[1963] | 1 | """Class Domain - |
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| 2 | 2D triangular domains for finite-volume computations of |
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| 3 | the Euler 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 Shallow Water Wave Equation |
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| 7 | |
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| 8 | |
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| 9 | U_t + E_x + G_y = 0 |
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| 10 | |
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| 11 | where |
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| 12 | |
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| 13 | U = [rho, mx, my, E] |
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| 14 | u = mx/rho |
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| 15 | v = my/rho |
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| 16 | |
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| 17 | E = [u rho, u mx + p, u my, u(E + p)] |
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| 18 | G = [v rho, v mx, v my + p, v(E + p)] |
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| 19 | |
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| 20 | and _t, _x, _y denote the derivative with respect to t, x and y respectively. |
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| 21 | |
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| 22 | The quantities are |
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| 23 | |
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| 24 | symbol variable name explanation |
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| 25 | x x horizontal distance from origin [m] |
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| 26 | y y vertical distance from origin [m] |
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| 27 | rho density density [kg/m^2] |
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| 28 | u speed in the x direction [m/s] |
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| 29 | v speed in the y direction [m/s] |
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| 30 | mx xmomentum momentum density in the x direction [kg/m/s^2] |
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| 31 | my ymomentum momentum density in the y direction [kg/m/s^2] |
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| 32 | E energy energy density [J/m^2] |
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| 33 | gamma gamma gamma law gas (1.4 for air) |
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| 34 | p pressure pressure [N/m |
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| 35 | |
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| 36 | |
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| 37 | The conserved quantities are rho, mx, my, E |
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| 38 | |
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| 39 | Gamma law relates pressure with conserved quantities |
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| 40 | |
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| 41 | p = (gamma-1)[E - rho/2(u^2 + v^2)] |
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| 42 | |
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| 43 | |
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| 44 | Ole Nielsen, Stephen Roberts, Duncan Gray, Christopher Zoppou |
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| 45 | Geoscience Australia, 2004 |
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| 46 | """ |
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| 47 | |
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| 48 | #Subversion keywords: |
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| 49 | # |
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| 50 | #$LastChangedDate: 2005-10-14 12:02:18 +1000 (Fri, 14 Oct 2005) $ |
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| 51 | #$LastChangedRevision: 1922 $ |
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| 52 | #$LastChangedBy: duncan $ |
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| 53 | |
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| 54 | |
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| 55 | from domain import * |
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| 56 | from region import * |
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| 57 | |
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| 58 | Generic_domain = Domain #Rename |
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| 59 | |
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| 60 | #Euler domain |
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| 61 | class Domain(Generic_domain): |
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| 62 | |
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| 63 | def __init__(self, coordinates, vertices, boundary = None, |
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| 64 | tagged_elements = None, geo_reference = None, |
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| 65 | use_inscribed_circle=False): |
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| 66 | |
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| 67 | conserved_quantities = ['density', 'xmomentum', 'ymomentum', 'energy'] |
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| 68 | other_quantities = ['pressure'] |
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| 69 | Generic_domain.__init__(self, coordinates, vertices, boundary, |
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| 70 | conserved_quantities, other_quantities, |
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| 71 | tagged_elements, geo_reference, use_inscribed_circle) |
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| 72 | |
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| 73 | from euler_config import minimum_allowed_density |
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| 74 | self.minimum_allowed_density = minimum_allowed_density |
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| 75 | |
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| 76 | #Realtime visualisation |
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| 77 | self.visualiser = None |
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| 78 | self.visualise = False |
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| 79 | self.visualise_color_stage = False |
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| 80 | self.visualise_stage_range = 1.0 |
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| 81 | self.visualise_timer = True |
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| 82 | self.visualise_range_z = None |
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| 83 | |
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| 84 | #Stored output |
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| 85 | self.store = False |
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| 86 | self.format = 'sww' |
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| 87 | self.smooth = False |
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| 88 | |
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| 89 | #Reduction operation for get_vertex_values |
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| 90 | from util import mean |
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| 91 | self.reduction = mean |
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| 92 | #self.reduction = min #Looks better near steep slopes |
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| 93 | |
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| 94 | self.quantities_to_be_stored = ['density', 'xmomentum', 'ymomentum', 'energy', 'pressure'] |
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| 95 | |
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| 96 | |
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| 97 | #Establish shortcuts to relevant quantities (for efficiency) |
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| 98 | self.rho = self.quantities['density'] |
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| 99 | self.mx = self.quantities['xmomentum'] |
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| 100 | self.my = self.quantities['ymomentum'] |
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| 101 | self.E = self.quantities['energy'] |
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| 102 | |
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| 103 | |
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| 104 | def initialise_visualiser(self,scale_z=1.0,rect=None): |
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| 105 | #Realtime visualisation |
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| 106 | if self.visualiser is None: |
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| 107 | from realtime_visualisation_new import Visualiser |
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| 108 | self.visualiser = Visualiser(self,scale_z,rect) |
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| 109 | self.visualise = True |
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| 110 | |
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| 111 | def check_integrity(self): |
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| 112 | Generic_domain.check_integrity(self) |
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| 113 | |
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| 114 | #Check that we are solving the Euler equation |
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| 115 | |
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| 116 | msg = 'First conserved quantity must be "density"' |
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| 117 | assert self.conserved_quantities[0] == 'stage', msg |
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| 118 | msg = 'Second conserved quantity must be "xmomentum"' |
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| 119 | assert self.conserved_quantities[1] == 'xmomentum', msg |
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| 120 | msg = 'Third conserved quantity must be "ymomentum"' |
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| 121 | assert self.conserved_quantities[2] == 'ymomentum', msg |
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| 122 | msg = 'Fourth conserved quantity must be "energy"' |
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| 123 | assert self.conserved_quantities[2] == 'ymomentum', msg |
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| 124 | |
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| 125 | def extrapolate_second_order_sw(self): |
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| 126 | #Call correct module function |
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| 127 | #(either from this module or C-extension) |
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| 128 | extrapolate_second_order_sw(self) |
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| 129 | |
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| 130 | def compute_fluxes(self): |
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| 131 | #Call correct module function |
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| 132 | #(either from this module or C-extension) |
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| 133 | compute_fluxes(self) |
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| 134 | |
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| 135 | def distribute_to_vertices_and_edges(self): |
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| 136 | #Call correct module function |
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| 137 | #(either from this module or C-extension) |
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| 138 | distribute_to_vertices_and_edges(self) |
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| 139 | |
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| 140 | |
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| 141 | def evolve(self, yieldstep = None, finaltime = None, |
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| 142 | skip_initial_step = False): |
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| 143 | """Specialisation of basic evolve method from parent class |
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| 144 | """ |
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| 145 | |
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| 146 | #Call check integrity here rather than from user scripts |
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| 147 | #self.check_integrity() |
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| 148 | |
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| 149 | msg = 'Parameter beta must be in the interval [0, 1[' |
