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8 changes: 4 additions & 4 deletions docs/pages.jl
Original file line number Diff line number Diff line change
Expand Up @@ -22,8 +22,7 @@ pages = Any[
"model_creation/examples/basic_CRN_library.md",
"model_creation/examples/programmatic_generative_linear_pathway.md",
"model_creation/examples/hodgkin_huxley_equation.md",
"model_creation/examples/smoluchowski_coagulation_equation.md"
]
"model_creation/examples/smoluchowski_coagulation_equation.md"]
],
"Model simulation and visualization" => Any[
"model_simulation/simulation_introduction.md",
Expand Down Expand Up @@ -51,8 +50,8 @@ pages = Any[
# "inverse_problems/structural_identifiability.md",
"inverse_problems/global_sensitivity_analysis.md",
"Examples" => Any[
"inverse_problems/examples/ode_fitting_oscillation.md"
]
"inverse_problems/examples/ode_fitting_oscillation.md",
"inverse_problems/examples/SPR_fitting.md"]
],
"Spatial modelling" => Any[
"spatial_modelling/lattice_reaction_systems.md",
Expand All @@ -65,3 +64,4 @@ pages = Any[
"API" => "api.md",
"Developer Documentation" => "devdocs/dev_guide.md"
]

110 changes: 110 additions & 0 deletions docs/src/inverse_problems/examples/SPR_fitting.md
Original file line number Diff line number Diff line change
@@ -0,0 +1,110 @@
# [Surface Plasmon Resonance Model Example](@id surface_plasmon_resonance_model_Example)
This tutorial shows how to programmatically construct a ['ReactionSystem'](@ref) corresponding to the chemistry underlying the [Surface Plasmon Resonance Model](https://en.wikipedia.org/wiki/Surface_plasmon_resonance) using [ModelingToolkit](http://docs.sciml.ai/ModelingToolkit/stable/)/[Catalyst](http://docs.sciml.ai/Catalyst/stable/). You can find a simpler constructruction of this model [here](https://docs.sciml.ai/Catalyst/stable/catalyst_applications/parameter_estimation/) in the example of parameter estimation.
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https://docs.sciml.ai/Catalyst/stable/catalyst_applications/parameter_estimation/

This seems to be a link from an older version of the docs that no longer works / exists.


Using the symbolic interface, we will create our states/species, define our reactions, and add a discrete event. This model is simulated and used to generate sample data points with added noise and then used to fit parameters in iterations. This event will correspond to the time at which the antibody stop binding to antigen and switch to dissociating.
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Suggested change
Using the symbolic interface, we will create our states/species, define our reactions, and add a discrete event. This model is simulated and used to generate sample data points with added noise and then used to fit parameters in iterations. This event will correspond to the time at which the antibody stop binding to antigen and switch to dissociating.
Using the DSL interface, we will create our states/species, define our reactions, and add a discrete event. This model is simulated and used to generate sample data points with added noise and then used to fit parameters in iterations. This event will correspond to the time at which the antibody stop binding to antigen and switch to dissociating.


We begin by importing some necessary packages.
```julia
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```julia
```@example spr_ex

All of these should be @example blocks so that they run dynamically.

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Check out the Documenter.jl documentation for information on how to use such blocks, or look at the other Catalyst tutorials.

using ModelingToolkit, Catalyst
using Optimization, OptimizatizationOptimJL
using Plots
```
In this example, the concentration of antigen,`\beta` is varied to determine the constant of proportionality, `\alpha`, `k_{on}`(association rate constant), and `k_{off}` (dissociation rate constant) which characterized the binding interaction between the antigen and the immobilized receptor molecules on the sensor slide. We start by defining our reaction equations, parameters, variables, event, and states.
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Note that single quotes are for code rendering not math. They won't render \beta as $\beta$. If you build the documentation locally on your computer and check it looks ok you can see issues such as this.

