Numerical solution of PDE:s, Part 9: 2D Ginzburg-Landau equation

In an earlier post, I described the 1-dimensional Ginzburg-Landau equation and showed how it can be linearized and solved with a implicit differencing scheme. The most interesting feature of the solutions was the appearance of seemingly random oscillations. A similar solution method is possible for the 2d version of the equation:

2dGL-large

where again \alpha and \beta are real valued constants.

An R language code for solving this with parameter values \alpha = 0 , \beta = 1.5 and an initial state A(x,0) which is a mixture of 2d plane waves is shown below.

library(graphics) #load the graphics library needed for plotting

lx <- 80.0 #length of the computational domain in x-direction
ly <- 80.0 #length of the computational domain in y-direction
lt <- 60.0 #length of the simulation time interval
nx <- 50 #number of discrete lattice points in x-direction
ny <- 50 #number of discrete lattice points in y-direction
nt <- 240 #number of timesteps
dx <- lx/nx #length of one discrete lattice cell in x-direction
dy <- ly/ny #length of one discrete lattice cell in y-direction
dt <- lt/nt #length of timestep

a <- 0
b <- 1.5

kappa1 = dt*(1+1i*a)/dx/dx
kappa2 = dt*(1+1i*b)

C = c(1:(nx*ny))
Cu = c(1:(nx*ny))
A2d = matrix(nrow=ny,ncol=nx)
xaxis <- c(0:(nx-1))*dx #the x values corresponding to the discrete lattice points
yaxis <- c(0:(ny-1))*dy #the y values corresponding to the discrete lattice points

A = matrix(nrow=(nx*ny),ncol=(nx*ny))
IP = matrix(nrow=4*nx,ncol=4*nx)

for (i in c(1:ny)) {
for (j in c(1:nx)) {
A2d[i,j] <- 0.01*exp(1i*5.21*i+1i*10.331*j)+0.01*exp(1i*15.71*i+1i*17.831*j)
}
}

for (k in c(1:nt)) { #main time stepping loop

for(i in c(1:ny)) {
for(j in c(1:nx)) {
C[(i-1)*nx+j] <- A2d[i,j]

}
}

for(i in c(1:(nx*ny))) {
for(j in c(1:(nx*ny))) {
A[i,j] <- 0
if(i==j && j!=1 && j!=nx && i!=1 && i!=ny) A[i,j] <- 1+2*kappa1+kappa2*abs(C[j])*abs(C[j]) - dt
if(i==j && (j==1 || j==nx) && i!=1 && i!=ny) A[i,j] <- 1+2*kappa1+kappa2*abs(C[j])*abs(C[j]) - dt
if(i==j && j!=1 && j!=nx && (i==1 || i==ny)) A[i,j] <- 1+2*kappa1+kappa2*abs(C[j])*abs(C[j]) - dt
if(i==j && (j==1 || j==nx) && (i==1 || i==ny)) A[i,j] <- 1+2*kappa1+kappa2*abs(C[j])*abs(C[j]) - dt
if(j==i+1 && (i%%nx != 0)) A[i,j] <- -kappa1
if(j==i-1 && (i%%nx != 1)) A[i,j] <- -kappa1
if(j==i+nx) A[i,j] <- -kappa1
if(j==i-nx) A[i,j] <- -kappa1
}
}

Cu <- solve(A,C)

for(i in c(1:ny)) {
for(j in c(1:nx)) {
if(i==1) Cu[(i-1)*nx+j]=Cu[i*nx+j]
if(i==ny) Cu[(i-1)*nx+j]=Cu[(i-2)*nx+j]
if(j==1) Cu[(i-1)*nx+j]=Cu[(i-1)*nx+j+1]
if(j==nx) Cu[(i-1)*nx+j]=Cu[(i-1)*nx+j-1]
}
}

for(i in c(1:ny)) {
for(j in c(1:nx)) {
A2d[i,j] <- Cu[(i-1)*nx+j]
}
}

for(l in c(1:(nx-1))) {
for(m in c(1:(nx-1))) { #make a bitmap with 4 times more pixels, using linear interpolation
IP[4*l-3,4*m-3] = A2d[l,m]
IP[4*l-2,4*m-3] = A2d[l,m]+0.25*(A2d[l+1,m]-A2d[l,m])
IP[4*l-1,4*m-3] = A2d[l,m]+0.5*(A2d[l+1,m]-A2d[l,m])
IP[4*l,4*m-3] = A2d[l,m]+0.75*(A2d[l+1,m]-A2d[l,m])
}
}

for(l in c(1:(4*nx))) {
for(m in c(1:(nx-1))) {
IP[l,4*m-2] = IP[l,4*m-3]+0.25*(IP[l,4*m+1]-IP[l,4*m-3])
IP[l,4*m-1] = IP[l,4*m-3]+0.5*(IP[l,4*m+1]-IP[l,4*m-3])
IP[l,4*m] = IP[l,4*m-3]+0.75*(IP[l,4*m+1]-IP[l,4*m-3])
}
}

#make plots of C(x,y) on every third timestep
jpeg(file = paste("plot_",k,".jpg",sep=""))
image(Re(IP),zlim=c(-3,3))
title(paste("Real part of solution A(x,y,t)",k*dt))
dev.off()

}

The code produces 2d plots of the real part of the solution on each timestep, and in the video shown below they have been combined into an animation.

In the animation we see the appearance of spiral patterns typical for these values of parameters \alpha,\beta . Other values of the parameters
produce different kinds of patterns, as is described in this link.

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