% Brusselator reaction-diffusion on a closed surface. % % du/dt = D1*lap_g(u) + A - (B+1)*u + u^2*v % dv/dt = D2*lap_g(v) + B*u - u^2*v % % Same scheme as models/schnakenberg.m. function [U, V, u, v] = init(noise, A, B) U = analys(A + noise); V = analys((B / A) * ones(numel(noise), 1)); u = synth(U); v = synth(V); end function [Un, Vn, u, v] = step(U, V, lam, filt, gx, gy, gz, Vtx, Vty, Vtz, Vpx, Vpy, Vpz, A, B, D1, D2, dt, niter) u = synth(U); v = synth(V); uuv = u .* u .* v; Bu = U + dt * analys(A - (B + 1) * u + uuv); Bv = V + dt * analys(B * u - uuv); Un = Bu ./ (1 + (dt * D1) * lam); Vn = Bv ./ (1 + (dt * D2) * lam); for k = 1:niter % dlap = lap_g - lap_s, evaluated at the current iterate (see % models/schnakenberg.m and docs/richardson-iteration.md for the % derivation). Fu = Un .* filt; Ftu = dtheta(Fu); Fpu = dphi(Fu); dux = Ftu .* Vtx + Fpu .* Vpx; duy = Ftu .* Vty + Fpu .* Vpy; duz = Ftu .* Vtz + Fpu .* Vpz; cux = analys(dux) .* filt; cuy = analys(duy) .* filt; cuz = analys(duz) .* filt; Ftcux = dtheta(cux); Fpcux = dphi(cux); Ftcuy = dtheta(cuy); Fpcuy = dphi(cuy); Ftcuz = dtheta(cuz); Fpcuz = dphi(cuz); lapu = Ftcux .* Vtx + Fpcux .* Vpx; lapu = lapu + Ftcuy .* Vty; lapu = lapu + Fpcuy .* Vpy; lapu = lapu + Ftcuz .* Vtz; lapu = lapu + Fpcuz .* Vpz; dLu = analys(lapu) + lam .* Un; Fv = Vn .* filt; Ftv = dtheta(Fv); Fpv = dphi(Fv); dvx = Ftv .* Vtx + Fpv .* Vpx; dvy = Ftv .* Vty + Fpv .* Vpy; dvz = Ftv .* Vtz + Fpv .* Vpz; cvx = analys(dvx) .* filt; cvy = analys(dvy) .* filt; cvz = analys(dvz) .* filt; Ftcvx = dtheta(cvx); Fpcvx = dphi(cvx); Ftcvy = dtheta(cvy); Fpcvy = dphi(cvy); Ftcvz = dtheta(cvz); Fpcvz = dphi(cvz); lapv = Ftcvx .* Vtx + Fpcvx .* Vpx; lapv = lapv + Ftcvy .* Vty; lapv = lapv + Fpcvy .* Vpy; lapv = lapv + Ftcvz .* Vtz; lapv = lapv + Fpcvz .* Vpz; dLv = analys(lapv) + lam .* Vn; Un = (Bu + (dt * D1) * dLu) ./ (1 + (dt * D1) * lam); Vn = (Bv + (dt * D2) * dLv) ./ (1 + (dt * D2) * lam); end end