🧪Advanced Chemical Engineering Science Unit 6 – Non-Ideal Behaviors & Equations of State
Non-ideal behaviors in gases occur when real-world conditions deviate from the ideal gas law assumptions. This unit explores how factors like high pressure and low temperature affect gas behavior, introducing the compressibility factor to quantify these deviations.
Equations of state, such as the virial equation and cubic equations, model real gas behavior more accurately. These mathematical relationships incorporate critical properties and intermolecular forces, enabling better predictions for chemical engineering applications like process design and phase equilibrium calculations.
Non-ideal behavior occurs when gases deviate from the assumptions of the ideal gas law at high pressures, low temperatures, or near the critical point
Compressibility factor (Z) quantifies the extent of non-ideal behavior and equals 1 for an ideal gas but varies with pressure and temperature for real gases
Equations of state (EOS) mathematically describe the relationship between pressure, volume, temperature, and composition for real gases
Virial equation expresses the compressibility factor as a power series expansion in terms of pressure or density
Cubic equations of state (van der Waals, Redlich-Kwong, Soave-Redlich-Kwong, Peng-Robinson) model non-ideal behavior using empirical parameters specific to each gas
Incorporate critical properties and acentric factor to improve accuracy
Intermolecular forces (van der Waals forces) and molecular size effects contribute to non-ideal behavior
Applications in chemical engineering include process design, equipment sizing, phase equilibrium calculations, and thermodynamic analysis
Ideal Gas Law Recap
Ideal gas law: PV=nRT, where P is pressure, V is volume, n is moles of gas, R is the universal gas constant, and T is absolute temperature
Assumes gas molecules are point particles with no intermolecular forces and elastic collisions
Valid for gases at low pressures and high temperatures, where intermolecular distances are large compared to molecular size
Ideal gas law derives from the kinetic theory of gases and combines Boyle's law, Charles's law, and Avogadro's law
Limitations arise when intermolecular forces become significant, and molecular size is non-negligible compared to intermolecular distances
Leads to deviations from ideal behavior
Molar volume of an ideal gas depends only on temperature and pressure, not on the nature of the gas
Compressibility factor (Z) equals 1 for an ideal gas at all conditions
Deviations from Ideal Behavior
Real gases deviate from ideal behavior due to intermolecular forces and molecular size effects
Attractive forces (van der Waals forces) reduce the pressure compared to an ideal gas
Repulsive forces at short distances increase the pressure
Finite molecular size reduces the available volume for molecular motion
Deviations become significant at high pressures, low temperatures, or near the critical point
Compressibility factor (Z) quantifies the extent of deviation from ideality
Z < 1 indicates dominant attractive forces (e.g., at moderate pressures)
Z > 1 indicates dominant repulsive forces (e.g., at high pressures)
Critical point represents the end of the vapor-liquid equilibrium curve, beyond which distinct liquid and gas phases do not exist
Reduced properties (reduced temperature, pressure, and volume) normalize the state variables with respect to critical properties
Enable comparison of different gases using the principle of corresponding states
Acentric factor (ω) characterizes the non-sphericity of molecules and affects the shape of the vapor-liquid equilibrium curve
Compressibility Factor
Compressibility factor (Z) relates the actual molar volume of a gas to the molar volume of an ideal gas at the same pressure and temperature
Z=nRTPV or Z=VidealVactual
Quantifies the deviation from ideal gas behavior
Z = 1 for an ideal gas
Z < 1 indicates attractive forces dominate (actual volume is smaller than ideal)
Z > 1 indicates repulsive forces dominate (actual volume is larger than ideal)
Varies with pressure and temperature for real gases
Generalized compressibility factor charts (Nelson-Obert or Standing-Katz) plot Z as a function of reduced pressure and reduced temperature
Allow estimation of Z without knowing the specific equation of state
Compressibility factor is essential for accurate calculations involving real gases, such as density, molar volume, and fugacity
Virial Equation of State
Virial equation expresses the compressibility factor as a power series expansion in terms of pressure or density
Z=1+B(T)RTP+C(T)(RTP)2+...
Z=1+B′(T)ρ+C′(T)ρ2+...
Virial coefficients (B, C, ...) depend on temperature and account for intermolecular interactions
B(T) represents two-body interactions, C(T) represents three-body interactions, and so on
Truncated after the second or third term for most applications
Suitable for low to moderate pressures and densities
Virial coefficients can be determined experimentally or estimated from intermolecular potential models (e.g., Lennard-Jones potential)
Provides a theoretical basis for understanding non-ideal behavior but may not be practical for complex mixtures or high-pressure applications
Cubic Equations of State
Cubic equations of state (EOS) model the pressure-volume-temperature relationship using a cubic polynomial in terms of molar volume
General form: P=V−bRT−V2+ubV+wb2a(T)
a(T) and b are empirical parameters related to attractive and repulsive forces, respectively
u and w are constants specific to each EOS
Van der Waals EOS: P=V−bRT−V2a
First cubic EOS to account for intermolecular forces and molecular size
Inaccurate for liquid densities and critical properties
Redlich-Kwong EOS: P=V−bRT−TV(V+b)a
Improves upon van der Waals EOS by introducing a temperature-dependent attractive term