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PISM, A Parallel Ice Sheet Model 2.2.2-d6b3a29ca committed by Constantine Khrulev on 2025-03-28
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BlatterTestXY.cc
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19
20#include "pism/stressbalance/blatter/verification/BlatterTestXY.hh"
21
22#include "pism/rheology/IsothermalGlen.hh"
23
24#include "pism/stressbalance/blatter/verification/manufactured_solutions.hh"
25
26namespace pism {
27namespace stressbalance {
28
29BlatterTestXY::BlatterTestXY(std::shared_ptr<const Grid> grid, int Mz, int coarsening_factor)
30 : Blatter(grid, Mz, coarsening_factor) {
31
32 // use the isothermal Glen flow law
33 m_flow_law.reset(new rheology::IsothermalGlen("stress_balance.blatter.", *m_config, m_EC));
34
35 // make sure we use the same Glen exponent
36 assert(m_flow_law->exponent() == 3.0);
37
38 // store constant hardness (enthalpy and pressure values are irrelevant)
39 m_B = m_flow_law->hardness(1e5, 0);
40}
41
43 const int *node_type,
44 const double *ice_bottom,
45 const double *sea_level) {
46 (void) face;
47 (void) node_type;
48 (void) ice_bottom;
49 (void) sea_level;
50
51 return false;
52}
53
54bool BlatterTestXY::dirichlet_node(const DMDALocalInfo &info, const fem::Element3::GlobalIndex& I) {
55 // use Dirichlet BC on the whole map-plane boundary
56 return (I.i == 0 or I.i == info.mx - 1 or
57 I.j == 0 or I.j == info.my - 1);
58}
59
60Vector2d BlatterTestXY::u_bc(double x, double y, double z) const {
61 (void) z;
62
63 return blatter_xy_exact(x, y);
64}
65
67 const double *surface,
68 const double *bed,
69 Vector2d *residual) {
70 (void) surface;
71 (void) bed;
72
73 // compute x and y coordinates of quadrature points
74 double
75 *x = m_work[0],
76 *y = m_work[1];
77 {
78 double
79 *x_nodal = m_work[2],
80 *y_nodal = m_work[3];
81
82 for (int n = 0; n < element.n_chi(); ++n) {
83 x_nodal[n] = element.x(n);
84 y_nodal[n] = element.y(n);
85 }
86
87 element.evaluate(x_nodal, x);
88 element.evaluate(y_nodal, y);
89 }
90
91 // loop over all quadrature points
92 for (unsigned int q = 0; q < element.n_pts(); ++q) {
93 auto W = element.weight(q) / m_scaling;
94
95 // loop over all test functions
96 for (int t = 0; t < element.n_chi(); ++t) {
97 const auto &psi = element.chi(q, t);
98
99 residual[t] += W * psi.val * blatter_xy_source(x[q], y[q], m_B);
100 }
101 }
102}
103
104} // end of namespace stressbalance
105} // end of namespace pism
const Config::ConstPtr m_config
configuration database used by this component
Definition Component.hh:158
This class represents a 2D vector field (such as ice velocity) at a certain grid point.
Definition Vector2d.hh:29
void evaluate(const T *x, T *vals, T *dx, T *dy, T *dz) const
Given nodal values, compute the values and partial derivatives at the quadrature points.
Definition Element.hh:285
int n_chi() const
Definition Element.hh:65
double weight(unsigned int q) const
Weight of the quadrature point q
Definition Element.hh:85
const Germ & chi(unsigned int q, unsigned int k) const
Definition Element.hh:73
unsigned int n_pts() const
Number of quadrature points.
Definition Element.hh:80
double y(int n) const
Definition Element.hh:376
double x(int n) const
Definition Element.hh:371
3D Q1 element
Definition Element.hh:358
Isothermal Glen ice allowing extra customization.
double m_B
constant ice hardness
void residual_source_term(const fem::Q1Element3 &element, const double *surface, const double *bed, Vector2d *residual)
bool marine_boundary(int face, const int *node_type, const double *ice_bottom, const double *sea_level)
Vector2d u_bc(double x, double y, double z) const
BlatterTestXY(std::shared_ptr< const Grid > grid, int Mz, int coarsening_factor)
bool dirichlet_node(const DMDALocalInfo &info, const fem::Element3::GlobalIndex &I)
double m_work[m_n_work][m_Nq]
Definition Blatter.hh:109
std::shared_ptr< rheology::FlowLaw > m_flow_law
#define n
Definition exactTestM.c:37
Vector2d blatter_xy_source(double x, double y, double B)
Vector2d blatter_xy_exact(double x, double y)