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| 150 | assert 0 <= self.beta < 1.0, msg |
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| 151 | |
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| 152 | #Initial update of vertex and edge values before any storage |
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| 153 | #and or visualisation |
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| 154 | self.distribute_to_vertices_and_edges() |
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| 155 | |
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| 156 | |
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| 157 | #Initialise real time viz if requested |
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| 158 | if self.visualise is True and self.time == 0.0: |
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| 159 | |
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| 160 | import realtime_visualisation_new as visualise |
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| 161 | self.initialise_visualiser() |
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| 162 | self.visualiser.setup_all() |
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| 163 | self.visualiser.update_timer() |
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| 164 | |
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| 165 | #Store model data, e.g. for visualisation |
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| 166 | if self.store is True and self.time == 0.0: |
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| 167 | self.initialise_storage() |
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| 168 | else: |
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| 169 | pass |
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| 170 | |
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| 171 | #Call basic machinery from parent class |
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| 172 | for t in Generic_domain.evolve(self, yieldstep, finaltime, |
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| 173 | skip_initial_step): |
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| 174 | #Real time viz |
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| 175 | if self.visualise is True: |
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| 176 | self.visualiser.update_all() |
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| 177 | self.visualiser.update_timer() |
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| 178 | |
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| 179 | #Store model data, e.g. for subsequent visualisation |
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| 180 | if self.store is True: |
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| 181 | self.store_timestep(self.quantities_to_be_stored) |
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| 182 | |
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| 183 | #FIXME: Could maybe be taken from specified list |
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| 184 | #of 'store every step' quantities |
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| 185 | |
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| 186 | #Pass control on to outer loop for more specific actions |
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| 187 | yield(t) |
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| 188 | |
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| 189 | |
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| 190 | def initialise_storage(self): |
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| 191 | """ |
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| 192 | Create and initialise self.writer object for storing data. |
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| 193 | Also, save x,y and bed elevation |
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| 194 | """ |
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| 195 | |
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| 196 | import data_manager |
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| 197 | |
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| 198 | #Initialise writer |
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| 199 | self.writer = data_manager.get_dataobject(self, mode = 'w') |
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| 200 | |
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| 201 | #Store vertices and connectivity |
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| 202 | self.writer.store_connectivity() |
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| 203 | |
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| 204 | |
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| 205 | def store_timestep(self, name): |
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| 206 | """Store named quantity and time. |
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| 207 | |
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| 208 | Precondition: |
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| 209 | self.write has been initialised |
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| 210 | """ |
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| 211 | self.writer.store_timestep(name) |
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| 212 | |
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| 213 | |
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| 214 | ####################MH 090605 new extrapolation function belonging to domain class |
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| 215 | def extrapolate_second_order_sw(domain): |
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| 216 | """extrapolate conserved quntities to the vertices of the triangles |
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| 217 | Python version to be written after the C version |
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| 218 | """ |
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| 219 | msg = 'Method extrapolate_second_order_sw should be implemented in C' |
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| 220 | raise msg |
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| 221 | ####################MH 090605 ########################################### |
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| 222 | |
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| 223 | def initialise_visualiser(self,scale_z=1.0,rect=None): |
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| 224 | #Realtime visualisation |
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| 225 | if self.visualiser is None: |
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| 226 | from realtime_visualisation_new import Visualiser |
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| 227 | from Numeric import array, Float |
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| 228 | |
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| 229 | if rect is None: |
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| 230 | rect = array(self.xy_extent, Float) |
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| 231 | |
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| 232 | self.visualiser = Visualiser(self,scale_z,rect) |
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| 233 | self.visualise = True |
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| 234 | |
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| 235 | |
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| 236 | #Rotation of momentum vector |
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| 237 | def rotate(q, normal, direction = 1): |
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| 238 | """Rotate the momentum component q (q[1], q[2]) |
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| 239 | from x,y coordinates to coordinates based on normal vector. |
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| 240 | |
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| 241 | If direction is negative the rotation is inverted. |
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| 242 | |
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| 243 | Input vector is preserved |
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| 244 | |
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| 245 | This function is specific to the shallow water wave equation |
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| 246 | """ |
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| 247 | |
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| 248 | from Numeric import zeros, Float |
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| 249 | |
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| 250 | assert len(q) == 3,\ |
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| 251 | 'Vector of conserved quantities must have length 3'\ |
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| 252 | 'for 2D shallow water equation' |
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| 253 | |
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| 254 | try: |
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| 255 | l = len(normal) |
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| 256 | except: |
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| 257 | raise 'Normal vector must be an Numeric array' |
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| 258 | |
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| 259 | assert l == 2, 'Normal vector must have 2 components' |
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| 260 | |
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| 261 | |
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| 262 | n1 = normal[0] |
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| 263 | n2 = normal[1] |
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| 264 | |
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| 265 | r = zeros(len(q), Float) #Rotated quantities |
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| 266 | r[0] = q[0] #First quantity, height, is not rotated |
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| 267 | |
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| 268 | if direction == -1: |
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| 269 | n2 = -n2 |
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| 270 | |
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| 271 | |
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| 272 | r[1] = n1*q[1] + n2*q[2] |
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| 273 | r[2] = -n2*q[1] + n1*q[2] |
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| 274 | |
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| 275 | return r |
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| 276 | |
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| 277 | |
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| 278 | |
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| 279 | #################################### |
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| 280 | # Flux computation |
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| 281 | def flux_function(normal, ql, qr, zl, zr): |
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| 282 | """Compute fluxes between volumes for the shallow water wave equation |
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| 283 | cast in terms of w = h+z using the 'central scheme' as described in |
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| 284 | |
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| 285 | Kurganov, Noelle, Petrova. 'Semidiscrete Central-Upwind Schemes For |
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| 286 | Hyperbolic Conservation Laws and Hamilton-Jacobi Equations'. |
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| 287 | Siam J. Sci. Comput. Vol. 23, No. 3, pp. 707-740. |
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| 288 | |
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| 289 | The implemented formula is given in equation (3.15) on page 714 |
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| 290 | |
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| 291 | Conserved quantities w, uh, vh are stored as elements 0, 1 and 2 |
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| 292 | in the numerical vectors ql an qr. |
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| 293 | |
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| 294 | Bed elevations zl and zr. |
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| 295 | """ |
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| 296 | |
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| 297 | from config import g, epsilon |
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| 298 | from math import sqrt |
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| 299 | from Numeric import array |
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| 300 | |
