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added example, fixed multi dependant variable case, verfied performan…
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…ce for special likelihood term
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AstitvaAggarwal committed Sep 1, 2023
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143 changes: 143 additions & 0 deletions docs/src/examples/Lotka_Volterra_BPINNs.md
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# Bayesian Physics informed Neural Network ODEs Solvers

Most of the scientific community deals with the basic problem of trying to mathematically model the reality around them and this often involves dynamical systems. The general trend to model these complex dynamical systems is through the use of differential equations.
Differential equation models often have non-measurable parameters.
The popular “forward-problem” of simulation consists of solving the differential equations for a given set of parameters, the “inverse problem” to simulation, known as parameter estimation, is the process of utilizing data to determine these model parameters.
Bayesian inference provides a robust approach to parameter estimation with quantified uncertainty.

## The Lotka-Volterra Model

The Lotka–Volterra equations, also known as the predator–prey equations, are a pair of first-order nonlinear differential equations.
These differential equations are frequently used to describe the dynamics of biological systems in which two species interact, one as a predator and the other as prey.
The populations change through time according to the pair of equations

$$
\begin{aligned}
\frac{\mathrm{d}x}{\mathrm{d}t} &= (\alpha - \beta y(t))x(t), \\
\frac{\mathrm{d}y}{\mathrm{d}t} &= (\delta x(t) - \gamma)y(t)
\end{aligned}
$$

where $x(t)$ and $y(t)$ denote the populations of prey and predator at time $t$, respectively, and $\alpha, \beta, \gamma, \delta$ are positive parameters.

We implement the Lotka-Volterra model and simulate it with parameters $\alpha = 1.5$, $\beta = 1$, $\gamma = 3$, and $\delta = 1$ and initial conditions $x(0) = y(0) = 1$.

```julia
# Define Lotka-Volterra model.
function lotka_volterra(du, u, p, t)
# Model parameters.
α, β, γ, δ = p
# Current state.
x, y = u

# Evaluate differential equations.
du[1] =- β * y) * x # prey
du[2] =* x - γ) * y # predator

return nothing
end

# Define initial-value problem.
u0 = [1.0, 1.0]
p = [1.5, 1.0, 3.0, 1.0]
tspan = (0.0, 10.0)
prob = ODEProblem(lotka_volterra, u0, tspan, p)

# Plot simulation.
plot(solve(prob, Tsit5()))

solution = solve(prob, Tsit5(); saveat = 0.05)

time = solution.t
u = hcat(solution.u...)
# BPINN AND TRAINING DATASET CREATION, NN create, Reconstruct
x = u[1, :] + 0.5 * randn(length(u[1, :]))
y = u[2, :] + 0.5 * randn(length(u[1, :]))
dataset = [x[1:50], y[1:50], time[1:50]]

# NN has 2 outputs as u -> [dx,dy]
chainlux1 = Lux.Chain(Lux.Dense(1, 6, Lux.tanh), Lux.Dense(6, 6, Lux.tanh),
Lux.Dense(6, 2))
chainflux1 = Flux.Chain(Flux.Dense(1, 6, tanh), Flux.Dense(6, 6, tanh), Flux.Dense(6, 2))
```

