Mercurial > repos > public > sbplib
annotate +scheme/Utux2d.m @ 1225:68ee061639a1 feature/rv
Make sure matrices are sparse.
author | Vidar Stiernström <vidar.stiernstrom@it.uu.se> |
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date | Wed, 06 Nov 2019 14:52:07 +0100 |
parents | 433c89bf19e0 |
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rev | line source |
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1 classdef Utux2d < scheme.Scheme |
591 | 2 properties |
3 m % Number of points in each direction, possibly a vector | |
4 h % Grid spacing | |
5 grid % Grid | |
6 order % Order accuracy for the approximation | |
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7 |
591 | 8 a % Wave speed a = [a1, a2]; |
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9 % Can either be a constant vector or a cell array of function handles. |
591 | 10 |
11 H % Discrete norm | |
595 | 12 H_x, H_y % Norms in the x and y directions |
13 Hi, Hx, Hy, Hxi, Hyi % Kroneckered norms | |
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14 H_w, H_e, H_s, H_n % Boundary quadratures |
591 | 15 |
16 % Derivatives | |
17 Dx, Dy | |
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18 |
591 | 19 % Boundary operators |
20 e_w, e_e, e_s, e_n | |
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21 |
591 | 22 D % Total discrete operator |
23 end | |
24 | |
25 | |
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26 methods |
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27 function obj = Utux2d(g ,order, a, fluxSplitting, opSet) |
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28 |
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29 default_arg('a',1/sqrt(2)*[1, 1]); |
591 | 30 default_arg('opSet',@sbp.D2Standard); |
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31 default_arg('fluxSplitting',[]); |
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32 |
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33 assertType(g, 'grid.Cartesian'); |
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34 if iscell(a) |
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35 a1 = grid.evalOn(g, a{1}); |
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36 a2 = grid.evalOn(g, a{2}); |
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37 a = {spdiag(a1), spdiag(a2)}; |
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38 else |
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39 a = {a(1), a(2)}; |
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40 end |
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41 |
591 | 42 m = g.size(); |
43 m_x = m(1); | |
44 m_y = m(2); | |
45 m_tot = g.N(); | |
46 | |
595 | 47 xlim = {g.x{1}(1), g.x{1}(end)}; |
48 ylim = {g.x{2}(1), g.x{2}(end)}; | |
591 | 49 obj.grid = g; |
50 | |
51 % Operator sets | |
52 ops_x = opSet(m_x, xlim, order); | |
53 ops_y = opSet(m_y, ylim, order); | |
54 Ix = speye(m_x); | |
55 Iy = speye(m_y); | |
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56 |
591 | 57 % Norms |
58 Hx = ops_x.H; | |
59 Hy = ops_y.H; | |
60 Hxi = ops_x.HI; | |
61 Hyi = ops_y.HI; | |
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62 |
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63 obj.H_w = Hy; |
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64 obj.H_e = Hy; |
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65 obj.H_s = Hx; |
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66 obj.H_n = Hx; |
595 | 67 obj.H_x = Hx; |
68 obj.H_y = Hy; | |
591 | 69 obj.H = kron(Hx,Hy); |
70 obj.Hi = kron(Hxi,Hyi); | |
71 obj.Hx = kron(Hx,Iy); | |
72 obj.Hy = kron(Ix,Hy); | |
73 obj.Hxi = kron(Hxi,Iy); | |
74 obj.Hyi = kron(Ix,Hyi); | |
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75 |
591 | 76 % Derivatives |
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77 if (isequal(opSet,@sbp.D1Upwind)) |
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78 Dx = (ops_x.Dp + ops_x.Dm)/2; |
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79 Dy = (ops_y.Dp + ops_y.Dm)/2; |
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80 obj.Dx = kron(Dx,Iy); |
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81 obj.Dy = kron(Ix,Dy); |
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82 DissOpx = (ops_x.Dm - ops_x.Dp)/2; |
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83 DissOpy = (ops_y.Dm - ops_y.Dp)/2; |
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84 DissOpx = kron(DissOpx,Iy); |
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85 DissOpy = kron(Ix,DissOpy); |
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86 |
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87 obj.D = -(a{1}*obj.Dx + a{2}*obj.Dy + fluxSplitting{1}*DissOpx + fluxSplitting{2}*DissOpy); |
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88 else |
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89 Dx = ops_x.D1; |
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90 Dy = ops_y.D1; |
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91 obj.Dx = kron(Dx,Iy); |
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92 obj.Dy = kron(Ix,Dy); |
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93 |
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94 obj.D = -(a{1}*obj.Dx + a{2}*obj.Dy); |
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95 end |
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96 |
591 | 97 % Boundary operators |
98 obj.e_w = kr(ops_x.e_l, Iy); | |
99 obj.e_e = kr(ops_x.e_r, Iy); | |
100 obj.e_s = kr(Ix, ops_y.e_l); | |
101 obj.e_n = kr(Ix, ops_y.e_r); | |
102 | |
103 obj.m = m; | |
104 obj.h = [ops_x.h ops_y.h]; | |
105 obj.order = order; | |
595 | 106 obj.a = a; |
591 | 107 end |
108 % Closure functions return the opertors applied to the own domain to close the boundary | |
109 % Penalty functions return the opertors to force the solution. In the case of an interface it returns the operator applied to the other doamin. | |
110 % boundary is a string specifying the boundary e.g. 'l','r' or 'e','w','n','s'. | |
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111 % type is a string specifying the type of boundary condition if there are several. %TBD Remove type here? Only dirichlet applicable? |
591 | 112 % data is a function returning the data that should be applied at the boundary. |
113 % neighbour_scheme is an instance of Scheme that should be interfaced to. | |
114 % neighbour_boundary is a string specifying which boundary to interface to. | |
115 function [closure, penalty] = boundary_condition(obj,boundary,type) | |
116 default_arg('type','dirichlet'); | |
1197 | 117 s = obj.getBoundarySign(boundary); |
118 e = obj.getBoundaryOperator('e', boundary); | |
119 H_1d = obj.getOneDirectionalNorm(boundary); | |
591 | 120 switch boundary |
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121 % Can only specify boundary condition where there is inflow |
