THERMO:010117One n=2 polytrope on a mole of monatomic gas: end state, first-law ledger, and entropyView access optionsThermo Polytropic N2 State And WorkThermo First Law Entropy ON Quasistatic PathEquilibrium states, work, heat, and the first lawThermodynamics · Mixed review—
THERMO:010118Insulated vacuum free expansion to twice the volume: vanishing transfers and R ln 2 of entropyView access optionsThermo Free Expansion First LawThermo Irreversible Entropy BY State FunctionEquilibrium states, work, heat, and the first lawThermodynamics · Mixed review—
THERMO:010119Steady adiabatic nozzle: exit speed 100 sqrt(31) and area 2009 over 200000 sqrt(31)View access optionsThermo Steady Flow Energy NozzleThermo Continuity Ideal Gas Exit AreaEquilibrium states, work, heat, and the first lawThermodynamics · Mixed review—
THERMO:010220Two finite bodies at 500 K and 320 K: reversible meeting at 400 K and 2000 J of workView access optionsThermo Finite Bodies Reversible WorkThermo Direct Contact Entropy GenerationEntropy and the second lawThermodynamics · Mixed review—
THERMO:010221Landauer bound for resetting one equiprobable degenerate bit: kB T ln 2 at 300 KView access optionsThermo Landauer Erasure Entropy BoundThermo Logical Irreversibility Versus ComputationEntropy and the second lawThermodynamics · Mixed review—
THERMO:010322Osmotic pressure from the solvent chemical potentialView access optionsChemical Potential EquilibriumOsmotic Pressure Dilute LimitThermodynamic potentials and Legendre transformsThermodynamics · Mixed review—
THERMO:010323A reversible reaction finds the Gibbs minimum at one-fifth conversionView access optionsReaction Gibbs EquilibriumGibbs Minimum CurvatureThermodynamic potentials and Legendre transformsThermodynamics · Mixed review—
THERMO:010424A virial gas changes its Joule-Thomson sign at twice the characteristic temperatureView access optionsJoule Thomson Response IdentityInversion Temperature Sign AnalysisResponse functions and stabilityThermodynamics · Mixed review—
THERMO:010425Curie response warms an isolated magnetic sample during magnetizationView access optionsMagnetic Maxwell RelationMagnetocaloric Adiabatic ResponseResponse functions and stabilityThermodynamics · Mixed review—
THERMO:010426A dry parcel tests atmospheric stability against two environmental lapse ratesView access optionsDry Adiabatic Lapse DerivationParcel Environment Stability TestResponse functions and stabilityThermodynamics · Mixed review—
THERMO:010527The binary lever rule is a component balance across a tie lineView access optionsBinary Lever RuleTwo Phase Component BalancePhase equilibrium and transitionsThermodynamics · Mixed review—
THERMO:010528A spherical nucleus crosses a capillarity free-energy barrierView access optionsHomogeneous Nucleation BarrierFree Energy Stationary Point ClassificationPhase equilibrium and transitionsThermodynamics · Mixed review—
THERMO:010529Gibbs' phase rule counts variables after equilibrium constraintsView access optionsGibbs Phase RuleEquilibrium Constraint CountingPhase equilibrium and transitionsThermodynamics · Mixed review—
THERMO:010630Two Einstein solids exchange four quanta with multiplicity-weighted probabilitiesView access optionsEinstein Solid MultiplicityMicrocanonical Energy ExchangeMicroscopic interpretation and ensembles bridgeThermodynamics · Mixed review—
THERMO:010631Effusion samples the Maxwell gas with a speed-weighted flux biasView access optionsMaxwell Speed MomentsEffusive Flux WeightingMicroscopic interpretation and ensembles bridgeThermodynamics · Mixed review—
THERMO:9907001A sealed, rigid 0.080 m³ pharmaceutical autoclave is loaded with a spatially uniform water charge and then isolated…View problem statementState First LawThermodynamics Problem SolvingEquilibrium states, work, heat, and the first lawThermodynamics · Calculation—
THERMO:9907002A natural-gas booster station draws gas from a 400 mm supply main, compresses it, and discharges it into a 250 mm d…View access optionsState First LawThermodynamics Problem SolvingEquilibrium states, work, heat, and the first lawThermodynamics · Calculation—
THERMO:9907003A food-process tank holds 0.240 m³ of aqueous brine.View access optionsState First LawThermodynamics Problem SolvingEquilibrium states, work, heat, and the first lawThermodynamics · Calculation—
THERMO:9907004At a fixed instant, a closed vessel contains 6.50 kg of a simple compressible fluid occupying 0.325 m³ at 480 kPa a…View access optionsState First LawThermodynamics Problem SolvingEquilibrium states, work, heat, and the first lawThermodynamics · Calculation—
THERMO:9907005A simple compressible pure substance occupies a closed vessel.View access optionsState First LawThermodynamics Problem SolvingEquilibrium states, work, heat, and the first lawThermodynamics · Calculation—
THERMO:9907006Three closed samples of a simple compressible pure fluid are prepared.View access optionsState First LawThermodynamics Problem SolvingEquilibrium states, work, heat, and the first lawThermodynamics · Calculation—
THERMO:9907007A mountain meteorological station records a mercury-barometer height of 562 mm.View access optionsState First LawThermodynamics Problem SolvingEquilibrium states, work, heat, and the first lawThermodynamics · Calculation—
THERMO:9907008A nitrogen header is connected to an open U-tube manometer.View access optionsState First LawThermodynamics Problem SolvingEquilibrium states, work, heat, and the first lawThermodynamics · Calculation—
THERMO:9907009An open rectangular settling tank contains three distinct, immiscible liquid layers: 0.55 m of gasoline (specific g…View access optionsState First LawThermodynamics Problem SolvingEquilibrium states, work, heat, and the first lawThermodynamics · Calculation—