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restart;#'therm_eq4.mws'.22-6-00. |
Chapter 4: Set of pre-written equations available.
Definition of enthalpy, canonical differential form, and specific form for a simple system
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eq4_2a:=H=U+p*V;eq4_2b:=dH=T*dS+V*dp+Sum(mu[i]*n[i],i=1..C);eq4_2c:=dh=T*ds+v*dp; |
Definition of Helmholz's function, canonical differential form, and specific form for a simple system
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eq4_3a:=F=U-T*S;eq4_3b:=dF=-S*dT-p*dV+Sum(mu[i]*n[i],i=1..C);eq4_3c:=df=-s*dT-p*dv; |
Definition of Gibbs's function, canonical differential form, and specific form for a simple system
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eq4_4a:=G=U+p*V-T*S+Sum(mu[i]*n[i],i=1..C);eq4_4b:=dG=-S*dT+V*dp+Sum(mu[i]*dn[i],i=1..C);eq4_4c:=dg=-s*dT+v*dp; |
Definition of the thermodynamic coefficients cp,alpha,kappa
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eq4_16_1:=c[p]=T*ds_dT_p;eq4_16_2:=alpha=(1/v)*diff(v(T,p),T);eq4_16_3:=kappa=(-1/v)*diff(v(T,p),p); |
General differential forms for s, h and v in terms of T and p
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eq4_17_1:=ds=c[p]/T*dT-alpha*v*dp;eq4_17_2:=dh=c[p]*dT-(1-alpha*T)*v*dp;eq4_17_3:=dv=alpha*v*dT-kappa*v*dp; |
Definition of the compressibility factor
Guggenheim's correlation for the corresponding states vapour pressure
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eq4_37:=ln(p[r])=K*(1-1/T[r]); |
Enthalpy variation for a perfect gas and for a real gas (through the compressibility corrections
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eq4_35_4:=Dh=c[p]*DT;eq4_40_1:=Dh=Dh[id]-Dh[cc2]+Dh[cc1]; |
WARNING. A list of all variables follows, to copy and paste to the save command (after Maple7 there is no saving all). CAUTION: After pasting all, I must MANUALLY delete system variables: like RealRange_...
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save eq4_16_1, eq4_16_2, eq4_16_3, eq4_17_1, eq4_17_2, eq4_17_3,eq4_2a, eq4_2b, eq4_2c, eq4_30, eq4_35_4, eq4_37, eq4_3a, eq4_3b, eq4_3c, eq4_40_1, eq4_4a, eq4_4b,eq4_4c, "../therm_eq4.m":` |