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122 % Extract the postivie resp. negative part of a, for the left |
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123 % resp. right boundaries, and set other values of a to zero. |
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124 % Then the closure will effectively only contribute to inflow boundaries |
591 | 125 case {'w','W','west','West'} |
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126 a_inflow = obj.a{1}; |
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127 a_inflow(a_inflow < 0) = 0; |
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128 case {'e','E','east','East'} |
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129 a_inflow = obj.a{1}; |
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130 a_inflow(a_inflow > 0) = 0; |
591 | 131 case {'s','S','south','South'} |
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132 a_inflow = obj.a{2}; |
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133 a_inflow(a_inflow < 0) = 0; |
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134 case {'n','N','north','North'} |
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135 a_inflow = obj.a{2}; |
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136 a_inflow(a_inflow > 0) = 0; |
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137 end |
1197 | 138 tau = s*a_inflow*e*H_1d; |
139 closure = obj.Hi*tau*e'; | |
591 | 140 penalty = -obj.Hi*tau; |
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141 end |
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142 |
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143 % type Struct that specifies the interface coupling. |
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144 % Fields: |
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145 % -- couplingType String, type of interface coupling |
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146 % % Default: 'upwind'. Other: 'centered' |
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147 % -- interpolation: type of interpolation, default 'none' |
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148 % -- interpolationDamping: damping on upstream and downstream sides, when using interpolation. |
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149 % Default {0,0} gives zero damping. |
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150 function [closure, penalty] = interface(obj,boundary,neighbour_scheme,neighbour_boundary,type) |
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151 |
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152 defaultType.couplingType = 'upwind'; |
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153 defaultType.interpolation = 'none'; |
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154 defaultType.interpolationDamping = {0,0}; |
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155 default_struct('type', defaultType); |
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156 |
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157 switch type.interpolation |
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158 case {'none', ''} |
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159 [closure, penalty] = interfaceStandard(obj,boundary,neighbour_scheme,neighbour_boundary,type); |
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160 case {'op','OP'} |
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161 [closure, penalty] = interfaceNonConforming(obj,boundary,neighbour_scheme,neighbour_boundary,type); |
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162 otherwise |
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163 error('Unknown type of interpolation: %s ', type.interpolation); |
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164 end |
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165 end |
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166 |
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167 function [closure, penalty] = interfaceStandard(obj,boundary,neighbour_scheme,neighbour_boundary,type) |
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168 couplingType = type.couplingType; |
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169 |
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170 % Get neighbour boundary operator |
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171 e_neighbour = neighbour_scheme.getBoundaryOperator('e', neighbour_boundary); |
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172 |
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173 switch couplingType |
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174 |
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175 % Upwind coupling (energy dissipation) |
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176 case 'upwind' |
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177 sigma_ds = -1; %"Downstream" penalty |
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178 sigma_us = 0; %"Upstream" penalty |
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179 |
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180 % Energy-preserving coupling (no energy dissipation) |
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181 case 'centered' |
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182 sigma_ds = -1/2; %"Downstream" penalty |
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183 sigma_us = 1/2; %"Upstream" penalty |
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184 |
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185 otherwise |
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186 error(['Interface coupling type ' couplingType ' is not available.']) |
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187 end |
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188 |
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189 switch boundary |
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190 case {'w','W','west','West'} |
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191 tau = sigma_ds*obj.a{1}*obj.e_w*obj.H_y; |
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192 closure = obj.Hi*tau*obj.e_w'; |
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193 penalty = -obj.Hi*tau*e_neighbour'; |
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194 case {'e','E','east','East'} |
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195 tau = sigma_us*obj.a{1}*obj.e_e*obj.H_y; |
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196 closure = obj.Hi*tau*obj.e_e'; |
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197 penalty = -obj.Hi*tau*e_neighbour'; |
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198 case {'s','S','south','South'} |
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199 tau = sigma_ds*obj.a{2}*obj.e_s*obj.H_x; |