We generate noisy observations to use for the parameter estimation tasks in this tutorial.
With the [`saveat` argument](https://docs.sciml.ai/latest/basics/common_solver_opts/) we can specify that the solution is stored only at `saveat` time units(default saveat=1 / 50.0).
To make the example more realistic we add random normally distributed noise to the simulation.


```julia
alg1 = NeuralPDE.BNNODE(chainflux1,
dataset = dataset,
draw_samples = 1000,
l2std = [
0.05,
0.05,
],
phystd = [
0.05,
0.05,
],
priorsNNw = (0.0,
3.0),
param = [
Normal(4.5,
5),
Normal(7,
2),
Normal(5,
2),
Normal(-4,
6),
],
n_leapfrog = 30, progress = true)

sol_flux_pestim = solve(prob, alg1)


alg2 = NeuralPDE.BNNODE(chainlux1,
dataset = dataset,
draw_samples = 1000,
l2std = [
0.05,
0.05,
],
phystd = [
0.05,
0.05,
],
priorsNNw = (0.0,
3.0),
param = [
Normal(4.5,
5),
Normal(7,
2),
Normal(5,
2),
Normal(-4,
6),
],
n_leapfrog = 30, progress = true)

sol_lux_pestim = solve(prob, alg2)

#testing timepoints must match saveat timepoints of solve() call
t=collect(Float64,prob.tspan[1]:1/50.0:prob.tspan[2])

# plotting solution for x,y(NN approximate by .estimated_nn_params)
plot(t,sol_flux_pestim.ensemblesol[1])
plot!(t,sol_flux_pestim.ensemblesol[2])
sol_flux_pestim.estimated_nn_params

# estimated ODE parameters \alpha, \beta , \delta ,\gamma
sol_flux_pestim.estimated_ode_params

# plotting solution for x,y(NN approximate by .estimated_nn_params)
plot(t,sol_lux_pestim.ensemblesol[1])
plot!(t,sol_lux_pestim.ensemblesol[2])
sol_lux_pestim.estimated_nn_params

# estimated ODE parameters \alpha, \beta , \delta ,\gamma
sol_lux_pestim.estimated_ode_params
```
35 changes: 30 additions & 5 deletions src/BPINN_ode.jl
Original file line number Diff line number Diff line change
Expand Up @@ -250,12 +250,37 @@ function DiffEqBase.__solve(prob::DiffEqBase.ODEProblem,
throw(error("Only Lux.AbstractExplicitLayer and Flux.Chain neural networks are supported"))
end

nnparams = length(θinit)
# contructing ensemble predictions
ensemblecurves = Vector{}[]
# check if NN output is more than 1
numoutput = size(luxar[1])[1]
if numoutput > 1
# Initialize a vector to store the separated outputs for each output dimension
output_matrices = [Vector{Vector{Float32}}() for _ in 1:numoutput]

# Loop through each element in `luxar`
for element in luxar
for i in 1:numoutput
push!(output_matrices[i], element[i, :]) # Append the i-th output (i-th row) to the i-th output_matrices
end
end

for r in 1:numoutput
ensem_r = hcat(output_matrices[r]...)'
ensemblecurve_r = prob.u0[r] .+
[Particles(ensem_r[:, i]) for i in 1:length(t)] .*
(t .- prob.tspan[1])
push!(ensemblecurves, ensemblecurve_r)
end

ensemblecurve = prob.u0 .+
[Particles(reduce(vcat, luxar)[:, i]) for i in 1:length(t)] .*
(t .- prob.tspan[1])
else
ensemblecurve = prob.u0 .+
[Particles(reduce(vcat, luxar)[:, i]) for i in 1:length(t)] .*
(t .- prob.tspan[1])
push!(ensemblecurves, ensemblecurve)
end

nnparams = length(θinit)
estimnnparams = [Particles(reduce(hcat, samples)[i, :]) for i in 1:nnparams]

if ninv == 0
Expand All @@ -265,5 +290,5 @@ function DiffEqBase.__solve(prob::DiffEqBase.ODEProblem,
for i in (nnparams + 1):(nnparams + ninv)]
end

BPINNsolution(fullsolution, ensemblecurve, estimnnparams, estimated_params)
BPINNsolution(fullsolution, ensemblecurves, estimnnparams, estimated_params)
end
12 changes: 8 additions & 4 deletions src/advancedHMC_MCMC.jl
Original file line number Diff line number Diff line change
Expand Up @@ -184,10 +184,14 @@ function physloglikelihood(Tar::LogTargetDensity, θ)
for i in 1:length(Tar.prob.u0)
# can add phystd[i] for u[i]
physlogprob += logpdf(MvNormal(nnsol[i, :],
LinearAlgebra.Diagonal(map(abs2,
Tar.phystd[i] .*
ones(length(physsol[i, :]))))),
physsol[i, :])
LinearAlgebra.Diagonal(
map(abs2,
Tar.phystd[i] .*
ones(length(physsol[i, :]))
)
)
),
physsol[i, :])
end
return physlogprob
end
Expand Down
22 changes: 12 additions & 10 deletions test/BPINN_Tests.jl
Original file line number Diff line number Diff line change
Expand Up @@ -5,6 +5,8 @@ using Flux, OptimizationOptimisers, AdvancedHMC, Lux
using Statistics, Random, Functors, ComponentArrays
using NeuralPDE, MonteCarloMeasurements

