1 | """ |
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2 | Finite-volume computations of the shallow water wave equation. |
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3 | |
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4 | Title: ANGUA shallow_water_domain - 2D triangular domains for finite-volume |
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5 | computations of the shallow water wave equation. |
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6 | |
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7 | |
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8 | Author: Ole Nielsen, Ole.Nielsen@ga.gov.au |
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9 | Stephen Roberts, Stephen.Roberts@anu.edu.au |
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10 | Duncan Gray, Duncan.Gray@ga.gov.au |
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11 | |
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12 | CreationDate: 2004 |
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13 | |
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14 | Description: |
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15 | This module contains a specialisation of class Domain from |
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16 | module domain.py consisting of methods specific to the |
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17 | Shallow Water Wave Equation |
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18 | |
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19 | U_t + E_x + G_y = S |
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20 | |
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21 | where |
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22 | |
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23 | U = [w, uh, vh] |
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24 | E = [uh, u^2h + gh^2/2, uvh] |
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25 | G = [vh, uvh, v^2h + gh^2/2] |
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26 | S represents source terms forcing the system |
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27 | (e.g. gravity, friction, wind stress, ...) |
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28 | |
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29 | and _t, _x, _y denote the derivative with respect to t, x and y |
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30 | respectively. |
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31 | |
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32 | |
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33 | The quantities are |
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34 | |
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35 | symbol variable name explanation |
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36 | x x horizontal distance from origin [m] |
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37 | y y vertical distance from origin [m] |
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38 | z elevation elevation of bed on which flow is modelled [m] |
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39 | h height water height above z [m] |
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40 | w stage absolute water level, w = z+h [m] |
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41 | u speed in the x direction [m/s] |
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42 | v speed in the y direction [m/s] |
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43 | uh xmomentum momentum in the x direction [m^2/s] |
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44 | vh ymomentum momentum in the y direction [m^2/s] |
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45 | |
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46 | eta mannings friction coefficient [to appear] |
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47 | nu wind stress coefficient [to appear] |
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48 | |
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49 | The conserved quantities are w, uh, vh |
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50 | |
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51 | Reference: |
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52 | Catastrophic Collapse of Water Supply Reservoirs in Urban Areas, |
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53 | Christopher Zoppou and Stephen Roberts, |
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54 | Journal of Hydraulic Engineering, vol. 127, No. 7 July 1999 |
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55 | |
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56 | Hydrodynamic modelling of coastal inundation. |
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57 | Nielsen, O., S. Roberts, D. Gray, A. McPherson and A. Hitchman |
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58 | In Zerger, A. and Argent, R.M. (eds) MODSIM 2005 International Congress on |
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59 | Modelling and Simulation. Modelling and Simulation Society of Australia and |
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60 | New Zealand, December 2005, pp. 518-523. ISBN: 0-9758400-2-9. |
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61 | http://www.mssanz.org.au/modsim05/papers/nielsen.pdf |
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62 | |
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63 | |
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64 | SeeAlso: |
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65 | TRAC administration of ANUGA (User Manuals etc) at |
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66 | https://datamining.anu.edu.au/anuga and Subversion repository at |
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67 | $HeadURL: anuga_core/source/anuga/shallow_water/shallow_water_domain.py $ |
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68 | |
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69 | Constraints: See GPL license in the user guide |
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70 | Version: 1.0 ($Revision: 7736 $) |
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71 | ModifiedBy: |
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72 | $Author: hudson $ |
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73 | $Date: 2010-05-24 02:30:34 +0000 (Mon, 24 May 2010) $ |
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74 | """ |
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75 | |
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76 | # Subversion keywords: |
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77 | # |
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78 | # $LastChangedDate: 2010-05-24 02:30:34 +0000 (Mon, 24 May 2010) $ |
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79 | # $LastChangedRevision: 7736 $ |
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80 | # $LastChangedBy: hudson $ |
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81 | |
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82 | |
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83 | import numpy as num |
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84 | |
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85 | from anuga.abstract_2d_finite_volumes.generic_domain \ |
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86 | import Generic_Domain |
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87 | |
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88 | from anuga.shallow_water.forcing import Cross_section |
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89 | from anuga.pmesh.mesh_interface import create_mesh_from_regions |
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90 | from anuga.utilities.numerical_tools import gradient, mean, ensure_numeric |
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91 | from anuga.geospatial_data.geospatial_data import ensure_geospatial |
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92 | |
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93 | from anuga.config import netcdf_mode_r, netcdf_mode_w, netcdf_mode_a |
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94 | |
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95 | from anuga.fit_interpolate.interpolate import Modeltime_too_late, \ |
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96 | Modeltime_too_early |
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97 | |
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98 | from anuga.geometry.polygon import inside_polygon, polygon_area, \ |
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99 | is_inside_polygon |
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100 | import anuga.utilities.log as log |
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101 | |
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102 | import types |
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103 | from types import IntType, FloatType |
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104 | from warnings import warn |
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105 | |
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106 | |
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107 | ################################################################################ |
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108 | # Shallow water domain |
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109 | ################################################################################ |
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110 | |
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111 | ## |
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112 | # @brief Class for a shallow water domain. |
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113 | class Domain(Generic_Domain): |
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114 | |
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115 | #conserved_quantities = ['stage', 'xmomentum', 'ymomentum'] |
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116 | #other_quantities = ['elevation', 'friction'] |
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117 | |
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118 | ## |
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119 | # @brief Instantiate a shallow water domain. |
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120 | # @param coordinates |