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| 301 | #Align momentums with x-axis |
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| 302 | q_left = rotate(ql, normal, direction = 1) |
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| 303 | q_right = rotate(qr, normal, direction = 1) |
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| 304 | |
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| 305 | z = (zl+zr)/2 #Take average of field values |
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| 306 | |
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| 307 | w_left = q_left[0] #w=h+z |
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| 308 | h_left = w_left-z |
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| 309 | uh_left = q_left[1] |
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| 310 | |
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| 311 | if h_left < epsilon: |
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| 312 | u_left = 0.0 #Could have been negative |
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| 313 | h_left = 0.0 |
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| 314 | else: |
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| 315 | u_left = uh_left/h_left |
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| 316 | |
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| 317 | |
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| 318 | w_right = q_right[0] #w=h+z |
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| 319 | h_right = w_right-z |
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| 320 | uh_right = q_right[1] |
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| 321 | |
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| 322 | |
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| 323 | if h_right < epsilon: |
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| 324 | u_right = 0.0 #Could have been negative |
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| 325 | h_right = 0.0 |
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| 326 | else: |
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| 327 | u_right = uh_right/h_right |
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| 328 | |
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| 329 | vh_left = q_left[2] |
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| 330 | vh_right = q_right[2] |
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| 331 | |
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| 332 | soundspeed_left = sqrt(g*h_left) |
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| 333 | soundspeed_right = sqrt(g*h_right) |
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| 334 | |
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| 335 | #Maximal wave speed |
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| 336 | s_max = max(u_left+soundspeed_left, u_right+soundspeed_right, 0) |
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| 337 | |
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| 338 | #Minimal wave speed |
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| 339 | s_min = min(u_left-soundspeed_left, u_right-soundspeed_right, 0) |
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| 340 | |
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| 341 | #Flux computation |
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| 342 | |
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| 343 | #FIXME(Ole): Why is it again that we don't |
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| 344 | #use uh_left and uh_right directly in the first entries? |
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| 345 | flux_left = array([u_left*h_left, |
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| 346 | u_left*uh_left + 0.5*g*h_left**2, |
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| 347 | u_left*vh_left]) |
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| 348 | flux_right = array([u_right*h_right, |
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| 349 | u_right*uh_right + 0.5*g*h_right**2, |
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| 350 | u_right*vh_right]) |
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| 351 | |
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| 352 | denom = s_max-s_min |
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| 353 | if denom == 0.0: |
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| 354 | edgeflux = array([0.0, 0.0, 0.0]) |
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| 355 | max_speed = 0.0 |
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| 356 | else: |
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| 357 | edgeflux = (s_max*flux_left - s_min*flux_right)/denom |
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| 358 | edgeflux += s_max*s_min*(q_right-q_left)/denom |
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| 359 | |
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| 360 | edgeflux = rotate(edgeflux, normal, direction=-1) |
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| 361 | max_speed = max(abs(s_max), abs(s_min)) |
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| 362 | |
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| 363 | return edgeflux, max_speed |
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| 364 | |
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| 365 | |
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| 366 | def compute_fluxes(domain): |
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| 367 | """Compute all fluxes and the timestep suitable for all volumes |
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| 368 | in domain. |
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| 369 | |
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| 370 | Compute total flux for each conserved quantity using "flux_function" |
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| 371 | |
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| 372 | Fluxes across each edge are scaled by edgelengths and summed up |
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| 373 | Resulting flux is then scaled by area and stored in |
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| 374 | explicit_update for each of the three conserved quantities |
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| 375 | stage, xmomentum and ymomentum |
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| 376 | |
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| 377 | The maximal allowable speed computed by the flux_function for each volume |
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| 378 | is converted to a timestep that must not be exceeded. The minimum of |
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| 379 | those is computed as the next overall timestep. |
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| 380 | |
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| 381 | Post conditions: |
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| 382 | domain.explicit_update is reset to computed flux values |
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| 383 | domain.timestep is set to the largest step satisfying all volumes. |
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| 384 | """ |
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| 385 | |
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| 386 | import sys |
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| 387 | from Numeric import zeros, Float |
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| 388 | |
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| 389 | N = domain.number_of_elements |
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| 390 | |
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| 391 | #Shortcuts |
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| 392 | Stage = domain.quantities['stage'] |
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| 393 | Xmom = domain.quantities['xmomentum'] |
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| 394 | Ymom = domain.quantities['ymomentum'] |
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| 395 | Bed = domain.quantities['elevation'] |
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| 396 | |
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| 397 | #Arrays |
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| 398 | stage = Stage.edge_values |
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| 399 | xmom = Xmom.edge_values |
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| 400 | ymom = Ymom.edge_values |
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| 401 | bed = Bed.edge_values |
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| 402 | |
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| 403 | stage_bdry = Stage.boundary_values |
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| 404 | xmom_bdry = Xmom.boundary_values |
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| 405 | ymom_bdry = Ymom.boundary_values |
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| 406 | |
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| 407 | flux = zeros(3, Float) #Work array for summing up fluxes |
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| 408 | |
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| 409 | |
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| 410 | #Loop |
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| 411 | timestep = float(sys.maxint) |
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| 412 | for k in range(N): |
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| 413 | |
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| 414 | flux[:] = 0. #Reset work array |
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| 415 | for i in range(3): |
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| 416 | #Quantities inside volume facing neighbour i |
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| 417 | ql = [stage[k, i], xmom[k, i], ymom[k, i]] |
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| 418 | zl = bed[k, i] |
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| 419 | |
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| 420 | #Quantities at neighbour on nearest face |
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| 421 | n = domain.neighbours[k,i] |
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| 422 | if n < 0: |
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| 423 | m = -n-1 #Convert negative flag to index |
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| 424 | qr = [stage_bdry[m], xmom_bdry[m], ymom_bdry[m]] |
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| 425 | zr = zl #Extend bed elevation to boundary |
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| 426 | else: |
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| 427 | m = domain.neighbour_edges[k,i] |
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| 428 | qr = [stage[n, m], xmom[n, m], ymom[n, m]] |
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| 429 | zr = bed[n, m] |
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| 430 | |
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| 431 | |
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| 432 | #Outward pointing normal vector |
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| 433 | normal = domain.normals[k, 2*i:2*i+2] |
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| 434 | |
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| 435 | #Flux computation using provided function |
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| 436 | edgeflux, max_speed = flux_function(normal, ql, qr, zl, zr) |
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| 437 | flux -= edgeflux * domain.edgelengths[k,i] |
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| 438 | |
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| 439 | #Update optimal_timestep |
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| 440 | try: |
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| 441 | timestep = min(timestep, 0.5*domain.radii[k]/max_speed) |
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| 442 | except ZeroDivisionError: |
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| 443 | pass |
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| 444 | |
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| 445 | #Normalise by area and store for when all conserved |
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| 446 | #quantities get updated |
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| 447 | flux /= domain.areas[k] |
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| 448 | Stage.explicit_update[k] = flux[0] |
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| 449 | Xmom.explicit_update[k] = flux[1] |
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| 450 | Ymom.explicit_update[k] = flux[2] |
