Q&A_-6- 10/20/2005(6) Ji-Sheng Chang

12
The Advanced Chemical Engi neering Thermodynamics Heat(q) and work(w) effect s in a process and internal energy(U) and ent halpy(H) at a change of st ates Q&A_-6- 10/20/2005(6) Ji-Sheng Chang

description

The Advanced Chemical Engineering Thermodynamics Heat(q) and work(w) effects in a process and internal energy(U) and enthalpy(H) at a change of states. Q&A_-6- 10/20/2005(6) Ji-Sheng Chang. Equations of a substance. The ideal gas behavior of a fluid - PowerPoint PPT Presentation

Transcript of Q&A_-6- 10/20/2005(6) Ji-Sheng Chang

Page 1: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

The Advanced Chemical Engineering Thermodynamics

Heat(q) and work(w) effects in a process and

internal energy(U) and enthalpy(H) at a change of states

Q&A_-6- 10/20/2005(6)

Ji-Sheng Chang

Page 2: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

Equations of a substance

The ideal gas behavior of a fluid Volumetric equation:

PV=nRT, or PV=RT

Thermal equation: U=U(T), ordU=Cv(T)dT, and ΔU=∫Cv(T)dT;dH=Cp(T)dT, and ΔH=∫Cp(T)dT.

Page 3: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

Equations for process calculations

Equations of work, heat, internal energy, and enthalpy for process calculations

1. The first law of thermodynamics for closed system… dU=dQirr.+dWirr.= dQrev.+dWrev.

2. Internal energy… dU=CvdT 3. Enthalpy… dH=CpdT 4. Work… dWrev.=-PdV 5. Heat flow… dQrev.=dU+PdV

Page 4: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

Heat and work

Equations of work and heat for process calculations

1. Work …

2. Heat flow …

PdVR

CpVdP

R

CvdQ

V

dVRTCvdTdQ

P

dPRTCpdTdQ

V

dVRTdW

P

dPRTRdTdW

Page 5: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

Isothermal process

Equations of work, heat, internal energy, and enthalpy for process calculations

ΔT=0; ΔU=∫Cv dT=0 ΔH=∫Cp dT=0

W=-PdV Q=W

Page 6: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

Isobaric process

Equations of work, heat, internal energy, and enthalpy for process calculations

ΔH=∫Cp dT ΔU=∫Cv dT Q=ΔH W=ΔU-Q

Page 7: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

Isochoric process

Equations of work, heat, internal energy, and enthalpy for process calculations

ΔH=∫Cp dT ΔU=∫Cv dT Q=ΔU W=0

Page 8: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

Adiabatic process

Equations of work, heat, internal energy, and enthalpy for process calculations

Q=0 dU=W; CvdT=-PdV for ideal gas:

TVγ-1=constant TP(1-γ)/γ=constant PVγ=constant ; γ=Cp/Cv PV=RT; PV/T= constant

V

dVR

T

dTCv

Page 9: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

Polytropic process

Equations of work, heat, internal energy, and enthalpy for process calculations

Polytropic process : PVσ=constant Isothermal process : σ=1 Isobaric process : σ=0 Isochoric process : σ=∞ Adiabatic process : σ=γ

Page 10: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

Enthalpy change for a state change

Sensible heat effects of a change of states ΔH=∫Cp dT

Latent heats of pure substances Theoretical model

Empirical models

TCpdHTT 2

1

dT

dPVTH

sat

Page 11: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

Standard enthalpy change

Standard heat of reaction ΔH(T0)rexa.

Standard heat of formation ΔH(T0)form.

Standard heat of combustion ΔH(T0)comb.

Page 12: Q&A_-6-   10/20/2005(6) Ji-Sheng Chang

The heat of reaction

Temperature dependence of heat of reaction

ΔH(T)=ΔH(TT0)+ΔH(T0)+ΔH(T0 T) sensible heat

latent heat sensible heat