Rheology Models Reference

The available rheology models for viscous flow are the Generalized Newtonian, Viscoelastic, and Thixotropic models.

Generalized Newtonian Model

The Generalized Newtonian model simulates the behavior of viscous non-Newtonian liquids. The type of Generalized Newtonian fluid can be selected through the Dynamic Viscosity property.

Theory Generalized Newtonian Fluid
Provided by [physics continuum] > Models > Rheology
Example Node Path Continua > Physics 1 > Models > Generalized Newtonian
Requires Flow: Viscous Flow
Activates Physics Models Automatically selected models:
  • Equation of State: Constant Density
  • Viscous Regime: Laminar
Material Methods See Dynamic Viscosity

Viscoelastic Model

The Viscoelastic model expresses the behavior of the fluid as the sum of the behaviors of 1–8 modes. Each mode acts according to a rheology law specified for it under the Material Properties node of the model. In this way, you can model behaviors that are intermediate between those behaviors produced by individual models.

Theory Viscoelastic Fluids
Provided by [physics continuum] > Models > Rheology
Example Node Paths Continua > Physics 1 > Models > Viscoelastic

Continua > Physics 1 > Models > Multiphase > Eulerian Phases > Phase 1 > Models > Viscoelastic

Requires Flow: Viscous Flow
Properties See Viscoelastic Properties
Activates Physics Models
Automatically selected models:
  • Equation of State: Constant Density
  • Viscous Regime: Laminar
Material Methods Viscoelastic mode n
Monitors Constitutive n

ExtraStress n

Field Functions
  • Extra Stress n
  • Rate of Deformation
  • Total Viscosity
  • Viscoelastic Equivalent Viscosity

Viscoelastic Properties

Number of Modes
The number of nodes Viscoelastic mode n that appear under Liquid > [liquid] > Material Properties. See Viscoelastic Mode N.
Square-root conformal
When On, the viscous solver uses a square-root conformal formulation that is stable at high Weissenberg numbers. Not applicable to the vertical temperature shift factor in non-isothermal simulations. When Off, the solver uses the formulation based on the stress tensor. The default is Off. Applicable to both single- and multiphase flows. See Viscoelastic Fluids.
SUPG
The value for the Streamline-Upwind-Petrov-Galerkin advection stabilization term τ SUPG in Eqn. (1040). The default value is 0.3.
DEVSS
The Discrete Elastic Viscous Split Stress stabilization factor for velocity-stress coupling, α in Eqn. (1024). The default value is 1.0.
Damping
The non-dimensional parameter for use with the PhanThien-Tanner/JS.-exp method. Set the parameter to a non-zero value to make convergence easier, at a cost of additional iterations. The default value is 0.0.
When the Square-root conformal property is On, a diffusion term is introduced to enhance numerical stabilization. The default of 0.0 works for most cases and meaning no numerical diffusion is added to the conformal formulation. Higher values assist convergence, but very high values, above 1.0, can result in lower accuracy.
Steady-State terms only
When On, this property removes the transient term d T / d t in the viscoelastic constitutive equation and introduces pseudo-equilibrium stresses. See Viscoelastic Fluids. This property is Off by default.

Thixotropic Model

The Thixotropic model simulates the behavior of fluids that reduce viscosity over time as shear increases and return to a more viscous state when the strain is removed. This model is supported for both single and multiphase flows.

Theory Thixotropic Flow
Provided by [physics continuum] > Models > Rheology
Example Node Paths Continua > Physics 1 > Models > Thixotropic

Continua > Physics 1 > Models > Multiphase > Eulerian Phases > Phase 1 > Models > Thixotropic

Requires Flow: Viscous Flow
Properties See Thixotropic Properties.
Activates Material Methods See Structure Variable and Thixotropic Factor.
Boundary Inputs See Thixotropic Boundary Settings.
Monitors Structure Variable
Field Functions Apparent Viscosity, Structure Variable

See Thixotropic Field Functions.

Thixotropic Properties

Diffusion
Numerical diffusivity, a constant used as a coefficient for a Hermitian (self-adjoint) term that is added to a kinetic equation, Eqn. (728) or Eqn. (729), for stabilization. The default value is 0.0, in which there is no contribution to these equations.
SUPG
The value for the Streamline-Upwind-Petrov-Galerkin advection stabilization term, β SUPG in Eqn. (1039). The default value is 1.0.

Material Property Methods for Rheology

Dynamic Viscosity

You can obtain suitable parameter values for the following viscosity models by curve-fitting an experimentally determined flow curve, giving the viscosity as a function of shear-rate, to the viscosity functions given by Eqn. (738), Eqn. (739), and Eqn. (740).