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| 451 | |
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| 452 | |
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| 453 | domain.timestep = timestep |
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| 454 | |
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| 455 | #MH090605 The following method belongs to the shallow_water domain class |
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| 456 | #see comments in the corresponding method in shallow_water_ext.c |
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| 457 | def extrapolate_second_order_sw_c(domain): |
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| 458 | """Wrapper calling C version of extrapolate_second_order_sw |
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| 459 | """ |
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| 460 | import sys |
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| 461 | from Numeric import zeros, Float |
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| 462 | |
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| 463 | N = domain.number_of_elements |
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| 464 | |
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| 465 | #Shortcuts |
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| 466 | Stage = domain.quantities['stage'] |
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| 467 | Xmom = domain.quantities['xmomentum'] |
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| 468 | Ymom = domain.quantities['ymomentum'] |
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| 469 | from shallow_water_ext import extrapolate_second_order_sw |
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| 470 | extrapolate_second_order_sw(domain,domain.surrogate_neighbours, |
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| 471 | domain.number_of_boundaries, |
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| 472 | domain.centroid_coordinates, |
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| 473 | Stage.centroid_values, |
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| 474 | Xmom.centroid_values, |
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| 475 | Ymom.centroid_values, |
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| 476 | domain.vertex_coordinates, |
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| 477 | Stage.vertex_values, |
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| 478 | Xmom.vertex_values, |
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| 479 | Ymom.vertex_values) |
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| 480 | |
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| 481 | def compute_fluxes_c(domain): |
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| 482 | """Wrapper calling C version of compute fluxes |
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| 483 | """ |
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| 484 | |
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| 485 | import sys |
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| 486 | from Numeric import zeros, Float |
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| 487 | |
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| 488 | N = domain.number_of_elements |
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| 489 | |
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| 490 | #Shortcuts |
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| 491 | Stage = domain.quantities['stage'] |
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| 492 | Xmom = domain.quantities['xmomentum'] |
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| 493 | Ymom = domain.quantities['ymomentum'] |
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| 494 | Bed = domain.quantities['elevation'] |
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| 495 | |
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| 496 | timestep = float(sys.maxint) |
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| 497 | from shallow_water_ext import compute_fluxes |
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| 498 | domain.timestep = compute_fluxes(timestep, domain.epsilon, domain.g, |
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| 499 | domain.neighbours, |
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| 500 | domain.neighbour_edges, |
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| 501 | domain.normals, |
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| 502 | domain.edgelengths, |
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| 503 | domain.radii, |
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| 504 | domain.areas, |
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| 505 | Stage.edge_values, |
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| 506 | Xmom.edge_values, |
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| 507 | Ymom.edge_values, |
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| 508 | Bed.edge_values, |
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| 509 | Stage.boundary_values, |
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| 510 | Xmom.boundary_values, |
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| 511 | Ymom.boundary_values, |
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| 512 | Stage.explicit_update, |
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| 513 | Xmom.explicit_update, |
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| 514 | Ymom.explicit_update, |
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| 515 | domain.already_computed_flux) |
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| 516 | |
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| 517 | |
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| 518 | #################################### |
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| 519 | # Module functions for gradient limiting (distribute_to_vertices_and_edges) |
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| 520 | |
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| 521 | def distribute_to_vertices_and_edges(domain): |
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| 522 | """Distribution from centroids to vertices specific to the |
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| 523 | shallow water wave |
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| 524 | equation. |
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| 525 | |
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| 526 | It will ensure that h (w-z) is always non-negative even in the |
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| 527 | presence of steep bed-slopes by taking a weighted average between shallow |
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| 528 | and deep cases. |
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| 529 | |
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| 530 | In addition, all conserved quantities get distributed as per either a |
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| 531 | constant (order==1) or a piecewise linear function (order==2). |
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| 532 | |
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| 533 | FIXME: more explanation about removal of artificial variability etc |
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| 534 | |
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| 535 | Precondition: |
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| 536 | All quantities defined at centroids and bed elevation defined at |
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| 537 | vertices. |
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| 538 | |
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| 539 | Postcondition |
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| 540 | Conserved quantities defined at vertices |
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| 541 | |
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| 542 | """ |
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| 543 | |
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| 544 | from config import optimised_gradient_limiter |
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| 545 | |
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| 546 | #Remove very thin layers of water |
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| 547 | protect_against_infinitesimal_and_negative_heights(domain) |
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| 548 | |
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| 549 | #Extrapolate all conserved quantities |
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| 550 | if optimised_gradient_limiter: |
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| 551 | #MH090605 if second order, |
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| 552 | #perform the extrapolation and limiting on |
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| 553 | #all of the conserved quantitie |
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| 554 | |
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| 555 | if (domain.order == 1): |
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| 556 | for name in domain.conserved_quantities: |
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| 557 | Q = domain.quantities[name] |
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| 558 | Q.extrapolate_first_order() |
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| 559 | elif domain.order == 2: |
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| 560 | domain.extrapolate_second_order_sw() |
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| 561 | else: |
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| 562 | raise 'Unknown order' |
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| 563 | else: |
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| 564 | #old code: |
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| 565 | for name in domain.conserved_quantities: |
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| 566 | Q = domain.quantities[name] |
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| 567 | if domain.order == 1: |
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| 568 | Q.extrapolate_first_order() |
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| 569 | elif domain.order == 2: |
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| 570 | Q.extrapolate_second_order() |
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| 571 | Q.limit() |
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| 572 | else: |
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| 573 | raise 'Unknown order' |
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| 574 | |
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| 575 | |
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| 576 | #Take bed elevation into account when water heights are small |
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| 577 | balance_deep_and_shallow(domain) |
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| 578 | |
---|
| 579 | #Compute edge values by interpolation |
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| 580 | for name in domain.conserved_quantities: |
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| 581 | Q = domain.quantities[name] |
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| 582 | Q.interpolate_from_vertices_to_edges() |
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| 583 | |
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| 584 | |
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| 585 | def protect_against_infinitesimal_and_negative_heights(domain): |
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| 586 | """Protect against infinitesimal heights and associated high velocities |
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| 587 | """ |
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| 588 | |
---|
| 589 | #Shortcuts |
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| 590 | wc = domain.quantities['stage'].centroid_values |
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| 591 | zc = domain.quantities['elevation'].centroid_values |
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| 592 | xmomc = domain.quantities['xmomentum'].centroid_values |
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| 593 | ymomc = domain.quantities['ymomentum'].centroid_values |
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| 594 | hc = wc - zc #Water depths at centroids |
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| 595 | |
---|
| 596 | #Update |
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| 597 | for k in range(domain.number_of_elements): |
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| 598 | |
---|
| 599 | if hc[k] < domain.minimum_allowed_height: |
