1 | """Class Domain - |
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2 | 2D triangular domains for finite-volume computations of |
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3 | the advection equation. |
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4 | |
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5 | This module contains a specialisation of class Domain from module domain.py |
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6 | consisting of methods specific to the advection equantion |
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7 | |
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8 | The equation is |
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9 | |
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10 | u_t + (v_1 u)_x + (v_2 u)_y = 0 |
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11 | |
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12 | There is only one conserved quantity, the stage u |
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13 | |
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14 | The advection equation is a very simple specialisation of the generic |
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15 | domain and may serve as an instructive example or a test of other |
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16 | components such as visualisation. |
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17 | |
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18 | Ole Nielsen, Stephen Roberts, Duncan Gray, Christopher Zoppou |
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19 | Geoscience Australia, 2004 |
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20 | """ |
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21 | |
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22 | |
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23 | #import logging, logging.config |
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24 | #logger = logging.getLogger('advection') |
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25 | #logger.setLevel(logging.WARNING) |
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26 | # |
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27 | #try: |
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28 | # logging.config.fileConfig('log.ini') |
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29 | #except: |
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30 | # pass |
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31 | |
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32 | |
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33 | from anuga.abstract_2d_finite_volumes.domain import * |
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34 | import anuga.utilities.log as log |
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35 | |
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36 | import numpy as num |
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37 | |
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38 | |
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39 | Generic_domain = Domain # Rename |
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40 | |
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41 | class Domain(Generic_domain): |
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42 | |
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43 | def __init__(self, |
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44 | coordinates, |
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45 | vertices, |
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46 | boundary = None, |
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47 | tagged_elements = None, |
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48 | geo_reference = None, |
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49 | use_inscribed_circle=False, |
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50 | velocity = None, |
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51 | full_send_dict=None, |
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52 | ghost_recv_dict=None, |
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53 | processor=0, |
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54 | numproc=1 |
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55 | ): |
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56 | |
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57 | conserved_quantities = ['stage'] |
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58 | other_quantities = [] |
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59 | Generic_domain.__init__(self, |
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60 | source=coordinates, |
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61 | triangles=vertices, |
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62 | boundary=boundary, |
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63 | conserved_quantities=conserved_quantities, |
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64 | other_quantities=other_quantities, |
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65 | tagged_elements=tagged_elements, |
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66 | geo_reference=geo_reference, |
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67 | use_inscribed_circle=use_inscribed_circle, |
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68 | full_send_dict=full_send_dict, |
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69 | ghost_recv_dict=ghost_recv_dict, |
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70 | processor=processor, |
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71 | numproc=numproc) |
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72 | |
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73 | if velocity is None: |
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74 | self.velocity = num.array([1,0],'d') |
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75 | else: |
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76 | self.velocity = num.array(velocity,'d') |
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77 | |
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78 | #Only first is implemented for advection |
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79 | self.set_default_order(1) |
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80 | self.set_beta(1.0) |
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81 | |
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82 | self.smooth = True |
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83 | |
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84 | def check_integrity(self): |
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85 | Generic_domain.check_integrity(self) |
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86 | |
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87 | msg = 'Conserved quantity must be "stage"' |
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88 | assert self.conserved_quantities[0] == 'stage', msg |
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89 | |
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90 | |
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91 | def distribute_to_vertices_and_edges(self): |
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92 | """Extrapolate conserved quantities from centroid to |
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93 | vertices and edge-midpoints for each volume |
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94 | |
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95 | Default implementation is straight first order, |
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96 | i.e. constant values throughout each element and |
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97 | no reference to non-conserved quantities. |
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98 | """ |
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99 | |
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100 | for name in self.conserved_quantities: |
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101 | Q = self.quantities[name] |
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102 | if self._order_ == 1: |
