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basic distribution and getters based on GRF.jl
Project.toml format add plot to tests fix global_rng consistency improved interface and seperated coeff vs function sampling constrained sampling from distribution and testing sample from prior test changed transforms to be more consistent and compatible with func dists removed dimensional ambiguities in ndims for functions and tested c->u and u->c get_logpdf -> logpdf 2D examples, unit tests done docstrings codecov docstrings format docstring? docstrings Darcy example removed additional sampling in KL adjusted tests for user dist, and new func construction removed unnecessary functions plot bugfix fixed bug runtest removed rng from build without coeffs, more robust tests rm rng codecov
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################## | ||
# Copied on 3/16/23 and modified from | ||
# https://github.com/Zhengyu-Huang/InverseProblems.jl/blob/master/Fluid/Darcy-2D.jl | ||
################## | ||
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using JLD2 | ||
using Statistics | ||
using LinearAlgebra | ||
using Distributions | ||
using Random | ||
using SparseArrays | ||
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mutable struct Setup_Param{FT <: AbstractFloat, IT <: Int} | ||
# physics | ||
N::IT # number of grid points for both x and y directions (including both ends) | ||
Δx::FT | ||
xx::AbstractVector{FT} # uniform grid [a, a+Δx, a+2Δx ... b] (in each dimension) | ||
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#for source term | ||
f_2d::AbstractMatrix{FT} | ||
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κ::AbstractMatrix{FT} | ||
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# observation locations is tensor product x_locs × y_locs | ||
x_locs::AbstractVector{IT} | ||
y_locs::AbstractVector{IT} | ||
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N_y::IT | ||
end | ||
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function Setup_Param( | ||
xx::AbstractVector{FT}, | ||
obs_ΔN::IT, | ||
κ::AbstractMatrix; | ||
seed::IT = 123, | ||
) where {FT <: AbstractFloat, IT <: Int} | ||
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N = length(xx) | ||
Δx = xx[2] - xx[1] | ||
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# logκ_2d, φ, λ, θ_ref = generate_θ_KL(xx, N_KL, d, τ, seed=seed) | ||
f_2d = compute_f_2d(xx) | ||
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x_locs = Array(obs_ΔN:obs_ΔN:(N - obs_ΔN)) | ||
y_locs = Array(obs_ΔN:obs_ΔN:(N - obs_ΔN)) | ||
N_y = length(x_locs) * length(y_locs) | ||
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Setup_Param(N, Δx, xx, f_2d, κ, x_locs, y_locs, N_y) | ||
end | ||
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#= | ||
A hardcoding source function, | ||
which assumes the computational domain is | ||
[0 1]×[0 1] | ||
f(x,y) = f(y), | ||
which dependes only on y | ||
=# | ||
function compute_f_2d(yy::AbstractVector{FT}) where {FT <: AbstractFloat} | ||
N = length(yy) | ||
f_2d = zeros(FT, N, N) | ||
for i in 1:N | ||
if (yy[i] <= 4 / 6) | ||
f_2d[:, i] .= 1000.0 | ||
elseif (yy[i] >= 4 / 6 && yy[i] <= 5 / 6) | ||
f_2d[:, i] .= 2000.0 | ||
elseif (yy[i] >= 5 / 6) | ||
f_2d[:, i] .= 3000.0 | ||
end | ||
end | ||
return f_2d | ||
end | ||
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""" | ||
run_G_ensemble(darcy,κs::AbstractMatrix) | ||
Computes the forward map `G` (`solve_Darcy_2D` followed by `compute_obs`) over an ensemble of `κ`'s, stored flat as columns of `κs` | ||
""" | ||
function run_G_ensemble(darcy, κs::AbstractMatrix) | ||
N_ens = size(κs, 2) # ens size | ||
nd = darcy.N_y #num obs | ||
g_ens = zeros(nd, N_ens) | ||
for i in 1:N_ens | ||
# run the model with the current parameters, i.e., map θ to G(θ) | ||
κ_i = reshape(κs[:, i], darcy.N, darcy.N) # unflatten | ||
h_i = solve_Darcy_2D(darcy, κ_i) # run model | ||
g_ens[:, i] = compute_obs(darcy, h_i) # observe solution | ||
end | ||
return g_ens | ||
end | ||
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#= | ||
return the unknow index for the grid point | ||
Since zero-Dirichlet boundary conditions are imposed on | ||
all four edges, the freedoms are only on interior points | ||
=# | ||
function ind(darcy::Setup_Param{FT, IT}, ix::IT, iy::IT) where {FT <: AbstractFloat, IT <: Int} | ||
return (ix - 1) + (iy - 2) * (darcy.N - 2) | ||
end | ||
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function ind_all(darcy::Setup_Param{FT, IT}, ix::IT, iy::IT) where {FT <: AbstractFloat, IT <: Int} | ||