# note that current testing bounds can be easily further tightened but have been inflated for support for Julia build v1
# on latest Julia version it performs much better for below tests
Random.seed!(100)

# for sampled params->lux ComponentArray
Expand Down Expand Up @@ -82,10 +84,10 @@ meanscurve2 = prob.u0 .+ (t .- prob.tspan[1]) .* luxmean
@test mean(abs.(physsol1 .- meanscurve2)) < 0.005

#--------------------- solve() call
@test mean(abs.(x̂1 .- sol1flux.ensemblesol)) < 0.05
@test mean(abs.(physsol0_1 .- sol1flux.ensemblesol)) < 0.05
@test mean(abs.(x̂1 .- sol1lux.ensemblesol)) < 0.05
@test mean(abs.(physsol0_1 .- sol1lux.ensemblesol)) < 0.05
@test mean(abs.(x̂1 .- sol1flux.ensemblesol[1])) < 0.05
@test mean(abs.(physsol0_1 .- sol1flux.ensemblesol[1])) < 0.05
@test mean(abs.(x̂1 .- sol1lux.ensemblesol[1])) < 0.05
@test mean(abs.(physsol0_1 .- sol1lux.ensemblesol[1])) < 0.05

## PROBLEM-1 (WITH PARAMETER ESTIMATION)
linear_analytic = (u0, p, t) -> u0 + sin(p * t) / (p)
Expand Down Expand Up @@ -189,10 +191,10 @@ meanscurve2 = prob.u0 .+ (t .- prob.tspan[1]) .* luxmean
@test abs(p - mean([fhsamples1[i][23] for i in 2000:2500])) < abs(0.2 * p)

#---------------------- solve() call
@test mean(abs.(x̂1 .- sol2flux.ensemblesol)) < 5e-1
@test mean(abs.(physsol1_1 .- sol2flux.ensemblesol)) < 5e-1
@test mean(abs.(x̂1 .- sol2lux.ensemblesol)) < 6e-2
@test mean(abs.(physsol1_1 .- sol2lux.ensemblesol)) < 6e-2
@test mean(abs.(x̂1 .- sol2flux.ensemblesol[1])) < 5e-1
@test mean(abs.(physsol1_1 .- sol2flux.ensemblesol[1])) < 5e-1
@test mean(abs.(x̂1 .- sol2lux.ensemblesol[1])) < 5e-1
@test mean(abs.(physsol1_1 .- sol2lux.ensemblesol[1])) < 5e-1

# ESTIMATED ODE PARAMETERS (NN1 AND NN2)
@test abs(p - sol2flux.estimated_ode_params[1]) < abs(0.1 * p)
Expand Down Expand Up @@ -350,14 +352,14 @@ param1 = mean(i[62] for i in fhsampleslux22[1000:1500])

#-------------------------- solve() call
# (flux chain)
@test mean(abs.(physsol2 .- sol3flux_pestim.ensemblesol)) < 8e-2
@test mean(abs.(physsol2 .- sol3flux_pestim.ensemblesol[1])) < 5e-2

# estimated parameters(flux chain)
param1 = sol3flux_pestim.estimated_ode_params[1]
@test abs(param1 - p) < abs(0.35 * p)

# (lux chain)
@prob mean(abs.(physsol2 .- sol3lux_pestim.ensemblesol)) < 5e-2
@prob mean(abs.(physsol2 .- sol3lux_pestim.ensemblesol[1])) < 5e-2

# estimated parameters(lux chain)
param1 = sol3lux_pestim.estimated_ode_params[1]
Expand Down

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