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Electric Potential Energy

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Electric Charge and Coulomb's LawPotential Energy: Gravitational and Elastic+1 moreElectric PotentialEnergy Storage in Capacitor Fields+1 more
potential-energy work electrostatics conservative-force

Core Idea

The electric force is conservative, meaning the work it does on a charge moving between two points is path-independent and equals the negative change in electric potential energy: W = −ΔU. For two point charges separated by distance r, the electric potential energy is U = kq₁q₂/r. The reference point is typically U = 0 at r → ∞. For systems of multiple charges, total potential energy is the sum over all unique pairs.

How It's Best Learned

Connect to gravitational potential energy — both are conservative forces with 1/r² dependence (gravitation analogous to Coulomb). Practice computing U for 2-charge, then 3-charge systems. Use energy conservation to find speeds of released charges.

Common Misconceptions

Explainer

You already know gravitational potential energy: U_grav = mgh near Earth's surface, and more generally U_grav = −Gm₁m₂/r for two masses. Electric potential energy has an identical mathematical structure. For two point charges q₁ and q₂ separated by distance r, the electric potential energy is U = kq₁q₂/r — the same 1/r dependence, with mass replaced by charge and G replaced by k. This is not a coincidence: both the gravitational and electric forces are conservative, inverse-square forces. The mathematical framework carries over directly.

The critical conceptual point is that potential energy belongs to the pair of charges, not to either charge individually. When you push two positive charges together, you do work against the repulsive force, and that work is stored in the configuration — in the field between them. If you release them, the electric force does the work back, converting that stored energy into kinetic energy. The formula U = kq₁q₂/r encodes the sign automatically: two like charges have positive U (you had to invest energy to bring them together), and two opposite charges have negative U (they naturally attract, and you would need to invest energy to separate them to infinity).

The reference point convention — setting U = 0 at r → ∞ — means every finite separation has a potential energy measured relative to "infinitely apart." This is the same convention used in planetary mechanics. Work-energy accounting follows the conservative force rule you know: the work done *by* the electric force equals −ΔU. If a positive charge moves from a region of high potential energy to low potential energy, the electric force does positive work, and the charge gains kinetic energy equal to the energy it loses. An external agent pushing the charge the other way must do positive work equal to +ΔU.

For systems of three or more charges, the total potential energy is the sum over all unique pairs: U_total = U₁₂ + U₁₃ + U₂₃. Each pair contributes independently. The factor of ½ in the general formula U = ½Σᵢ qᵢVᵢ (where Vᵢ is the potential at charge i due to all other charges) avoids counting each pair twice — an algebraic identity that becomes important when charges are continuous distributions. The physical interpretation remains the same: U_total is the energy stored in the assembly, and it equals the work an external agent must do to assemble the configuration, bringing each charge in from infinity one by one.

Practice Questions 5 questions

Prerequisite Chain

Understanding ZeroThe Number ZeroCounting to FiveCounting to 10Counting to 20Counting a Set of Objects Up to 20Cardinality: The Last Number CountedMatching Numerals to QuantitiesSubitizing Small QuantitiesAddition Within 10Number Bonds to 10Addition Within 20Doubles and Near DoublesDoubles Facts Within 10Near Doubles Facts Within 20Mental Math Strategies for AdditionMental Math: Adding and Subtracting TensAddition Within 100Repeated Addition as MultiplicationMultiplication as Equal GroupsMultiplication: ArraysBasic Multiplication Facts (0s, 1s, 2s, 5s, 10s)Multiplication Facts Within 100Division as Equal SharingDivision as Grouping (Measurement Division)Division: Grouping (Repeated Subtraction) ModelDivision: Fair Sharing ModelDivision as Equal SharingDivision as GroupingBasic Division FactsDivision Facts Within 100Multiplication and Division Fact FamiliesRelationship Between Multiplication and DivisionDivision Facts as Inverse of MultiplicationRemainders and Quotients in DivisionDivision Word ProblemsMulti-Step Word ProblemsSolving Multi-Step Word ProblemsMultiplication Word ProblemsDivision Word ProblemsIntroduction to Long DivisionFactors and MultiplesPrime and Composite NumbersEquivalent FractionsRelating Fractions and DecimalsDecimal Place ValueIntegers and the Number LineComparing and Ordering IntegersAbsolute ValueAdding IntegersSubtracting IntegersMultiplying IntegersDividing IntegersUnit RatesProportionsPercent ConceptConverting Between Fractions, Decimals, and PercentsOperations with Rational NumbersTwo-Step EquationsSolving Multi-Step EquationsEquations with Variables on Both SidesAngle Pairs: Complementary, Supplementary, and VerticalParallel Lines and TransversalsCorresponding AnglesAlternate Interior AnglesTriangle Angle Sum TheoremExterior Angle TheoremTriangle Inequality TheoremSimilar Triangles: AA SimilaritySimilar Triangles: SSS and SAS SimilarityProportions in Similar TrianglesRight Triangle Trigonometry IntroductionSine, Cosine, and Tangent RatiosTrigonometric Ratios ReviewRadian MeasureConverting Between Degrees and RadiansThe Unit CircleGraphing Sine and CosineGraphing Tangent and Reciprocal Trigonometric FunctionsDerivatives of Trigonometric FunctionsAntiderivativesIndefinite IntegralsBasic Integration RulesRiemann SumsDefinite Integral DefinitionDouble Integrals: Definition and SetupIterated Integrals and Fubini's TheoremDouble Integrals over Rectangular RegionsDouble Integrals over General RegionsApplications of Double Integrals: Area, Mass, and MomentsWork Done by a ForcePotential Energy: Gravitational and ElasticElectric Potential Energy

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