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|
200 closure = obj.Hi*tau*obj.e_s'; |
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201 penalty = -obj.Hi*tau*e_neighbour'; |
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changeset
|
202 case {'n','N','north','North'} |
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diff
changeset
|
203 tau = sigma_us*obj.a{2}*obj.e_n*obj.H_x; |
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changeset
|
204 closure = obj.Hi*tau*obj.e_n'; |
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diff
changeset
|
205 penalty = -obj.Hi*tau*e_neighbour'; |
605
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595
diff
changeset
|
206 end |
610
b7b3c11fab4d
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Martin Almquist <malmquist@stanford.edu>
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605
diff
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|
207 |
914
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diff
changeset
|
208 end |
610
b7b3c11fab4d
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605
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|
209 |
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210 function [closure, penalty] = interfaceNonConforming(obj,boundary,neighbour_scheme,neighbour_boundary,type) |
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211 |
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212 % User can request special interpolation operators by specifying type.interpOpSet |
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213 default_field(type, 'interpOpSet', @sbp.InterpOpsOP); |
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214 |
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215 interpOpSet = type.interpOpSet; |
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216 couplingType = type.couplingType; |
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|
217 interpolationDamping = type.interpolationDamping; |
610
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diff
changeset
|
218 |
914
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diff
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|
219 % Get neighbour boundary operator |
997
78db023a7fe3
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Martin Almquist <malmquist@stanford.edu>
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diff
changeset
|
220 e_neighbour = neighbour_scheme.getBoundaryOperator('e', neighbour_boundary); |
905
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|
221 |
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|
222 switch couplingType |
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|
223 |
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diff
changeset
|
224 % Upwind coupling (energy dissipation) |
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changeset
|
225 case 'upwind' |
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changeset
|
226 sigma_ds = -1; %"Downstream" penalty |
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diff
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|
227 sigma_us = 0; %"Upstream" penalty |
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|
228 |
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diff
changeset
|
229 % Energy-preserving coupling (no energy dissipation) |
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diff
changeset
|
230 case 'centered' |
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diff
changeset
|
231 sigma_ds = -1/2; %"Downstream" penalty |
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diff
changeset
|
232 sigma_us = 1/2; %"Upstream" penalty |
666
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610
diff
changeset
|
233 |
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diff
changeset
|
234 otherwise |
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910
diff
changeset
|
235 error(['Interface coupling type ' couplingType ' is not available.']) |
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diff
changeset
|
236 end |
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changeset
|
237 |
50cafc4b9e40
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diff
changeset
|
238 int_damp_us = interpolationDamping{1}; |
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changeset
|
239 int_damp_ds = interpolationDamping{2}; |
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changeset
|
240 |
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diff
changeset
|
241 % u denotes the solution in the own domain |
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diff
changeset
|
242 % v denotes the solution in the neighbour domain |
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243 % Find the number of grid points along the interface |
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|
244 switch boundary |
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changeset
|
245 case {'w','e'} |
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|
246 m_u = obj.m(2); |
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|
247 case {'s','n'} |
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changeset
|
248 m_u = obj.m(1); |
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|
249 end |
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|
250 m_v = size(e_neighbour, 2); |
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|
251 |
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changeset
|
252 % Build interpolation operators |
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|
253 intOps = interpOpSet(m_u, m_v, obj.order, neighbour_scheme.order); |
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changeset
|
254 Iu2v = intOps.Iu2v; |
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|
255 Iv2u = intOps.Iv2u; |
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|
256 |
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changeset
|
257 I_local2neighbour_ds = intOps.Iu2v.bad; |
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changeset
|
258 I_local2neighbour_us = intOps.Iu2v.good; |
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changeset
|
259 I_neighbour2local_ds = intOps.Iv2u.good; |
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changeset
|
260 I_neighbour2local_us = intOps.Iv2u.bad; |
914
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|
261 |
50cafc4b9e40
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diff
changeset
|
262 I_back_forth_us = I_neighbour2local_us*I_local2neighbour_us; |
50cafc4b9e40
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parents:
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diff
changeset
|
263 I_back_forth_ds = I_neighbour2local_ds*I_local2neighbour_ds; |
666
2d85f17a8aec
Add possibility for damping terms at interpolation interface.
