Electric Power

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Core Idea

Electric power is the rate at which electrical energy is converted to other forms: P = IV, measured in watts (W = J/s). For a resistor, this becomes P = I²R = V²/R using Ohm's law. Power dissipated as heat in a resistor (Joule heating) is always positive regardless of current direction. Over time, energy E = Pt is consumed; utility companies bill in kilowatt-hours (kWh), where 1 kWh = 3.6 MJ.

How It's Best Learned

Derive the three forms of the power formula from P = IV and V = IR. Apply to real-world problems: light bulb wattage, household circuits, and transmission line losses to understand why high-voltage transmission is efficient.

Common Misconceptions

Explainer

From your study of work and energy, you know that power is the rate of doing work: P = dW/dt, measured in watts. In a circuit, charges are the carriers of energy. When a charge q moves through a potential difference V, the work done on it is W = qV. Dividing both sides by time, the rate at which energy is delivered is P = (q/t) × V = IV, where I = q/t is the current. This gives the fundamental formula P = IV: power equals current times voltage. Every watt delivered to a circuit element represents one joule of energy per second flowing into it.

For a resistor obeying Ohm's law (V = IR), you can substitute to get two equivalent forms. Replacing V with IR gives P = I × (IR) = I²R; replacing I with V/R gives P = (V/R) × V = V²/R. All three formulas — P = IV, P = I²R, P = V²/R — are equivalent for a resistor, but they differ in which variable is held fixed. In a series circuit, the same current flows through all elements, so P = I²R is most useful; resistance increases power dissipation. In a parallel circuit, all elements share the same voltage, so P = V²/R is most useful; resistance decreases power dissipation. Choosing the wrong formula when the context implies the other is a common error.

The energy converted in a resistor appears as heat — this is Joule heating. It is irreversible: unlike energy stored in a capacitor or compressed spring, the heat dissipated cannot be converted back to electrical energy by the resistor. The total energy consumed over time t is E = Pt. Electric utility companies measure this in kilowatt-hours: a device drawing 1 kW for one hour consumes 1 kWh = 3.6 MJ. A 100 W light bulb running for 10 hours uses 1 kWh.

Understanding power also explains long-distance electrical transmission. Moving a given amount of power P at high voltage V requires only a small current I = P/V. Since transmission line losses scale as I²R (the Joule heating formula with fixed line resistance R), halving the current cuts losses by a factor of four. This is why power plants step voltage up to hundreds of thousands of volts for transmission, then step it back down for residential use. The physics is P = I²R: reduce I to reduce wasted heat in the lines.

Practice Questions 5 questions

Prerequisite Chain

Counting to 10Counting to 20Understanding ZeroThe Number ZeroCounting to FiveOne-to-One CorrespondenceCombining Small Groups Within 5Addition Within 10Addition Within 20Two-Digit Addition Without RegroupingTwo-Digit Addition with RegroupingAddition Within 100Repeated Addition as MultiplicationMultiplication 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 100Two-Digit by One-Digit DivisionDivision with RemaindersRemainders and Quotients in DivisionDivision Word ProblemsIntroduction to Long DivisionFactors and MultiplesPrime and Composite NumbersEquivalent FractionsRelating Fractions and DecimalsDecimal Place ValueReading and Writing DecimalsComparing and Ordering DecimalsAdding and Subtracting DecimalsMultiplying DecimalsDividing DecimalsDividing FractionsMixed Number ArithmeticOrder of OperationsInteger Order of OperationsVariable ExpressionsCombining Like TermsOne-Step EquationsTwo-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 IntroductionTrigonometric Ratios ReviewRadian MeasureConverting Between Degrees and RadiansThe Unit CircleGraphing Sine and CosineGraphing Tangent and Reciprocal Trigonometric FunctionsDerivatives of Trigonometric FunctionsAntiderivativesIterated Integrals and Fubini's TheoremDouble Integrals in Cartesian CoordinatesDouble Integrals over Rectangular RegionsDouble Integrals in Polar CoordinatesDouble Integrals: Definition and SetupIterated Integrals and Fubini's TheoremDouble Integrals over Rectangular RegionsDouble Integrals over General RegionsApplications of Double Integrals: Area, Mass, and MomentsTriple Integrals in Cartesian CoordinatesTriple Integrals in Cylindrical and Spherical CoordinatesChange of Variables and the Jacobian DeterminantApplications of Triple Integrals: Volume and MassVector Fields and Their RepresentationsLine Integrals of Vector FieldsConservative Vector Fields and Potential FunctionsElectric PotentialElectric Current and ResistanceOhm's LawElectric Power

Longest path: 86 steps · 382 total prerequisite topics

Prerequisites (2)

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