| Parameter | Definition |
|---|---|
| Gibbs Phase Rule | F = C - P + 2, where F = degrees of freedom, C = number of components, P = number of phases |
| Degrees of Freedom | Number of intensive variables that can be independently varied without changing the number of phases |
| Phase | Homogeneous, physically distinct portion of a system separated by definite boundaries |
| Component | Chemically independent constituents of a system |
| Criterion | Mathematical Expression |
|---|---|
| Temperature Equality | Tα = Tβ = Tγ = ... for all phases |
| Pressure Equality | Pα = Pβ = Pγ = ... for all phases (no curved interfaces) |
| Chemical Potential Equality | μiα = μiβ = μiγ = ... for each component i in all phases |
| Fugacity Equality | fiα = fiβ = fiγ = ... for each component i in all phases |
| Equation | Expression |
|---|---|
| Raoult's Law | yiP = xiPisat, where yi = vapor mole fraction, xi = liquid mole fraction |
| K-value (Ideal) | Ki = yi/xi = Pisat/P |
| Relative Volatility | αij = Ki/Kj = (yi/xi)/(yj/xj) = Pisat/Pjsat |
| Bubble Point (T) | ΣxiPisat(T) = P |
| Dew Point (T) | Σyi/Ki = ΣyiP/Pisat(T) = 1 |
| Equation | Expression |
|---|---|
| Modified Raoult's Law | yiφiP = xiγiPisat, where γi = activity coefficient, φi = fugacity coefficient |
| Low Pressure Form | yiP = xiγiPisat (assumes φi ≈ 1) |
| Activity | ai = γixi |
| K-value (Non-Ideal) | Ki = (γiPisat)/(φiP) |
| Correlation | Equation |
|---|---|
| Antoine Equation | log10Psat = A - B/(C + T), where T in °C or K, Psat in mmHg or kPa |
| Clausius-Clapeyron | d(ln Psat)/dT = ΔHvap/(RT²) |
| Integrated C-C | ln(P2sat/P1sat) = -(ΔHvap/R)(1/T2 - 1/T1) |
| Model | Equation |
|---|---|
| Two-Suffix Margules | ln γ1 = Ax2²; ln γ2 = Ax1² |
| Three-Suffix Margules | ln γ1 = x2²[A12 + 2(A21 - A12)x1]; ln γ2 = x1²[A21 + 2(A12 - A21)x2] |
| Component | Equation |
|---|---|
| Component 1 | ln γ1 = A12/[1 + (A12x1)/(A21x2)]² |
| Component 2 | ln γ2 = A21/[1 + (A21x2)/(A12x1)]² |
| Expression | Equation |
|---|---|
| Binary System | ln γ1 = -ln(x1 + Λ12x2) + x2[Λ12/(x1 + Λ12x2) - Λ21/(x2 + Λ21x1)] |
| Wilson Parameter | Λij = (VjL/ViL)exp[-(λij - λii)/(RT)] |
| Parameter | Definition |
|---|---|
| Binary Activity Coefficient | ln γ1 = x2²[τ21(G21/(x1 + x2G21))² + (τ12G12)/(x2 + x1G12)²] |
| G Parameters | G12 = exp(-α12τ12); G21 = exp(-α21τ21) |
| τ Parameters | τ12 = (g12 - g22)/(RT); τ21 = (g21 - g11)/(RT) |
| α Parameter | Non-randomness parameter, 0.2 ≤ α ≤ 0.47 for most systems |
| Type | Characteristics |
|---|---|
| Minimum Boiling | xi = yi for all i; positive deviation from Raoult's Law; γi > 1 |
| Maximum Boiling | xi = yi for all i; negative deviation from Raoult's Law; γi <> |
| Azeotrope Condition | γ1P1sat = γ2P2sat at azeotropic composition |
| Concept | Description |
|---|---|
| Equilibrium Condition | xiαγiα = xiβγiβ for each component in phases α and β |
| Mutual Solubility | Concentrations of components in each phase at equilibrium |
| Distribution Coefficient | KD,i = xiβ/xiα |
| Plait Point | Point on phase diagram where two liquid phases become identical in composition |
| Parameter | Definition |
|---|---|
| Distribution Ratio | KD = concentration in extract/concentration in raffinate |
