 \text{ V}

The negative sign means the proton moved from higher to lower potential. So the potential difference between start and end is 50 V, with the starting point at the higher potential.

Common Misconceptions

  • Misconception: Electric potential and electric potential energy are the same thing.
    Actually: Electric potential and electric potential energy are not the same thing. Potential (VV) is energy per unit charge at a point, while potential energy (UE=qΔVU_E = q\Delta V change) depends on the charge placed there.
  • Misconception: Positive work by the field always means the charge moves toward lower potential in space.
    Actually: Positive work by the field does not always mean the charge moves toward lower potential in space. For a negative charge, the field does positive work as it moves toward higher potential. Track the sign of qq in ΔUE=qΔV\Delta U_E = q\Delta V.
  • Misconception: A charge speeding up breaks energy conservation.
    Actually: A charge speeding up does not break energy conservation. The kinetic energy gained came from a drop in electric potential energy, so the total stays constant.
  • Misconception: ΔV\Delta V being negative automatically means potential energy decreases.
    Actually: ΔV\Delta V being negative does not automatically mean potential energy decreases. The sign of ΔUE\Delta U_E depends on the product qΔVq\Delta V, so a negative charge in a negative ΔV\Delta V gives a positive ΔUE\Delta U_E.
  • Misconception: Electric work depends on the path the charge takes.
    Actually: Electric work is path independent because the electrostatic force is conservative. Only the start and end potentials matter, not the route the charge takes.

Practice Questions for 9.3

1 of 10

To verify that the electric potential VV outside a charged metal sphere is proportional to 1/r1/r, a student releases a proton from rest at the surface (r=Rr=R) and measures its speed vv at various distances r>Rr > R. Which plot should be linear?

A.

Plot the square of the speed versus the natural log of the distance rr.

B.

Plot the square of the speed versus the reciprocal of the distance rr.

C.

Plot the speed versus the difference in the reciprocals of the distances.

D.

Plot the speed versus the reciprocal of the square of the distance rr.

Vocabulary

The following words are mentioned explicitly in the AP® course framework for this topic.

Term

Definition

charged object

An object that possesses electric charge and can experience forces from electric and magnetic fields.

conservation of energy

The principle that the total energy in an isolated system remains constant as energy changes forms or transfers between parts of the system.

electric potential

The electric potential energy per unit charge at a point in space, describing the work done per unit charge to move a test charge from a reference point to that location.

electric potential energy

The energy stored in a capacitor due to the separation of charge, equal to the work done by an external force to separate the charges.

kinetic energy

The energy of motion possessed by an object.

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