• super_rb
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  • 2020-01-04 00:48
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利用matlab软件编写的格子玻尔兹曼方法模拟的圆柱绕流问题,并实现了可视化
格子玻尔兹曼圆柱绕流.zip
  • 格子玻尔兹曼圆柱绕流.txt
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % cylinder.m: Flow around a cyliner, using LBM %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % This program is free software; you can redistribute it and/or % modify it under the terms of the GNU General Public License % as published by the Free Software Foundation; either version 2 % of the License, or (at your option) any later version. % This program is distributed in the hope that it will be useful, % but WITHOUT ANY WARRANTY; without even the implied warranty of % MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the % GNU General Public License for more details. % You should have received a copy of the GNU General Public % License along with this program; if not, write to the Free % Software Foundation, Inc., 51 Franklin Street, Fifth Floor, % Boston, MA 02110-1301, USA. %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% clear % GENERAL FLOW CONSTANTS(一般流动常数) lx = 250; ly = 51; obst_x = lx/5+1; % position of the cylinder; (exact obst_y = ly/2+1; % y-symmetry is avoided)(圆柱的位置,避免y轴精确的对称) obst_r = ly/10+1; % radius of the cylinder圆柱半径 uMax = 0.02; % maximum velocity of Poiseuille inflow泊肖叶最大流入速度 Re = 100; % Reynolds number雷诺数 nu = uMax * 2.*obst_r / Re; % kinematic viscosity运动粘度 omega = 1. / (3*nu+1./2.); % relaxation parameter松弛参数=1/τ maxT = 40000; % total number of iterations迭代总数 tPlot = 5; % cycles周期数 % D2Q9 LATTICE CONSTANTSD2Q9格子常数 t = [4/9, 1/9,1/9,1/9,1/9, 1/36,1/36,1/36,1/36];%权重 cx = [ 0, 1, 0, -1, 0, 1, -1, -1, 1]; cy = [ 0, 0, 1, 0, -1, 1, 1, -1, -1]; opp = [ 1, 4, 5, 2, 3, 8, 9, 6, 7]; col = 2:(ly-1); [y,x] = meshgrid(1:ly,1:lx); obst = (x-obst_x).^2 + (y-obst_y).^2 <= obst_r.^2; obst(:,[1,ly]) = 1;%反弹边界 bbRegion = find(obst);%反弹边界索引 % INITIAL CONDITION: (rho=0, u=0) ==> fIn(i) = t(i)初始条件 fIn = reshape( t' * ones(1,lx*ly), 9, lx, ly); %t' * ones(1,lx*ly) 9行一列乘一行lx*ly列=9行lx*ly列 % MAIN LOOP (TIME CYCLES)主循环(时间周期) for cycle = 1:maxT % MACROSCOPIC VARIABLES宏观变量 rho = sum(fIn); ux = reshape ( ... (cx * reshape(fIn,9,lx*ly)), 1,lx,ly) ./rho; %cx一行九列乘九行lx*ly列等于一行,lx*ly列 uy = reshape ( ... (cy * reshape(fIn,9,lx*ly)), 1,lx,ly) ./rho; % MACROSCOPIC (DIRICHLET) BOUNDARY CONDITIONS宏观(狄氏)边界条件 % Inlet: Poiseuille profile入口泊肖叶配置 L = ly-2; y = col-1.5; ux(:,1,col) = 4 * uMax / (L*L) * (y.*L-y.*y);%入口按照泊肖叶公式给出速度分布 uy(:,1,col) = 0; rho(:,1,col) = 1 ./ (1-ux(:,1,col)) .* ( ... sum(fIn([1,3,5],1,col)) + ... 2*sum(fIn([4,7,8],1,col)) ); % Outlet: Zero gradient on rho/ux出口:rho / ux上的零梯度 rho(:,lx,col) = rho(:,lx-1,col); uy(:,lx,col) = 0; ux(:,lx,col) = ux(:,lx-1,col); % COLLISION STEP碰撞步骤 for i=1:9 cu = 3*(cx(i)*ux+cy(i)*uy); fEq(i,:,:) = rho .* t(i) .* ... ( 1 + cu + 1/2*(cu.*cu) ... - 3/2*(ux.^2+uy.^2) ); fOut(i,:,:) = fIn(i,:,:) - ... omega .* (fIn(i,:,:)-fEq(i,:,:)); end % MICROSCOPIC BOUNDARY CONDITIONS微观边界条件?????????不懂 for i=1:9 % Left boundary左边界 fOut(i,1,col) = fEq(i,1,col) + ... 18*t(i)*cx(i)*cy(i)* ( fIn(8,1,col) - ... fIn(7,1,col)-fEq(8,1,col)+fEq(7,1,col) ); % Right boundary右边界 fOut(i,lx,col) = fEq(i,lx,col) + ... 18*t(i)*cx(i)*cy(i)* ( fIn(6,lx,col) - ... fIn(9,lx,col)-fEq(6,lx,col)+fEq(9,lx,col) ); % Bounce back region反弹区域 fOut(i,bbRegion) = fIn(opp(i),bbRegion); end % STREAMING STEP传输过程 for i=1:9 fIn(i,:,:) = ... circshift(fOut(i,:,:), [0,cx(i),cy(i)]); end % VISUALIZATION可视化 if (mod(cycle,tPlot)==0) u = reshape(sqrt(ux.^2+uy.^2),lx,ly); u(bbRegion) = nan; imagesc(u'); axis equal off; drawnow end end
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