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// ------------------------------------------------------------------------
//
// SPDX-License-Identifier: LGPL-2.1-or-later
// Copyright (C) 2007 - 2023 by the deal.II authors
//
// This file is part of the deal.II library.
//
// Part of the source code is dual licensed under Apache-2.0 WITH
// LLVM-exception OR LGPL-2.1-or-later. Detailed license information
// governing the source code and code contributions can be found in
// LICENSE.md and CONTRIBUTING.md at the top level directory of deal.II.
//
// ------------------------------------------------------------------------
#ifndef dealii_flow_function_h
#define dealii_flow_function_h
#include <deal.II/base/config.h>
#include <deal.II/base/function.h>
#include <deal.II/base/mutex.h>
#include <deal.II/base/point.h>
DEAL_II_NAMESPACE_OPEN
namespace Functions
{
/**
* Base class for analytic solutions to incompressible flow problems.
*
* Additional to the Function interface, this function provides for an
* offset of the pressure: if the pressure of the computed solution has an
* integral mean value different from zero, this value can be given to
* pressure_adjustment() in order to compute correct pressure errors.
*
* @note Derived classes should implement pressures with integral mean value
* zero always.
*
* @note Thread safety: Some of the functions make use of internal data to
* compute values. Therefore, every thread should obtain its own object of
* derived classes.
*
* @ingroup functions
*/
template <int dim>
class FlowFunction : public Function<dim>
{
public:
/**
* Constructor, setting up some internal data structures.
*/
FlowFunction();
/**
* Virtual destructor.
*/
virtual ~FlowFunction() override = default;
/**
* Store an adjustment for the pressure function, such that its mean value
* is <tt>p</tt>.
*/
void
pressure_adjustment(double p);
/**
* Values in a structure more suitable for vector valued functions. The
* outer vector is indexed by solution component, the inner by quadrature
* point.
*/
virtual void
vector_values(const std::vector<Point<dim>> &points,
std::vector<std::vector<double>> &values) const override = 0;
/**
* Gradients in a structure more suitable for vector valued functions. The
* outer vector is indexed by solution component, the inner by quadrature
* point.
*/
virtual void
vector_gradients(
const std::vector<Point<dim>> &points,
std::vector<std::vector<Tensor<1, dim>>> &gradients) const override = 0;
/**
* Force terms in a structure more suitable for vector valued functions.
* The outer vector is indexed by solution component, the inner by
* quadrature point.
*
* @warning This is not the true Laplacian, but the force term to be used
* as right hand side in Stokes' equations
*/
virtual void
vector_laplacians(const std::vector<Point<dim>> &points,
std::vector<std::vector<double>> &values) const = 0;
virtual void
vector_value(const Point<dim> &points,
Vector<double> &value) const override;
virtual double
value(const Point<dim> &points,
const unsigned int component) const override;
virtual void
vector_value_list(const std::vector<Point<dim>> &points,
std::vector<Vector<double>> &values) const override;
virtual void
vector_gradient_list(
const std::vector<Point<dim>> &points,
std::vector<std::vector<Tensor<1, dim>>> &gradients) const override;
/**
* The force term in the momentum equation.
*/
virtual void
vector_laplacian_list(const std::vector<Point<dim>> &points,
std::vector<Vector<double>> &values) const override;
/**
* Return an estimate for the memory consumption, in bytes, of this object.
*/
virtual std::size_t
memory_consumption() const override;
protected:
/**
* Mean value of the pressure to be added by derived classes.
*/
double mean_pressure;
private:
/**
* A mutex that guards the following scratch arrays.
*/
mutable Threads::Mutex mutex;
/**
* Auxiliary values for the usual Function interface.
*/
mutable std::vector<std::vector<double>> aux_values;
/**
* Auxiliary values for the usual Function interface.
*/
mutable std::vector<std::vector<Tensor<1, dim>>> aux_gradients;
};
/**
* Laminar pipe flow in two and three dimensions. The channel stretches
* along the <i>x</i>-axis and has radius @p radius. The @p Reynolds number
* is used to scale the pressure properly for a Navier-Stokes problem.
*
* @ingroup functions
*/
template <int dim>
class PoisseuilleFlow : public FlowFunction<dim>
{
public:
/**
* Construct an object for the given channel radius <tt>r</tt> and the
* Reynolds number <tt>Re</tt>.
*/
PoisseuilleFlow(const double r, const double Re);
virtual ~PoisseuilleFlow() override = default;
virtual void
vector_values(const std::vector<Point<dim>> &points,
std::vector<std::vector<double>> &values) const override;
virtual void
vector_gradients(
const std::vector<Point<dim>> &points,
std::vector<std::vector<Tensor<1, dim>>> &gradients) const override;
virtual void
vector_laplacians(const std::vector<Point<dim>> &points,
std::vector<std::vector<double>> &values) const override;
private:
const double inv_sqr_radius;
const double Reynolds;
};
/**
* Artificial divergence free function with homogeneous boundary conditions
* on the cube [-1,1]<sup>dim</sup>.