MethodCorresponding Method Node
Constant
Constant
Exposes Viscosity μ in Eqn. (696). The value is independent of shear rate and temperature. See Newtonian Fluids.
Field Function
Field Function
Allows you to set a scalar field function to specify viscosity.
Newtonian

Allows you to specify a viscosity that depends on temperature but is independent of shear rate. Temperature dependency is achieved by time-temperature superposition. For viscoelastic models, you specify here the viscosity that is shifted according to the selected temperature-shift law replacing the solvent viscosity μs in Eqn. (707). The shifted polymer viscosity and the relaxation time that you specify for the chosen viscoelastic model under Viscoelastic Mode N replace the polymer viscosity μ0 and the relaxation time λ respectively in any constitutive equation. See Eqn. (742), Eqn. (743), and Eqn. (744).

For generalized Newtonian fluids, the specified viscosity is shifted according to the selected temperature-shift law.

Newtonian
Exposes Viscosity μref in Eqn. (737). This option is available only when the Viscous Energy model is activated and the Horizontal and Vertical Temperature Shift Factors are set to any method available for Time-Temperature Superposition.
Non-Newtonian Generalized Carreau-Yasuda Fluid
Non-Newtonian Generalized Carreau-Yasuda Fluid
Exposes the following terms from Eqn. (740):
  • Power Constant n
  • a Parameter a
  • Zero Shear Viscosity μ0
  • Infinite Shear Viscosity μ
  • Relaxation Time λ
Also provides the Viscosity Under-Relaxation Factor, which you can reduce to improve convergence.
Non-Newtonian Generalized Cross Fluid
Non-Newtonian Generalized Cross Fluid
Exposes the following terms from Eqn. (739):
  • Cross Rate Constant m
  • Zero Shear Viscosity μ0
  • Infinite Shear Viscosity μ
  • Critical Shear Rate γ˙c
Non-Newtonian Generalized Power Law
This method combines two rheology models:
  • Herschel-Bulkley
  • Power Law/Ostwald-de Waele
Generalized Power Law
Exposes the following terms from Eqn. (738):
  • Consistency Factor k
  • Power Law Exponent n
  • Yield Stress Threshold τ0
  • Yielding Viscosity μ0
  • Minimum Viscosity Limit and Maximum Viscosity Limit: minimum and maximum values allowed for μ

To obtain the Power Law/Ostwald de Waele viscosity function, set the yield stress τ0=0. See Eqn. (701).

Viscoelastic Mode N
You set the number of Viscoelastic Modes in the Viscoelastic model. Simcenter STAR-CCM+ adds this number of material property nodes. For each Viscoelastic Mode, choose the Method then set the properties within the corresponding method node.
MethodCorresponding Method Node
Oldroyd-B
Oldroyd-B
Exposes Viscosity μ0 and Lambda λ from Eqn. (711).
GiesekusLeonov
GiesekusLeonov
Exposes Viscosity μ0, Lambda λ, and Alpha α from Eqn. (718).
PhanThien-Tanner/JS.-lin
PhanThien-Tanner/JS.-lin
Exposes Viscosity μ0, Lambda λ, Epsilon ϵ, and Xi ξ from Eqn. (714).
PhanThien-Tanner/JS.-exp
PhanThien-Tanner/JS.-exp
Exposes Viscosity μ0, Lambda λ, Epsilon ϵ, and Xi ξ from Eqn. (716).
Extended PomPom
Extended PomPom
Exposes Viscosity μ0, Lambda λ, and Alpha α from Eqn. (720). Also Q and 1/eps 1/ϵ from Eqn. (721).
Rolie-Poly
Rolie-Poly
Exposes Viscosity μ0, Lambda λ, and Rouse Relaxation Time λR from Eqn. (723). Also exposes Beta β and delta δ from Eqn. (724).
Structure Variable
Selects the model describing the time evolution of structure parameter λ, measuring the level of microstructure in the thixotropic phase.
MethodCorresponding Method Node
Generic Kinetic
Generic Kinetic
Exposes kinetic rate constants k1 and k2 and model parameters a, b, c and d from Eqn. (728). This is the default.
Irreversible Structural Breakdown
Irreversible Structural Breakdown
Exposes kinetic constant k, model parameters e and f, and the steady state value of the structure parameter λss from Eqn. (729).
Thixotropic Factor
Selects the viscosity η of the thixotropic phase.
MethodCorresponding Method Node
Power-Law
Power-Law
Exposes exponent n from Eqn. (730). This is the default.
Field Function
Field Function
Used to specify a scalar field function.

Thixotropic Boundary Settings

Mass Flow Inlet, Velocity Inlet
Structure Variable Condition Specification
At inlets, flow can be specified as either initially fully developed or already thixotropic.
MethodCorresponding Physics Value Nodes
Structured condition
At the inlet, the thixotropic fluid has a fully structured network, the Structure Variable λ=1.
None.
Fully-developed condition
Used when conditions upstream and entrace effects are irrelevant, and only the region of fully-developed flow matters.
None.

Thixotropic Field Functions

Apparent Viscosity
The apparent viscosity as given by Eqn. (730). This value is defined at the cell center and can depend on time, shear rate, temperature, and structure variable λ.
Structure Variable
Structure parameter λ in Eqn. (728) and Eqn. (729).