Sherwood Number Properties

The Sherwood Number is a dimensionless mass transfer coefficient. It represents the ratio of the convective mass transfer to the rate of diffusive mass transport across the boundary between two fluid phases.

The Continuous Phase Sherwood Number is used in the calculation of the mass transfer rate from the continuous phase to the dispersed phase. For the reverse mass transfer, from the dispersed phase to the continuous phase, the Dispersed Phase Sherwood Number is used.

The Sherwood Number is used in the following calculations:

  • Dissolution (Dissolution Mass Transfer Rate model)

    See Eqn. (2062) (continuous phase) and Eqn. (2062) (dispersed phase).

  • Droplet Evaporation (Single Component Droplet Evaporation Rate and Multicomponent Droplet Evaporation Mass Transfer Rate models)

    See Eqn. (2055) (continuous phase).

  • Solute Crystallization (Single Component Crystal Growth model)

    See Eqn. (2414) (continuous phase).

Sherwood Number Properties

Dimensions
Dimensionless.
Method
The method to use for specifying the Sherwood number that is used in the mass transfer rate calculation.
MethodCorresponding Method Node
Ranz-Marshall

The Sherwood number is computed using the Ranz-Marshall correlation (Eqn. (2063)).

Ranz-Marshall
Armenante-Kirwan

The model for mass transfer to micro-particles that was proposed by Armenante and Kirwan ([428]).

This method is available only for turbulent flow regimes.

Armenante-Kirwan

The Armenante-Kirwan node has the following properties:

  • Turbulent Reynolds Number Exponent

    This value is β in Eqn. (2420).

  • Prandtl Number Exponent

    This value is γ in Eqn. (2420).

  • Relative Density Difference Exponent

    This value is δ in Eqn. (2420).

  • Calibration Factor

    This value is α in Eqn. (2420).