Using the Mathur-Saxena Averaging Method for Dynamic Viscosity

This method becomes available when the multi-component gas model is used. Selecting this method provides the choice of the Chapman-Enskog method for Dynamic Viscosity on the Mixture Component level.

The following properties show up on the mixture component level:

  • Dipole momentum – a measure of polarity of a covalent bond in the molecule (always given in Debye)
  • Lennard-Jones characteristic length – the collision diameter (always given in Angstroms)
  • Lennard-Jones energy – the potential energy of attraction (given in K)

These properties have only one method available for their calculation: Constant. These values are used for calculating the dynamic viscosity of the individual component for the Chapman-Enskog method.

When the Method property of the Dynamic Viscosity node is set to Mathur-Saxena Averaging, the Multi-Component Gas > Material Properties > Dynamic Viscosity > Mathur-Saxena Averaging node appears.

The Mathur-Saxena Averaging methods for Dynamic Viscosity and Thermal Conductivity are specifications of the Multi-Component Mathur-Saxena Averaging Property method < Φ > where Φ is a material property. This method uses the following formula to compute the property on the mixture level, using values that are given for the individual mixture components ( X i is the mole fraction of component i ):

Figure 1. EQUATION_DISPLAY
Φ=12(1nXiΦi+(1nXiΦi)-1)
(144)

When the option is set, each component within the Gas Components manager has a Dynamic Viscosity node that contains the Chapman-Enskog node. See Using the Chapman-Enskog Method for Dynamic Viscosity.