Vapor-liquid equilibrium is crucial for understanding absorption and stripping processes. Henry's law , Raoult's law , and K-values help predict how components distribute between phases. Absorption and stripping factors quantify the ease of separating components in these operations.
Mass transfer in gas-liquid systems involves concentration gradients and film resistances. The two-film theory models interface behavior, while overall mass transfer coefficients combine individual resistances. Understanding these concepts is essential for designing efficient absorption and stripping columns.
Vapor-Liquid Equilibrium and Mass Transfer in Absorption/Stripping
Vapor-liquid equilibrium in absorption
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Henry's law for dilute solutions describes solute concentration in vapor phase proportional to liquid phase
Expression: y = H x y = Hx y = H x relates mole fractions in vapor (y) and liquid (x) phases
H H H : Henry's constant varies with temperature, pressure (atm⋅L/mol)
Raoult's law for ideal solutions predicts vapor pressure of components in liquid mixture
Expression: y i = x i P i ∗ / P y_i = x_i P_i^*/P y i = x i P i ∗ / P calculates vapor composition from liquid composition
P i ∗ P_i^* P i ∗ : vapor pressure of pure component i i i at system temperature (kPa)
P P P : total system pressure (kPa)
K-values (vapor-liquid distribution ratios) measure tendency of component to vaporize
K i = y i / x i K_i = y_i/x_i K i = y i / x i represents ratio of mole fractions in vapor and liquid phases
Related to equilibrium constant, indicates relative volatility of components
Absorption factor quantifies ease of absorption process
A = L / ( m G ) A = L/(mG) A = L / ( m G ) compares liquid flow rate to product of gas flow rate and equilibrium line slope
L L L : liquid flow rate (mol/h), G G G : gas flow rate (mol/h), m m m : slope of equilibrium line
Stripping factor measures difficulty of removing solute from liquid phase
S = m G / L = 1 / A S = mG/L = 1/A S = m G / L = 1/ A inverse of absorption factor
Higher stripping factor indicates easier removal of solute from liquid
Mass transfer in gas-liquid systems
Two-film theory models mass transfer resistance at gas-liquid interface
Gas film resistance limits transfer of sparingly soluble gases (O₂ in water)
Liquid film resistance controls transfer of highly soluble gases (NH₃ in water)
Overall mass transfer coefficient combines individual film resistances
1 / K G = 1 / k G + m / k L 1/K_G = 1/k_G + m/k_L 1/ K G = 1/ k G + m / k L relates overall coefficient to gas and liquid film coefficients
K G K_G K G : overall gas-phase coefficient, k G k_G k G : gas-phase coefficient, k L k_L k L : liquid-phase coefficient
Concentration gradients drive mass transfer between phases
Steeper gradients lead to faster mass transfer rates
Diffusion in gas and liquid phases follows Fick's law
Flux proportional to concentration gradient and diffusion coefficient
Interfacial area affects absorption/stripping efficiency
Larger area increases mass transfer rate (packed columns, spray towers)
Mass transfer coefficients for columns
Gas-phase mass transfer coefficient (k G k_G k G ) estimated using dimensionless correlations
Sherwood number relates mass transfer to fluid flow and diffusion (Re, Sc)
Liquid-phase mass transfer coefficient (k L k_L k L ) predicted by theoretical models
Penetration theory assumes unsteady-state diffusion into liquid elements
Surface renewal theory considers continuous replacement of liquid surface
Overall mass transfer coefficient (K G K_G K G or K L K_L K L ) combines individual resistances
K G K_G K G used for gas-phase controlled systems, K L K_L K L for liquid-phase controlled
Specific interfacial area (a a a ) measures available surface for mass transfer
Defined as surface area per unit volume of column (m²/m³)
Volumetric mass transfer coefficient (K G a K_Ga K G a or K L a K_La K L a ) crucial for column design
Combines mass transfer coefficient and interfacial area
Empirical correlations estimate coefficients for different packing types
Random packing (Raschig rings, Pall rings) and structured packing (corrugated sheets)
Theoretical stages for separation
McCabe-Thiele method graphically determines number of equilibrium stages
Operating line represents material balance between phases
Equilibrium curve shows composition relationship at equilibrium
Step-wise construction between operating line and equilibrium curve
Kremser equation for absorbers calculates theoretical stages analytically
N = log [ ( A − 1 ) ( y 1 / y N + 1 − 1 / A ) + 1 ] log A N = \frac{\log[(A-1)(y_1/y_{N+1} - 1/A) + 1]}{\log A} N = l o g A l o g [( A − 1 ) ( y 1 / y N + 1 − 1/ A ) + 1 ]
N N N : number of theoretical stages, y 1 y_1 y 1 : inlet gas composition, y N + 1 y_{N+1} y N + 1 : outlet gas composition
Kremser equation for strippers determines stages for liquid purification
N = log [ ( S − 1 ) ( x N / x 0 − 1 / S ) + 1 ] log S N = \frac{\log[(S-1)(x_N/x_0 - 1/S) + 1]}{\log S} N = l o g S l o g [( S − 1 ) ( x N / x 0 − 1/ S ) + 1 ]
x N x_N x N : inlet liquid composition, x 0 x_0 x 0 : outlet liquid composition
Height equivalent to a theoretical plate (HETP) relates packed height to stages
HETP = total packed height / number of theoretical stages (m)
Height of a transfer unit (HTU) and number of transfer units (NTU) alternative approach
HTU represents height of column in which concentration change equals driving force
NTU measures difficulty of separation, analogous to number of stages