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| 600 | #Control stage |
---|
| 601 | if hc[k] < domain.epsilon: |
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| 602 | wc[k] = zc[k] # Contain 'lost mass' error |
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| 603 | |
---|
| 604 | #Control momentum |
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| 605 | xmomc[k] = ymomc[k] = 0.0 |
---|
| 606 | |
---|
| 607 | |
---|
| 608 | def protect_against_infinitesimal_and_negative_heights_c(domain): |
---|
| 609 | """Protect against infinitesimal heights and associated high velocities |
---|
| 610 | """ |
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| 611 | |
---|
| 612 | #Shortcuts |
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| 613 | wc = domain.quantities['stage'].centroid_values |
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| 614 | zc = domain.quantities['elevation'].centroid_values |
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| 615 | xmomc = domain.quantities['xmomentum'].centroid_values |
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| 616 | ymomc = domain.quantities['ymomentum'].centroid_values |
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| 617 | |
---|
| 618 | from shallow_water_ext import protect |
---|
| 619 | |
---|
| 620 | protect(domain.minimum_allowed_height, domain.epsilon, |
---|
| 621 | wc, zc, xmomc, ymomc) |
---|
| 622 | |
---|
| 623 | |
---|
| 624 | |
---|
| 625 | def h_limiter(domain): |
---|
| 626 | """Limit slopes for each volume to eliminate artificial variance |
---|
| 627 | introduced by e.g. second order extrapolator |
---|
| 628 | |
---|
| 629 | limit on h = w-z |
---|
| 630 | |
---|
| 631 | This limiter depends on two quantities (w,z) so it resides within |
---|
| 632 | this module rather than within quantity.py |
---|
| 633 | """ |
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| 634 | |
---|
| 635 | from Numeric import zeros, Float |
---|
| 636 | |
---|
| 637 | N = domain.number_of_elements |
---|
| 638 | beta_h = domain.beta_h |
---|
| 639 | |
---|
| 640 | #Shortcuts |
---|
| 641 | wc = domain.quantities['stage'].centroid_values |
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| 642 | zc = domain.quantities['elevation'].centroid_values |
---|
| 643 | hc = wc - zc |
---|
| 644 | |
---|
| 645 | wv = domain.quantities['stage'].vertex_values |
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| 646 | zv = domain.quantities['elevation'].vertex_values |
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| 647 | hv = wv-zv |
---|
| 648 | |
---|
| 649 | hvbar = zeros(hv.shape, Float) #h-limited values |
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| 650 | |
---|
| 651 | #Find min and max of this and neighbour's centroid values |
---|
| 652 | hmax = zeros(hc.shape, Float) |
---|
| 653 | hmin = zeros(hc.shape, Float) |
---|
| 654 | |
---|
| 655 | for k in range(N): |
---|
| 656 | hmax[k] = hmin[k] = hc[k] |
---|
| 657 | for i in range(3): |
---|
| 658 | n = domain.neighbours[k,i] |
---|
| 659 | if n >= 0: |
---|
| 660 | hn = hc[n] #Neighbour's centroid value |
---|
| 661 | |
---|
| 662 | hmin[k] = min(hmin[k], hn) |
---|
| 663 | hmax[k] = max(hmax[k], hn) |
---|
| 664 | |
---|
| 665 | |
---|
| 666 | #Diffences between centroids and maxima/minima |
---|
| 667 | dhmax = hmax - hc |
---|
| 668 | dhmin = hmin - hc |
---|
| 669 | |
---|
| 670 | #Deltas between vertex and centroid values |
---|
| 671 | dh = zeros(hv.shape, Float) |
---|
| 672 | for i in range(3): |
---|
| 673 | dh[:,i] = hv[:,i] - hc |
---|
| 674 | |
---|
| 675 | #Phi limiter |
---|
| 676 | for k in range(N): |
---|
| 677 | |
---|
| 678 | #Find the gradient limiter (phi) across vertices |
---|
| 679 | phi = 1.0 |
---|
| 680 | for i in range(3): |
---|
| 681 | r = 1.0 |
---|
| 682 | if (dh[k,i] > 0): r = dhmax[k]/dh[k,i] |
---|
| 683 | if (dh[k,i] < 0): r = dhmin[k]/dh[k,i] |
---|
| 684 | |
---|
| 685 | phi = min( min(r*beta_h, 1), phi ) |
---|
| 686 | |
---|
| 687 | #Then update using phi limiter |
---|
| 688 | for i in range(3): |
---|
| 689 | hvbar[k,i] = hc[k] + phi*dh[k,i] |
---|
| 690 | |
---|
| 691 | return hvbar |
---|
| 692 | |
---|
| 693 | |
---|
| 694 | |
---|
| 695 | def h_limiter_c(domain): |
---|
| 696 | """Limit slopes for each volume to eliminate artificial variance |
---|
| 697 | introduced by e.g. second order extrapolator |
---|
| 698 | |
---|
| 699 | limit on h = w-z |
---|
| 700 | |
---|
| 701 | This limiter depends on two quantities (w,z) so it resides within |
---|
| 702 | this module rather than within quantity.py |
---|
| 703 | |
---|
| 704 | Wrapper for c-extension |
---|
| 705 | """ |
---|
| 706 | |
---|
| 707 | from Numeric import zeros, Float |
---|
| 708 | |
---|
| 709 | N = domain.number_of_elements |
---|
| 710 | beta_h = domain.beta_h |
---|
| 711 | |
---|
| 712 | #Shortcuts |
---|
| 713 | wc = domain.quantities['stage'].centroid_values |
---|
| 714 | zc = domain.quantities['elevation'].centroid_values |
---|
| 715 | hc = wc - zc |
---|
| 716 | |
---|
| 717 | wv = domain.quantities['stage'].vertex_values |
---|
| 718 | zv = domain.quantities['elevation'].vertex_values |
---|
| 719 | hv = wv - zv |
---|
| 720 | |
---|
| 721 | #Call C-extension |
---|
| 722 | from shallow_water_ext import h_limiter_sw as h_limiter |
---|
| 723 | hvbar = h_limiter(domain, hc, hv) |
---|
| 724 | |
---|
| 725 | return hvbar |
---|
| 726 | |
---|
| 727 | |
---|
| 728 | def balance_deep_and_shallow(domain): |
---|
| 729 | """Compute linear combination between stage as computed by |
---|
| 730 | gradient-limiters limiting using w, and stage computed by |
---|
| 731 | gradient-limiters limiting using h (h-limiter). |
---|
| 732 | The former takes precedence when heights are large compared to the |
---|
| 733 | bed slope while the latter takes precedence when heights are |
---|
| 734 | relatively small. Anything in between is computed as a balanced |
---|
| 735 | linear combination in order to avoid numerical disturbances which |
---|
| 736 | would otherwise appear as a result of hard switching between |
---|
| 737 | modes. |
---|
| 738 | |
---|
| 739 | The h-limiter is always applied irrespective of the order. |
---|
| 740 | """ |
---|
| 741 | |
---|
| 742 | #Shortcuts |
---|
| 743 | wc = domain.quantities['stage'].centroid_values |
---|
| 744 | zc = domain.quantities['elevation'].centroid_values |
---|
| 745 | hc = wc - zc |
---|
| 746 | |
---|
| 747 | wv = domain.quantities['stage'].vertex_values |
---|
| 748 | zv = domain.quantities['elevation'].vertex_values |
---|
| 749 | hv = wv-zv |
---|
| 750 | |
---|
| 751 | #Limit h |
---|
| 752 | hvbar = h_limiter(domain) |
---|
| 753 | |
---|
| 754 | for k in range(domain.number_of_elements): |
---|
| 755 | #Compute maximal variation in bed elevation |
---|
| 756 | # This quantitiy is |
---|
| 757 | # dz = max_i abs(z_i - z_c) |
---|
| 758 | # and it is independent of dimension |
---|
| 759 | # In the 1d case zc = (z0+z1)/2 |
---|
| 760 | # In the 2d case zc = (z0+z1+z2)/3 |
---|
| 761 | |
---|
| 762 | dz = max(abs(zv[k,0]-zc[k]), |
---|
| 763 | abs(zv[k,1]-zc[k]), |
---|
| 764 | abs(zv[k,2]-zc[k])) |
---|
| 765 | |
---|
| 766 | |
---|
| 767 | hmin = min( hv[k,:] ) |
---|
| 768 | |
---|
| 769 | #Create alpha in [0,1], where alpha==0 means using the h-limited |
---|
| 770 | #stage and alpha==1 means using the w-limited stage as |
---|
| 771 | #computed by the gradient limiter (both 1st or 2nd order) |
---|
| 772 | |
---|
| 773 | #If hmin > dz/2 then alpha = 1 and the bed will have no effect |
---|
| 774 | #If hmin < 0 then alpha = 0 reverting to constant height above bed. |
---|
| 775 | |
---|
| 776 | if dz > 0.0: |
---|
| 777 | alpha = max( min( 2*hmin/dz, 1.0), 0.0 ) |
---|
| 778 | else: |
---|
| 779 | #Flat bed |
---|
| 780 | alpha = 1.0 |
---|
| 781 | |
---|
| 782 | #Let |
---|
| 783 | # |
---|
| 784 | # wvi be the w-limited stage (wvi = zvi + hvi) |
---|
| 785 | # wvi- be the h-limited state (wvi- = zvi + hvi-) |
---|
| 786 | # |
---|
| 787 | # |
---|
| 788 | #where i=0,1,2 denotes the vertex ids |
---|
| 789 | # |
---|
| 790 | #Weighted balance between w-limited and h-limited stage is |
---|
| 791 | # |
---|
| 792 | # wvi := (1-alpha)*(zvi+hvi-) + alpha*(zvi+hvi) |
---|
| 793 | # |
---|
| 794 | #It follows that the updated wvi is |
---|
| 795 | # wvi := zvi + (1-alpha)*hvi- + alpha*hvi |
---|
| 796 | # |
---|
| 797 | # Momentum is balanced between constant and limited |
---|
| 798 | |
---|
| 799 | |
---|
| 800 | #for i in range(3): |
---|
| 801 | # wv[k,i] = zv[k,i] + hvbar[k,i] |
---|
| 802 | |
---|
| 803 | #return |
---|
| 804 | |
---|
| 805 | if alpha < 1: |
---|
| 806 | |
---|
| 807 | for i in range(3): |
---|
| 808 | wv[k,i] = zv[k,i] + (1-alpha)*hvbar[k,i] + alpha*hv[k,i] |
---|
| 809 | |
---|
| 810 | #Momentums at centroids |
---|
| 811 | xmomc = domain.quantities['xmomentum'].centroid_values |
---|
| 812 | ymomc = domain.quantities['ymomentum'].centroid_values |
---|
| 813 | |
---|
| 814 | #Momentums at vertices |
---|
| 815 | xmomv = domain.quantities['xmomentum'].vertex_values |
---|
| 816 | ymomv = domain.quantities['ymomentum'].vertex_values |
---|
| 817 | |
---|
| 818 | # Update momentum as a linear combination of |
---|
| 819 | # xmomc and ymomc (shallow) and momentum |
---|
| 820 | # from extrapolator xmomv and ymomv (deep). |
---|
| 821 | xmomv[k,:] = (1-alpha)*xmomc[k] + alpha*xmomv[k,:] |
---|
| 822 | ymomv[k,:] = (1-alpha)*ymomc[k] + alpha*ymomv[k,:] |
---|
| 823 | |
---|
| 824 | |
---|
| 825 | def balance_deep_and_shallow_c(domain): |
---|
| 826 | """Wrapper for C implementation |
---|
| 827 | """ |
---|
| 828 | |
---|
| 829 | #Shortcuts |
---|
| 830 | wc = domain.quantities['stage'].centroid_values |
---|
| 831 | zc = domain.quantities['elevation'].centroid_values |
---|
| 832 | hc = wc - zc |
---|
| 833 | |
---|
| 834 | wv = domain.quantities['stage'].vertex_values |
---|
| 835 | zv = domain.quantities['elevation'].vertex_values |
---|
| 836 | hv = wv - zv |
---|
| 837 | |
---|
| 838 | #Momentums at centroids |
---|
| 839 | xmomc = domain.quantities['xmomentum'].centroid_values |
---|
| 840 | ymomc = domain.quantities['ymomentum'].centroid_values |
---|
| 841 | |
---|
| 842 | #Momentums at vertices |
---|
| 843 | xmomv = domain.quantities['xmomentum'].vertex_values |
---|
| 844 | ymomv = domain.quantities['ymomentum'].vertex_values |
---|
| 845 | |
---|
| 846 | #Limit h |
---|
| 847 | hvbar = h_limiter(domain) |
---|
| 848 | |
---|
| 849 | #This is how one would make a first order h_limited value |
---|
| 850 | #as in the old balancer (pre 17 Feb 2005): |
---|
| 851 | #from Numeric import zeros, Float |
---|
| 852 | #hvbar = zeros( (len(hc), 3), Float) |
---|
| 853 | #for i in range(3): |
---|
| 854 | # hvbar[:,i] = hc[:] |
---|
| 855 | |
---|
| 856 | from shallow_water_ext import balance_deep_and_shallow |
---|
| 857 | balance_deep_and_shallow(wc, zc, hc, wv, zv, hv, hvbar, |
---|
| 858 | xmomc, ymomc, xmomv, ymomv) |
---|
| 859 | |
---|
| 860 | |
---|
| 861 | |
---|
| 862 | |
---|
| 863 | ############################################### |
---|
| 864 | #Boundaries - specific to the shallow water wave equation |
---|
| 865 | class Reflective_boundary(Boundary): |
---|
| 866 | """Reflective boundary returns same conserved quantities as |
---|
| 867 | those present in its neighbour volume but reflected. |
---|
| 868 | |
---|
| 869 | This class is specific to the shallow water equation as it |
---|
| 870 | works with the momentum quantities assumed to be the second |
---|
| 871 | and third conserved quantities. |
---|
| 872 | """ |
---|
| 873 | |
---|
| 874 | def __init__(self, domain = None): |
---|
| 875 | Boundary.__init__(self) |
---|
| 876 | |
---|
| 877 | if domain is None: |
---|
| 878 | msg = 'Domain must be specified for reflective boundary' |
---|
| 879 | raise msg |
---|
| 880 | |
---|
| 881 | #Handy shorthands |
---|
| 882 | self.stage = domain.quantities['stage'].edge_values |
---|
| 883 | self.xmom = domain.quantities['xmomentum'].edge_values |
---|
| 884 | self.ymom = domain.quantities['ymomentum'].edge_values |
---|
| 885 | self.normals = domain.normals |
---|
| 886 | |
---|
| 887 | from Numeric import zeros, Float |
---|
| 888 | self.conserved_quantities = zeros(3, Float) |
---|
| 889 | |
---|
| 890 | def __repr__(self): |
---|
| 891 | return 'Reflective_boundary' |
---|
| 892 | |
---|
| 893 | |
---|
| 894 | def evaluate(self, vol_id, edge_id): |
---|
| 895 | """Reflective boundaries reverses the outward momentum |
---|
| 896 | of the volume they serve. |
---|
| 897 | """ |
---|
| 898 | |
---|
| 899 | q = self.conserved_quantities |
---|
| 900 | q[0] = self.stage[vol_id, edge_id] |
---|
| 901 | q[1] = self.xmom[vol_id, edge_id] |
---|
| 902 | q[2] = self.ymom[vol_id, edge_id] |
---|
| 903 | |
---|
| 904 | normal = self.normals[vol_id, 2*edge_id:2*edge_id+2] |
---|
| 905 | |
---|
| 906 | |
---|
| 907 | r = rotate(q, normal, direction = 1) |
---|
| 908 | r[1] = -r[1] |
---|
| 909 | q = rotate(r, normal, direction = -1) |
---|
| 910 | |
---|
| 911 | return q |
---|
| 912 | |
---|
| 913 | |
---|
| 914 | |
---|
