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ThermalConvection2D.jl
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ThermalConvection2D.jl
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const USE_GPU = false # Use GPU? If this is set false, then no GPU needs to be available
using ParallelStencil
using ParallelStencil.FiniteDifferences2D
@static if USE_GPU
@init_parallel_stencil(CUDA, Float64, 2)
else
@init_parallel_stencil(Threads, Float64, 2)
end
using Plots, Printf, Statistics, LinearAlgebra
@parallel function assign!(A::Data.Array, B::Data.Array)
@all(A) = @all(B)
return
end
@parallel function compute_error!(Err_A::Data.Array, A::Data.Array)
@all(Err_A) = @all(Err_A) - @all(A)
return
end
@parallel function compute_0!(RogT::Data.Array, Eta::Data.Array, ∇V::Data.Array, T::Data.Array, Vx::Data.Array, Vy::Data.Array, ρ0gα::Data.Number, η0::Data.Number, dη_dT::Data.Number, ΔT::Data.Number, dx::Data.Number, dy::Data.Number)
@all(RogT) = ρ0gα*@all(T)
@all(Eta) = η0*(1.0 - dη_dT*(@all(T) + ΔT/2.0))
@all(∇V) = @d_xa(Vx)/dx + @d_ya(Vy)/dy
return
end
@parallel function compute_1!(Pt::Data.Array, τxx::Data.Array, τyy::Data.Array, σxy::Data.Array, Eta::Data.Array, ∇V::Data.Array, Vx::Data.Array, Vy::Data.Array, dτ_iter::Data.Number, β::Data.Number, dx::Data.Number, dy::Data.Number)
@all(Pt) = @all(Pt) - dτ_iter/β*@all(∇V)
@all(τxx) = 2.0*@all(Eta)*(@d_xa(Vx)/dx - 1.0/3.0*@all(∇V))
@all(τyy) = 2.0*@all(Eta)*(@d_ya(Vy)/dy - 1.0/3.0*@all(∇V))
@all(σxy) = 2.0*@av(Eta)*(0.5*(@d_yi(Vx)/dy + @d_xi(Vy)/dx))
return
end
@parallel function compute_2!(Rx::Data.Array, Ry::Data.Array, dVxdτ::Data.Array, dVydτ::Data.Array, Pt::Data.Array, RogT::Data.Array, τxx::Data.Array, τyy::Data.Array, σxy::Data.Array, ρ::Data.Number, dampX::Data.Number, dampY::Data.Number, dτ_iter::Data.Number, dx::Data.Number, dy::Data.Number)
@all(Rx) = 1.0/ρ *(@d_xi(τxx)/dx + @d_ya(σxy)/dy - @d_xi(Pt)/dx )
@all(Ry) = 1.0/ρ *(@d_yi(τyy)/dy + @d_xa(σxy)/dx - @d_yi(Pt)/dy + @av_yi(RogT))
@all(dVxdτ) = dampX*@all(dVxdτ) + @all(Rx)*dτ_iter
@all(dVydτ) = dampY*@all(dVydτ) + @all(Ry)*dτ_iter
return
end
@parallel function update_V!(Vx::Data.Array, Vy::Data.Array, dVxdτ::Data.Array, dVydτ::Data.Array, dτ_iter::Data.Number)
@inn(Vx) = @inn(Vx) + @all(dVxdτ)*dτ_iter
@inn(Vy) = @inn(Vy) + @all(dVydτ)*dτ_iter
return
end
@parallel function compute_qT!(qTx::Data.Array, qTy::Data.Array, T::Data.Array, DcT::Data.Number, dx::Data.Number, dy::Data.Number)
@all(qTx) = -DcT*@d_xi(T)/dx
@all(qTy) = -DcT*@d_yi(T)/dy
return
end
@parallel_indices (ix,iy) function advect_T!(dT_dt::Data.Array, qTx::Data.Array, qTy::Data.Array, T::Data.Array, Vx::Data.Array, Vy::Data.Array, dx::Data.Number, dy::Data.Number)
if (ix<=size(dT_dt, 1) && iy<=size(dT_dt, 2)) dT_dt[ix,iy] = -((qTx[ix+1,iy]-qTx[ix,iy])/dx + (qTy[ix,iy+1]-qTy[ix,iy])/dy) -
(Vx[ix+1,iy+1]>0)*Vx[ix+1,iy+1]*(T[ix+1,iy+1]-T[ix ,iy+1])/dx -
(Vx[ix+2,iy+1]<0)*Vx[ix+2,iy+1]*(T[ix+2,iy+1]-T[ix+1,iy+1])/dx -
(Vy[ix+1,iy+1]>0)*Vy[ix+1,iy+1]*(T[ix+1,iy+1]-T[ix+1,iy ])/dy -
(Vy[ix+1,iy+2]<0)*Vy[ix+1,iy+2]*(T[ix+1,iy+2]-T[ix+1,iy+1])/dy end
return
end
@parallel function update_T!(T::Data.Array, T_old::Data.Array, dT_dt::Data.Array, dt::Data.Number)
@inn(T) = @inn(T_old) + @all(dT_dt)*dt
return
end
@parallel_indices (ix,iy) function no_fluxY_T!(T::Data.Array)
if (ix==size(T, 1) && iy<=size(T ,2)) T[ix,iy] = T[ix-1,iy] end
if (ix==1 && iy<=size(T ,2)) T[ix,iy] = T[ix+1,iy] end
return
end
@parallel_indices (iy) function bc_x!(A::Data.Array)
A[1 , iy] = A[2 , iy]
A[end, iy] = A[end-1, iy]
return
end
@parallel_indices (ix) function bc_y!(A::Data.Array)
A[ix, 1 ] = A[ix, 2 ]
A[ix, end] = A[ix, end-1]
return
end
##################################################
@views function ThermalConvection2D()
# Physics - dimentionally independent scales
ly = 1.0 # domain extend, m
η0 = 1.0 # viscosity, Pa*s
DcT = 1.0 # heat diffusivity, m^2/s
ΔT = 1.0 # initial temperature perturbation K
# Physics - nondim numbers
Ra = 1e7 # Raleigh number = ρ0*g*α*ΔT*ly^3/η0/DcT
Pra = 1e3 # Prandtl number = η0/ρ0/DcT
ar = 3 # aspect ratio
# Physics - dimentionally dependent parameters
lx = ar*ly # domain extend, m
w = 1e-2*ly # initial perturbation standard deviation, m
ρ0gα = Ra*η0*DcT/ΔT/ly^3 # thermal expansion
dη_dT = 1e-10/ΔT # viscosity's temperature dependence
# Numerics
nx, ny = 96*ar-1, 96-1 # numerical grid resolutions; should be a mulitple of 32-1 for optimal GPU perf
iterMax = 5*10^4 # maximal number of pseudo-transient iterations
nt = 3000 # total number of timesteps
nout = 10 # frequency of plotting
nerr = 100 # frequency of error checking
ε = 1e-4 # nonlinear absolute tolerence
dmp = 2 # damping paramter
st = 5 # quiver plotting spatial step
# Derived numerics
dx, dy = lx/(nx-1), ly/(ny-1) # cell size
ρ = 1.0/Pra*η0/DcT # density
dt_diff = 1.0/4.1*min(dx,dy)^2/DcT # diffusive CFL timestep limiter
dτ_iter = 1.0/6.1*min(dx,dy)/sqrt(η0/ρ) # iterative CFL pseudo-timestep limiter
β = 6.1*dτ_iter^2/min(dx,dy)^2/ρ # numerical bulk compressibility
dampX = 1.0-dmp/nx # damping term for the x-momentum equation
dampY = 1.0-dmp/ny # damping term for the y-momentum equation
# Array allocations
T = @zeros(nx ,ny )
T .= Data.Array([ΔT*exp(-(((ix-1)*dx-0.5*lx)/w)^2 -(((iy-1)*dy-0.5*ly)/w)^2) for ix=1:size(T,1), iy=1:size(T,2)])
T[:,1 ] .= ΔT/2.0
T[:,end] .= -ΔT/2.0
T_old = @zeros(nx ,ny )
Pt = @zeros(nx ,ny )
∇V = @zeros(nx ,ny )
Vx = @zeros(nx+1,ny )
Vy = @zeros(nx ,ny+1)