*
* The function in 2d is
* @f[
* \left(\begin{array}{c}u\\v\\p\end{array}\right)
* \left(\begin{array}{c}\cos^2x \sin y\cos y\\-\sin x\cos x\cos^2y\\
* \sin x\cos x\sin y\cos y\end{array}\right)
* @f]
* @ingroup functions
*/
template <int dim>
class StokesCosine : public FlowFunction<dim>
{
public:
/**
* Constructor setting the Reynolds number required for pressure
* computation and scaling of the right hand side.
*/
StokesCosine(const double viscosity = 1., const double reaction = 0.);
/**
* Change the viscosity and the reaction parameter.
*/
void
set_parameters(const double viscosity, const double reaction);
virtual ~StokesCosine() override = default;
virtual void
vector_values(const std::vector<Point<dim>> &points,
std::vector<std::vector<double>> &values) const override;
virtual void
vector_gradients(
const std::vector<Point<dim>> &points,
std::vector<std::vector<Tensor<1, dim>>> &gradients) const override;
virtual void
vector_laplacians(const std::vector<Point<dim>> &points,
std::vector<std::vector<double>> &values) const override;
private:
/// The viscosity
double viscosity;
/// The reaction parameter
double reaction;
};
/**
* A singular solution to Stokes' equations on a 2d L-shaped domain.
*
* This function satisfies $-\triangle \mathbf{u} + \nabla p = 0$ and
* represents a typical singular solution around a reentrant corner of an
* L-shaped domain that can be created using GridGenerator::hyper_L(). The
* velocity vanishes on the two faces of the re-entrant corner and
* $\nabla\mathbf{u}$ and $p$ are singular at the origin while they are
* smooth in the rest of the domain because they can be written as a product
* of a smooth function and the term $r^{\lambda-1}$ where $r$ is the radius
* and $\lambda \approx 0.54448$ is a fixed parameter.
*
* Taken from Houston, Schötzau, Wihler, proceeding ENUMATH 2003.
*
* @ingroup functions
*/
class StokesLSingularity : public FlowFunction<2>
{
public:
/// Constructor setting up some data.
StokesLSingularity();
virtual void
vector_values(const std::vector<Point<2>> &points,
std::vector<std::vector<double>> &values) const override;
virtual void
vector_gradients(
const std::vector<Point<2>> &points,
std::vector<std::vector<Tensor<1, 2>>> &gradients) const override;
virtual void
vector_laplacians(const std::vector<Point<2>> &points,
std::vector<std::vector<double>> &values) const override;
private:
/// The auxiliary function Psi.
double
Psi(double phi) const;
/// The derivative of Psi()
double
Psi_1(double phi) const;
/// The 2nd derivative of Psi()
double
Psi_2(double phi) const;
/// The 3rd derivative of Psi()
double
Psi_3(double phi) const;
/// The 4th derivative of Psi()
double
Psi_4(double phi) const;
/// The angle of the reentrant corner, set to 3*pi/2
const double omega;
/// The exponent of the radius, computed as the solution to
/// $\sin(\lambda\omega)+\lambda \sin(\omega)=0$
static const double lambda;
/// Cosine of lambda times omega
const double coslo;
/// Auxiliary variable 1+lambda
const double lp;
/// Auxiliary variable 1-lambda
const double lm;
};
/**
* Flow solution in 2d by Kovasznay (1947).
*
* This function is valid on the half plane right of the line <i>x=1/2</i>.
*
* @ingroup functions
*/
class Kovasznay : public FlowFunction<2>
{
public:
/**
* Construct an object for the give Reynolds number <tt>Re</tt>. If the
* parameter <tt>Stokes</tt> is true, the right hand side of the momentum
* equation returned by vector_laplacians() contains the nonlinearity,
* such that the Kovasznay solution can be obtained as the solution to a
* Stokes problem.
*/
Kovasznay(const double Re, bool Stokes = false);
virtual ~Kovasznay() override = default;
virtual void
vector_values(const std::vector<Point<2>> &points,
std::vector<std::vector<double>> &values) const override;
virtual void
vector_gradients(
const std::vector<Point<2>> &points,
std::vector<std::vector<Tensor<1, 2>>> &gradients) const override;
virtual void
vector_laplacians(const std::vector<Point<2>> &points,
std::vector<std::vector<double>> &values) const override;
/// The value of lambda.
double
lambda() const;
private:
const double Reynolds;
double lbda;
double p_average;
const bool stokes;
};
} // namespace Functions
DEAL_II_NAMESPACE_CLOSE
#endif
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