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September 1, 2021 20:31
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using LinearAlgebra | |
using SparseArrays | |
using DifferentialEquations | |
using DiffEqOperators | |
using BlockBandedMatrices | |
using DiffEqOperators | |
using RecursiveFactorization | |
mutable struct Single_Stack | |
L::Float64 | |
N::Int64 | |
t::Float64 | |
ρ::Array{Float64,1} | |
w::Array{Float64,1} | |
ρθ::Array{Float64,1} | |
ρ_res::Array{Float64,1} | |
w_res::Array{Float64,1} | |
ρθ_res::Array{Float64,1} | |
_grav::Float64 | |
γ::Float64 | |
_R_m::Float64 | |
Π::Function | |
end | |
function combine!(ρ, w, ρθ, u) | |
N = length(ρ) | |
u[1:N] .= ρ | |
u[N+1:2N] .= ρθ | |
u[2N+1:3N+1] .= w | |
end | |
function split!(u, ρ, w, ρθ) | |
N = length(ρ) | |
ρ .= u[1:N] | |
ρθ .= u[N+1:2N] | |
w .= u[2N+1:3N+1] | |
end | |
function compute_wave_speed(ρ, w, ρθ, _R_m, _C_p, γ, _MSLP) | |
p = ( ρθ * _R_m / _MSLP^(_R_m/_C_p) ).^(γ) | |
c = sqrt.(γ*p./ρ) | |
return maximum(w) + maximum(c) | |
end | |
function DecayingTemperatureProfile(z::Float64; T_virt_surf, T_min_ref, _R_d, _grav, _MSLP) | |
# Scale height for surface temperature | |
H_sfc = _R_d * T_virt_surf / _grav | |
H_t = H_sfc | |
z′ = z / H_t | |
tanh_z′ = tanh(z′) | |
ΔTv = T_virt_surf - T_min_ref | |
Tv = T_virt_surf - ΔTv * tanh_z′ | |
ΔTv′ = ΔTv / T_virt_surf | |
p = -H_t * (z′ + ΔTv′ * (log(1 - ΔTv′ * tanh_z′) - log(1 + tanh_z′) + z′)) | |
p /= H_sfc * (1 - ΔTv′^2) | |
p = _MSLP * exp(p) | |
ρ = p/(_R_d*Tv) | |
return (Tv, p, ρ) | |
end | |
function spatial_residual(du, u, ss::Single_Stack, t) | |
@info "Tendency computation!!!!" t | |
# u is a N+(N-1)+N vector | |
N, L = ss.N, ss.L | |
Δz = L/N | |
_grav = ss._grav | |
Π = ss.Π | |
ρ, w, ρθ = ss.ρ, ss.w, ss.ρθ | |
ρ_res, w_res, ρθ_res = ss.ρ_res, ss.w_res, ss.ρθ_res | |
if eltype(u) != eltype(w) | |
ρ = similar(ρ, eltype(u)) | |
w = similar(w, eltype(u)) | |
ρθ = similar(ρθ, eltype(u)) | |
ρ_res = similar(ρ_res, eltype(u)) | |
w_res = similar(w_res, eltype(u)) | |
ρθ_res = similar(ρθ_res, eltype(u)) | |
end | |
split!(u, ρ, w, ρθ) | |
for i = 1:N | |
ρ₊ = (i == N ? 0.0 : (ρ[i] + ρ[i+1])/2.0) | |
ρ₋ = (i == 1 ? 0.0 : (ρ[i] + ρ[i-1])/2.0) | |
ρ_res[i] = -(w[i+1]ρ₊ - w[i]ρ₋)/Δz | |
ρθ₊ = (i == N ? 0.0 : (ρθ[i] + ρθ[i+1])/2.0) | |
ρθ₋ = (i == 1 ? 0.0 : (ρθ[i] + ρθ[i-1])/2.0) | |
ρθ_res[i] = -(w[i+1]ρθ₊ - w[i]ρθ₋)/Δz | |
end | |
w_res[1] = w_res[N+1] = 0 | |
for i = 2:N | |
w_res[i] = -1/2*(ρθ[i-1]/ρ[i-1] + ρθ[i]/ρ[i]) *(Π(ρθ[i]) - Π(ρθ[i-1]))/Δz - _grav | |
end | |
combine!(ρ_res, w_res, ρθ_res, du) | |
# @info "norm(du) = ", norm(du) | |
end | |
function RK4!(f, u0, ss::Single_Stack, T, Δt) | |
u = copy(u0) | |
k1, k2, k3, k4 = similar(u0), similar(u0), similar(u0), similar(u0) | |
Nt = Int64(round(T / Δt)) | |
t = 0 | |
for i = 1:Nt | |
f(k1, u, ss, t) | |
f(k2, u + Δt/2*k1, ss, t+Δt/2) | |
f(k3, u + Δt/2*k2, ss, t+Δt/2) | |
f(k4, u + Δt*k3, ss, t+Δt) | |
u .+= Δt/6*(k1 + 2k2 + 2k3 + k4) | |
t += Δt | |
end | |
return u | |
end | |
function jacobian!(J,u,ss,t) | |
@info "Jacobian computation!!!!" t | |
# N cells | |
N = div(length(u) - 1 , 3) | |
ρ, ρθ, w = u[1:N], u[N+1:2N], u[2N+1:3N+1] | |
# construct cell center | |
ρh = [ρ[1] ; (ρ[1:N-1] + ρ[2:N])/2.0; ρ[N]] | |
ρθh = [ρθ[1]; (ρθ[1:N-1] + ρθ[2:N])/2.0; ρθ[N]] | |
