Public Member Functions | Private Attributes | List of all members
oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM > Class Template Reference

A GeneralisedNewtonianConstitutiveEquation class defining a Herschel-Bulkley fluid using Tanner and Milthorpe's (1983) regularisation with a smooth transition using a quadratic. More...

#include <generalised_newtonian_constitutive_models.h>

+ Inheritance diagram for oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >:

Public Member Functions

 HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation (double *yield_stress_pt, double *flow_index_pt, double *critical_second_invariant_pt)
 "Cutoff regularised" Herschel Bulkley constitutive equation
 
double calculate_cutoff_viscosity ()
 Function that calculates the viscosity at the cutoff invariant Note: this is NOT the viscosity at zero I2.
 
double calculate_zero_shear_viscosity ()
 Function that calculates the viscosity at zero I2.
 
void report_cut_off_values (double &cut_off_invariant, double &cut_off_viscosity, double &zero_shear_viscosity)
 Report cutoff values.
 
double viscosity (const double &second_invariant_of_rate_of_strain_tensor)
 Viscosity ratio as a fct of strain rate invariant.
 
double dviscosity_dinvariant (const double &second_invariant_of_rate_of_strain_tensor)
 Deriv of viscosity w.r.t. strain rate invariant.
 
- Public Member Functions inherited from oomph::GeneralisedNewtonianConstitutiveEquation< DIM >
 GeneralisedNewtonianConstitutiveEquation ()
 Empty constructor.
 
virtual ~GeneralisedNewtonianConstitutiveEquation ()
 Empty virtual destructor.
 

Private Attributes

doubleYield_stress_pt
 yield stress tau_y
 
doubleFlow_index_pt
 power law index n
 
doubleCritical_second_invariant_pt
 value of the second invariant below which we have constant (Newtonian) viscosity – assumed to be always positive
 
double a
 We use a quadratic function to smoothly blend from the Herschel Bulkley model at the cut-off to a constant viscosity as the strain rate /approaches zero; this way we avoid the discontinuity of the gradient at the cut-off, which is present in the classic Tanner Milthorpe regularisation.
 
double b
 
double c
 
double alpha
 Fraction of the cut-off strain rate below which the viscosity is constant 0 <= alpha < 1.
 

Detailed Description

template<unsigned DIM>
class oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >

A GeneralisedNewtonianConstitutiveEquation class defining a Herschel-Bulkley fluid using Tanner and Milthorpe's (1983) regularisation with a smooth transition using a quadratic.

Definition at line 358 of file generalised_newtonian_constitutive_models.h.

Constructor & Destructor Documentation

◆ HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation()

template<unsigned DIM>
oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation ( double yield_stress_pt,
double flow_index_pt,
double critical_second_invariant_pt 
)
inline

Member Function Documentation

◆ calculate_cutoff_viscosity()

template<unsigned DIM>
double oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >::calculate_cutoff_viscosity ( )
inline

◆ calculate_zero_shear_viscosity()

template<unsigned DIM>
double oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >::calculate_zero_shear_viscosity ( )
inline

◆ dviscosity_dinvariant()

template<unsigned DIM>
double oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >::dviscosity_dinvariant ( const double second_invariant_of_rate_of_strain_tensor)
inlinevirtual

◆ report_cut_off_values()

template<unsigned DIM>
void oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >::report_cut_off_values ( double cut_off_invariant,
double cut_off_viscosity,
double zero_shear_viscosity 
)
inline

◆ viscosity()

template<unsigned DIM>
double oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >::viscosity ( const double second_invariant_of_rate_of_strain_tensor)
inlinevirtual

Member Data Documentation

◆ a

We use a quadratic function to smoothly blend from the Herschel Bulkley model at the cut-off to a constant viscosity as the strain rate /approaches zero; this way we avoid the discontinuity of the gradient at the cut-off, which is present in the classic Tanner Milthorpe regularisation.

Definition at line 377 of file generalised_newtonian_constitutive_models.h.

Referenced by oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >::calculate_zero_shear_viscosity(), oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >::dviscosity_dinvariant(), oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation(), and oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >::viscosity().

◆ alpha

◆ b

◆ c

◆ Critical_second_invariant_pt

template<unsigned DIM>
double* oomph::HerschelBulkleyTanMilRegWithBlendingConstitutiveEquation< DIM >::Critical_second_invariant_pt
private

◆ Flow_index_pt

◆ Yield_stress_pt


The documentation for this class was generated from the following file: