From 726ec09882e97363dd910eda02f467b35d8c58e0 Mon Sep 17 00:00:00 2001 From: Astrid Giuliani Date: Tue, 9 Jul 2024 18:10:56 +0200 Subject: [PATCH] fix pages names and add problem def --- docs/make.jl | 8 ++++---- docs/src/index.md | 29 ++++++++++++++++++++++++++++- 2 files changed, 32 insertions(+), 5 deletions(-) diff --git a/docs/make.jl b/docs/make.jl index 76fca97..815b1be 100644 --- a/docs/make.jl +++ b/docs/make.jl @@ -4,11 +4,11 @@ makedocs( sitename = "AveragedKepler", format = Documenter.HTML(prettyurls = false), pages = [ - "Home" => "index.md", + "Problem definition" => "index.md", "3D Visualization" => [ - "synthesis.md", - "spheres.md", - "geodesics.md", + "Optimal Synthesis" => "synthesis.md", + "Spheres" => "spheres.md", + "Geodesics" => "geodesics.md", ], ] ) diff --git a/docs/src/index.md b/docs/src/index.md index 3359da5..ed2594a 100644 --- a/docs/src/index.md +++ b/docs/src/index.md @@ -1 +1,28 @@ -# Averaged Kepler problem \ No newline at end of file +# The averaged Kepler problem + +We consider the Hamiltonian + +$$ + H(r, \theta, p_r, p_\theta) = v p_\theta + \Vert p \Vert_{g} +$$ + +where $v$ is a constant, $p = (p_r, p_\theta)$, and $\Vert \cdot \Vert_{g}$ is the norm induced by the metric + +$$ + g = \mathrm{d}r^2 + m_\lambda^2(r)\, \mathrm{d}\theta^2, \quad + m_\lambda^2(r) = \frac{\sin^2 r}{1 - \lambda \sin^2 r} +$$ + +with $\lambda = 4/5$. + +Along the geodesics, we have $H+p^0 = 0$. The parameter $p^0$ is constant equal to $-1$ (hyperbolic), $0$ (abnormal) or $1$ (elliptic). + +**Remark.** We can parameterize the geodesics by the norm of the initial convector, setting $\Vert{p_0}\Vert_g = 1$. +This amounts to parameterize by the initial angle $\alpha_0$: +$$ + p_r = \sin \alpha_0, \quad p_\theta = m_\lambda(r) \cos \alpha_0. +$$ +In that case, the hyperbolic geodeics are given by +$$ + p_\theta\, v + 1 = v\, m_\lambda(r) \cos \alpha_0 + 1 > 0. +$$ \ No newline at end of file