| Selectivity | β = (KD,solute)/(KD,carrier) |
| Extraction Factor | E = KD(S/F), where S = solvent flow, F = feed flow |
| Property | Description |
|---|---|
| Three Phases | Vapor phase in equilibrium with two immiscible liquid phases |
| Total Pressure | P = P1sat + P2sat for partially miscible binary at low mutual solubility |
| Vapor Composition | y1 = P1sat/(P1sat + P2sat) |
| Degrees of Freedom | F = C - P + 2 = 2 - 3 + 2 = 1 for binary VLLE |
| Equation | Expression |
|---|---|
| Ideal Solubility | ln xi = -(ΔHfus/R)(1/T - 1/Tm), where Tm = melting point |
| Non-Ideal Solubility | ln(γixi) = -(ΔHfus/R)(1/T - 1/Tm) |
| Eutectic Point | Lowest temperature at which liquid phase exists for binary system |
| Method | Expression |
|---|---|
| Fugacity from EOS | ln(fi/P) = ln φi = ∫∞V[(∂P/∂ni)T,V,nj - RT/V]dV - ln Z |
| Equilibrium Condition | φiVyiP = φiLxiP |
| K-value from EOS | Ki = yi/xi = φiL/φiV |
| Parameter | Expression |
|---|---|
| Equation | (P + a/V²)(V - b) = RT |
| Parameter a | a = 27R²Tc²/(64Pc) |
| Parameter b | b = RTc/(8Pc) |
| Parameter | Expression |
|---|---|
| Equation | P = RT/(V - b) - a/(T0.5V(V + b)) |
| Parameter a | a = 0.42748R²Tc2.5/Pc |
| Parameter b | b = 0.08664RTc/Pc |
| Parameter | Expression |
|---|---|
| Equation | P = RT/(V - b) - aα/(V(V + b)) |
| Parameter a | a = 0.42748R²Tc²/Pc |
| Parameter b | b = 0.08664RTc/Pc |
| α Function | α = [1 + m(1 - Tr0.5)]², where Tr = T/Tc |
| Parameter m | m = 0.480 + 1.574ω - 0.176ω², where ω = acentric factor |
| Parameter | Expression |
|---|---|
| Equation | P = RT/(V - b) - aα/(V(V + b) + b(V - b)) |
| Parameter a | a = 0.45724R²Tc²/Pc |
| Parameter b | b = 0.07780RTc/Pc |
| α Function | α = [1 + κ(1 - Tr0.5)]² |
| Parameter κ | κ = 0.37464 + 1.54226ω - 0.26992ω² |
| Rule | Expression |
|---|---|
| van der Waals One-Fluid | am = ΣΣyiyjaij; bm = Σyibi |
| Combining Rule | aij = (aiaj)0.5(1 - kij), where kij = binary interaction parameter |
| Geometric Mean | bij = (bi + bj)/2 |
| Definition | Expression |
|---|---|
| Z Factor | Z = PV/(RT) |
| Cubic Form (SRK/PR) | Z³ - Z² + (A - B - B²)Z - AB = 0 |
| Reduced Parameters | A = aαP/(R²T²); B = bP/(RT) |
| Property | Definition |
|---|---|
| Fugacity | Corrected pressure for non-ideal behavior: dGi = RTd(ln fi) |
| Fugacity Coefficient | φi = fi/(yiP) for vapor; φi = fi/(xiP) for liquid |
| Activity Coefficient | γi = fi/(xifi0), where fi0 = standard state fugacity |
| Phase | Expression |
|---|---|
| Vapor | ln(f/P) = ∫0P[(Z - 1)/P]dP |
| Liquid at Saturation | fisat = φisatPisat |
| Poynting Correction | fi = φisatPisatexp[ViL(P - Pisat)/(RT)] |
| Equation | Expression |
|---|---|
| Material Balance | zi = xiL + yiV, where zi = feed composition, L + V = 1 |
| Rachford-Rice | Σ[zi(Ki - 1)/(1 + V(Ki - 1))] = 0 |
| Liquid Composition | xi = zi/[1 + V(Ki - 1)] |
| Vapor Composition | yi = Kizi/[1 + V(Ki - 1)] |
| Equation | Expression |
|---|---|
| Henry's Law | fi = xiHi, where Hi = Henry's constant |
| Low Pressure Form | yiP = xiHi |
| Temperature Dependence | d(ln H)/dT = -ΔHsol/(RT²) |
| Combined Approach | For dilute solute: use Henry's Law; for solvent: use Raoult's Law |
