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Update docs/src/catalyst_applications/dynamical_systems.md
Co-authored-by: George Datseris <[email protected]>
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docs/src/catalyst_applications/dynamical_systems.md

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@@ -55,7 +55,7 @@ More information on how to compute basins of attractions for ODEs using Dynamica
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While Lyapunov exponents can be used for other purposes, they are primarily used to characterise [*chaotic behaviours*](https://en.wikipedia.org/wiki/Chaos_theory) (where small changes in initial conditions has large effect on the resulting trajectories). Generally, an ODE exhibit chaotic behaviour if its attractor(s) have *at least one* positive Lyapunov exponent. Practically, Lyapunov exponents can be computed using DynamicalSystems.jl's `lyapunovspectrum` function. Here we will use it to investigate two models, one which exhibits chaos and one which do not.
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First, let us consider the [Willamowski–Rössler](https://www.degruyter.com/document/doi/10.1515/zna-1980-0308/html?lang=en) model, which is known to exhibit chaotic behaviours.
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First, let us consider the [Willamowski–Rössler](https://www.degruyter.com/document/doi/10.1515/zna-1980-0308/html?lang=en) model, which is known to exhibit chaotic behaviour.
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```@example dynamical_systems_lyapunov
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using Catalyst
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wr_model = @reaction_network begin

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