| 915 | class Transmissive_Momentum_Set_Stage_boundary(Boundary): |
---|
| 916 | """Returns same momentum conserved quantities as |
---|
| 917 | those present in its neighbour volume. Sets stage |
---|
| 918 | |
---|
| 919 | Underlying domain must be specified when boundary is instantiated |
---|
| 920 | """ |
---|
| 921 | |
---|
| 922 | def __init__(self, domain = None, function=None): |
---|
| 923 | Boundary.__init__(self) |
---|
| 924 | |
---|
| 925 | if domain is None: |
---|
| 926 | msg = 'Domain must be specified for this type boundary' |
---|
| 927 | raise msg |
---|
| 928 | |
---|
| 929 | if function is None: |
---|
| 930 | msg = 'Function must be specified for this type boundary' |
---|
| 931 | raise msg |
---|
| 932 | |
---|
| 933 | self.domain = domain |
---|
| 934 | self.function = function |
---|
| 935 | |
---|
| 936 | def __repr__(self): |
---|
| 937 | return 'Transmissive_Momentum_Set_Stage_boundary(%s)' %self.domain |
---|
| 938 | |
---|
| 939 | def evaluate(self, vol_id, edge_id): |
---|
| 940 | """Transmissive Momentum Set Stage boundaries return the edge momentum |
---|
| 941 | values of the volume they serve. |
---|
| 942 | """ |
---|
| 943 | |
---|
| 944 | q = self.domain.get_conserved_quantities(vol_id, edge = edge_id) |
---|
| 945 | value = self.function(self.domain.time) |
---|
| 946 | q[0] = value[0] |
---|
| 947 | return q |
---|
| 948 | |
---|
| 949 | |
---|
| 950 | #FIXME: Consider this (taken from File_boundary) to allow |
---|
| 951 | #spatial variation |
---|
| 952 | #if vol_id is not None and edge_id is not None: |
---|
| 953 | # i = self.boundary_indices[ vol_id, edge_id ] |
---|
| 954 | # return self.F(t, point_id = i) |
---|
| 955 | #else: |
---|
| 956 | # return self.F(t) |
---|
| 957 | |
---|
| 958 | |
---|
| 959 | |
---|
| 960 | class Dirichlet_Discharge_boundary(Boundary): |
---|
| 961 | """Sets stage (h0) - FIXME: Should we use w0? |
---|
| 962 | Sets momentum (wh0) in the inward normal direction. |
---|
| 963 | |
---|
| 964 | Underlying domain must be specified when boundary is instantiated |
---|
| 965 | """ |
---|
| 966 | |
---|
| 967 | def __init__(self, domain = None, h0=None, wh0=None): |
---|
| 968 | Boundary.__init__(self) |
---|
| 969 | |
---|
| 970 | if domain is None: |
---|
| 971 | msg = 'Domain must be specified for this type boundary' |
---|
| 972 | raise msg |
---|
| 973 | |
---|
| 974 | if h0 is None: |
---|
| 975 | h0 = 0.0 |
---|
| 976 | |
---|
| 977 | if wh0 is None: |
---|
| 978 | wh0 = 0.0 |
---|
| 979 | |
---|
| 980 | self.domain = domain |
---|
| 981 | self.h0 = h0 |
---|
| 982 | self.wh0 = wh0 |
---|
| 983 | |
---|
| 984 | def __repr__(self): |
---|
| 985 | return 'Dirichlet_Discharge_boundary(%s)' %self.domain |
---|
| 986 | |
---|
| 987 | def evaluate(self, vol_id, edge_id): |
---|
| 988 | """Set discharge in the (inward) normal direction |
---|
| 989 | """ |
---|
| 990 | |
---|
| 991 | normal = self.domain.get_normal(vol_id,edge_id) |
---|
| 992 | q = [self.h0, -self.wh0*normal[0], -self.wh0*normal[1]] |
---|
| 993 | return q |
---|
| 994 | |
---|
| 995 | |
---|
| 996 | #FIXME: Consider this (taken from File_boundary) to allow |
---|
| 997 | #spatial variation |
---|
| 998 | #if vol_id is not None and edge_id is not None: |
---|
| 999 | # i = self.boundary_indices[ vol_id, edge_id ] |
---|
| 1000 | # return self.F(t, point_id = i) |
---|
| 1001 | #else: |
---|
| 1002 | # return self.F(t) |
---|
| 1003 | |
---|
| 1004 | |
---|
| 1005 | |
---|
| 1006 | #class Spatio_temporal_boundary(Boundary): |
---|
| 1007 | # """The spatio-temporal boundary, reads values for the conserved |
---|
| 1008 | # quantities from an sww NetCDF file, and returns interpolated values |
---|
| 1009 | # at the midpoints of each associated boundaty segment. |
---|
| 1010 | # Time dependency is interpolated linearly as in util.File_function.# |
---|
| 1011 | # |
---|
| 1012 | # Example: |
---|
| 1013 | # Bf = Spatio_temporal_boundary('source_file.sww', domain) |
---|
| 1014 | # |
---|
| 1015 | # """ |
---|
| 1016 | Spatio_temporal_boundary = File_boundary |
---|
| 1017 | |
---|
| 1018 | |
---|
| 1019 | |
---|
| 1020 | |
---|
| 1021 | ######################### |
---|
| 1022 | #Standard forcing terms: |
---|
| 1023 | # |
---|
| 1024 | def gravity(domain): |
---|
| 1025 | """Apply gravitational pull in the presence of bed slope |
---|
| 1026 | """ |
---|
| 1027 | |
---|
| 1028 | from util import gradient |
---|
| 1029 | from Numeric import zeros, Float, array, sum |
---|
| 1030 | |
---|
| 1031 | xmom = domain.quantities['xmomentum'].explicit_update |
---|
| 1032 | ymom = domain.quantities['ymomentum'].explicit_update |
---|
| 1033 | |
---|
| 1034 | Stage = domain.quantities['stage'] |
---|
| 1035 | Elevation = domain.quantities['elevation'] |
---|
| 1036 | h = Stage.edge_values - Elevation.edge_values |
---|
| 1037 | v = Elevation.vertex_values |
---|
| 1038 | |
---|
| 1039 | x = domain.get_vertex_coordinates() |
---|
| 1040 | g = domain.g |
---|
| 1041 | |
---|
| 1042 | for k in range(domain.number_of_elements): |
---|
| 1043 | avg_h = sum( h[k,:] )/3 |
---|
| 1044 | |
---|
| 1045 | #Compute bed slope |
---|
| 1046 | x0, y0, x1, y1, x2, y2 = x[k,:] |
---|
| 1047 | z0, z1, z2 = v[k,:] |
---|
| 1048 | |
---|
| 1049 | zx, zy = gradient(x0, y0, x1, y1, x2, y2, z0, z1, z2) |
---|
| 1050 | |
---|
| 1051 | #Update momentum |
---|
| 1052 | xmom[k] += -g*zx*avg_h |
---|
| 1053 | ymom[k] += -g*zy*avg_h |
---|
| 1054 | |
---|
| 1055 | |
---|
| 1056 | def gravity_c(domain): |
---|
| 1057 | """Wrapper calling C version |
---|
| 1058 | """ |
---|
| 1059 | |
---|
| 1060 | xmom = domain.quantities['xmomentum'].explicit_update |
---|
| 1061 | ymom = domain.quantities['ymomentum'].explicit_update |
---|
| 1062 | |
---|
| 1063 | Stage = domain.quantities['stage'] |
---|
| 1064 | Elevation = domain.quantities['elevation'] |
---|
| 1065 | h = Stage.edge_values - Elevation.edge_values |
---|
| 1066 | v = Elevation.vertex_values |
---|
| 1067 | |
---|
| 1068 | x = domain.get_vertex_coordinates() |
---|
| 1069 | g = domain.g |
---|
| 1070 | |
---|
| 1071 | |
---|
| 1072 | from shallow_water_ext import gravity |
---|
| 1073 | gravity(g, h, v, x, xmom, ymom) |
---|
| 1074 | |
---|
| 1075 | |
---|
| 1076 | def manning_friction(domain): |
---|
| 1077 | """Apply (Manning) friction to water momentum |
---|
| 1078 | """ |
---|
| 1079 | |
---|
| 1080 | from math import sqrt |
---|
| 1081 | |
---|
| 1082 | w = domain.quantities['stage'].centroid_values |
---|
| 1083 | z = domain.quantities['elevation'].centroid_values |
---|
| 1084 | h = w-z |
---|
| 1085 | |
---|
| 1086 | uh = domain.quantities['xmomentum'].centroid_values |
---|
| 1087 | vh = domain.quantities['ymomentum'].centroid_values |
---|
| 1088 | eta = domain.quantities['friction'].centroid_values |
---|
| 1089 | |
---|
| 1090 | xmom_update = domain.quantities['xmomentum'].semi_implicit_update |
---|
| 1091 | ymom_update = domain.quantities['ymomentum'].semi_implicit_update |
---|
| 1092 | |
---|
| 1093 | N = domain.number_of_elements |
---|
| 1094 | eps = domain.minimum_allowed_height |
---|
| 1095 | g = domain.g |
---|
| 1096 | |
---|
| 1097 | for k in range(N): |
---|
| 1098 | if eta[k] >= eps: |
---|
| 1099 | if h[k] >= eps: |
---|
| 1100 | S = -g * eta[k]**2 * sqrt((uh[k]**2 + vh[k]**2)) |
---|
| 1101 | S /= h[k]**(7.0/3) |
---|
| 1102 | |
---|
| 1103 | #Update momentum |
---|
| 1104 | xmom_update[k] += S*uh[k] |
---|
| 1105 | ymom_update[k] += S*vh[k] |
---|
| 1106 | |
---|
| 1107 | |
---|
| 1108 | def manning_friction_c(domain): |
---|
| 1109 | """Wrapper for c version |
---|
| 1110 | """ |
---|
| 1111 | |
---|
| 1112 | |
---|
| 1113 | xmom = domain.quantities['xmomentum'] |
---|
| 1114 | ymom = domain.quantities['ymomentum'] |
---|
| 1115 | |
---|
| 1116 | w = domain.quantities['stage'].centroid_values |
---|
| 1117 | z = domain.quantities['elevation'].centroid_values |
---|
| 1118 | |
---|
| 1119 | uh = xmom.centroid_values |
---|
| 1120 | vh = ymom.centroid_values |
---|
| 1121 | eta = domain.quantities['friction'].centroid_values |
---|
| 1122 | |
---|
| 1123 | xmom_update = xmom.semi_implicit_update |
---|
| 1124 | ymom_update = ymom.semi_implicit_update |
---|
| 1125 | |
---|
| 1126 | N = domain.number_of_elements |
---|
| 1127 | eps = domain.minimum_allowed_height |
---|
| 1128 | g = domain.g |
---|
| 1129 | |
---|
| 1130 | from shallow_water_ext import manning_friction |
---|
| 1131 | manning_friction(g, eps, w, z, uh, vh, eta, xmom_update, ymom_update) |
---|
| 1132 | |
---|
| 1133 | |
---|
| 1134 | def linear_friction(domain): |
---|
| 1135 | """Apply linear friction to water momentum |
---|
| 1136 | |
---|
| 1137 | Assumes quantity: 'linear_friction' to be present |
---|
| 1138 | """ |
---|
| 1139 | |
---|
| 1140 | from math import sqrt |
---|
| 1141 | |
---|
| 1142 | w = domain.quantities['stage'].centroid_values |
---|
| 1143 | z = domain.quantities['elevation'].centroid_values |
---|
| 1144 | h = w-z |
---|
| 1145 | |
---|
| 1146 | uh = domain.quantities['xmomentum'].centroid_values |
---|
| 1147 | vh = domain.quantities['ymomentum'].centroid_values |
---|
| 1148 | tau = domain.quantities['linear_friction'].centroid_values |
---|
| 1149 | |
---|
| 1150 | xmom_update = domain.quantities['xmomentum'].semi_implicit_update |
---|
| 1151 | ymom_update = domain.quantities['ymomentum'].semi_implicit_update |
---|
| 1152 | |
---|
| 1153 | N = domain.number_of_elements |
---|
| 1154 | eps = domain.minimum_allowed_height |
---|
| 1155 | g = domain.g #Not necessary? Why was this added? |
---|
| 1156 | |
---|
| 1157 | for k in range(N): |
---|
| 1158 | if tau[k] >= eps: |
---|
| 1159 | if h[k] >= eps: |
---|
| 1160 | S = -tau[k]/h[k] |
---|
| 1161 | |
---|
| 1162 | #Update momentum |
---|
| 1163 | xmom_update[k] += S*uh[k] |
---|
| 1164 | ymom_update[k] += S*vh[k] |
---|
| 1165 | |
---|
| 1166 | |
---|
| 1167 | |
---|
| 1168 | def check_forcefield(f): |
---|
| 1169 | """Check that f is either |
---|
| 1170 | 1: a callable object f(t,x,y), where x and y are vectors |
---|
| 1171 | and that it returns an array or a list of same length |
---|
| 1172 | as x and y |
---|
| 1173 | 2: a scalar |
---|
| 1174 | """ |
---|
| 1175 | |
---|
| 1176 | from Numeric import ones, Float, array |
---|
| 1177 | |
---|
| 1178 | |
---|
| 1179 | if callable(f): |
---|
| 1180 | N = 3 |
---|
| 1181 | x = ones(3, Float) |
---|
| 1182 | y = ones(3, Float) |
---|
| 1183 | try: |
---|
| 1184 | q = f(1.0, x=x, y=y) |
---|
| 1185 | except Exception, e: |
---|
| 1186 | msg = 'Function %s could not be executed:\n%s' %(f, e) |
---|
| 1187 | #FIXME: Reconsider this semantics |
---|
| 1188 | raise msg |
---|
| 1189 | |
---|
| 1190 | try: |
---|
| 1191 | q = array(q).astype(Float) |
---|
| 1192 | except: |
---|
| 1193 | msg = 'Return value from vector function %s could ' %f |
---|
| 1194 | msg += 'not be converted into a Numeric array of floats.\n' |
---|
| 1195 | msg += 'Specified function should return either list or array.' |
---|
| 1196 | raise msg |
---|
| 1197 | |
---|
| 1198 | #Is this really what we want? |
---|
| 1199 | msg = 'Return vector from function %s ' %f |
---|
| 1200 | msg += 'must have same lenght as input vectors' |
---|
| 1201 | assert len(q) == N, msg |
---|
| 1202 | |
---|
| 1203 | else: |
---|
| 1204 | try: |
---|
| 1205 | f = float(f) |
---|
| 1206 | except: |
---|
| 1207 | msg = 'Force field %s must be either a scalar' %f |
---|
| 1208 | msg += ' or a vector function' |
---|
| 1209 | raise msg |
---|
| 1210 | return f |
---|
| 1211 | |
---|
| 1212 | |
---|
| 1213 | class Wind_stress: |
---|
| 1214 | """Apply wind stress to water momentum in terms of |
---|
| 1215 | wind speed [m/s] and wind direction [degrees] |
---|
| 1216 | """ |
---|
| 1217 | |
---|
| 1218 | def __init__(self, *args, **kwargs): |
---|
| 1219 | """Initialise windfield from wind speed s [m/s] |
---|
| 1220 | and wind direction phi [degrees] |
---|
| 1221 | |
---|
| 1222 | Inputs v and phi can be either scalars or Python functions, e.g. |
---|
| 1223 | |
---|
| 1224 | W = Wind_stress(10, 178) |
---|
| 1225 | |
---|
| 1226 | #FIXME - 'normal' degrees are assumed for now, i.e. the |
---|
| 1227 | vector (1,0) has zero degrees. |
---|
| 1228 | We may need to convert from 'compass' degrees later on and also |
---|
| 1229 | map from True north to grid north. |
---|
| 1230 | |
---|
| 1231 | Arguments can also be Python functions of t,x,y as in |
---|
| 1232 | |
---|
| 1233 | def speed(t,x,y): |
---|
| 1234 | ... |
---|
| 1235 | return s |
---|
| 1236 | |
---|
| 1237 | def angle(t,x,y): |
---|
| 1238 | ... |
---|
| 1239 | return phi |
---|
| 1240 | |
---|
| 1241 | where x and y are vectors. |
---|
| 1242 | |
---|
| 1243 | and then pass the functions in |
---|
| 1244 | |
---|
| 1245 | W = Wind_stress(speed, angle) |
---|
| 1246 | |
---|
| 1247 | The instantiated object W can be appended to the list of |
---|
| 1248 | forcing_terms as in |
---|
| 1249 | |
---|
| 1250 | Alternatively, one vector valued function for (speed, angle) |
---|
| 1251 | can be applied, providing both quantities simultaneously. |
---|
| 1252 | As in |
---|
