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Reading Time: 6 min
Last Updated: March 17, 2026
Main Ideas: 4
Reading Time: 6 min
Last Updated: March 17, 2026
Main Ideas: 4

Topic 10.4 Notes – Electric Potential Energy

Verified for 2027 AP® Physics 2 Exam
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Electric potential energy is the energy stored in a system of charges because of their positions relative to each other. It connects Coulomb’s law to conservation of energy. In this topic, you describe what electric potential energy means physically and calculate it for systems of up to four point charges.

What Electric Potential Energy Is

Electric potential energy UU is the energy stored in a system of charges due to their separation.

Two key ideas:

  • It equals the work an external force must do to bring charges from infinitely far apart (where U=0U = 0) to their current positions.
  • It belongs to the system of charges, not to just one charge by itself.

The zero reference point is defined at infinity. When charges are infinitely separated, we say U=0U = 0.

This mirrors gravitational potential energy:

  • Both come from conservative forces.
  • Energy depends only on positions, not the path taken.
  • Total mechanical energy E=K+UE = K + U is conserved (if isolated).

The Sign of UU

The sign tells you about attraction vs. repulsion.

  • Like charges (+/+ or −/−)
    • They repel.
    • You must push them together.
    • U>0U > 0
  • Unlike charges (+/−)
    • They attract.
    • They naturally move together and release energy.
    • U<0U < 0

If a system has negative UU, it’s a bound system. You must add energy to pull the charges apart to infinity.

Electric Potential Energy Between Two Point Charges

For two point charges, the equation you need is

U=kq1q2r U = k \frac{q_{1} q_{2}}{r}

  • k=8.99×109 N⋅m2/C2k = 8.99 \times 10^{9} \text{ N}\cdot\text{m}^{2}/\text{C}^{2}
  • q1,q2q_{1}, q_{2} in coulombs
  • rr in meters
  • UU in joules

If you graph this equation for opposite charges, you get a curve like this:

Study guide illustration

Electric potential energy vs. separation for opposite charges

How to Think About the Variables

  • Larger charge magnitudes → larger ∣U∣|U|.
  • Larger distance rr → smaller ∣U∣|U|.
  • The product q1q2q_{1} q_{2} determines the sign.

On the graph, notice that for an attractive pair the potential energy is negative and approaches 0 as rr becomes very large. As the charges get closer together, UU becomes more negative.

Quick reasoning example:

Suppose q1q_{1} and q2q_{2} are both positive. If you cut the distance in half, since U∝1/rU \propto 1/r, the potential energy doubles. On a multiple-choice question, they often test this proportional reasoning instead of full calculation.

Work and Separation

If the current potential energy is UU, then:

  • Work required to separate the charges to infinity Wexternal=−U W_{\text{external}} = -U

If UU is negative (attractive pair), separating them requires positive work.

That sign logic shows up constantly on FRQs.

Total Electric Potential Energy of Multiple Charges

For 3 or 4 point charges, the total potential energy is the sum of all unique pairs.

Utotal=∑kqiqjrij U_{\text{total}} = \sum k \frac{q_{i} q_{j}}{r_{ij}}

You calculate each pair separately and add them algebraically.

Number of Pairs

  • 2 charges → 1 pair
  • 3 charges → 3 pairs
  • 4 charges → 6 pairs

For three charges q1,q2,q3q_{1}, q_{2}, q_{3}:

Utotal=kq1q2r12+kq1q3r13+kq2q3r23 U_{\text{total}} = k\frac{q_{1} q_{2}}{r_{12}} + k\frac{q_{1} q_{3}}{r_{13}} + k\frac{q_{2} q_{3}}{r_{23}}

You never double-count.

How This Looks Physically

For three charges arranged in space, each pair has its own separation distance.

Study guide illustration

Three point charges and their pairwise separations

Each side of the triangle corresponds to one interaction term in the total energy: r12r_{12}, r13r_{13}, and r23r_{23}.

On tests, the hardest part is usually:

  • Finding the correct distances (geometry).
  • Keeping track of signs when adding terms.

Reminder: AP Physics 2 limits you to four or fewer point charges. No continuous charge distributions.

Conservation of Energy in Electric Systems

Because electric forces are conservative:

Etotal=K+U=constant E_{\text{total}} = K + U = \text{constant}

If opposite charges move closer:

  • UU becomes more negative.
  • KK increases.

If like charges are pushed closer:

  • UU increases.
  • External work must add energy.

The connection between force and energy is:

Welectric=−ΔU W_{\text{electric}} = -\Delta U

That negative sign is huge. When the electric force does positive work, potential energy decreases.

On FRQs, you’re often asked to explain this in words. A strong answer says something like:
“As the charges move closer, the electric force does positive work on the system, so electric potential energy decreases and kinetic energy increases to conserve total energy.”

Key Takeaways

Electric potential energy is a property of the system of charges, not one charge alone.
The zero reference point for electric potential energy is at infinity.
The sign of UU comes from the product q1q2q_{1} q_{2}, not from distance.
For multiple charges, add kqiqjrijk \frac{q_{i} q_{j}}{r_{ij}} for every unique pair.
The work required to separate charges to infinity equals −U -U .
In isolated systems, when UU decreases, KK must increase so that K+UK + U stays constant.

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Notes

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