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121 | # @param vertices |
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122 | # @param boundary |
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123 | # @param tagged_elements |
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124 | # @param geo_reference |
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125 | # @param use_inscribed_circle |
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126 | # @param mesh_filename |
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127 | # @param use_cache |
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128 | # @param verbose |
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129 | # @param evolved_quantities |
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130 | # @param full_send_dict |
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131 | # @param ghost_recv_dict |
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132 | # @param processor |
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133 | # @param numproc |
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134 | # @param number_of_full_nodes |
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135 | # @param number_of_full_triangles |
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136 | def __init__(self, |
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137 | coordinates=None, |
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138 | vertices=None, |
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139 | boundary=None, |
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140 | tagged_elements=None, |
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141 | geo_reference=None, |
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142 | use_inscribed_circle=False, |
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143 | mesh_filename=None, |
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144 | use_cache=False, |
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145 | verbose=False, |
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146 | conserved_quantities = None, |
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147 | evolved_quantities = None, |
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148 | other_quantities = None, |
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149 | full_send_dict=None, |
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150 | ghost_recv_dict=None, |
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151 | processor=0, |
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152 | numproc=1, |
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153 | number_of_full_nodes=None, |
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154 | number_of_full_triangles=None): |
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155 | |
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156 | # Define quantities for the shallow_water domain |
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157 | if conserved_quantities == None: |
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158 | conserved_quantities = ['stage', 'xmomentum', 'ymomentum'] |
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159 | |
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160 | if evolved_quantities == None: |
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161 | evolved_quantities = ['stage', 'xmomentum', 'ymomentum'] |
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162 | |
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163 | if other_quantities == None: |
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164 | other_quantities = ['elevation', 'friction'] |
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165 | |
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166 | Generic_Domain.__init__(self, |
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167 | coordinates, |
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168 | vertices, |
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169 | boundary, |
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170 | conserved_quantities, |
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171 | evolved_quantities, |
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172 | other_quantities, |
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173 | tagged_elements, |
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174 | geo_reference, |
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175 | use_inscribed_circle, |
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176 | mesh_filename, |
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177 | use_cache, |
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178 | verbose, |
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179 | full_send_dict, |
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180 | ghost_recv_dict, |
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181 | processor, |
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182 | numproc, |
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183 | number_of_full_nodes=number_of_full_nodes, |
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184 | number_of_full_triangles=number_of_full_triangles) |
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185 | |
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186 | self.set_defaults() |
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187 | |
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188 | |
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189 | self.forcing_terms.append(manning_friction_implicit) |
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190 | self.forcing_terms.append(gravity) |
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191 | |
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192 | # Stored output |
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193 | self.store = True |
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194 | self.set_store_vertices_uniquely(False) |
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195 | |
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196 | self.quantities_to_be_stored = {'elevation': 1, |
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197 | 'stage': 2, |
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198 | 'xmomentum': 2, |
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199 | 'ymomentum': 2} |
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200 | |
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201 | |
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202 | |
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203 | |
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204 | ## |
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205 | # @brief Set default values, usually read in from a config file |
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206 | # @param flag |
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207 | def set_defaults(self): |
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208 | """Set the default values in this routine. That way we can inherit class |
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209 | and just over redefine the defaults for the new class |
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210 | """ |
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211 | |
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212 | from anuga.config import minimum_storable_height |
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213 | from anuga.config import minimum_allowed_height, maximum_allowed_speed |
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214 | from anuga.config import g, epsilon, beta_w, beta_w_dry,\ |
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215 | beta_uh, beta_uh_dry, beta_vh, beta_vh_dry, tight_slope_limiters |
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216 | from anuga.config import alpha_balance |
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217 | from anuga.config import optimise_dry_cells |
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218 | from anuga.config import optimised_gradient_limiter |
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219 | from anuga.config import use_edge_limiter |
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220 | from anuga.config import use_centroid_velocities |
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221 | |
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222 | |
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223 | |
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224 | self.set_minimum_allowed_height(minimum_allowed_height) |
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225 | self.maximum_allowed_speed = maximum_allowed_speed |
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226 | |
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227 | self.g = g |
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228 | self.beta_w = beta_w |
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229 | self.beta_w_dry = beta_w_dry |
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230 | self.beta_uh = beta_uh |
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231 | self.beta_uh_dry = beta_uh_dry |
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232 | self.beta_vh = beta_vh |
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233 | self.beta_vh_dry = beta_vh_dry |
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234 | self.alpha_balance = alpha_balance |
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235 | |
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236 | self.tight_slope_limiters = tight_slope_limiters |
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237 | self.optimise_dry_cells = optimise_dry_cells |
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238 | |
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239 | |
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240 | self.set_new_mannings_function(False) |
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241 | |
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242 | self.minimum_storable_height = minimum_storable_height |
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243 | |
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244 | # Limiters |
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245 | self.use_edge_limiter = use_edge_limiter |
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246 | self.optimised_gradient_limiter = optimised_gradient_limiter |