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103 | Q.extrapolate_first_order() |
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104 | elif self._order_ == 2: |
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105 | Q.extrapolate_second_order_and_limit_by_edge() |
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106 | #Q.limit() |
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107 | else: |
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108 | raise 'Unknown order' |
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109 | #Q.interpolate_from_vertices_to_edges() |
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110 | |
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111 | |
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112 | |
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113 | |
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114 | def flux_function(self, normal, ql, qr, zl=None, zr=None): |
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115 | """Compute outward flux as inner product between velocity |
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116 | vector v=(v_1, v_2) and normal vector n. |
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117 | |
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118 | if <n,v> > 0 flux direction is outward bound and its magnitude is |
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119 | determined by the quantity inside volume: ql. |
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120 | Otherwise it is inbound and magnitude is determined by the |
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121 | quantity outside the volume: qr. |
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122 | """ |
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123 | |
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124 | v1 = self.velocity[0] |
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125 | v2 = self.velocity[1] |
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126 | |
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127 | |
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128 | normal_velocity = v1*normal[0] + v2*normal[1] |
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129 | |
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130 | if normal_velocity < 0: |
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131 | flux = qr * normal_velocity |
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132 | else: |
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133 | flux = ql * normal_velocity |
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134 | |
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135 | max_speed = abs(normal_velocity) |
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136 | return flux, max_speed |
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137 | |
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138 | |
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139 | |
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140 | def compute_fluxes(self): |
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141 | """Compute all fluxes and the timestep suitable for all volumes |
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142 | in domain. |
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143 | |
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144 | Compute total flux for each conserved quantity using "flux_function" |
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145 | |
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146 | Fluxes across each edge are scaled by edgelengths and summed up |
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147 | Resulting flux is then scaled by area and stored in |
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148 | domain.explicit_update |
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149 | |
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150 | The maximal allowable speed computed by the flux_function |
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151 | for each volume |
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152 | is converted to a timestep that must not be exceeded. The minimum of |
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153 | those is computed as the next overall timestep. |
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154 | |
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155 | Post conditions: |
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156 | domain.explicit_update is reset to computed flux values |
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157 | domain.timestep is set to the largest step satisfying all volumes. |
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158 | """ |
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159 | |
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160 | import sys |
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161 | from anuga.config import max_timestep |
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162 | |
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163 | |
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164 | huge_timestep = float(sys.maxint) |
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165 | Stage = self.quantities['stage'] |
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166 | |
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167 | """ |
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168 | log.critical("======================================") |
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169 | log.critical("BEFORE compute_fluxes") |
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170 | log.critical("stage_update=%s" % str(Stage.explicit_update)) |
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171 | log.critical("stage_edge=%s" % str(Stage.edge_values)) |
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172 | log.critical("stage_bdry=%s" % str(Stage.boundary_values)) |
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173 | log.critical("neighbours=%s" % str(self.neighbours)) |
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174 | log.critical("neighbour_edges=%s" % str(self.neighbour_edges)) |
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175 | log.critical("normals=%s" % str(self.normals)) |
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176 | log.critical("areas=%s" % str(self.areas)) |
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177 | log.critical("radii=%s" % str(self.radii)) |
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178 | log.critical("edgelengths=%s" % str(self.edgelengths)) |
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179 | log.critical("tri_full_flag=%s" % str(self.tri_full_flag)) |
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180 | log.critical("huge_timestep=%s" % str(huge_timestep)) |
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181 | log.critical("max_timestep=%s" % str(max_timestep)) |
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182 | log.critical("velocity=%s" % str(self.velocity)) |
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183 | """ |
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184 | |
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185 | import advection_ext |
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186 | self.flux_timestep = advection_ext.compute_fluxes(self, Stage, huge_timestep, max_timestep) |
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187 | |
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188 | |
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189 | |
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190 | ## def evolve(self, |
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191 | ## yieldstep = None, |
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192 | ## finaltime = None, |
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193 | ## duration = None, |
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194 | ## skip_initial_step = False): |
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195 | |
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196 | ## """Specialisation of basic evolve method from parent class |
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197 | ## """ |
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198 | |