return ix + (iy - 1) * darcy.N | ||
end | ||
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#= | ||
solve Darcy equation with finite difference method: | ||
-∇(κ∇h) = f | ||
with Dirichlet boundary condition, h=0 on ∂Ω | ||
=# | ||
function solve_Darcy_2D(darcy::Setup_Param{FT, IT}, κ_2d::AbstractMatrix{FT}) where {FT <: AbstractFloat, IT <: Int} | ||
Δx, N = darcy.Δx, darcy.N | ||
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indx = IT[] | ||
indy = IT[] | ||
vals = FT[] | ||
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f_2d = darcy.f_2d | ||
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𝓒 = Δx^2 | ||
for iy in 2:(N - 1) | ||
for ix in 2:(N - 1) | ||
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ixy = ind(darcy, ix, iy) | ||
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#top | ||
if iy == N - 1 | ||
#ft = -(κ_2d[ix, iy] + κ_2d[ix, iy+1])/2.0 * (0 - h_2d[ix,iy]) | ||
push!(indx, ixy) | ||
push!(indy, ixy) | ||
push!(vals, (κ_2d[ix, iy] + κ_2d[ix, iy + 1]) / 2.0 / 𝓒) | ||
else | ||
#ft = -(κ_2d[ix, iy] + κ_2d[ix, iy+1])/2.0 * (h_2d[ix,iy+1] - h_2d[ix,iy]) | ||
append!(indx, [ixy, ixy]) | ||
append!(indy, [ixy, ind(darcy, ix, iy + 1)]) | ||
append!( | ||
vals, | ||
[(κ_2d[ix, iy] + κ_2d[ix, iy + 1]) / 2.0 / 𝓒, -(κ_2d[ix, iy] + κ_2d[ix, iy + 1]) / 2.0 / 𝓒], | ||
) | ||
end | ||
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#bottom | ||
if iy == 2 | ||
#fb = (κ_2d[ix, iy] + κ_2d[ix, iy-1])/2.0 * (h_2d[ix,iy] - 0) | ||
push!(indx, ixy) | ||
push!(indy, ixy) | ||
push!(vals, (κ_2d[ix, iy] + κ_2d[ix, iy - 1]) / 2.0 / 𝓒) | ||
else | ||
#fb = (κ_2d[ix, iy] + κ_2d[ix, iy-1])/2.0 * (h_2d[ix,iy] - h_2d[ix,iy-1]) | ||
append!(indx, [ixy, ixy]) | ||
append!(indy, [ixy, ind(darcy, ix, iy - 1)]) | ||
append!( | ||
vals, | ||
[(κ_2d[ix, iy] + κ_2d[ix, iy - 1]) / 2.0 / 𝓒, -(κ_2d[ix, iy] + κ_2d[ix, iy - 1]) / 2.0 / 𝓒], | ||
) | ||
end | ||
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#right | ||
if ix == N - 1 | ||
#fr = -(κ_2d[ix, iy] + κ_2d[ix+1, iy])/2.0 * (0 - h_2d[ix,iy]) | ||
push!(indx, ixy) | ||
push!(indy, ixy) | ||
push!(vals, (κ_2d[ix, iy] + κ_2d[ix + 1, iy]) / 2.0 / 𝓒) | ||
else | ||
#fr = -(κ_2d[ix, iy] + κ_2d[ix+1, iy])/2.0 * (h_2d[ix+1,iy] - h_2d[ix,iy]) | ||
append!(indx, [ixy, ixy]) | ||
append!(indy, [ixy, ind(darcy, ix + 1, iy)]) | ||
append!( | ||
vals, | ||
[(κ_2d[ix, iy] + κ_2d[ix + 1, iy]) / 2.0 / 𝓒, -(κ_2d[ix, iy] + κ_2d[ix + 1, iy]) / 2.0 / 𝓒], | ||
) | ||
end | ||
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#left | ||
if ix == 2 | ||
#fl = (κ_2d[ix, iy] + κ_2d[ix-1, iy])/2.0 * (h_2d[ix,iy] - 0) | ||
push!(indx, ixy) | ||
push!(indy, ixy) | ||
push!(vals, (κ_2d[ix, iy] + κ_2d[ix - 1, iy]) / 2.0 / 𝓒) | ||
else | ||
#fl = (κ_2d[ix, iy] + κ_2d[ix-1, iy])/2.0 * (h_2d[ix,iy] - h_2d[ix-1,iy]) | ||
append!(indx, [ixy, ixy]) | ||
append!(indy, [ixy, ind(darcy, ix - 1, iy)]) | ||
append!( | ||
vals, | ||
[(κ_2d[ix, iy] + κ_2d[ix - 1, iy]) / 2.0 / 𝓒, -(κ_2d[ix, iy] + κ_2d[ix - 1, iy]) / 2.0 / 𝓒], | ||
) | ||
end | ||
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end | ||
end | ||
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df = sparse(indx, indy, vals, (N - 2)^2, (N - 2)^2) | ||
# Multithread does not support sparse matrix solver | ||
h = df \ (f_2d[2:(N - 1), 2:(N - 1)])[:] | ||
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h_2d = zeros(FT, N, N) | ||
h_2d[2:(N - 1), 2:(N - 1)] .= reshape(h, N - 2, N - 2) | ||
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return h_2d | ||
end | ||
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#= | ||
Compute observation values | ||
=# | ||
function compute_obs(darcy::Setup_Param{FT, IT}, h_2d::AbstractMatrix{FT}) where {FT <: AbstractFloat, IT <: Int} | ||
# X---X(1)---X(2) ... X(obs_N)---X | ||
obs_2d = h_2d[darcy.x_locs, darcy.y_locs] | ||
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return obs_2d[:] | ||
end |
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[deps] | ||
Distributions = "31c24e10-a181-5473-b8eb-7969acd0382f" | ||
EnsembleKalmanProcesses = "aa8a2aa5-91d8-4396-bcef-d4f2ec43552d" | ||
GaussianRandomFields = "e4b2fa32-6e09-5554-b718-106ed5adafe9" | ||
JLD2 = "033835bb-8acc-5ee8-8aae-3f567f8a3819" | ||
LinearAlgebra = "37e2e46d-f89d-539d-b4ee-838fcccc9c8e" | ||
Plots = "91a5bcdd-55d7-5caf-9e0b-520d859cae80" | ||
Random = "9a3f8284-a2c9-5f02-9a11-845980a1fd5c" | ||
SparseArrays = "2f01184e-e22b-5df5-ae63-d93ebab69eaf" | ||
Statistics = "10745b16-79ce-11e8-11f9-7d13ad32a3b2" |
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