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247 | self.use_centroid_velocities = use_centroid_velocities |
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248 | |
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249 | ## |
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250 | # @brief |
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251 | # @param flag |
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252 | def set_new_mannings_function(self, flag=True): |
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253 | """Cludge to allow unit test to pass, but to |
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254 | also introduce new mannings friction function |
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255 | which takes into account the slope of the bed. |
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256 | The flag is tested in the python wrapper |
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257 | mannings_friction_implicit |
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258 | """ |
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259 | if flag: |
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260 | self.use_new_mannings = True |
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261 | else: |
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262 | self.use_new_mannings = False |
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263 | |
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264 | |
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265 | ## |
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266 | # @brief |
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267 | # @param flag |
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268 | def set_use_edge_limiter(self, flag=True): |
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269 | """Cludge to allow unit test to pass, but to |
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270 | also introduce new edge limiting. The flag is |
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271 | tested in distribute_to_vertices_and_edges |
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272 | """ |
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273 | if flag: |
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274 | self.use_edge_limiter = True |
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275 | else: |
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276 | self.use_edge_limiter = False |
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277 | |
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278 | |
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279 | |
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280 | ## |
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281 | # @brief |
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282 | # @param beta |
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283 | def set_all_limiters(self, beta): |
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284 | """Shorthand to assign one constant value [0,1] to all limiters. |
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285 | 0 Corresponds to first order, where as larger values make use of |
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286 | the second order scheme. |
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287 | """ |
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288 | |
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289 | self.beta_w = beta |
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290 | self.beta_w_dry = beta |
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291 | self.quantities['stage'].beta = beta |
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292 | |
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293 | self.beta_uh = beta |
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294 | self.beta_uh_dry = beta |
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295 | self.quantities['xmomentum'].beta = beta |
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296 | |
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297 | self.beta_vh = beta |
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298 | self.beta_vh_dry = beta |
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299 | self.quantities['ymomentum'].beta = beta |
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300 | |
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301 | ## |
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302 | # @brief |
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303 | # @param flag |
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304 | # @param reduction |
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305 | def set_store_vertices_uniquely(self, flag, reduction=None): |
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306 | """Decide whether vertex values should be stored uniquely as |
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307 | computed in the model (True) or whether they should be reduced to one |
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308 | value per vertex using self.reduction (False). |
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309 | """ |
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310 | |
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311 | # FIXME (Ole): how about using the word "continuous vertex values" or |
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312 | # "continuous stage surface" |
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313 | self.smooth = not flag |
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314 | |
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315 | # Reduction operation for get_vertex_values |
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316 | if reduction is None: |
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317 | self.reduction = mean |
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318 | #self.reduction = min #Looks better near steep slopes |
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319 | |
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320 | ## |
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321 | # @brief Set the minimum depth that will be written to an SWW file. |
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322 | # @param minimum_storable_height The minimum stored height (in m). |
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323 | def set_minimum_storable_height(self, minimum_storable_height): |
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324 | """Set the minimum depth that will be recognised when writing |
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325 | to an sww file. This is useful for removing thin water layers |
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326 | that seems to be caused by friction creep. |
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327 | |
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328 | The minimum allowed sww depth is in meters. |
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329 | """ |
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330 | |
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331 | self.minimum_storable_height = minimum_storable_height |
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332 | |
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333 | ## |
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334 | # @brief |
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335 | # @param minimum_allowed_height |
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336 | def set_minimum_allowed_height(self, minimum_allowed_height): |
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337 | """Set minimum depth that will be recognised in the numerical scheme. |
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338 | |
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339 | The minimum allowed depth is in meters. |
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340 | |
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341 | The parameter H0 (Minimal height for flux computation) |
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342 | is also set by this function |
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343 | """ |
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344 | |
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345 | #FIXME (Ole): rename H0 to minimum_allowed_height_in_flux_computation |
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346 | |
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347 | #FIXME (Ole): Maybe use histogram to identify isolated extreme speeds |
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348 | #and deal with them adaptively similarly to how we used to use 1 order |
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349 | #steps to recover. |
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350 | |
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351 | self.minimum_allowed_height = minimum_allowed_height |
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352 | self.H0 = minimum_allowed_height |
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353 | |
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354 | ## |
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355 | # @brief |
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356 | # @param maximum_allowed_speed |
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357 | def set_maximum_allowed_speed(self, maximum_allowed_speed): |
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358 | """Set the maximum particle speed that is allowed in water |
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359 | shallower than minimum_allowed_height. This is useful for |
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360 | controlling speeds in very thin layers of water and at the same time |
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361 | allow some movement avoiding pooling of water. |
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362 | """ |
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363 | |
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364 | self.maximum_allowed_speed = maximum_allowed_speed |
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365 | |
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366 | ## |
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367 | # @brief |
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368 | # @param points_file_block_line_size |