| 1253 | W = Wind_stress(F), where returns (speed, angle) for each t. |
---|
| 1254 | |
---|
| 1255 | domain.forcing_terms.append(W) |
---|
| 1256 | """ |
---|
| 1257 | |
---|
| 1258 | from config import rho_a, rho_w, eta_w |
---|
| 1259 | from Numeric import array, Float |
---|
| 1260 | |
---|
| 1261 | if len(args) == 2: |
---|
| 1262 | s = args[0] |
---|
| 1263 | phi = args[1] |
---|
| 1264 | elif len(args) == 1: |
---|
| 1265 | #Assume vector function returning (s, phi)(t,x,y) |
---|
| 1266 | vector_function = args[0] |
---|
| 1267 | s = lambda t,x,y: vector_function(t,x=x,y=y)[0] |
---|
| 1268 | phi = lambda t,x,y: vector_function(t,x=x,y=y)[1] |
---|
| 1269 | else: |
---|
| 1270 | #Assume info is in 2 keyword arguments |
---|
| 1271 | |
---|
| 1272 | if len(kwargs) == 2: |
---|
| 1273 | s = kwargs['s'] |
---|
| 1274 | phi = kwargs['phi'] |
---|
| 1275 | else: |
---|
| 1276 | raise 'Assumes two keyword arguments: s=..., phi=....' |
---|
| 1277 | |
---|
| 1278 | self.speed = check_forcefield(s) |
---|
| 1279 | self.phi = check_forcefield(phi) |
---|
| 1280 | |
---|
| 1281 | self.const = eta_w*rho_a/rho_w |
---|
| 1282 | |
---|
| 1283 | |
---|
| 1284 | def __call__(self, domain): |
---|
| 1285 | """Evaluate windfield based on values found in domain |
---|
| 1286 | """ |
---|
| 1287 | |
---|
| 1288 | from math import pi, cos, sin, sqrt |
---|
| 1289 | from Numeric import Float, ones, ArrayType |
---|
| 1290 | |
---|
| 1291 | xmom_update = domain.quantities['xmomentum'].explicit_update |
---|
| 1292 | ymom_update = domain.quantities['ymomentum'].explicit_update |
---|
| 1293 | |
---|
| 1294 | N = domain.number_of_elements |
---|
| 1295 | t = domain.time |
---|
| 1296 | |
---|
| 1297 | if callable(self.speed): |
---|
| 1298 | xc = domain.get_centroid_coordinates() |
---|
| 1299 | s_vec = self.speed(t, xc[:,0], xc[:,1]) |
---|
| 1300 | else: |
---|
| 1301 | #Assume s is a scalar |
---|
| 1302 | |
---|
| 1303 | try: |
---|
| 1304 | s_vec = self.speed * ones(N, Float) |
---|
| 1305 | except: |
---|
| 1306 | msg = 'Speed must be either callable or a scalar: %s' %self.s |
---|
| 1307 | raise msg |
---|
| 1308 | |
---|
| 1309 | |
---|
| 1310 | if callable(self.phi): |
---|
| 1311 | xc = domain.get_centroid_coordinates() |
---|
| 1312 | phi_vec = self.phi(t, xc[:,0], xc[:,1]) |
---|
| 1313 | else: |
---|
| 1314 | #Assume phi is a scalar |
---|
| 1315 | |
---|
| 1316 | try: |
---|
| 1317 | phi_vec = self.phi * ones(N, Float) |
---|
| 1318 | except: |
---|
| 1319 | msg = 'Angle must be either callable or a scalar: %s' %self.phi |
---|
| 1320 | raise msg |
---|
| 1321 | |
---|
| 1322 | assign_windfield_values(xmom_update, ymom_update, |
---|
| 1323 | s_vec, phi_vec, self.const) |
---|
| 1324 | |
---|
| 1325 | |
---|
| 1326 | def assign_windfield_values(xmom_update, ymom_update, |
---|
| 1327 | s_vec, phi_vec, const): |
---|
| 1328 | """Python version of assigning wind field to update vectors. |
---|
| 1329 | A c version also exists (for speed) |
---|
| 1330 | """ |
---|
| 1331 | from math import pi, cos, sin, sqrt |
---|
| 1332 | |
---|
| 1333 | N = len(s_vec) |
---|
| 1334 | for k in range(N): |
---|
| 1335 | s = s_vec[k] |
---|
| 1336 | phi = phi_vec[k] |
---|
| 1337 | |
---|
| 1338 | #Convert to radians |
---|
| 1339 | phi = phi*pi/180 |
---|
| 1340 | |
---|
| 1341 | #Compute velocity vector (u, v) |
---|
| 1342 | u = s*cos(phi) |
---|
| 1343 | v = s*sin(phi) |
---|
| 1344 | |
---|
| 1345 | #Compute wind stress |
---|
| 1346 | S = const * sqrt(u**2 + v**2) |
---|
| 1347 | xmom_update[k] += S*u |
---|
| 1348 | ymom_update[k] += S*v |
---|
| 1349 | |
---|
| 1350 | |
---|
| 1351 | |
---|
| 1352 | ############################## |
---|
| 1353 | #OBSOLETE STUFF |
---|
| 1354 | |
---|
| 1355 | def balance_deep_and_shallow_old(domain): |
---|
| 1356 | """Compute linear combination between stage as computed by |
---|
| 1357 | gradient-limiters and stage computed as constant height above bed. |
---|
| 1358 | The former takes precedence when heights are large compared to the |
---|
| 1359 | bed slope while the latter takes precedence when heights are |
---|
| 1360 | relatively small. Anything in between is computed as a balanced |
---|
| 1361 | linear combination in order to avoid numerical disturbances which |
---|
| 1362 | would otherwise appear as a result of hard switching between |
---|
| 1363 | modes. |
---|
| 1364 | """ |
---|
| 1365 | |
---|
| 1366 | #OBSOLETE |
---|
| 1367 | |
---|
| 1368 | #Shortcuts |
---|
| 1369 | wc = domain.quantities['stage'].centroid_values |
---|
| 1370 | zc = domain.quantities['elevation'].centroid_values |
---|
| 1371 | hc = wc - zc |
---|
| 1372 | |
---|
| 1373 | wv = domain.quantities['stage'].vertex_values |
---|
| 1374 | zv = domain.quantities['elevation'].vertex_values |
---|
| 1375 | hv = wv-zv |
---|
| 1376 | |
---|
| 1377 | |
---|
| 1378 | #Computed linear combination between constant stages and and |
---|
| 1379 | #stages parallel to the bed elevation. |
---|
| 1380 | for k in range(domain.number_of_elements): |
---|
| 1381 | #Compute maximal variation in bed elevation |
---|
| 1382 | # This quantitiy is |
---|
| 1383 | # dz = max_i abs(z_i - z_c) |
---|
| 1384 | # and it is independent of dimension |
---|
| 1385 | # In the 1d case zc = (z0+z1)/2 |
---|
| 1386 | # In the 2d case zc = (z0+z1+z2)/3 |
---|
| 1387 | |
---|
| 1388 | dz = max(abs(zv[k,0]-zc[k]), |
---|
| 1389 | abs(zv[k,1]-zc[k]), |
---|
| 1390 | abs(zv[k,2]-zc[k])) |
---|
| 1391 | |
---|
| 1392 | |
---|
| 1393 | hmin = min( hv[k,:] ) |
---|
| 1394 | |
---|
| 1395 | #Create alpha in [0,1], where alpha==0 means using shallow |
---|
| 1396 | #first order scheme and alpha==1 means using the stage w as |
---|
| 1397 | #computed by the gradient limiter (1st or 2nd order) |
---|
| 1398 | # |
---|
| 1399 | #If hmin > dz/2 then alpha = 1 and the bed will have no effect |
---|
| 1400 | #If hmin < 0 then alpha = 0 reverting to constant height above bed. |
---|
| 1401 | |
---|
| 1402 | if dz > 0.0: |
---|
| 1403 | alpha = max( min( 2*hmin/dz, 1.0), 0.0 ) |
---|
| 1404 | else: |
---|
| 1405 | #Flat bed |
---|
| 1406 | alpha = 1.0 |
---|
| 1407 | |
---|
| 1408 | #Weighted balance between stage parallel to bed elevation |
---|
| 1409 | #(wvi = zvi + hc) and stage as computed by 1st or 2nd |
---|
| 1410 | #order gradient limiter |
---|
| 1411 | #(wvi = zvi + hvi) where i=0,1,2 denotes the vertex ids |
---|
| 1412 | # |
---|
| 1413 | #It follows that the updated wvi is |
---|
| 1414 | # wvi := (1-alpha)*(zvi+hc) + alpha*(zvi+hvi) = |
---|
| 1415 | # zvi + hc + alpha*(hvi - hc) |
---|
| 1416 | # |
---|
| 1417 | #Note that hvi = zc+hc-zvi in the first order case (constant). |
---|
| 1418 | |
---|
| 1419 | if alpha < 1: |
---|
| 1420 | for i in range(3): |
---|
| 1421 | wv[k,i] = zv[k,i] + hc[k] + alpha*(hv[k,i]-hc[k]) |
---|
| 1422 | |
---|
| 1423 | |
---|
| 1424 | #Momentums at centroids |
---|
| 1425 | xmomc = domain.quantities['xmomentum'].centroid_values |
---|
| 1426 | ymomc = domain.quantities['ymomentum'].centroid_values |
---|
| 1427 | |
---|
| 1428 | #Momentums at vertices |
---|
| 1429 | xmomv = domain.quantities['xmomentum'].vertex_values |
---|
| 1430 | ymomv = domain.quantities['ymomentum'].vertex_values |
---|
| 1431 | |
---|
| 1432 | # Update momentum as a linear combination of |
---|
| 1433 | # xmomc and ymomc (shallow) and momentum |
---|
| 1434 | # from extrapolator xmomv and ymomv (deep). |
---|
| 1435 | xmomv[k,:] = (1-alpha)*xmomc[k] + alpha*xmomv[k,:] |
---|
| 1436 | ymomv[k,:] = (1-alpha)*ymomc[k] + alpha*ymomv[k,:] |
---|
| 1437 | |
---|
| 1438 | |
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| 1439 | |
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| 1440 | |
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| 1441 | |
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| 1442 | ########################### |
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| 1443 | ########################### |
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| 1444 | #Geometries |
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| 1445 | |
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| 1446 | |
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| 1447 | #FIXME: Rethink this way of creating values. |
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| 1448 | |
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| 1449 | |
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| 1450 | class Weir: |
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| 1451 | """Set a bathymetry for weir with a hole and a downstream gutter |
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| 1452 | x,y are assumed to be in the unit square |
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| 1453 | """ |
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| 1454 | |
---|
| 1455 | def __init__(self, stage): |
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| 1456 | self.inflow_stage = stage |
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| 1457 | |
---|
| 1458 | def __call__(self, x, y): |
---|
| 1459 | from Numeric import zeros, Float |
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| 1460 | from math import sqrt |
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| 1461 | |
---|
| 1462 | N = len(x) |
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| 1463 | assert N == len(y) |
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| 1464 | |
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| 1465 | z = zeros(N, Float) |
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| 1466 | for i in range(N): |
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| 1467 | z[i] = -x[i]/2 #General slope |
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| 1468 | |
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| 1469 | #Flattish bit to the left |
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| 1470 | if x[i] < 0.3: |
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| 1471 | z[i] = -x[i]/10 |
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| 1472 | |
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| 1473 | #Weir |
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| 1474 | if x[i] >= 0.3 and x[i] < 0.4: |
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| 1475 | z[i] = -x[i]+0.9 |
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| 1476 | |
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| 1477 | #Dip |
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| 1478 | x0 = 0.6 |
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| 1479 | #depth = -1.3 |
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| 1480 | depth = -1.0 |
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| 1481 | #plateaux = -0.9 |
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| 1482 | plateaux = -0.6 |
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| 1483 | if y[i] < 0.7: |
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| 1484 | if x[i] > x0 and x[i] < 0.9: |
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| 1485 | z[i] = depth |
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| 1486 | |
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| 1487 | #RHS plateaux |
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| 1488 | if x[i] >= 0.9: |
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| 1489 | z[i] = plateaux |
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| 1490 | |
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| 1491 | |
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| 1492 | elif y[i] >= 0.7 and y[i] < 1.5: |
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| 1493 | #Restrict and deepen |
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| 1494 | if x[i] >= x0 and x[i] < 0.8: |
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| 1495 | z[i] = depth-(y[i]/3-0.3) |
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| 1496 | #z[i] = depth-y[i]/5 |
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| 1497 | #z[i] = depth |
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| 1498 | elif x[i] >= 0.8: |
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| 1499 | #RHS plateaux |
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| 1500 | z[i] = plateaux |
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| 1501 | |
---|
| 1502 | elif y[i] >= 1.5: |
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| 1503 | if x[i] >= x0 and x[i] < 0.8 + (y[i]-1.5)/1.2: |
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| 1504 | #Widen up and stay at constant depth |
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| 1505 | z[i] = depth-1.5/5 |
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| 1506 | elif x[i] >= 0.8 + (y[i]-1.5)/1.2: |
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| 1507 | #RHS plateaux |
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| 1508 | z[i] = plateaux |
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| 1509 | |
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| 1510 | |
