chapter 9 energy, enthalpy and thermochemistry

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Chapter 9 Energy, Enthalpy and Thermochemistr y The study of energy and its interconv ersions is called thermodynamics. Kinetic Energy: energy due to the mot ion of the object (1/2 mv 2 ) Potential Energy: energy due to posit ion or composition Heat: the transfer of energy between two objects due to a temperature diff erence Work: a force acting over a distance

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Chapter 9 Energy, Enthalpy and Thermochemistry. The study of energy and its interconversions is called thermodynamics . Kinetic Energy: energy due to the motion of the object (1/2 mv 2 ) Potential Energy: energy due to position or composition - PowerPoint PPT Presentation

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  • Chapter 9Energy, Enthalpy and ThermochemistryThe study of energy and its interconversions is called thermodynamics.Kinetic Energy: energy due to the motion of the object (1/2 mv2)Potential Energy: energy due to position or compositionHeat: the transfer of energy between two objects due to a temperature differenceWork: a force acting over a distance

  • Figure 9.1 (a): Initial position of balls

  • Figure 9.1 (b): Final position of balls

  • Energy of Matters

  • State FunctionA property of the system depends only on its present state. A state function does not depend in any way on the systems past.Energy is a state function, but work and heat are not state function

  • Combustion of methane

  • Nitrogen/oxygen

  • First Law of ThermodynamicsThe energy of the universe is constant

    In closed systemE= U=q+w (=+)q: the heat added to the system during the processw: the work done on the system during the processq>0 heat flows into the system from the surroundingsq0 work is done on the system by the surroundingsw

  • P-V Work

  • P-V Work

  • Enthalpy ()The heat qp absorbed in a constant-pressure process equals the systems enthalpy change.

  • For a chemical reaction H=Hproducts-HreactantsIf HreactantsHproducts (exothermic)

    Consider a constant-volume processdw=-PdV=0 ()U=q+w=qvU=qv

  • Heat Capacity ()

  • Thermodynamics of Ideal Gases

  • Heat Capacity of Heating an Ideal Monatomic GasUnder constant volume, the energy flowing into the gas is used to increase the translational energy of the gas molecules.

  • Heat Capacity of Ideal Monatomic Gases

    GasCv(J/K mol)Cp(J/K mol)He12.4720.8

    Ne12.4720.8 Ar12.4720.8

  • Heat Capacity of Diatomic Gases

  • Heat Capacity of Polyatomic Gases

  • Heat Capacity of Heating a Polyatomic GasPolyatomic gases have observed values for Cv that are significantly greater than 3/2 R.This larger value for Cv results because polyatomic molecules absorb energy to excite rotational and vibrational motions in addition to translational motions.

  • Cv and Cp of molecules

  • Cv and Cp of Monatomic Gas

  • Cv and Cp of H2O at 373K

  • 2 mol of monatomic ideal gasCalculate q, w, U and H for both pathway

  • TA=122K, TC=366K, TB=183K, TD=61K Cv=3/2R, Cp=5/2RPath 1(AC)w1=-PV=-2atm(30-10)L101.3J/Latm=-4.05103Jq1=qp=nCpT=25/2(R)(366-122)=1.01104J=H1U1=nCvT= 23/2(R)(366-122)=6.08103JPath 2(CB)q2=qv=nCvT=23/2(R)(183-366)=-4.56103J=U2H2=nCpT= 25/2(R)(183-366)=-7.6103JV=0 w2 =-PV =0

  • Path 3(AD)q3=qv=nCvT=23/2(R)(61-122)=-1.52103J=U3H3=nCpT= 25/2(R)(61-122)=-2.53103JV=0 w2 =-PV =0Path 4(DB)w1=-PV=-1atm(30-10)L101.3J/Latm=-2.03103Jq4=qp=nCpT=25/2(R)(183-61)=5.08104J=H4U4=nCvT= 23/2(R)(183-61)=3.05103J

  • SummaryPath 1qpath1=q1+q2=5.5 103Jwpath1=w1+w2= -4.05103JHpath1= H1 +H2= 2.55103JUpath1= U1 +U2= 1.52103JPath 2qpath2=q3+q4=3.56103Jwpath2=w3+w4= -2.03103JHpath2= H3 +H4= 2.55103JUpath2= U3 +U4= 1.52103J

  • CalorimetrySpecific heat capacity with unit JK-1g-1Molar heat capacity with unit JK-1mol-1

  • A constant-pressure calorimetry is used in determining the change in enthalpy equals the heat.H=qp=nCpTCoffee Cup Calorimeter

  • V=0U=qv+0=qvU=qv=nCv T

    Bomb Calorimeter

  • 2SO2(g)+O2(g)2SO3(g) H=-198 KJ2 mol. 1 mol. 2 mol.Calculate H and U

  • P is constant, H=qp=-198 KJ (energy flow out of system)U= qp +ww=-PV and V=n(RT/P)T and P are constant, n=nfinal-ninitial=-1 molSo w=-PV=-Pn (RT/P) =- nRT=-(-1)(8.314)(298)=2.48 kJU= qp +w=-198 kJ+2.48 kJ=-196 kJ

  • Hesss LawIf a reaction is carried out in a series of steps, H for the reaction will be equal to the sum of the enthalpy changes for the individual stepsThe overall enthalpy change for the process is independent of the number of steps or the particular nature of the path by which the reaction is carried out.

  • Consider the combustion reaction of methane to form CO2 and liquid H2OCH4(g) + 2O2(g) CO2(g) + 2H2O(l) H1 =-890KJ/mol This reaction can be thought of as occurring in two steps:CH4(g) + 2O2(g) CO2(g) + 2H2O(g) H2 = -802 kJ/mol2H2O(g)2H2O(l) H3 =-88KJ/molH1 = H2 + H3

  • Standard Enthalpies of FormationThe change in enthalpy that accompanies the formation of 1 mole of a compound from its elements with all substances in their standard states.The superscript zero indicates that the corresponding process has been carried out under standard conditions.

  • Petroleum and Natural Gas Coal

    Present Sources of EnergyNew Energy SourcesCoal ConversionHydrogen as a fuel

  • CO2 capture