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369 | def set_points_file_block_line_size(self, points_file_block_line_size): |
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370 | """Set the minimum depth that will be recognised when writing |
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371 | to an sww file. This is useful for removing thin water layers |
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372 | that seems to be caused by friction creep. |
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373 | |
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374 | The minimum allowed sww depth is in meters. |
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375 | """ |
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376 | self.points_file_block_line_size = points_file_block_line_size |
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377 | |
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378 | |
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379 | # FIXME: Probably obsolete in its curren form |
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380 | ## |
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381 | # @brief Set the quantities that will be written to an SWW file. |
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382 | # @param q The quantities to be written. |
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383 | # @note Param 'q' may be None, single quantity or list of quantity strings. |
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384 | # @note If 'q' is None, no quantities will be stored in the SWW file. |
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385 | def set_quantities_to_be_stored(self, q): |
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386 | """Specify which quantities will be stored in the sww file |
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387 | |
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388 | q must be either: |
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389 | - a dictionary with quantity names |
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390 | - a list of quantity names (for backwards compatibility) |
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391 | - None |
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392 | |
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393 | The format of the dictionary is as follows |
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394 | |
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395 | quantity_name: flag where flag must be either 1 or 2. |
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396 | If flag is 1, the quantity is considered static and will be |
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397 | stored once at the beginning of the simulation in a 1D array. |
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398 | |
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399 | If flag is 2, the quantity is considered time dependent and |
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400 | it will be stored at each yieldstep by appending it to the |
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401 | appropriate 2D array in the sww file. |
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402 | |
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403 | If q is None, storage will be switched off altogether. |
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404 | |
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405 | Once the simulation has started and thw sww file opened, |
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406 | this function will have no effect. |
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407 | |
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408 | The format, where q is a list of names is for backwards compatibility only. |
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409 | It will take the specified quantities to be time dependent and assume |
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410 | 'elevation' to be static regardless. |
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411 | """ |
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412 | |
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413 | if q is None: |
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414 | self.quantities_to_be_stored = {} |
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415 | self.store = False |
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416 | return |
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417 | |
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418 | # Check correcness |
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419 | for quantity_name in q: |
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420 | msg = ('Quantity %s is not a valid conserved quantity' |
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421 | % quantity_name) |
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422 | assert quantity_name in self.quantities, msg |
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423 | |
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424 | if type(q) == types.ListType: |
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425 | |
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426 | msg = 'List arguments to set_quantities_to_be_stored ' |
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427 | msg += 'has been deprecated and will be removed in future ' |
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428 | msg += 'versions of ANUGA.' |
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429 | msg += 'Please use dictionary argument instead' |
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430 | warn(msg, DeprecationWarning) |
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431 | |
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432 | |
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433 | |
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434 | # FIXME: Raise deprecation warning |
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435 | tmp = {} |
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436 | for x in q: |
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437 | tmp[x] = 2 |
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438 | tmp['elevation'] = 1 |
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439 | q = tmp |
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440 | |
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441 | assert type(q) == types.DictType |
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442 | self.quantities_to_be_stored = q |
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443 | |
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444 | ## |
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445 | # @brief |
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446 | # @param indices |
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447 | def get_wet_elements(self, indices=None): |
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448 | """Return indices for elements where h > minimum_allowed_height |
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449 | |
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450 | Optional argument: |
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451 | indices is the set of element ids that the operation applies to. |
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452 | |
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453 | Usage: |
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454 | indices = get_wet_elements() |
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455 | |
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456 | Note, centroid values are used for this operation |
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457 | """ |
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458 | |
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459 | # Water depth below which it is considered to be 0 in the model |
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460 | # FIXME (Ole): Allow this to be specified as a keyword argument as well |
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461 | from anuga.config import minimum_allowed_height |
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462 | |
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463 | elevation = self.get_quantity('elevation').\ |
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464 | get_values(location='centroids', indices=indices) |
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465 | stage = self.get_quantity('stage').\ |
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466 | get_values(location='centroids', indices=indices) |
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467 | depth = stage - elevation |
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468 | |
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469 | # Select indices for which depth > 0 |
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470 | wet_indices = num.compress(depth > minimum_allowed_height, |
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471 | num.arange(len(depth))) |
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472 | return wet_indices |
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473 | |
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474 | ## |
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475 | # @brief |
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476 | # @param indices |
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477 | def get_maximum_inundation_elevation(self, indices=None): |
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478 | """Return highest elevation where h > 0 |
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479 | |
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480 | Optional argument: |
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481 | indices is the set of element ids that the operation applies to. |
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482 | |
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483 | Usage: |
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484 | q = get_maximum_inundation_elevation() |
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485 | |
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486 | Note, centroid values are used for this operation |
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487 | """ |
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488 | |
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489 | wet_elements = self.get_wet_elements(indices) |