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parents:
610
diff
changeset
|
264 |
2d85f17a8aec
Add possibility for damping terms at interpolation interface.
Martin Almquist <malmquist@stanford.edu>
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610
diff
changeset
|
265 |
942
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changeset
|
266 switch boundary |
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changeset
|
267 case {'w','W','west','West'} |
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268 tau = sigma_ds*obj.a{1}*obj.e_w*obj.H_y; |
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changeset
|
269 closure = obj.Hi*tau*obj.e_w'; |
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changeset
|
270 penalty = -obj.Hi*tau*I_neighbour2local_ds*e_neighbour'; |
666
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Add possibility for damping terms at interpolation interface.
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parents:
610
diff
changeset
|
271 |
942
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changeset
|
272 beta = int_damp_ds*obj.a{1}... |
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|
273 *obj.e_w*obj.H_y; |
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274 closure = closure + obj.Hi*beta*I_back_forth_ds*obj.e_w' - obj.Hi*beta*obj.e_w'; |
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275 case {'e','E','east','East'} |
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276 tau = sigma_us*obj.a{1}*obj.e_e*obj.H_y; |
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277 closure = obj.Hi*tau*obj.e_e'; |
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278 penalty = -obj.Hi*tau*I_neighbour2local_us*e_neighbour'; |
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279 |
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280 beta = int_damp_us*obj.a{1}... |
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281 *obj.e_e*obj.H_y; |
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282 closure = closure + obj.Hi*beta*I_back_forth_us*obj.e_e' - obj.Hi*beta*obj.e_e'; |
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283 case {'s','S','south','South'} |
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284 tau = sigma_ds*obj.a{2}*obj.e_s*obj.H_x; |
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285 closure = obj.Hi*tau*obj.e_s'; |
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286 penalty = -obj.Hi*tau*I_neighbour2local_ds*e_neighbour'; |
666
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287 |
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288 beta = int_damp_ds*obj.a{2}... |
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289 *obj.e_s*obj.H_x; |
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290 closure = closure + obj.Hi*beta*I_back_forth_ds*obj.e_s' - obj.Hi*beta*obj.e_s'; |
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291 case {'n','N','north','North'} |
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292 tau = sigma_us*obj.a{2}*obj.e_n*obj.H_x; |
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293 closure = obj.Hi*tau*obj.e_n'; |
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294 penalty = -obj.Hi*tau*I_neighbour2local_us*e_neighbour'; |
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295 |
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296 beta = int_damp_us*obj.a{2}... |
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297 *obj.e_n*obj.H_x; |
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298 closure = closure + obj.Hi*beta*I_back_forth_us*obj.e_n' - obj.Hi*beta*obj.e_n'; |
591 | 299 end |
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300 |
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301 |
591 | 302 end |
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303 |
1197 | 304 % Returns the boundary sign. The right boundary is considered the positive boundary |
305 % boundary -- string | |
306 function s = getBoundarySign(obj, boundary) | |
307 assertIsMember(boundary, {'w', 'e', 's', 'n'}) | |
308 switch boundary | |
309 case {'e','n'} | |
310 s = 1; | |
311 case {'w','s'} | |
312 s = -1; | |
313 end | |
314 end | |
315 | |
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316 % Returns the boundary operator op for the boundary specified by the string boundary. |
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317 % op -- string |
997
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318 % boundary -- string |
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319 function o = getBoundaryOperator(obj, op, boundary) |
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320 assertIsMember(op, {'e'}) |
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321 assertIsMember(boundary, {'w', 'e', 's', 'n'}) |
997
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322 |
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323 o = obj.([op, '_', boundary]); |
997
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324 end |
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325 |
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326 % Returns square boundary quadrature matrix, of dimension |
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327 % corresponding to the number of boundary points |
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328 % |
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329 % boundary -- string |
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330 function H_b = getBoundaryQuadrature(obj, boundary) |
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331 assertIsMember(boundary, {'w', 'e', 's', 'n'}) |
997
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332 |
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333 H_b = obj.(['H_', boundary]); |
997
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334 end |
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335 |
1197 | 336 % Returns square boundary quadrature matrix, of dimension |
337 % corresponding to the number of boundary points | |
338 % | |
339 % boundary -- string | |
340 function H_1d = getOneDirectionalNorm(obj, boundary) | |
341 assertIsMember(boundary, {'w', 'e', 's', 'n'}) | |
342 switch boundary | |
343 case {'w','e'} | |
344 H_1d = obj.H_y; | |
345 case {'s','n'} | |
346 H_1d = obj.H_x; | |
347 end | |
348 end | |
349 | |
591 | 350 function N = size(obj) |
351 N = obj.m; | |
352 end | |
353 | |
354 end | |
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355 end |