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199 | ## #Call basic machinery from parent class |
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200 | ## for t in Generic_domain.evolve(self, |
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201 | ## yieldstep=yieldstep, |
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202 | ## finaltime=finaltime, |
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203 | ## duration=duration, |
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204 | ## skip_initial_step=skip_initial_step): |
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205 | |
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206 | ## #Pass control on to outer loop for more specific actions |
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207 | ## yield(t) |
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208 | |
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209 | |
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210 | |
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211 | |
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212 | def compute_fluxes_python(self): |
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213 | """Compute all fluxes and the timestep suitable for all volumes |
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214 | in domain. |
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215 | |
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216 | Compute total flux for each conserved quantity using "flux_function" |
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217 | |
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218 | Fluxes across each edge are scaled by edgelengths and summed up |
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219 | Resulting flux is then scaled by area and stored in |
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220 | domain.explicit_update |
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221 | |
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222 | The maximal allowable speed computed by the flux_function |
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223 | for each volume |
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224 | is converted to a timestep that must not be exceeded. The minimum of |
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225 | those is computed as the next overall timestep. |
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226 | |
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227 | Post conditions: |
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228 | domain.explicit_update is reset to computed flux values |
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229 | domain.timestep is set to the largest step satisfying all volumes. |
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230 | """ |
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231 | |
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232 | import sys |
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233 | from anuga.config import max_timestep |
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234 | |
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235 | N = len(self) |
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236 | |
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237 | neighbours = self.neighbours |
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238 | neighbour_edges = self.neighbour_edges |
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239 | normals = self.normals |
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240 | |
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241 | areas = self.areas |
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242 | radii = self.radii |
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243 | edgelengths = self.edgelengths |
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244 | |
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245 | timestep = max_timestep #FIXME: Get rid of this |
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246 | |
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247 | #Shortcuts |
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248 | Stage = self.quantities['stage'] |
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249 | |
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250 | #Arrays |
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251 | stage = Stage.edge_values |
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252 | |
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253 | stage_bdry = Stage.boundary_values |
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254 | |
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255 | flux = num.zeros(1, num.float) #Work array for summing up fluxes |
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256 | |
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257 | #Loop |
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258 | for k in range(N): |
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259 | optimal_timestep = float(sys.maxint) |
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260 | |
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261 | flux[:] = 0. #Reset work array |
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262 | for i in range(3): |
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263 | #Quantities inside volume facing neighbour i |
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264 | ql = stage[k, i] |
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265 | |
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266 | #Quantities at neighbour on nearest face |
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267 | n = neighbours[k,i] |
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268 | if n < 0: |
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269 | m = -n-1 #Convert neg flag to index |
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270 | qr = stage_bdry[m] |
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271 | else: |
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272 | m = neighbour_edges[k,i] |
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273 | qr = stage[n, m] |
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274 | |
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275 | |
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276 | #Outward pointing normal vector |
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277 | normal = normals[k, 2*i:2*i+2] |
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278 | |
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279 | #Flux computation using provided function |
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280 | edgeflux, max_speed = self.flux_function(normal, ql, qr) |
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281 | flux -= edgeflux * edgelengths[k,i] |
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282 | |
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283 | #Update optimal_timestep |
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284 | if self.tri_full_flag[k] == 1 : |
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285 | try: |
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286 | optimal_timestep = min(optimal_timestep, radii[k]/max_speed) |
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287 | except ZeroDivisionError: |
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288 | pass |
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289 | |
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290 | #Normalise by area and store for when all conserved |
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291 | #quantities get updated |
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292 | flux /= areas[k] |
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293 | Stage.explicit_update[k] = flux[0] |
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294 | |
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295 | timestep = min(timestep, optimal_timestep) |
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296 | |
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297 | self.timestep = timestep |
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298 | |
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