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490 | return self.get_quantity('elevation').\ |
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491 | get_maximum_value(indices=wet_elements) |
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492 | |
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493 | ## |
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494 | # @brief |
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495 | # @param indices |
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496 | def get_maximum_inundation_location(self, indices=None): |
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497 | """Return location of highest elevation where h > 0 |
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498 | |
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499 | Optional argument: |
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500 | indices is the set of element ids that the operation applies to. |
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501 | |
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502 | Usage: |
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503 | q = get_maximum_inundation_location() |
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504 | |
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505 | Note, centroid values are used for this operation |
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506 | """ |
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507 | |
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508 | wet_elements = self.get_wet_elements(indices) |
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509 | return self.get_quantity('elevation').\ |
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510 | get_maximum_location(indices=wet_elements) |
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511 | |
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512 | |
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513 | |
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514 | ## |
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515 | # @brief Get the total flow through an arbitrary poly line. |
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516 | # @param polyline Representation of desired cross section. |
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517 | # @param verbose True if this method is to be verbose. |
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518 | # @note 'polyline' may contain multiple sections allowing complex shapes. |
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519 | # @note Assume absolute UTM coordinates. |
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520 | def get_flow_through_cross_section(self, polyline, verbose=False): |
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521 | """Get the total flow through an arbitrary poly line. |
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522 | |
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523 | This is a run-time equivalent of the function with same name |
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524 | in data_manager.py |
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525 | |
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526 | Input: |
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527 | polyline: Representation of desired cross section - it may contain |
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528 | multiple sections allowing for complex shapes. Assume |
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529 | absolute UTM coordinates. |
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530 | Format [[x0, y0], [x1, y1], ...] |
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531 | |
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532 | Output: |
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533 | Q: Total flow [m^3/s] across given segments. |
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534 | """ |
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535 | |
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536 | |
---|
537 | cross_section = Cross_section(self, polyline, verbose) |
---|
538 | |
---|
539 | return cross_section.get_flow_through_cross_section() |
---|
540 | |
---|
541 | |
---|
542 | |
---|
543 | |
---|
544 | ## |
---|
545 | # @brief |
---|
546 | # @param polyline Representation of desired cross section. |
---|
547 | # @param kind Select energy type to compute ('specific' or 'total'). |
---|
548 | # @param verbose True if this method is to be verbose. |
---|
549 | # @note 'polyline' may contain multiple sections allowing complex shapes. |
---|
550 | # @note Assume absolute UTM coordinates. |
---|
551 | def get_energy_through_cross_section(self, polyline, |
---|
552 | kind='total', |
---|
553 | verbose=False): |
---|
554 | """Obtain average energy head [m] across specified cross section. |
---|
555 | |
---|
556 | Inputs: |
---|
557 | polyline: Representation of desired cross section - it may contain |
---|
558 | multiple sections allowing for complex shapes. Assume |
---|
559 | absolute UTM coordinates. |
---|
560 | Format [[x0, y0], [x1, y1], ...] |
---|
561 | kind: Select which energy to compute. |
---|
562 | Options are 'specific' and 'total' (default) |
---|
563 | |
---|
564 | Output: |
---|
565 | E: Average energy [m] across given segments for all stored times. |
---|
566 | |
---|
567 | The average velocity is computed for each triangle intersected by |
---|
568 | the polyline and averaged weighted by segment lengths. |
---|
569 | |
---|
570 | The typical usage of this function would be to get average energy of |
---|
571 | flow in a channel, and the polyline would then be a cross section |
---|
572 | perpendicular to the flow. |
---|
573 | |
---|
574 | #FIXME (Ole) - need name for this energy reflecting that its dimension |
---|
575 | is [m]. |
---|
576 | """ |
---|
577 | |
---|
578 | |
---|
579 | |
---|
580 | cross_section = Cross_section(self, polyline, verbose) |
---|
581 | |
---|
582 | return cross_section.get_energy_through_cross_section(kind) |
---|
583 | |
---|
584 | |
---|
585 | ## |
---|
586 | # @brief Run integrity checks on shallow water domain. |
---|
587 | def check_integrity(self): |
---|
588 | Generic_Domain.check_integrity(self) |
---|
589 | |
---|
590 | #Check that we are solving the shallow water wave equation |
---|
591 | msg = 'First conserved quantity must be "stage"' |
---|
592 | assert self.conserved_quantities[0] == 'stage', msg |
---|
593 | msg = 'Second conserved quantity must be "xmomentum"' |
---|
594 | assert self.conserved_quantities[1] == 'xmomentum', msg |
---|
595 | msg = 'Third conserved quantity must be "ymomentum"' |
---|
596 | assert self.conserved_quantities[2] == 'ymomentum', msg |
---|
597 | |
---|
598 | ## |
---|
599 | # @brief |
---|
600 | def extrapolate_second_order_sw(self): |
---|
601 | #Call correct module function (either from this module or C-extension) |
---|
602 | extrapolate_second_order_sw(self) |
---|
603 | |
---|
604 | ## |
---|
605 | # @brief |
---|
606 | def compute_fluxes(self): |
---|
607 | #Call correct module function (either from this module or C-extension) |
---|
608 | compute_fluxes(self) |
---|
609 | |
---|
610 | ## |
---|
611 | # @brief |
---|
612 | def distribute_to_vertices_and_edges(self): |
---|
613 | # Call correct module function |
---|
614 | if self.use_edge_limiter: |
---|
615 | distribute_using_edge_limiter(self) |
---|
616 | else: |
---|
617 | distribute_using_vertex_limiter(self) |
---|
618 | |
---|
619 | |
---|
620 | |
---|
621 | ## |
---|
622 | # @brief Evolve the model by one step. |
---|
623 | # @param yieldstep |
---|
624 | # @param finaltime |
---|
625 | # @param duration |
---|
626 | # @param skip_initial_step |
---|
627 | def evolve(self, |
---|
628 | yieldstep=None, |
---|
629 | finaltime=None, |
---|
630 | duration=None, |
---|
631 | skip_initial_step=False): |
---|
632 | """Specialisation of basic evolve method from parent class""" |
---|
633 | |
---|
634 | # Call check integrity here rather than from user scripts |
---|
635 | # self.check_integrity() |
---|
636 | |
---|
637 | msg = 'Attribute self.beta_w must be in the interval [0, 2]' |
---|
638 | assert 0 <= self.beta_w <= 2.0, msg |
---|
639 | |
---|
640 | # Initial update of vertex and edge values before any STORAGE |
---|
641 | # and or visualisation. |
---|
642 | # This is done again in the initialisation of the Generic_Domain |
---|
643 | # evolve loop but we do it here to ensure the values are ok for storage. |
---|
644 | self.distribute_to_vertices_and_edges() |
---|
645 | |
---|
646 | if self.store is True and self.time == 0.0: |
---|
647 | self.initialise_storage() |
---|
648 | |
---|
649 | # Call basic machinery from parent class |
---|
650 | for t in Generic_Domain.evolve(self, yieldstep=yieldstep, |
---|
651 | finaltime=finaltime, duration=duration, |
---|
652 | skip_initial_step=skip_initial_step): |
---|
653 | # Store model data, e.g. for subsequent visualisation |
---|
654 | if self.store is True: |
---|
655 | self.store_timestep() |
---|
656 | |
---|
657 | # Pass control on to outer loop for more specific actions |
---|
658 | yield(t) |
---|
659 | |
---|
660 | ## |
---|
661 | # @brief |
---|
662 | def initialise_storage(self): |
---|
663 | """Create and initialise self.writer object for storing data. |
---|
664 | Also, save x,y and bed elevation |
---|
665 | """ |
---|
666 | |
---|
667 | from anuga.shallow_water.sww_file import SWW_file |
---|
668 | |
---|
669 | # Initialise writer |
---|
670 | self.writer = SWW_file(self) |
---|
671 | |
---|
672 | # Store vertices and connectivity |
---|
673 | self.writer.store_connectivity() |
---|
674 | |
---|
675 | ## |
---|
676 | # @brief |
---|
677 | # @param name |
---|
678 | def store_timestep(self): |
---|
679 | """Store time dependent quantities and time. |
---|
680 | |
---|
681 | Precondition: |
---|
682 | self.writer has been initialised |
---|
683 | """ |
---|
684 | |
---|
685 | self.writer.store_timestep() |
---|
686 | |
---|
687 | ## |
---|
688 | # @brief Get time stepping statistics string for printing. |
---|
689 | # @param track_speeds |
---|
690 | # @param triangle_id |
---|
691 | def timestepping_statistics(self, |
---|
692 | track_speeds=False, |
---|
693 | triangle_id=None): |
---|
694 | """Return string with time stepping statistics for printing or logging |
---|
695 | |
---|
696 | Optional boolean keyword track_speeds decides whether to report |
---|
697 | location of smallest timestep as well as a histogram and percentile |
---|
698 | report. |
---|
699 | """ |
---|
700 | |
---|