```julia
osys = @reaction_network begin
@variables t
@parameters k_on=100.0 k_off α
@species A(t)B(t)

@discrete_events begin
t == switch_time => [k_on ~ 0.0]
end

α*k_on, A --> B
k_off, B --> A
end

switch_time = 2.0

tspan = (0.0, 4.0)
alpha_list = [0.1, 0.2, 0.3, 0.4] #list of concentrations
```
Iterating over values of `\alpha`, now we create a list of ODE solutions and set the initial conditions of our states and parameters.
```julia
results_list = []

u0 = [:A => 10.0, :B => 0.0]
p_real = [k_on => 100.0, k_off => 10.0, α => 1.0]
oprob = ODEProblem(osys, u0, tspan, p_real)
sample_times = range(tspan[1]; stop = tspan[2], length = 1001)

for alpha in alpha_list
p_real = [k_on => 100.0, k_off => 10.0, α => alpha]
oprobr = remake(oprob, p=p_real)
sol_real = solve(oprobr, Tsit5(); tstops = sample_times)

push!(results_list, sol_real(sample_times))
end
```
```@example ceq3
default(; lw = 3, framestyle = :box, size = (800, 400))
p = plot()
plot(p, sample_times, results_list[1][2,:])
plot!(p, sample_times, results_list[2][2,:])
plot!(p, sample_times, results_list[3][2,:])
plot!(p, sample_times, results_list[4][2,:])
Comment on lines +52 to +55
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Just use a loop.


sample_vals = []
for result in results_list
sample_val = Array(result)
sample_val .*= (1 .+ .1 * rand(Float64, size(sample_val)) .- .01)
push!(sample_vals, sample_val)
end

for val in sample_vals
scatter!(p, sample_times, val[2,:]; color = [:blue :red], legend = nothing)
end
plot(p)
```
Next, we create a function to fit the parameters. Here we are using `NelderMead()`. In order to achieve a better fit, we are incorporating all of our solutions into the loss function. We will fit seperately the association and dissociation signals so for the first estimate, `tend < switch_time`.
```julia
function optimise_p(pinit, tend)
function loss(p, _)
newtimes = filter(<=(tend), sample_times)
solutions = []
for alpha in alpha_list
newprob = remake(oprob; tspan = (0.0, tend), p = [k_on => p[1],k_off => p[2],α => alpha])
sol = Array(solve(newprob, Tsit5(); saveat = newtimes, tstops = switch_time))
push!(solutions,sol[2,:])
end
loss = 0
for (idx, solution) in enumerate(solutions)
loss += sum(abs2, p[3]*solution .- sample_vals[idx][2, 1:size(sol,2)])
end

return loss
end

optf = OptimizationFunction(loss)

optprob = OptimizationProblem(optf, pinit)
sol = solve(optprob, Optim.NelderMead())

return sol.u
end

p_estimate = optimise_p([100.0, 10.0, 1.0], 1.5)
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p_estimate = optimise_p([100.0, 10.0, 1.0], 1.5)
p_estimate = optimise_p([100.0, 10.0, 1.0], 1.5)

Shouldn't tend here by switch_time? Why are you setting it to be smaller?

```
Finally, we remake the solution using the estimate, fit the entire time span for some `alpha`, and plot the solution.
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But you don't seem to be fitting a second time using the parameters from the first fit?

```julia
alpha = 0.2
newprob = remake(oprob; tspan = (0.0, 4.0), p = [k_on => p_estimate[1], k_off => p_estimate[2], α => alpha])
newsol = solve(newprob, Tsit5(); tstops = switch_time)

#plotting simulated sample date with new solution
default(; lw = 3, framestyle = :box, size = (800, 400))

scatter!(sample_times, sample_vals; color = [:darkblue :darkred], legend = nothing)

plot!(newsol[2,:]; legend = nothing, color = [:blue :red], linestyle = :dash, tspan= (0.0, 4.0))
```
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