Types of Work: Mechanical PdV and Beyond

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Core Idea

While PdV work (mechanical work against external pressure) is the most common form in thermodynamics, other work types include electrical work, surface work, and magnetic work. The first law generalizes as dU = đQ - đW_total, where W includes all forms of work done by the system; for a closed system with only PdV work, this simplifies to dU = đQ - PdV. Understanding which work terms apply is essential for applying the first law correctly to diverse physical systems.

How It's Best Learned

Solve problems with multiple work terms: a gas expanding against external pressure plus electrical work. Compare systems where PdV work dominates versus those where other work matters.

Common Misconceptions

Explainer

The first law says dU = đQ - đW. You've already learned that a system's internal energy changes when it receives heat or does work. But what counts as "work"? In introductory thermodynamics, work usually means PdV work — the mechanical work done when a gas expands against external pressure. When a piston pushes outward against pressure P, the work done by the gas is W = ∫P dV. This arises directly from the force-times-displacement picture you know from mechanics: pressure is force per area, and volume change is area times displacement, so P·dV is force times distance.

The first law is more general than any single work type, however. A battery discharging through a resistor does electrical work — charge moving through a potential difference. A soap bubble growing does surface work against surface tension — γ dA, where γ is the surface tension coefficient and dA is the change in area. A magnetized material does magnetic work — μ₀ H dM, where H is the applied field and M is the magnetization. In each case the work term has the same mathematical structure: an intensive variable (pressure, voltage, surface tension, magnetic field) multiplied by the differential of an extensive variable (volume, charge, area, magnetization). The total work is the sum of all applicable terms: đW_total = P dV + electrical + surface + magnetic + ....

For most large-scale gas problems, PdV dominates and all other terms are negligible — which is why introductory courses start there. But at small scales, the calculus changes. Inside a living cell, surface tension at membrane interfaces contributes meaningfully. Inside a lithium-ion battery, electrical work is the whole story. Inside a ferromagnet being magnetized, magnetic work is the relevant term. Knowing which work terms belong in a given situation is the first step in correctly applying the first law; including irrelevant terms wastes effort, while omitting relevant ones produces wrong answers.

Sign convention is a persistent source of confusion. The physics convention writes dU = đQ - đW, so work done *by* the system is positive (an expanding gas does positive work, losing internal energy). The engineering convention writes dU = đQ + đW, so work done *on* the system is positive (a compressor putting energy into a gas does positive work). Both conventions are self-consistent — they define đW with opposite signs. Always identify which convention a textbook or problem is using, and never mix them within a single calculation. When in doubt, state your convention explicitly before solving.

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 MomentsCenter of MassConservation of Linear MomentumElastic CollisionsInelastic CollisionsCoefficient of RestitutionCollision Analysis and Real-World ApplicationsTwo-Body Collisions in the Center-of-Mass FrameReduced Mass and Two-Body ProblemsKinematics in Two DimensionsProjectile MotionCircular Motion: KinematicsRotational KinematicsTorqueMoment of InertiaRotational Kinetic EnergyThe Work-Energy TheoremConservation of Mechanical EnergyFirst Law of ThermodynamicsTypes of Work: Mechanical PdV and Beyond

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