File:2 body problem on a sphere.gif
2_body_problem_on_a_sphere.gif (480 × 480 pixels, file size: 2.67 MB, MIME type: image/gif, looped, 200 frames, 20 s)
Captions
Summary[edit]
Description2 body problem on a sphere.gif |
English: The 2-body problem on a plane produces nice elliptical orbits. But the 2-body problem on a sphere (meaning that the distance is computed as the great-circle distance) can easily get quite chaotic. |
Date | |
Source | https://twitter.com/j_bertolotti/status/1263482519606919168 |
Author | Jacopo Bertolotti |
Permission (Reusing this file) |
https://twitter.com/j_bertolotti/status/1030470604418428929 |
Mathematica 12.0 code[edit]
ctop[p_, r_] := CoordinateTransform["Cartesian" -> "Spherical", p + {Sqrt[r^2 - 1], 0, 0}] m1 = 1; m2 = 1; G = 40; dist[\[Theta]1_, \[Theta]2_, \[Phi]1_, \[Phi]2_, r_] := r ArcTan[(\[Sqrt]((Cos[\[Pi]/2 - \[Theta]2] Sin[ RealAbs[\[Phi]1 - \[Phi]2]])^2 + (Cos[\[Pi]/ 2 - \[Theta]1] Sin[\[Pi]/2 - \[Theta]2] - Sin[\[Pi]/2 - \[Theta]1] Cos[\[Pi]/2 - \[Theta]2] Cos[ RealAbs[\[Phi]1 - \[Phi]2]])^2))/(Sin[\[Pi]/ 2 - \[Theta]1] Sin[\[Pi]/2 - \[Theta]2] + Cos[\[Pi]/2 - \[Theta]1] Cos[\[Pi]/2 - \[Theta]2] Cos[ RealAbs[\[Phi]1 - \[Phi]2]])] rl = 1000; point1l = ctop[{0, 0, 4}, rl] // N point2l = ctop[{0, 0.1, -3}, rl] // N stoc1l = CoordinateTransform[ "Spherical" -> "Cartesian", {rl, \[Theta]1[t], \[Phi]1[t]}]; stoc2l = CoordinateTransform[ "Spherical" -> "Cartesian", {rl, \[Theta]2[t], \[Phi]2[t]}]; L[t_] := m1/2 Total@(D[stoc1l, t]^2) + m2/2 Total@(D[stoc2l, t]^2) + ((m1 + m2) G)/ dist[\[Theta]1[t], \[Theta]2[t], \[Phi]1[t], \[Phi]2[t], rl] eq\[Theta]1 = D[D[L[t], \[Theta]1'[t] ], t] - D[L[t], \[Theta]1[t]] ; eq\[Phi]1 = D[D[L[t], \[Phi]1'[t] ], t] - D[L[t], \[Phi]1[t]] ; eq\[Theta]2 = D[D[L[t], \[Theta]2'[t] ], t] - D[L[t], \[Theta]2[t]] ; eq\[Phi]2 = D[D[L[t], \[Phi]2'[t] ], t] - D[L[t], \[Phi]2[t]] ; soll = NDSolve[{eq\[Theta]1 == 0, eq\[Phi]1 == 0, eq\[Theta]2 == 0, eq\[Phi]2 == 0, \[Theta]1[0] == point1l[[2]], \[Phi]1[0] == point1l[[3]], \[Theta]2[0] == point2l[[2]], \[Phi]2[0] == point2l[[3]], \[Theta]1'[0] == 0., \[Phi]1'[0] == -3/ rl, \[Theta]2'[0] == 0., \[Phi]2'[0] == 3/rl}, {\[Theta]1[ t], \[Phi]1[t], \[Theta]2[t], \[Phi]2[t]}, {t, 0, 200}] rs = 10; point1s = ctop[{0, 