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| 1511 | #Hole in weir (slightly higher than inflow condition) |
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| 1512 | if x[i] >= 0.3 and x[i] < 0.4 and y[i] > 0.2 and y[i] < 0.4: |
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| 1513 | z[i] = -x[i]+self.inflow_stage + 0.02 |
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| 1514 | |
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| 1515 | #Channel behind weir |
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| 1516 | x0 = 0.5 |
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| 1517 | if x[i] >= 0.4 and x[i] < x0 and y[i] > 0.2 and y[i] < 0.4: |
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| 1518 | z[i] = -x[i]+self.inflow_stage + 0.02 |
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| 1519 | |
---|
| 1520 | if x[i] >= x0 and x[i] < 0.6 and y[i] > 0.2 and y[i] < 0.4: |
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| 1521 | #Flatten it out towards the end |
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| 1522 | z[i] = -x0+self.inflow_stage + 0.02 + (x0-x[i])/5 |
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| 1523 | |
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| 1524 | #Hole to the east |
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| 1525 | x0 = 1.1; y0 = 0.35 |
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| 1526 | #if x[i] < -0.2 and y < 0.5: |
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| 1527 | if sqrt((2*(x[i]-x0))**2 + (2*(y[i]-y0))**2) < 0.2: |
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| 1528 | z[i] = sqrt(((x[i]-x0))**2 + ((y[i]-y0))**2)-1.0 |
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| 1529 | |
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| 1530 | #Tiny channel draining hole |
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| 1531 | if x[i] >= 1.14 and x[i] < 1.2 and y[i] >= 0.4 and y[i] < 0.6: |
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| 1532 | z[i] = -0.9 #North south |
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| 1533 | |
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| 1534 | if x[i] >= 0.9 and x[i] < 1.18 and y[i] >= 0.58 and y[i] < 0.65: |
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| 1535 | z[i] = -1.0 + (x[i]-0.9)/3 #East west |
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| 1536 | |
---|
| 1537 | |
---|
| 1538 | |
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| 1539 | #Stuff not in use |
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| 1540 | |
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| 1541 | #Upward slope at inlet to the north west |
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| 1542 | #if x[i] < 0.0: # and y[i] > 0.5: |
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| 1543 | # #z[i] = -y[i]+0.5 #-x[i]/2 |
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| 1544 | # z[i] = x[i]/4 - y[i]**2 + 0.5 |
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| 1545 | |
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| 1546 | #Hole to the west |
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| 1547 | #x0 = -0.4; y0 = 0.35 # center |
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| 1548 | #if sqrt((2*(x[i]-x0))**2 + (2*(y[i]-y0))**2) < 0.2: |
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| 1549 | # z[i] = sqrt(((x[i]-x0))**2 + ((y[i]-y0))**2)-0.2 |
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| 1550 | |
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| 1551 | |
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| 1552 | |
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| 1553 | |
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| 1554 | |
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| 1555 | return z/2 |
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| 1556 | |
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| 1557 | class Weir_simple: |
---|
| 1558 | """Set a bathymetry for weir with a hole and a downstream gutter |
---|
| 1559 | x,y are assumed to be in the unit square |
---|
| 1560 | """ |
---|
| 1561 | |
---|
| 1562 | def __init__(self, stage): |
---|
| 1563 | self.inflow_stage = stage |
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| 1564 | |
---|
| 1565 | def __call__(self, x, y): |
---|
| 1566 | from Numeric import zeros, Float |
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| 1567 | |
---|
| 1568 | N = len(x) |
---|
| 1569 | assert N == len(y) |
---|
| 1570 | |
---|
| 1571 | z = zeros(N, Float) |
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| 1572 | for i in range(N): |
---|
| 1573 | z[i] = -x[i] #General slope |
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| 1574 | |
---|
| 1575 | #Flat bit to the left |
---|
| 1576 | if x[i] < 0.3: |
---|
| 1577 | z[i] = -x[i]/10 #General slope |
---|
| 1578 | |
---|
| 1579 | #Weir |
---|
| 1580 | if x[i] > 0.3 and x[i] < 0.4: |
---|
| 1581 | z[i] = -x[i]+0.9 |
---|
| 1582 | |
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| 1583 | #Dip |
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| 1584 | if x[i] > 0.6 and x[i] < 0.9: |
---|
| 1585 | z[i] = -x[i]-0.5 #-y[i]/5 |
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| 1586 | |
---|
| 1587 | #Hole in weir (slightly higher than inflow condition) |
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| 1588 | if x[i] > 0.3 and x[i] < 0.4 and y[i] > 0.2 and y[i] < 0.4: |
---|
| 1589 | z[i] = -x[i]+self.inflow_stage + 0.05 |
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| 1590 | |
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| 1591 | |
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| 1592 | return z/2 |
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| 1593 | |
---|
| 1594 | |
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| 1595 | |
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| 1596 | class Constant_stage: |
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| 1597 | """Set an initial condition with constant stage |
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| 1598 | """ |
---|
| 1599 | def __init__(self, s): |
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| 1600 | self.s = s |
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| 1601 | |
---|
| 1602 | def __call__(self, x, y): |
---|
| 1603 | return self.s |
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| 1604 | |
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| 1605 | class Constant_height: |
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| 1606 | """Set an initial condition with constant water height, e.g |
---|
| 1607 | stage s = z+h |
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| 1608 | """ |
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| 1609 | |
---|
| 1610 | def __init__(self, W, h): |
---|
| 1611 | self.W = W |
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| 1612 | self.h = h |
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| 1613 | |
---|
| 1614 | def __call__(self, x, y): |
---|
| 1615 | if self.W is None: |
---|
| 1616 | from Numeric import ones, Float |
---|
| 1617 | return self.h*ones(len(x), Float) |
---|
| 1618 | else: |
---|
| 1619 | return self.W(x,y) + self.h |
---|
| 1620 | |
---|
| 1621 | |
---|
| 1622 | |
---|
| 1623 | |
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| 1624 | def compute_fluxes_python(domain): |
---|
| 1625 | """Compute all fluxes and the timestep suitable for all volumes |
---|
| 1626 | in domain. |
---|
| 1627 | |
---|
| 1628 | Compute total flux for each conserved quantity using "flux_function" |
---|
| 1629 | |
---|
| 1630 | Fluxes across each edge are scaled by edgelengths and summed up |
---|
| 1631 | Resulting flux is then scaled by area and stored in |
---|
| 1632 | explicit_update for each of the three conserved quantities |
---|
| 1633 | stage, xmomentum and ymomentum |
---|
| 1634 | |
---|
| 1635 | The maximal allowable speed computed by the flux_function for each volume |
---|
| 1636 | is converted to a timestep that must not be exceeded. The minimum of |
---|
| 1637 | those is computed as the next overall timestep. |
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| 1638 | |
---|
| 1639 | Post conditions: |
---|
| 1640 | domain.explicit_update is reset to computed flux values |
---|
| 1641 | domain.timestep is set to the largest step satisfying all volumes. |
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| 1642 | """ |
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| 1643 | |
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| 1644 | import sys |
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| 1645 | from Numeric import zeros, Float |
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| 1646 | |
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| 1647 | N = domain.number_of_elements |
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| 1648 | |
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| 1649 | #Shortcuts |
---|
| 1650 | Stage = domain.quantities['stage'] |
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| 1651 | Xmom = domain.quantities['xmomentum'] |
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| 1652 | Ymom = domain.quantities['ymomentum'] |
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| 1653 | Bed = domain.quantities['elevation'] |
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| 1654 | |
---|
| 1655 | #Arrays |
---|
| 1656 | stage = Stage.edge_values |
---|
| 1657 | xmom = Xmom.edge_values |
---|
| 1658 | ymom = Ymom.edge_values |
---|
| 1659 | bed = Bed.edge_values |
---|
| 1660 | |
---|
| 1661 | stage_bdry = Stage.boundary_values |
---|
| 1662 | xmom_bdry = Xmom.boundary_values |
---|
| 1663 | ymom_bdry = Ymom.boundary_values |
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| 1664 | |
---|
| 1665 | flux = zeros((N,3), Float) #Work array for summing up fluxes |
---|
| 1666 | |
---|
| 1667 | #Loop |
---|
| 1668 | timestep = float(sys.maxint) |
---|
| 1669 | for k in range(N): |
---|
| 1670 | |
---|
| 1671 | for i in range(3): |
---|
| 1672 | #Quantities inside volume facing neighbour i |
---|
| 1673 | ql = [stage[k, i], xmom[k, i], ymom[k, i]] |
---|
| 1674 | zl = bed[k, i] |
---|
| 1675 | |
---|
| 1676 | #Quantities at neighbour on nearest face |
---|
| 1677 | n = domain.neighbours[k,i] |
---|
| 1678 | if n < 0: |
---|
| 1679 | m = -n-1 #Convert negative flag to index |
---|
| 1680 | qr = [stage_bdry[m], xmom_bdry[m], ymom_bdry[m]] |
---|
| 1681 | zr = zl #Extend bed elevation to boundary |
---|
| 1682 | else: |
---|
| 1683 | m = domain.neighbour_edges[k,i] |
---|
| 1684 | qr = [stage[n, m], xmom[n, m], ymom[n, m]] |
---|
| 1685 | zr = bed[n, m] |
---|
| 1686 | |
---|
| 1687 | |
---|
| 1688 | #Outward pointing normal vector |
---|
| 1689 | normal = domain.normals[k, 2*i:2*i+2] |
---|
| 1690 | |
---|
| 1691 | #Flux computation using provided function |
---|
| 1692 | edgeflux, max_speed = flux_function(normal, ql, qr, zl, zr) |
---|
| 1693 | |
---|
| 1694 | flux[k,:] = edgeflux |
---|
| 1695 | |
---|
| 1696 | return flux |
---|
| 1697 | |
---|
| 1698 | |
---|
| 1699 | |
---|
| 1700 | |
---|
| 1701 | |
---|
| 1702 | |
---|
| 1703 | |
---|
| 1704 | ############################################## |
---|
| 1705 | #Initialise module |
---|
| 1706 | |
---|
| 1707 | |
---|
| 1708 | from utilities import compile |
---|
| 1709 | if compile.can_use_C_extension('shallow_water_ext.c'): |
---|
| 1710 | #Replace python version with c implementations |
---|
| 1711 | |
---|
| 1712 | from shallow_water_ext import rotate, assign_windfield_values |
---|
| 1713 | compute_fluxes = compute_fluxes_c |
---|
| 1714 | extrapolate_second_order_sw=extrapolate_second_order_sw_c |
---|
| 1715 | gravity = gravity_c |
---|
| 1716 | manning_friction = manning_friction_c |
---|
| 1717 | h_limiter = h_limiter_c |
---|
| 1718 | balance_deep_and_shallow = balance_deep_and_shallow_c |
---|
| 1719 | protect_against_infinitesimal_and_negative_heights = protect_against_infinitesimal_and_negative_heights_c |
---|
| 1720 | |
---|
| 1721 | |
---|
| 1722 | #distribute_to_vertices_and_edges = distribute_to_vertices_and_edges_c #(like MH's) |
---|
| 1723 | |
---|
| 1724 | |
---|
| 1725 | |
---|
| 1726 | #Optimisation with psyco |
---|
| 1727 | from config import use_psyco |
---|
| 1728 | if use_psyco: |
---|
| 1729 | try: |
---|
| 1730 | import psyco |
---|
| 1731 | except: |
---|
| 1732 | import os |
---|
| 1733 | if os.name == 'posix' and os.uname()[4] == 'x86_64': |
---|
| 1734 | pass |
---|
| 1735 | #Psyco isn't supported on 64 bit systems, but it doesn't matter |
---|
| 1736 | else: |
---|
| 1737 | msg = 'WARNING: psyco (speedup) could not import'+\ |
---|
| 1738 | ', you may want to consider installing it' |
---|
| 1739 | print msg |
---|
| 1740 | else: |
---|
| 1741 | psyco.bind(Domain.distribute_to_vertices_and_edges) |
---|
| 1742 | psyco.bind(Domain.compute_fluxes) |
---|
| 1743 | |
---|
| 1744 | if __name__ == "__main__": |
---|
| 1745 | pass |
---|