add draft of material for Friday
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material/5_fri/optimizing_julia/optimizing_julia.jl
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material/5_fri/optimizing_julia/optimizing_julia.jl
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# # Optimizing Julia code
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# This session provides an introduction to optimizing Julia code.
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# The examples are developed with Julia v1.9.3.
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# First, we install all required packages
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import Pkg
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Pkg.activate(@__DIR__)
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Pkg.instantiate()
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# The markdown file is created from the source code using
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# [Literate.jl](https://github.com/fredrikekre/Literate.jl).
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# You can create the markdown file via
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using Literate
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Literate.markdown(joinpath(@__DIR__, "optimizing_julia.jl");
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flavor = Literate.CommonMarkFlavor())
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# ## Basics
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#
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# The Julia manual contains basic information about performance.
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# In particular, you should be familiar with
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#
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# - https://docs.julialang.org/en/v1/manual/performance-tips/
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# - https://docs.julialang.org/en/v1/manual/style-guide/
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#
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# if you care about performance.
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# ## Example: A linear advection simulation
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#
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# This is a classical partial differential equation (PDE) simulation setup.
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# If you are not familiar with it, just ignore what's going on - but we need
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# an example. This one is similar to several problematic cases I have seen
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# in practice.
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# First, we generate initial data and store it in a file.
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using HDF5
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x = range(-1.0, 1.0, length = 1000)
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dx = step(x)
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h5open("initial_data.h5", "w") do io
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u0 = sinpi.(x)
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write_dataset(io, "x", collect(x))
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write_dataset(io, "u0", u0)
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end
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# Next, we write our simulation code as a function - as we have learned from
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# the performance tips!
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function simulate()
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x, u0 = h5open("initial_data.h5", "r") do io
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read_dataset(io, "x"), read_dataset(io, "u0")
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end
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t = 0
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u = u0
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while t < t_end
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u = u + dt * rhs(u)
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t = t + dt
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end
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return t, x, u, u0
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end
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function rhs(u)
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du = similar(u)
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for i in eachindex(u)
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im1 = i == firstindex(u) ? lastindex(u) : (i - 1)
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du[i] = -(u[i] - u[im1]) / dx
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end
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return du
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end
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# Now, we can define our parameters, run a simulation,
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# and plot the results.
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using Plots, LaTeXStrings
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t_end = 2.5
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dt = 0.9 * dx
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t, x, u, u0 = simulate()
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plot(x, u0; label = L"u_0", xguide = L"x")
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plot!(x, u; label = L"u")
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# Maybe you can already spot problems in the code above.
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# Anyway, before you begin optimizing some code, you should
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# test it and make sure it's correct. Let's assume this is the
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# case here. You should write tests making sure that the code
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# continues to work as expected while we optimize it. We will
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# not do this here right now.
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# ## Profiling
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#
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# First, we need to measure the performance of our code to
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# see whether it's already reasonable. For this, you can use
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# `@time` - or better BenchmarkTools.jl.
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using BenchmarkTools
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@benchmark simulate()
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# This shows quite a lot of allocations - typically a bad sign
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# if you are working with numerical simulations.
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# There are also profiling tools available in Julia.
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# Some of them are already loaded in the Visual Studio Code
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# extension for Julia. If you prefer working in the REPL,
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# you can install ProfileView.jl (`@profview simulate()`) and
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# PProf.jl (`pprof()` after creating a profile via `@profview`).
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@profview simulate()
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# Task: Optimize the code!
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# ## Introduction to generic Julia code and AD
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#
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# One of the strengths of Julia is that you can use quite a few
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# modern tools like AD. However, you need to learn Julia a bit
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# to use everything efficiently.
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# Here, we concentrate on ForwardDiff.jl.
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using ForwardDiff
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using Statistics
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function foo0(x)
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vector = zeros(typeof(x), 100)
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foo0!(vector, x)
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end
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function foo0!(vector, scalar)
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for i in eachindex(vector)
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vector[i] = atan(i * scalar) / π
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end
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for _ in 1:1000
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for i in eachindex(vector)
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vector[i] = cos(vector[i])
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end
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end
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return mean(vector)
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end
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let x = 2 * π
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@show foo0(x)
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@show ForwardDiff.derivative(foo0, x)
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@benchmark foo0($x)
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end
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# The code above is basically a fixed point iteration.
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# By doing some analysis, one could figure out that it
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# should converge to the solution `x` of `x == cos(x)`,
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# the "Dottie number". See https://en.wikipedia.org/wiki/Dottie_number
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using SimpleNonlinearSolve
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function dottie_number()
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f(u, p) = cos(u) - u
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bounds = (0.0, 2.0)
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prob = IntervalNonlinearProblem(f, bounds)
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sol = solve(prob, ITP())
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return sol.u
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end
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dottie_number()
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# Next, we introduce a custom struct. Can you spot the problems?
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struct MyData1
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scalar
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vector
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end
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function foo1(x)
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data = MyData1(x, zeros(typeof(x), 100))
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foo1!(data)
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end
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function foo1!(data)
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(; scalar, vector) = data
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for i in eachindex(vector)
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vector[i] = atan(i * scalar) / π
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end
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for _ in 1:1000
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for i in eachindex(vector)
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vector[i] = cos(vector[i])
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end
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end
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return mean(vector)
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end
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let x = 2 * π
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@show foo1(x)
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@show ForwardDiff.derivative(foo1, x)
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@benchmark foo1($x)
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end
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# We can fix type instabilities by introducing types explicitly.
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# But we lose the possibility to use AD this way!
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struct MyData2
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scalar::Float64
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vector::Vector{Float64}
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end
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function foo2(x)
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data = MyData2(x, zeros(typeof(x), 100))
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foo1!(data)
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end
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let x = 2 * π
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@show foo2(x)
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@benchmark foo2($x)
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end
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let x = 2 * π
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ForwardDiff.derivative(foo2, x)
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end
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# Thus, we need parametric types!
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struct MyData3{T}
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scalar::T
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vector::Vector{T}
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end
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function foo3(x)
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data = MyData3(x, zeros(typeof(x), 100))
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foo1!(data)
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end
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let x = 2 * π
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@show foo3(x)
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@show ForwardDiff.derivative(foo3, x)
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@benchmark foo3($x)
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end
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