| Property | Expression |
|---|---|
| Excess Gibbs Energy | GE = G - Gid = RT Σxiln γi |
| Excess Enthalpy | HE = H - Hid |
| Excess Entropy | SE = S - Sid |
| Excess Volume | VE = V - Vid |
| Form | Expression |
|---|---|
| General | Σxid(ln γi) = 0 at constant T and P |
| Binary | x1d(ln γ1) + x2d(ln γ2) = 0 |
| Consistency Test | ∫01ln(γ1/γ2)dx1 = 0 for thermodynamically consistent data |
| Relationship | Expression |
|---|---|
| From GE | ln γi = [∂(nGE/RT)/∂ni]T,P,nj |
| Temperature Dependence | [∂ln γi/∂T]P,x = -HiE/(RT²) |
| Infinite Dilution | γi∞ = limit as xi → 0 |
| Property | Definition |
|---|---|
| Critical Temperature | Highest temperature at which liquid and vapor can coexist |
| Critical Pressure | Vapor pressure at critical temperature |
| Critical Volume | Molar volume at critical point |
| Critical Criteria | (∂P/∂V)T = 0 and (∂²P/∂V²)T = 0 |
| Property | Definition |
|---|---|
| Reduced Temperature | Tr = T/Tc |
| Reduced Pressure | Pr = P/Pc |
| Reduced Volume | Vr = V/Vc |
| Acentric Factor | ω = -log10(Prsat)Tr=0.7 - 1.000 |
| Correlation | Expression |
|---|---|
| Compressibility | Z = Z(0) + ωZ(1), where Z(0) and Z(1) are functions of Tr and Pr |
| Fugacity Coefficient | ln φ = ln φ(0) + ω ln φ(1) |
| Lee-Kesler | Three-parameter corresponding states using ω |
| Type | Equation |
|---|---|
| Bubble Point T | ΣKi(T)xi = 1 at specified P |
| Bubble Point P | P = ΣxiKiP at specified T (rearranged form) |
| Vapor Composition | yi = Kixi |
| Type | Equation |
|---|---|
| Dew Point T | Σyi/Ki(T) = 1 at specified P |
| Dew Point P | Σyi/Ki = 1 at specified T |
| Liquid Composition | xi = yi/Ki |
| Method | Expression |
|---|---|
| Wilson Approximation | Ki = (Pc,i/P)exp[5.373(1 + ωi)(1 - Tc,i/T)] |
| DePriester Charts | Graphical correlation of K vs T and P for light hydrocarbons |
| Type | Characteristics |
|---|---|
| T-x-y (Isobaric) | Temperature vs composition at constant pressure; upper curve = bubble point, lower curve = dew point |
| P-x-y (Isothermal) | Pressure vs composition at constant temperature; upper curve = dew point, lower curve = bubble point |
| x-y Diagram | y vs x at constant T or P; 45° line = x = y; equilibrium curve above = more volatile in vapor |
| Test | Criterion |
|---|---|
| Redlich-Kister | |∫01ln(γ1/γ2)dx1| < 0.01="" for="" consistent=""> |
| Herington Test | D - J < 10,="" where="" d="">+ - A-|/(A+ + A-), J = 150|Tmax - Tmin|/Tmin |
| Parameter | Description |
|---|---|
| Supercritical Fluid | T > Tc and P > Pc; properties between liquid and gas |
| Solvent Power | Increases with density (pressure); tuneable by adjusting P and T |
| Common Solvents | CO₂ (Tc = 31.1°C, Pc = 73.8 bar); ethane; propane |
| Model | Application |
|---|---|
| Flory-Huggins | Activity coefficients for polymer-solvent systems |
| UNIFAC-FV | Free-volume modification for polymers |
| SAFT | Statistical Associating Fluid Theory for complex molecules |
| Model | Description |
|---|---|
| Debye-Hückel | Activity coefficients for dilute electrolytes based on ionic strength |
| Pitzer Equations | Virial expansion for concentrated electrolytes |
| NRTL-Electrolyte | Extension of NRTL for systems with ions |