701 | from anuga.config import epsilon, g |
---|
702 | |
---|
703 | # Call basic machinery from parent class |
---|
704 | msg = Generic_Domain.timestepping_statistics(self, track_speeds, |
---|
705 | triangle_id) |
---|
706 | |
---|
707 | if track_speeds is True: |
---|
708 | # qwidth determines the text field used for quantities |
---|
709 | qwidth = self.qwidth |
---|
710 | |
---|
711 | # Selected triangle |
---|
712 | k = self.k |
---|
713 | |
---|
714 | # Report some derived quantities at vertices, edges and centroid |
---|
715 | # specific to the shallow water wave equation |
---|
716 | z = self.quantities['elevation'] |
---|
717 | w = self.quantities['stage'] |
---|
718 | |
---|
719 | Vw = w.get_values(location='vertices', indices=[k])[0] |
---|
720 | Ew = w.get_values(location='edges', indices=[k])[0] |
---|
721 | Cw = w.get_values(location='centroids', indices=[k]) |
---|
722 | |
---|
723 | Vz = z.get_values(location='vertices', indices=[k])[0] |
---|
724 | Ez = z.get_values(location='edges', indices=[k])[0] |
---|
725 | Cz = z.get_values(location='centroids', indices=[k]) |
---|
726 | |
---|
727 | name = 'depth' |
---|
728 | Vh = Vw-Vz |
---|
729 | Eh = Ew-Ez |
---|
730 | Ch = Cw-Cz |
---|
731 | |
---|
732 | s = ' %s: vertex_values = %.4f,\t %.4f,\t %.4f\n'\ |
---|
733 | %(name.ljust(qwidth), Vh[0], Vh[1], Vh[2]) |
---|
734 | |
---|
735 | s += ' %s: edge_values = %.4f,\t %.4f,\t %.4f\n'\ |
---|
736 | %(name.ljust(qwidth), Eh[0], Eh[1], Eh[2]) |
---|
737 | |
---|
738 | s += ' %s: centroid_value = %.4f\n'\ |
---|
739 | %(name.ljust(qwidth), Ch[0]) |
---|
740 | |
---|
741 | msg += s |
---|
742 | |
---|
743 | uh = self.quantities['xmomentum'] |
---|
744 | vh = self.quantities['ymomentum'] |
---|
745 | |
---|
746 | Vuh = uh.get_values(location='vertices', indices=[k])[0] |
---|
747 | Euh = uh.get_values(location='edges', indices=[k])[0] |
---|
748 | Cuh = uh.get_values(location='centroids', indices=[k]) |
---|
749 | |
---|
750 | Vvh = vh.get_values(location='vertices', indices=[k])[0] |
---|
751 | Evh = vh.get_values(location='edges', indices=[k])[0] |
---|
752 | Cvh = vh.get_values(location='centroids', indices=[k]) |
---|
753 | |
---|
754 | # Speeds in each direction |
---|
755 | Vu = Vuh/(Vh + epsilon) |
---|
756 | Eu = Euh/(Eh + epsilon) |
---|
757 | Cu = Cuh/(Ch + epsilon) |
---|
758 | name = 'U' |
---|
759 | s = ' %s: vertex_values = %.4f,\t %.4f,\t %.4f\n'\ |
---|
760 | %(name.ljust(qwidth), Vu[0], Vu[1], Vu[2]) |
---|
761 | |
---|
762 | s += ' %s: edge_values = %.4f,\t %.4f,\t %.4f\n'\ |
---|
763 | %(name.ljust(qwidth), Eu[0], Eu[1], Eu[2]) |
---|
764 | |
---|
765 | s += ' %s: centroid_value = %.4f\n'\ |
---|
766 | %(name.ljust(qwidth), Cu[0]) |
---|
767 | |
---|
768 | msg += s |
---|
769 | |
---|
770 | Vv = Vvh/(Vh + epsilon) |
---|
771 | Ev = Evh/(Eh + epsilon) |
---|
772 | Cv = Cvh/(Ch + epsilon) |
---|
773 | name = 'V' |
---|
774 | s = ' %s: vertex_values = %.4f,\t %.4f,\t %.4f\n'\ |
---|
775 | %(name.ljust(qwidth), Vv[0], Vv[1], Vv[2]) |
---|
776 | |
---|
777 | s += ' %s: edge_values = %.4f,\t %.4f,\t %.4f\n'\ |
---|
778 | %(name.ljust(qwidth), Ev[0], Ev[1], Ev[2]) |
---|
779 | |
---|
780 | s += ' %s: centroid_value = %.4f\n'\ |
---|
781 | %(name.ljust(qwidth), Cv[0]) |
---|
782 | |
---|
783 | msg += s |
---|
784 | |
---|
785 | # Froude number in each direction |
---|
786 | name = 'Froude (x)' |
---|
787 | Vfx = Vu/(num.sqrt(g*Vh) + epsilon) |
---|
788 | Efx = Eu/(num.sqrt(g*Eh) + epsilon) |
---|
789 | Cfx = Cu/(num.sqrt(g*Ch) + epsilon) |
---|
790 | |
---|
791 | s = ' %s: vertex_values = %.4f,\t %.4f,\t %.4f\n'\ |
---|
792 | %(name.ljust(qwidth), Vfx[0], Vfx[1], Vfx[2]) |
---|
793 | |
---|
794 | s += ' %s: edge_values = %.4f,\t %.4f,\t %.4f\n'\ |
---|
795 | %(name.ljust(qwidth), Efx[0], Efx[1], Efx[2]) |
---|
796 | |
---|
797 | s += ' %s: centroid_value = %.4f\n'\ |
---|
798 | %(name.ljust(qwidth), Cfx[0]) |
---|
799 | |
---|
800 | msg += s |
---|
801 | |
---|
802 | name = 'Froude (y)' |
---|
803 | Vfy = Vv/(num.sqrt(g*Vh) + epsilon) |
---|
804 | Efy = Ev/(num.sqrt(g*Eh) + epsilon) |
---|
805 | Cfy = Cv/(num.sqrt(g*Ch) + epsilon) |
---|
806 | |
---|
807 | s = ' %s: vertex_values = %.4f,\t %.4f,\t %.4f\n'\ |
---|
808 | %(name.ljust(qwidth), Vfy[0], Vfy[1], Vfy[2]) |
---|
809 | |
---|
810 | s += ' %s: edge_values = %.4f,\t %.4f,\t %.4f\n'\ |
---|
811 | %(name.ljust(qwidth), Efy[0], Efy[1], Efy[2]) |
---|
812 | |
---|
813 | s += ' %s: centroid_value = %.4f\n'\ |
---|
814 | %(name.ljust(qwidth), Cfy[0]) |
---|
815 | |
---|
816 | msg += s |
---|
817 | |
---|
818 | return msg |
---|
819 | |
---|
820 | |
---|
821 | |
---|
822 | def compute_boundary_flows(self): |
---|
823 | """Compute boundary flows at current timestep. |
---|
824 | |
---|
825 | Quantities computed are: |
---|
826 | Total inflow across boundary |
---|
827 | Total outflow across boundary |
---|
828 | Flow across each tagged boundary segment |
---|
829 | """ |
---|
830 | |
---|
831 | # Run through boundary array and compute for each segment |
---|
832 | # the normal momentum ((uh, vh) dot normal) times segment length. |
---|
833 | # Based on sign accumulate this into boundary_inflow and boundary_outflow. |
---|
834 | |
---|
835 | # Compute flows along boundary |
---|
836 | |
---|
837 | uh = self.get_quantity('xmomentum').get_values(location='edges') |
---|
838 | vh = self.get_quantity('ymomentum').get_values(location='edges') |
---|
839 | |
---|
840 | # Loop through edges that lie on the boundary and calculate |
---|
841 | # flows |
---|
842 | boundary_flows = {} |
---|
843 | total_boundary_inflow = 0.0 |
---|
844 | total_boundary_outflow = 0.0 |
---|
845 | for vol_id, edge_id in self.boundary: |
---|
846 | # Compute normal flow across edge. Since normal vector points |
---|
847 | # away from triangle, a positive sign means that water |
---|
848 | # flows *out* from this triangle. |
---|
849 | |
---|
850 | momentum = [uh[vol_id, edge_id], vh[vol_id, edge_id]] |
---|
851 | normal = self.mesh.get_normal(vol_id, edge_id) |
---|
852 | length = self.mesh.get_edgelength(vol_id, edge_id) |
---|
853 | normal_flow = num.dot(momentum, normal)*length |
---|
854 | |
---|
855 | # Reverse sign so that + is taken to mean inflow |
---|
856 | # and - means outflow. This is more intuitive. |
---|
857 | edge_flow = -normal_flow |
---|
858 | |
---|
859 | # Tally up inflows and outflows separately |
---|
860 | if edge_flow > 0: |
---|
861 | # Flow is inflow |
---|
862 | total_boundary_inflow += edge_flow |
---|
863 | else: |
---|
864 | # Flow is outflow |
---|
865 | total_boundary_outflow += edge_flow |
---|
866 | |
---|
867 | # Tally up flows by boundary tag |
---|
868 | tag = self.boundary[(vol_id, edge_id)] |
---|
869 | |
---|
870 | if tag not in boundary_flows: |
---|
871 | boundary_flows[tag] = 0.0 |
---|
872 | boundary_flows[tag] += edge_flow |
---|
873 | |
---|
874 | |
---|
875 | return boundary_flows, total_boundary_inflow, total_boundary_outflow |
---|
876 | |
---|
877 | |
---|
878 | def compute_forcing_flows(self): |
---|
879 | """Compute flows in and out of domain due to forcing terms. |
---|
880 | |
---|
881 | Quantities computed are: |
---|
882 | |
---|
883 | |
---|
884 | Total inflow through forcing terms |
---|
885 | Total outflow through forcing terms |
---|
886 | Current total volume in domain |
---|
887 | |
---|
888 | """ |
---|
889 | |
---|
890 | #FIXME(Ole): We need to separate what part of explicit_update was |
---|
891 | # due to the normal flux calculations and what is due to forcing terms. |
---|
892 | |
---|
893 | pass |
---|
894 | |
---|
895 | |
---|
896 | def compute_total_volume(self): |
---|
897 | """Compute total volume (m^3) of water in entire domain |
---|
898 | """ |
---|
899 | |
---|
900 | area = self.mesh.get_areas() |
---|
901 | volume = 0.0 |
---|
902 | |
---|
903 | stage = self.get_quantity('stage').get_values(location='centroids') |
---|
904 | elevation = self.get_quantity('elevation').get_values(location='centroids') |
---|
905 | depth = stage-elevation |
---|
906 | |
---|
907 | return num.sum(depth*area) |
---|
908 | |
---|
909 | |
---|
910 | def volumetric_balance_statistics(self): |
---|
911 | """Create volumetric balance report suitable for printing or logging. |
---|
912 | """ |
---|
913 | |
---|
914 | (boundary_flows, total_boundary_inflow, |
---|
915 | total_boundary_outflow) = self.compute_boundary_flows() |
---|
916 | |
---|
917 | s = '---------------------------\n' |
---|
918 | s += 'Volumetric balance report:\n' |
---|
919 | s += '--------------------------\n' |
---|
920 | s += 'Total boundary inflow [m^3/s]: %.2f\n' % total_boundary_inflow |
---|
921 | s += 'Total boundary outflow [m^3/s]: %.2f\n' % total_boundary_outflow |
---|
922 | s += 'Net boundary flow by tags [m^3/s]\n' |
---|
923 | for tag in boundary_flows: |
---|
924 | s += ' %s [m^3/s]: %.2f\n' % (tag, boundary_flows[tag]) |
---|
925 | |
---|
926 | s += 'Total net boundary flow [m^3/s]: %.2f\n' % (total_boundary_inflow + total_boundary_outflow) |
---|
927 | s += 'Total volume in domain [m^3]: %.2f\n' % self.compute_total_volume() |
---|
928 | |
---|
929 | # The go through explicit forcing update and record the rate of change for stage and |
---|
930 | # record into forcing_inflow and forcing_outflow. Finally compute integral |
---|
931 | # of depth to obtain total volume of domain. |
---|
932 | |
---|
933 | # FIXME(Ole): This part is not yet done. |
---|
934 | |
---|
935 | return s |
---|
936 | |
---|
937 | ################################################################################ |
---|
938 | # End of class Shallow Water Domain |
---|
939 | ################################################################################ |
---|
940 | |
---|
941 | #----------------- |
---|
942 | # Flux computation |
---|
943 | #----------------- |
---|
944 | |
---|
945 | ## @brief Compute fluxes and timestep suitable for all volumes in domain. |
---|
946 | # @param domain The domain to calculate fluxes for. |
---|
947 | def compute_fluxes(domain): |
---|
948 | """Compute fluxes and timestep suitable for all volumes in domain. |
---|
949 | |
---|
950 | Compute total flux for each conserved quantity using "flux_function" |
---|
951 | |
---|
952 | Fluxes across each edge are scaled by edgelengths and summed up |
---|
953 | Resulting flux is then scaled by area and stored in |
---|
954 | explicit_update for each of the three conserved quantities |
---|
955 | stage, xmomentum and ymomentum |
---|
956 | |
---|
957 | The maximal allowable speed computed by the flux_function for each volume |
---|
958 | is converted to a timestep that must not be exceeded. The minimum of |
---|
959 | those is computed as the next overall timestep. |
---|
960 | |
---|
