integration of heat capacities

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  • 8/13/2019 Integration of Heat Capacities

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    Integration of Heat Capacities

    More ElaborateHeat Capacity Correlations for Wider Temperature

    Ranges in 7

    th

    Edition of Perrys Chemical Engineering HandbookTable 2-198 p.2-178-182

    Cp=C1+C2(C3/T/(sinh(C3/T))2+C4(C5/T/cosh(C5/T))

    2

    Temp in Degrees Kelvin

    Cp Expressed in Joules/kmol/oK

    sinh(C3/T) = (e(C3/T)

    - e-(C3/T)

    )/2

    cosh(C5/T) = (e(C5/T)

    + e-(C5/T)

    )/2

    Refer to Table B.2 in Felder & Rousseau

    (Form 1)CP= a +bT+CT2+dT

    3

    (Form 2) Cp= a + bT +C/T2

    Cp(Kilojoules/Mol/oK)

    Be Careful about Interpreting Constant Correctly

    from Felder & Rousseau

    Compound state Form Temp ax103bx10

    5 cx10

    8 dx10

    12

    Acetone l 1oC 123.0 18.6

    g 1oC 71.96 20.10 -12.78 34.76

    CaO c 2 K 41.84 2.03 -4.52x1010

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    Cp(Acetone Liq) = 0.123+18.6x10-5

    T where T inoC

    Cp(Acetone Gas) = 0.07196+20.10x10-5

    T-12.78x10-8

    T2+34.76x10

    -12 T

    3

    where T inoC

    Cp(CaO Solid) = 0.04184+2.03x10-5

    T +-4.52x102T

    -2where T in

    oK

    Be careful with Cp (Liq Water)=75.4 x10-3

    KJ/mol/oC=75.4KJ/Kmol/

    oC

    Other Heat Capacity Formulas

    For Liquids & Solids (Cp & Cv) about the same

    For Ideal Gases

    Cp=Cv+R

    Change in Specific Internal Energy

    For Process Undergoing Change in Volume & Temperature

    ),(),( 2211 VTVT

    dTCU

    T

    T

    v2

    1

    Exact for Ideal GasesGood for Real Gases if Volume Constant

    Good Approximation for Liquids & Solids

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    Change in Specific Enthalpy when T & P both Change

    (T1,P1) (T2,P2)

    Consider Two Step Path

    (T1,P1)(T1,P2)(T2,P2)For Ideal Gases

    2

    1

    2

    1

    2

    1

    )()( 1

    T

    T

    p

    T

    T

    p

    T

    T

    p dTCdTCRTdTCPVH

    Also For Ideal & Real Gases if P Constant

    2

    1

    T

    T

    pdTCH

    However for Solids & Liquids

    2

    1

    2

    1

    )(T

    T

    p

    T

    T

    p dTCPVdTCVPH

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    Use of Kopps Rule to Approximate Heat CapacitiesRefer to Perrys Handbook for Contributions of

    Organic Functional Groups

    Refer to Table B.10 (Atomic Heat Capacities)

    Cpa (J/g-atomoC)

    Element Solid Liquid

    C 7.5 12

    H 9.6 18

    B 11 20

    Si 16 24

    O 17 25

    F 21 29

    P 23 31

    S 26 31

    All Others 26 33

    Cp(SiO2Solid)= 16+2*17 = 50 J/Mol/oC

    Cp(SiO2Liquid) = 24 + 2*25 = =74 J/Mol/oC

    Enthalpy Changes of Mixtures of Gases or Liquids

    80

    25

    80

    25

    )tan(75)(50 dTeLiqOcCdTDecaneLiqCH pp

    Key Assumption: Ignoring the Heat of Mixing

    Heater50 Moles/hr

    C10H22(Liq)

    75Moles

    C8H18(Liq)

    @25oC

    50 Moles/hr

    C10H22(Liq)

    75Moles C8H18@80

    oC

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    For Very Dilute Solutions (Based Heat Capacity on Solvent &

    Ignore Solute

    Calculation of Change in Enthalpy

    80

    25

    )(1000 dTDecaneLiqCH p

    Key Assumption: Neglect Heat of Mixing

    Calculation of Heat Capacity of a Mixture &

    Enthalpy Change for Mixture(Neglect Heat of Mixing)

    dTTCH

    TCyTC

    T

    T

    mixp

    i

    piimixp

    2

    1

    )()(

    )()()(

    Heater1 MoleOctane(liq)

    1000 Moles

    Decane(liq)

    @25oC

    1 MoleOctane(liq)

    1000 Moles

    Decane(liq)

    @80oC