Advanced Chemical Engineering Science

🧪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.

Key Concepts

  • 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=nRTPV = 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=PVnRTZ = \frac{PV}{nRT} or Z=VactualVidealZ = \frac{V_{\text{actual}}}{V_{\text{ideal}}}
  • 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)PRT+C(T)(PRT)2+...Z = 1 + B(T)\frac{P}{RT} + C(T)\left(\frac{P}{RT}\right)^2 + ...
    • Z=1+B(T)ρ+C(T)ρ2+...Z = 1 + B'(T)\rho + C'(T)\rho^2 + ...
  • 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=RTVba(T)V2+ubV+wb2P = \frac{RT}{V-b} - \frac{a(T)}{V^2 + ubV + wb^2}
    • 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=RTVbaV2P = \frac{RT}{V-b} - \frac{a}{V^2}
    • First cubic EOS to account for intermolecular forces and molecular size
    • Inaccurate for liquid densities and critical properties
  • Redlich-Kwong EOS: P=RTVbaTV(V+b)P = \frac{RT}{V-b} - \frac{a}{\sqrt{T}V(V+b)}
    • Improves upon van der Waals EOS by introducing a temperature-dependent attractive term
  • Soave-Redlich-Kwong (SRK) EOS: P=RTVba(T)V(V+b)P = \frac{RT}{V-b} - \frac{a(T)}{V(V+b)}
    • Incorporates the acentric factor to better represent the shape of the vapor-liquid equilibrium curve
  • Peng-Robinson (PR) EOS: P=RTVba(T)V(V+b)+b(Vb)P = \frac{RT}{V-b} - \frac{a(T)}{V(V+b)+b(V-b)}
    • Further improves the accuracy of liquid density and vapor pressure predictions
  • Cubic EOS require critical properties and acentric factor as input parameters
  • Widely used in process simulation and design due to their simplicity and reasonable accuracy

Applications in Chemical Engineering

  • Process design and simulation
    • Accurate prediction of thermodynamic properties (density, enthalpy, entropy) for real gases
    • Sizing of equipment (compressors, heat exchangers, separators) based on realistic gas behavior
  • Phase equilibrium calculations
    • Vapor-liquid equilibrium (VLE) for distillation, absorption, and stripping operations
    • Liquid-liquid equilibrium (LLE) for extraction processes
    • Vapor-liquid-liquid equilibrium (VLLE) for complex separations
  • Equations of state are used in conjunction with mixing rules and activity coefficient models for mixtures
  • Thermodynamic analysis
    • Calculation of departure functions (enthalpy, entropy) from ideal gas behavior
    • Estimation of fugacity coefficients and chemical potentials
  • Process optimization and control
    • Accurate models for real gas behavior enable better process performance and efficiency
  • Pipeline design and compressor selection
    • Accounting for non-ideal gas behavior in pressure drop and compressibility calculations
  • Reservoir engineering and enhanced oil recovery
    • Modeling the behavior of gases and gas mixtures in porous media

Problem-Solving Techniques

  • Identify the appropriate equation of state (EOS) for the given system and conditions
    • Ideal gas law for low pressures and high temperatures
    • Cubic EOS (SRK, PR) for moderate to high pressures and near-critical conditions
    • Virial equation for low to moderate pressures and densities
  • Determine the required input parameters for the chosen EOS
    • Critical properties (temperature, pressure, volume)
    • Acentric factor
    • Mixing rules and binary interaction parameters for mixtures
  • Use generalized compressibility factor charts (Nelson-Obert or Standing-Katz) for quick estimations
  • Solve the EOS analytically or numerically for the desired property (e.g., molar volume, density)
    • Cubic EOS require solving a cubic polynomial, which may have multiple real roots
    • Select the physically meaningful root based on the phase and stability criteria
  • Iterate the solution if necessary for temperature- or pressure-dependent properties
  • Validate the results using experimental data or other reliable sources
  • Perform sensitivity analysis to assess the impact of uncertainties in input parameters or EOS selection
  • Consider the limitations and assumptions of the chosen EOS and interpret the results accordingly


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AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.
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