961 | Post conditions: |
---|
962 | domain.explicit_update is reset to computed flux values |
---|
963 | domain.timestep is set to the largest step satisfying all volumes. |
---|
964 | |
---|
965 | This wrapper calls the underlying C version of compute fluxes |
---|
966 | """ |
---|
967 | |
---|
968 | import sys |
---|
969 | from shallow_water_ext import compute_fluxes_ext_central \ |
---|
970 | as compute_fluxes_ext |
---|
971 | |
---|
972 | N = len(domain) # number_of_triangles |
---|
973 | |
---|
974 | # Shortcuts |
---|
975 | Stage = domain.quantities['stage'] |
---|
976 | Xmom = domain.quantities['xmomentum'] |
---|
977 | Ymom = domain.quantities['ymomentum'] |
---|
978 | Bed = domain.quantities['elevation'] |
---|
979 | |
---|
980 | timestep = float(sys.maxint) |
---|
981 | |
---|
982 | flux_timestep = compute_fluxes_ext(timestep, |
---|
983 | domain.epsilon, |
---|
984 | domain.H0, |
---|
985 | domain.g, |
---|
986 | domain.neighbours, |
---|
987 | domain.neighbour_edges, |
---|
988 | domain.normals, |
---|
989 | domain.edgelengths, |
---|
990 | domain.radii, |
---|
991 | domain.areas, |
---|
992 | domain.tri_full_flag, |
---|
993 | Stage.edge_values, |
---|
994 | Xmom.edge_values, |
---|
995 | Ymom.edge_values, |
---|
996 | Bed.edge_values, |
---|
997 | Stage.boundary_values, |
---|
998 | Xmom.boundary_values, |
---|
999 | Ymom.boundary_values, |
---|
1000 | Stage.explicit_update, |
---|
1001 | Xmom.explicit_update, |
---|
1002 | Ymom.explicit_update, |
---|
1003 | domain.already_computed_flux, |
---|
1004 | domain.max_speed, |
---|
1005 | int(domain.optimise_dry_cells)) |
---|
1006 | |
---|
1007 | domain.flux_timestep = flux_timestep |
---|
1008 | |
---|
1009 | ################################################################################ |
---|
1010 | # Module functions for gradient limiting |
---|
1011 | ################################################################################ |
---|
1012 | |
---|
1013 | ## |
---|
1014 | # @brief Wrapper for C version of extrapolate_second_order_sw. |
---|
1015 | # @param domain The domain to operate on. |
---|
1016 | # @note MH090605 The following method belongs to the shallow_water domain class |
---|
1017 | # see comments in the corresponding method in shallow_water_ext.c |
---|
1018 | def extrapolate_second_order_sw(domain): |
---|
1019 | """Wrapper calling C version of extrapolate_second_order_sw""" |
---|
1020 | |
---|
1021 | import sys |
---|
1022 | from shallow_water_ext import extrapolate_second_order_sw as extrapol2 |
---|
1023 | |
---|
1024 | N = len(domain) # number_of_triangles |
---|
1025 | |
---|
1026 | # Shortcuts |
---|
1027 | Stage = domain.quantities['stage'] |
---|
1028 | Xmom = domain.quantities['xmomentum'] |
---|
1029 | Ymom = domain.quantities['ymomentum'] |
---|
1030 | Elevation = domain.quantities['elevation'] |
---|
1031 | |
---|
1032 | extrapol2(domain, |
---|
1033 | domain.surrogate_neighbours, |
---|
1034 | domain.number_of_boundaries, |
---|
1035 | domain.centroid_coordinates, |
---|
1036 | Stage.centroid_values, |
---|
1037 | Xmom.centroid_values, |
---|
1038 | Ymom.centroid_values, |
---|
1039 | Elevation.centroid_values, |
---|
1040 | domain.vertex_coordinates, |
---|
1041 | Stage.vertex_values, |
---|
1042 | Xmom.vertex_values, |
---|
1043 | Ymom.vertex_values, |
---|
1044 | Elevation.vertex_values, |
---|
1045 | int(domain.optimise_dry_cells)) |
---|
1046 | |
---|
1047 | ## |
---|
1048 | # @brief Distribution from centroids to vertices specific to the SWW eqn. |
---|
1049 | # @param domain The domain to operate on. |
---|
1050 | def distribute_using_vertex_limiter(domain): |
---|
1051 | """Distribution from centroids to vertices specific to the SWW equation. |
---|
1052 | |
---|
1053 | It will ensure that h (w-z) is always non-negative even in the |
---|
1054 | presence of steep bed-slopes by taking a weighted average between shallow |
---|
1055 | and deep cases. |
---|
1056 | |
---|
1057 | In addition, all conserved quantities get distributed as per either a |
---|
1058 | constant (order==1) or a piecewise linear function (order==2). |
---|
1059 | |
---|
1060 | FIXME: more explanation about removal of artificial variability etc |
---|
1061 | |
---|
1062 | Precondition: |
---|
1063 | All quantities defined at centroids and bed elevation defined at |
---|
1064 | vertices. |
---|
1065 | |
---|
1066 | Postcondition |
---|
1067 | Conserved quantities defined at vertices |
---|
1068 | """ |
---|
1069 | |
---|
1070 | # Remove very thin layers of water |
---|
1071 | protect_against_infinitesimal_and_negative_heights(domain) |
---|
1072 | |
---|
1073 | # Extrapolate all conserved quantities |
---|
1074 | if domain.optimised_gradient_limiter: |
---|
1075 | # MH090605 if second order, |
---|
1076 | # perform the extrapolation and limiting on |
---|
1077 | # all of the conserved quantities |
---|
1078 | |
---|
1079 | if (domain._order_ == 1): |
---|
1080 | for name in domain.conserved_quantities: |
---|
1081 | Q = domain.quantities[name] |
---|
1082 | Q.extrapolate_first_order() |
---|
1083 | elif domain._order_ == 2: |
---|
1084 | domain.extrapolate_second_order_sw() |
---|
1085 | else: |
---|
1086 | raise 'Unknown order' |
---|
1087 | else: |
---|
1088 | # Old code: |
---|
1089 | for name in domain.conserved_quantities: |
---|
1090 | Q = domain.quantities[name] |
---|
1091 | |
---|
1092 | if domain._order_ == 1: |
---|
1093 | Q.extrapolate_first_order() |
---|
1094 | elif domain._order_ == 2: |
---|
1095 | Q.extrapolate_second_order_and_limit_by_vertex() |
---|
1096 | else: |
---|
1097 | raise 'Unknown order' |
---|
1098 | |
---|
1099 | # Take bed elevation into account when water heights are small |
---|
1100 | balance_deep_and_shallow(domain) |
---|
1101 | |
---|
1102 | # Compute edge values by interpolation |
---|
1103 | for name in domain.conserved_quantities: |
---|
1104 | Q = domain.quantities[name] |
---|
1105 | Q.interpolate_from_vertices_to_edges() |
---|
1106 | |
---|
1107 | ## |
---|
1108 | # @brief Distribution from centroids to edges specific to the SWW eqn. |
---|
1109 | # @param domain The domain to operate on. |
---|
1110 | def distribute_using_edge_limiter(domain): |
---|
1111 | """Distribution from centroids to edges specific to the SWW eqn. |
---|
1112 | |
---|
1113 | It will ensure that h (w-z) is always non-negative even in the |
---|
1114 | presence of steep bed-slopes by taking a weighted average between shallow |
---|
1115 | and deep cases. |
---|
1116 | |
---|
1117 | In addition, all conserved quantities get distributed as per either a |
---|
1118 | constant (order==1) or a piecewise linear function (order==2). |
---|
1119 | |
---|
1120 | |
---|
1121 | Precondition: |
---|
1122 | All quantities defined at centroids and bed elevation defined at |
---|
1123 | vertices. |
---|
1124 | |
---|
1125 | Postcondition |
---|
1126 | Conserved quantities defined at vertices |
---|
1127 | """ |
---|
1128 | |
---|
1129 | # Remove very thin layers of water |
---|
1130 | protect_against_infinitesimal_and_negative_heights(domain) |
---|
1131 | |
---|
1132 | for name in domain.conserved_quantities: |
---|
1133 | Q = domain.quantities[name] |
---|
1134 | if domain._order_ == 1: |
---|
1135 | Q.extrapolate_first_order() |
---|
1136 | elif domain._order_ == 2: |
---|
1137 | Q.extrapolate_second_order_and_limit_by_edge() |
---|
1138 | else: |
---|
1139 | raise 'Unknown order' |
---|
1140 | |
---|
1141 | balance_deep_and_shallow(domain) |
---|
1142 | |
---|
1143 | # Compute edge values by interpolation |
---|
1144 | for name in domain.conserved_quantities: |
---|
1145 | Q = domain.quantities[name] |
---|
1146 | Q.interpolate_from_vertices_to_edges() |
---|
1147 | |
---|
1148 | ## |
---|
1149 | # @brief Protect against infinitesimal heights and associated high velocities. |
---|
1150 | # @param domain The domain to operate on. |
---|
1151 | def protect_against_infinitesimal_and_negative_heights(domain): |
---|
1152 | """Protect against infinitesimal heights and associated high velocities""" |
---|
1153 | |
---|
1154 | from shallow_water_ext import protect |
---|
1155 | |
---|
1156 | # Shortcuts |
---|
1157 | wc = domain.quantities['stage'].centroid_values |
---|
1158 | zc = domain.quantities['elevation'].centroid_values |
---|
1159 | xmomc = domain.quantities['xmomentum'].centroid_values |
---|
1160 | ymomc = domain.quantities['ymomentum'].centroid_values |
---|
1161 | |
---|
1162 | protect(domain.minimum_allowed_height, domain.maximum_allowed_speed, |
---|
1163 | domain.epsilon, wc, zc, xmomc, ymomc) |
---|
1164 | |
---|
1165 | ## |
---|
1166 | # @brief Wrapper for C function balance_deep_and_shallow_c(). |
---|
1167 | # @param domain The domain to operate on. |
---|
1168 | def balance_deep_and_shallow(domain): |
---|
1169 | """Compute linear combination between stage as computed by |
---|
1170 | gradient-limiters limiting using w, and stage computed by |
---|
1171 | gradient-limiters limiting using h (h-limiter). |
---|
1172 | The former takes precedence when heights are large compared to the |
---|
1173 | bed slope while the latter takes precedence when heights are |
---|
1174 | relatively small. Anything in between is computed as a balanced |
---|
1175 | linear combination in order to avoid numerical disturbances which |
---|
1176 | would otherwise appear as a result of hard switching between |
---|
1177 | modes. |
---|
1178 | |
---|
1179 | Wrapper for C implementation |
---|
1180 | """ |
---|
1181 | |
---|
1182 | from shallow_water_ext import balance_deep_and_shallow \ |
---|
1183 | as balance_deep_and_shallow_c |
---|
1184 | |
---|
1185 | # Shortcuts |
---|
1186 | wc = domain.quantities['stage'].centroid_values |
---|
1187 | zc = domain.quantities['elevation'].centroid_values |
---|
1188 | wv = domain.quantities['stage'].vertex_values |
---|
1189 | zv = domain.quantities['elevation'].vertex_values |
---|
1190 | |
---|
1191 | # Momentums at centroids |
---|
1192 | xmomc = domain.quantities['xmomentum'].centroid_values |
---|
1193 | ymomc = domain.quantities['ymomentum'].centroid_values |
---|
1194 | |
---|
1195 | # Momentums at vertices |
---|
1196 | xmomv = domain.quantities['xmomentum'].vertex_values |
---|
1197 | ymomv = domain.quantities['ymomentum'].vertex_values |
---|
1198 | |
---|
1199 | balance_deep_and_shallow_c(domain, |
---|
1200 | wc, zc, wv, zv, wc, |
---|
1201 | xmomc, ymomc, xmomv, ymomv) |
---|
1202 | |
---|
1203 | |
---|
1204 | |
---|
1205 | ################################################################################ |
---|
1206 | # Standard forcing terms |
---|
1207 | ################################################################################ |
---|
1208 | |
---|
1209 | ## |
---|