Πc = Π.(ρθ) | |
Πh = [NaN64; (Πc[1:N-1] + Πc[2:N])/2.0; NaN64] | |
Δzh = [NaN64; (Δz[1:N-1] + Δz[2:N])/2.0; NaN64] | |
for i = 1:N | |
J[i, i+2N] = ρh[i]/Δz[i] | |
J[i, i+2N+1] = -ρh[i+1]/Δz[i] | |
end | |
for i = 1:N | |
J[i+N, i+2N] = ρθh[i]/Δz[i] | |
J[i+N, i+2N+1] = -ρθh[i+1]/Δz[i] | |
end | |
# 0 for i = 1, N+1 | |
for i = 2:N | |
J[i+2N, (i-1)] = -_grav/(2*ρh[i]) | |
J[i+2N, (i-1)+1] = -_grav/(2*ρh[i]) | |
J[i+2N, (i-1)+N] = (γ - 1)*Πh[i]./(ρh[i]*Δzh[i]) | |
J[i+2N, (i-1)+1+N] = -(γ - 1)*Πh[i]./(ρh[i]*Δzh[i]) | |
end | |
# D_ρ = diagm(0=>-ρh/Δz, -1=>ρh/Δz)[1:N, 1:N-1] | |
# D_Θ = diagm(0=>-ρθh/Δz, -1=>ρθh/Δz)[1:N, 1:N-1] | |
# G_W = (γ - 1) * diagm(0=>Πh./ρh/Δz, 1=>-Πh./ρh/Δz)[1:N-1, 1:N] | |
# A_W = diagm(0=>-ones(N-1)./ρh/2, 1=>-ones(N-1)./ρh/2)[1:N-1, 1:N] | |
# P = ([zeros(N,N) D_ρ zeros(N,N); | |
# A_W*_grav zeros(N-1,N-1) G_W | |
# zeros(N,N) D_Θ zeros(N,N)]) | |
end | |
function discrete_hydrostatic_balance!(ρ, w, ρθ, Δz::Float64, _grav::Float64, Π::Function) | |
for i = 1:length(ρ)-1 | |
ρ[i+1] = ρθ[i+1]/(-2Δz*_grav/(Π(ρθ[i+1]) - Π(ρθ[i])) - ρθ[i]/ρ[i]) | |
end | |
end | |
function linsolve!(::Type{Val{:init}},f,u0;kwargs...) | |
function _linsolve!(x,A,b,update_matrix=false;kwargs...) | |
_A = RecursiveFactorization.lu!(A) | |
ldiv!(x,_A,b) | |
end | |
end | |
const DHB = false | |
const ndays = 2 | |
const N = 30 | |
const L = 30e3 | |
const Δz0 = L/N | |
const _MSLP = 1e5 | |
const _grav = 9.8 | |
const _R_m = 287.058 | |
const γ = 1.4 | |
const _C_p = _R_m * γ / (γ - 1) | |
const _C_v = _R_m / (γ - 1) | |
const _R_d = _R_m | |
function Π(ρθ) | |
ρθ > 0 || return NaN | |
_C_p*(_R_d*ρθ/_MSLP)^(_R_m/_C_v) | |
end | |
ρ = zeros(Float64, N) | |
ρθ = zeros(Float64, N) | |
w = zeros(Float64, N+1) | |
Δz = zeros(N+1) .+ L/N | |
for i = 1:N | |
z = (i-0.5)*L/N | |
Tvᵢ, pᵢ, ρᵢ = DecayingTemperatureProfile(z; T_virt_surf = 280.0, T_min_ref = 230.0, _R_d = _R_d, _grav = _grav, _MSLP = _MSLP) | |
ρ[i] = ρᵢ | |
ρθ[i] = ρᵢ*Tvᵢ*(_MSLP/pᵢ)^(_R_m/_C_p) | |
end | |
if DHB | |
discrete_hydrostatic_balance!(ρ, w, ρθ, Δz0, _grav, Π) | |
end | |
ss = Single_Stack(L, N, 0.0, copy(ρ), copy(w), copy(ρθ),copy(ρ), copy(w), copy(ρθ), _grav, γ, _R_m, Π) | |
max_wave_speed = compute_wave_speed(ρ, w, ρθ, _R_m, _C_p, γ, _MSLP) | |
@info "maximum Δt (cfl = 1) = " Δz0 / max_wave_speed | |
u0 = zeros(3*N+1) | |
combine!(ρ, w, ρθ, u0) | |
Δt = 600.0 | |
jac_prototype = zeros(3N+1, 3N+1) | |
jacobian!(jac_prototype,u0,ss,0.0) | |
jac_prototype = sparse(jac_prototype) | |
f = ODEFunction(spatial_residual, jac=jacobian!); #, jac_prototype = jac_prototype); | |
prob_ode_hydrostatic_balance = ODEProblem(f,u0,(0.,86400 * ndays),ss); | |
u1 = solve(prob_ode_hydrostatic_balance, Rosenbrock23(), dt = Δt, reltol=0.1) | |
u2 = solve(prob_ode_hydrostatic_balance, Rosenbrock23(linsolve=linsolve!), dt = Δt, reltol=0.1) | |
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[deps] | |
BlockBandedMatrices = "ffab5731-97b5-5995-9138-79e8c1846df0" | |
DiffEqOperators = "9fdde737-9c7f-55bf-ade8-46b3f136cc48" | |
DifferentialEquations = "0c46a032-eb83-5123-abaf-570d42b7fbaa" | |
LinearAlgebra = "37e2e46d-f89d-539d-b4ee-838fcccc9c8e" | |
RecursiveFactorization = "f2c3362d-daeb-58d1-803e-2bc74f2840b4" | |
SparseArrays = "2f01184e-e22b-5df5-ae63-d93ebab69eaf" |
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