RogT = @zeros(nx ,ny )
Eta = @zeros(nx ,ny )
τxx = @zeros(nx ,ny )
τyy = @zeros(nx ,ny )
σxy = @zeros(nx-1,ny-1)
Rx = @zeros(nx-1,ny-2)
Ry = @zeros(nx-2,ny-1)
dVxdτ = @zeros(nx-1,ny-2)
dVydτ = @zeros(nx-2,ny-1)
dτVx = @zeros(nx-1,ny-2)
dτVy = @zeros(nx-2,ny-1)
qTx = @zeros(nx-1,ny-2)
qTy = @zeros(nx-2,ny-1)
dT_dt = @zeros(nx-2,ny-2)
ErrP = @zeros(nx ,ny )
ErrV = @zeros(nx ,ny+1)
# Preparation of visualisation
ENV["GKSwstype"]="nul"; if isdir("viz2D_out")==false mkdir("viz2D_out") end; loadpath = "./viz2D_out/"; anim = Animation(loadpath,String[])
println("Animation directory: $(anim.dir)")
X, Y = -lx/2:dx:lx/2, -ly/2:dy:ly/2
Xc, Yc = [x for x=X, y=Y], [y for x=X,y=Y]
Xp, Yp = Xc[1:st:end,1:st:end], Yc[1:st:end,1:st:end]
# Time loop
err_evo1=[]; err_evo2=[]
for it = 1:nt
@parallel assign!(T_old, T)
errV, errP = 2*ε, 2*ε; iter=1; niter=0
while (errV > ε || errP > ε) && iter <= iterMax
@parallel assign!(ErrV, Vy)
@parallel assign!(ErrP, Pt)
@parallel compute_0!(RogT, Eta, ∇V, T, Vx, Vy, ρ0gα, η0, dη_dT, ΔT, dx, dy)
@parallel compute_1!(Pt, τxx, τyy, σxy, Eta, ∇V, Vx, Vy, dτ_iter, β, dx, dy)
@parallel compute_2!(Rx, Ry, dVxdτ, dVydτ, Pt, RogT, τxx, τyy, σxy, ρ, dampX, dampY, dτ_iter, dx, dy)
@parallel update_V!(Vx, Vy, dVxdτ, dVydτ, dτ_iter)
@parallel (1:size(Vx,1)) bc_y!(Vx)
@parallel (1:size(Vy,2)) bc_x!(Vy)
@parallel compute_error!(ErrV, Vy)
@parallel compute_error!(ErrP, Pt)
if mod(iter,nerr) == 0
errV = maximum(abs.(Array(ErrV)))/(1e-12 + maximum(abs.(Array(Vy))))
errP = maximum(abs.(Array(ErrP)))/(1e-12 + maximum(abs.(Array(Pt))))
push!(err_evo1, max(errV, errP)); push!(err_evo2,iter)
# @printf("Total steps = %d, errV=%1.3e, errP=%1.3e \n", iter, errV, errP)
end
iter+=1; niter+=1
end
# Thermal solver
@parallel compute_qT!(qTx, qTy, T, DcT, dx, dy)
@parallel advect_T!(dT_dt, qTx, qTy, T, Vx, Vy, dx, dy)
dt_adv = min(dx/maximum(abs.(Array(Vx))), dy/maximum(abs.(Array(Vy))))/2.1
dt = min(dt_diff, dt_adv)
@parallel update_T!(T, T_old, dT_dt, dt)
@parallel no_fluxY_T!(T)
@printf("it = %d (iter = %d), errV=%1.3e, errP=%1.3e \n", it, niter, errV, errP)
# Visualization
if mod(it,nout)==0
heatmap(X, Y, Array(T)', aspect_ratio=1, xlims=(X[1], X[end]), ylims=(Y[1], Y[end]), c=:inferno, clims=(-0.1,0.1), title="T° (it = $it of $nt)")
Vxp = 0.5*(Vx[1:st:end-1,1:st:end ]+Vx[2:st:end,1:st:end])
Vyp = 0.5*(Vy[1:st:end ,1:st:end-1]+Vy[1:st:end,2:st:end])
Vscale = 1/maximum(sqrt.(Vxp.^2 + Vyp.^2)) * dx*(st-1)
quiver!(Xp[:], Yp[:], quiver=(Vxp[:]*Vscale, Vyp[:]*Vscale), lw=0.1, c=:blue); frame(anim)
# display( quiver!(Xp[:], Yp[:], quiver=(Vxp[:]*Vscale, Vyp[:]*Vscale), lw=0.1, c=:blue) )
end
end
gif(anim, "ThermalConvect2D.gif", fps = 15)
return
end
ThermalConvection2D()