1210 | # @brief Apply gravitational pull in the presence of bed slope. |
---|
1211 | # @param domain The domain to apply gravity to. |
---|
1212 | # @note Wrapper for C function gravity_c(). |
---|
1213 | def gravity(domain): |
---|
1214 | """Apply gravitational pull in the presence of bed slope |
---|
1215 | Wrapper calls underlying C implementation |
---|
1216 | """ |
---|
1217 | |
---|
1218 | from shallow_water_ext import gravity as gravity_c |
---|
1219 | |
---|
1220 | xmom_update = domain.quantities['xmomentum'].explicit_update |
---|
1221 | ymom_update = domain.quantities['ymomentum'].explicit_update |
---|
1222 | |
---|
1223 | stage = domain.quantities['stage'] |
---|
1224 | elevation = domain.quantities['elevation'] |
---|
1225 | |
---|
1226 | h = stage.centroid_values - elevation.centroid_values |
---|
1227 | z = elevation.vertex_values |
---|
1228 | |
---|
1229 | x = domain.get_vertex_coordinates() |
---|
1230 | g = domain.g |
---|
1231 | |
---|
1232 | gravity_c(g, h, z, x, xmom_update, ymom_update) #, 1.0e-6) |
---|
1233 | |
---|
1234 | ## |
---|
1235 | # @brief Apply friction to a surface (implicit). |
---|
1236 | # @param domain The domain to apply Manning friction to. |
---|
1237 | # @note Wrapper for C function manning_friction_c(). |
---|
1238 | def manning_friction_implicit(domain): |
---|
1239 | """Apply (Manning) friction to water momentum |
---|
1240 | Wrapper for c version |
---|
1241 | """ |
---|
1242 | |
---|
1243 | from shallow_water_ext import manning_friction_old |
---|
1244 | from shallow_water_ext import manning_friction_new |
---|
1245 | |
---|
1246 | xmom = domain.quantities['xmomentum'] |
---|
1247 | ymom = domain.quantities['ymomentum'] |
---|
1248 | |
---|
1249 | x = domain.get_vertex_coordinates() |
---|
1250 | |
---|
1251 | w = domain.quantities['stage'].centroid_values |
---|
1252 | z = domain.quantities['elevation'].vertex_values |
---|
1253 | |
---|
1254 | uh = xmom.centroid_values |
---|
1255 | vh = ymom.centroid_values |
---|
1256 | eta = domain.quantities['friction'].centroid_values |
---|
1257 | |
---|
1258 | xmom_update = xmom.semi_implicit_update |
---|
1259 | ymom_update = ymom.semi_implicit_update |
---|
1260 | |
---|
1261 | N = len(domain) |
---|
1262 | eps = domain.minimum_allowed_height |
---|
1263 | g = domain.g |
---|
1264 | |
---|
1265 | if domain.use_new_mannings: |
---|
1266 | manning_friction_new(g, eps, x, w, uh, vh, z, eta, xmom_update, ymom_update) |
---|
1267 | else: |
---|
1268 | manning_friction_old(g, eps, w, uh, vh, z, eta, xmom_update, ymom_update) |
---|
1269 | |
---|
1270 | |
---|
1271 | ## |
---|
1272 | # @brief Apply friction to a surface (explicit). |
---|
1273 | # @param domain The domain to apply Manning friction to. |
---|
1274 | # @note Wrapper for C function manning_friction_c(). |
---|
1275 | def manning_friction_explicit(domain): |
---|
1276 | """Apply (Manning) friction to water momentum |
---|
1277 | Wrapper for c version |
---|
1278 | """ |
---|
1279 | |
---|
1280 | from shallow_water_ext import manning_friction_old |
---|
1281 | from shallow_water_ext import manning_friction_new |
---|
1282 | |
---|
1283 | xmom = domain.quantities['xmomentum'] |
---|
1284 | ymom = domain.quantities['ymomentum'] |
---|
1285 | |
---|
1286 | x = domain.get_vertex_coordinates() |
---|
1287 | |
---|
1288 | w = domain.quantities['stage'].centroid_values |
---|
1289 | z = domain.quantities['elevation'].vertex_values |
---|
1290 | |
---|
1291 | uh = xmom.centroid_values |
---|
1292 | vh = ymom.centroid_values |
---|
1293 | eta = domain.quantities['friction'].centroid_values |
---|
1294 | |
---|
1295 | xmom_update = xmom.explicit_update |
---|
1296 | ymom_update = ymom.explicit_update |
---|
1297 | |
---|
1298 | N = len(domain) |
---|
1299 | eps = domain.minimum_allowed_height |
---|
1300 | g = domain.g |
---|
1301 | |
---|
1302 | |
---|
1303 | if domain.use_new_mannings: |
---|
1304 | manning_friction_new(g, eps, x, w, uh, vh, z, eta, xmom_update, ymom_update) |
---|
1305 | else: |
---|
1306 | manning_friction_old(g, eps, w, uh, vh, z, eta, xmom_update, ymom_update) |
---|
1307 | |
---|
1308 | |
---|
1309 | |
---|
1310 | # FIXME (Ole): This was implemented for use with one of the analytical solutions (Sampson?) |
---|
1311 | ## |
---|
1312 | # @brief Apply linear friction to a surface. |
---|
1313 | # @param domain The domain to apply Manning friction to. |
---|
1314 | # @note Is this still used (30 Oct 2007)? |
---|
1315 | def linear_friction(domain): |
---|
1316 | """Apply linear friction to water momentum |
---|
1317 | |
---|
1318 | Assumes quantity: 'linear_friction' to be present |
---|
1319 | """ |
---|
1320 | |
---|
1321 | from math import sqrt |
---|
1322 | |
---|
1323 | w = domain.quantities['stage'].centroid_values |
---|
1324 | z = domain.quantities['elevation'].centroid_values |
---|
1325 | h = w-z |
---|
1326 | |
---|
1327 | uh = domain.quantities['xmomentum'].centroid_values |
---|
1328 | vh = domain.quantities['ymomentum'].centroid_values |
---|
1329 | tau = domain.quantities['linear_friction'].centroid_values |
---|
1330 | |
---|
1331 | xmom_update = domain.quantities['xmomentum'].semi_implicit_update |
---|
1332 | ymom_update = domain.quantities['ymomentum'].semi_implicit_update |
---|
1333 | |
---|
1334 | N = len(domain) # number_of_triangles |
---|
1335 | eps = domain.minimum_allowed_height |
---|
1336 | g = domain.g #Not necessary? Why was this added? |
---|
1337 | |
---|
1338 | for k in range(N): |
---|
1339 | if tau[k] >= eps: |
---|
1340 | if h[k] >= eps: |
---|
1341 | S = -tau[k]/h[k] |
---|
1342 | |
---|
1343 | #Update momentum |
---|
1344 | xmom_update[k] += S*uh[k] |
---|
1345 | ymom_update[k] += S*vh[k] |
---|
1346 | |
---|
1347 | def depth_dependent_friction(domain, default_friction, |
---|
1348 | surface_roughness_data, |
---|
1349 | verbose=False): |
---|
1350 | """Returns an array of friction values for each wet element adjusted for depth. |
---|
1351 | |
---|
1352 | Inputs: |
---|
1353 | domain - computational domain object |
---|
1354 | default_friction - depth independent bottom friction |
---|
1355 | surface_roughness_data - N x 5 array of n0, d1, n1, d2, n2 values for each |
---|
1356 | friction region. |
---|
1357 | |
---|
1358 | Outputs: |
---|
1359 | wet_friction - Array that can be used directly to update friction as follows: |
---|
1360 | domain.set_quantity('friction', wet_friction) |
---|
1361 | |
---|
1362 | |
---|
1363 | |
---|
1364 | """ |
---|
1365 | |
---|
1366 | import numpy as num |
---|
1367 | |
---|
1368 | # Create a temp array to store updated depth dependent friction for wet elements |
---|
1369 | # EHR this is outwardly inneficient but not obvious how to avoid recreating each call?????? |
---|
1370 | N=len(domain) |
---|
1371 | wet_friction = num.zeros(N, num.float) |
---|
1372 | wet_friction[:] = default_n0 # Initially assign default_n0 to all array so sure have no zeros values |
---|
1373 | |
---|
1374 | |
---|
1375 | depth = domain.create_quantity_from_expression('stage - elevation') # create depth instance for this timestep |
---|
1376 | # Recompute depth as vector |
---|
1377 | d = depth.get_values(location='centroids') |
---|
1378 | |
---|
1379 | # rebuild the 'friction' values adjusted for depth at this instant |
---|
1380 | for i in domain.get_wet_elements(): # loop for each wet element in domain |
---|
1381 | |
---|
1382 | # Get roughness data for each element |
---|
1383 | n0 = float(surface_roughness_data[i,0]) |
---|
1384 | d1 = float(surface_roughness_data[i,1]) |
---|
1385 | n1 = float(surface_roughness_data[i,2]) |
---|
1386 | d2 = float(surface_roughness_data[i,3]) |
---|
1387 | n2 = float(surface_roughness_data[i,4]) |
---|
1388 | |
---|
1389 | |
---|
1390 | # Recompute friction values from depth for this element |
---|
1391 | |
---|
1392 | if d[i] <= d1: |
---|
1393 | depth_dependent_friction = n1 |
---|
1394 | elif d[i] >= d2: |
---|
1395 | depth_dependent_friction = n2 |
---|
1396 | else: |
---|
1397 | depth_dependent_friction = n1+((n2-n1)/(d2-d1))*(d[i]-d1) |
---|
1398 | |
---|
1399 | # check sanity of result |
---|
1400 | if (depth_dependent_friction < 0.010 or depth_dependent_friction > 9999.0) : |
---|
1401 | log.critical('%s >>>> WARNING: computed depth_dependent friction ' |
---|
1402 | 'out of range, ddf%f, n1=%f, n2=%f' |
---|
1403 | % (model_data.basename, |
---|
1404 | depth_dependent_friction, n1, n2)) |
---|
1405 | |
---|
1406 | # update depth dependent friction for that wet element |
---|
1407 | wet_friction[i] = depth_dependent_friction |
---|
1408 | |
---|
1409 | # EHR add code to show range of 'friction across domain at this instant as sanity check????????? |
---|
1410 | |
---|
1411 | if verbose : |
---|
1412 | nvals=domain.get_quantity('friction').get_values(location='centroids') # return array of domain nvals |
---|
1413 | n_min=min(nvals) |
---|
1414 | n_max=max(nvals) |
---|
1415 | |
---|
1416 | log.critical(' ++++ calculate_depth_dependent_friction - ' |
---|
1417 | 'Updated friction - range %7.3f to %7.3f' |
---|
1418 | % (n_min, n_max)) |
---|
1419 | |
---|
1420 | return wet_friction |
---|
1421 | |
---|
1422 | |
---|
1423 | |
---|
1424 | ################################################################################ |
---|
1425 | # Initialise module |
---|
1426 | ################################################################################ |
---|
1427 | |
---|
1428 | from anuga.utilities import compile |
---|
1429 | if compile.can_use_C_extension('shallow_water_ext.c'): |
---|
1430 | # Underlying C implementations can be accessed |
---|
1431 | from shallow_water_ext import assign_windfield_values |
---|
1432 | else: |
---|
1433 | msg = 'C implementations could not be accessed by %s.\n ' % __file__ |
---|
1434 | msg += 'Make sure compile_all.py has been run as described in ' |
---|
1435 | msg += 'the ANUGA installation guide.' |
---|
1436 | raise Exception, msg |
---|
1437 | |
---|
1438 | # Optimisation with psyco |
---|
1439 | from anuga.config import use_psyco |
---|
1440 | if use_psyco: |
---|
1441 | try: |
---|
1442 | import psyco |
---|
1443 | except: |
---|
1444 | import os |
---|
1445 | if os.name == 'posix' and os.uname()[4] in ['x86_64', 'ia64']: |
---|
1446 | pass |
---|
1447 | #Psyco isn't supported on 64 bit systems, but it doesn't matter |
---|
1448 | else: |
---|
1449 | msg = ('WARNING: psyco (speedup) could not be imported, ' |
---|
1450 | 'you may want to consider installing it') |
---|
1451 | log.critical(msg) |
---|
1452 | else: |
---|
1453 | psyco.bind(Domain.distribute_to_vertices_and_edges) |
---|
1454 | psyco.bind(Domain.compute_fluxes) |
---|
1455 | |
---|
1456 | |
---|
1457 | if __name__ == "__main__": |
---|
1458 | pass |
---|