0, 4}, rs] // N point2s = ctop[{0, 0.1, -3}, rs] // N stoc1s = CoordinateTransform[ "Spherical" -> "Cartesian", {rs, \[Theta]1[t], \[Phi]1[t]}]; stoc2s = CoordinateTransform[ "Spherical" -> "Cartesian", {rs, \[Theta]2[t], \[Phi]2[t]}]; L[t_] := m1/2 Total@(D[stoc1s, t]^2) + m2/2 Total@(D[stoc2s, t]^2) + ((m1 + m2) G)/ dist[\[Theta]1[t], \[Theta]2[t], \[Phi]1[t], \[Phi]2[t], rs] eq\[Theta]1 = D[D[L[t], \[Theta]1'[t] ], t] - D[L[t], \[Theta]1[t]] ; eq\[Phi]1 = D[D[L[t], \[Phi]1'[t] ], t] - D[L[t], \[Phi]1[t]] ; eq\[Theta]2 = D[D[L[t], \[Theta]2'[t] ], t] - D[L[t], \[Theta]2[t]] ; eq\[Phi]2 = D[D[L[t], \[Phi]2'[t] ], t] - D[L[t], \[Phi]2[t]] ; sols = NDSolve[{eq\[Theta]1 == 0, eq\[Phi]1 == 0, eq\[Theta]2 == 0, eq\[Phi]2 == 0, \[Theta]1[0] == point1s[[2]], \[Phi]1[0] == point1s[[3]], \[Theta]2[0] == point2s[[2]], \[Phi]2[0] == point2s[[3]], \[Theta]1'[0] == 0., \[Phi]1'[0] == -6/ rs, \[Theta]2'[0] == 0., \[Phi]2'[0] == 6/rs}, {\[Theta]1[ t], \[Phi]1[t], \[Theta]2[t], \[Phi]2[t]}, {t, 0, 500}] p0 = Table[ Show[ ContourPlot3D[(x + Sqrt[rl^2 - 1])^2 + (y)^2 + (z)^2 == rl^2, {x, -50, 50}, {y, -50, 50}, {z, -50, 50}, ContourStyle -> None, Mesh -> 5, MeshStyle -> Directive[ White], Background -> Black, Boxed -> False, Axes -> False, PlotPoints -> 80] , Graphics3D[{ Orange, Sphere[Evaluate[{rl Cos[\[Phi]1[t]] Sin[\[Theta]1[t]] - Sqrt[ rl^2 - 1], rl Sin[\[Theta]1[t]] Sin[\[Phi]1[t]], rl Cos[\[Theta]1[t]]} /. soll][[1]] /. {t -> \[Tau]}, 1], Cyan, Sphere[ Evaluate[{rl Cos[\[Phi]2[t]] Sin[\[Theta]2[t]] - Sqrt[ rl^2 - 1], rl Sin[\[Theta]2[t]] Sin[\[Phi]2[t]], rl Cos[\[Theta]2[t]]} /. soll][[1]] /. {t -> \[Tau]}, 1] }] , ParametricPlot3D[ Evaluate[{rl Cos[\[Phi]1[t]] Sin[\[Theta]1[t]] - Sqrt[rl^2 - 1], rl Sin[\[Theta]1[t]] Sin[\[Phi]1[t]], rl Cos[\[Theta]1[t]]} /. soll][[1]], {t, 0.01, \[Tau]}, PlotStyle -> {Opacity[0.5], Orange}] , ParametricPlot3D[ Evaluate[{rl Cos[\[Phi]2[t]] Sin[\[Theta]2[t]] - Sqrt[rl^2 - 1], rl Sin[\[Theta]2[t]] Sin[\[Phi]2[t]], rl Cos[\[Theta]2[t]]} /. soll][[1]], {t, 0.001, \[Tau]}, PlotStyle -> {Opacity[0.5], Cyan}] , ViewVector -> {{40, 0, 0}, {0, 0, 0}}, ViewAngle -> 50*Degree ] , {\[Tau], 0, 66.4, 1}]; sinstep[t_] := Sin[\[Pi]/2 t]^2; p1 = Table[ Show[ ContourPlot3D[(x + Sqrt[rl^2 - 1])^2 + (y)^2 + (z)^2 == rl^2, {x, -50, 50}, {y, -50, 50}, {z, -50, 50}, ContourStyle -> None, Mesh -> 5, MeshStyle -> Directive[ White], Background -> Black, Boxed -> False, Axes -> False, PlotPoints -> 80] , Graphics3D[{ Orange, Sphere[Evaluate[{rl Cos[\[Phi]1[t]] Sin[\[Theta]1[t]] - Sqrt[ rl^2 - 1], rl Sin[\[Theta]1[t]] Sin[\[Phi]1[t]], rl Cos[\[Theta]1[t]]} /. soll][[1]] /. {t -> 0}, 1], Cyan, Sphere[ Evaluate[{rl Cos[\[Phi]2[t]] Sin[\[Theta]2[t]] - Sqrt[ rl^2 - 1], rl Sin[\[Theta]2[t]] Sin[\[Phi]2[t]], rl Cos[\[Theta]2[t]]} /. soll][[1]] /. {t -> 0}, 1] }] , ParametricPlot3D[ Evaluate[{rl Cos[\[Phi]1[t]] Sin[\[Theta]1[t]] - Sqrt[rl^2 - 1], rl Sin[\[Theta]1[t]] Sin[\[Phi]1[t]], rl Cos[\[Theta]1[t]]} /. soll][[1]], {t, 0, 33.2}, PlotStyle -> {Opacity[0.5 - 0.5 sinstep[\[Tau]] ], Orange}] , ParametricPlot3D[ Evaluate[{rl Cos[\[Phi]2[t]] Sin[\[Theta]2[t]] - Sqrt[rl^2 - 1], rl Sin[\[Theta]2[t]] Sin[\[Phi]2[t]], rl Cos[\[Theta]2[t]]} /. soll][[1]], {t, 0, 33.2}, PlotStyle -> {Opacity[0.5 - 0.5 sinstep[\[Tau]] ], Cyan}] , ViewVector -> {sinstep[\[Tau]] ({20, -20, 20} - {40, 0, 0}) + {40, 0, 0}, {0, 0, 0}}, ViewAngle -> 50*Degree ] , {\[Tau], 0, 1, 0.1}]; p2 = Table[ Show[ ContourPlot3D[(x + Sqrt[(sinstep[\[Tau]] (rs - rl) + rl)^2 - 1])^2 + (y)^2 + (z)^2 == (sinstep[\[Tau]] (rs - rl) + rl)^2, {x, -50, 50}, {y, -50, 50}, {z, -50, 50}, ContourStyle -> None, Mesh -> 5, MeshStyle -> Directive[ White], Background -> Black, Boxed -> False, Axes -> False, PlotPoints -> 80] , Graphics3D[{ Orange, Sphere[Evaluate[{rl Cos[\[Phi]1[t]] Sin[\[Theta]1[t]] - Sqrt[ rl^2 - 1], rl Sin[\[Theta]1[t]] Sin[\[Phi]1[t]], rl Cos[\[Theta]1[t]]} /. soll][[1]] /. {t -> 0}, 1], Cyan, Sphere[ Evaluate[{rl Cos[\[Phi]2[t]] Sin[\[Theta]2[t]] - Sqrt[ rl^2 - 1], rl Sin[\[Theta]2[t]] Sin[\[Phi]2[t]], rl Cos[\[Theta]2[t]]} /. soll][[1]] /. {t -> 0}, 1] }] , ViewVector -> {{20, -20, 20}, {0, 0, 0}}, ViewAngle -> 50*Degree ] , {\[Tau], 0, 1, 0.05}]; p3 = Table[ Show[ ContourPlot3D[(x + Sqrt[rs^2 - 1])^2 + (y)^2 + (z)^2 == rs^2, {x, -50, 50}, {y, -50, 50}, {z, -50, 50}, ContourStyle -> None, Mesh -> 5, MeshStyle -> Directive[ White], Background -> Black, Boxed -> False, Axes -> False, PlotPoints -> 30] , Graphics3D[{ Orange, Sphere[Evaluate[{rs Cos[\[Phi]1[t]] Sin[\[Theta]1[t]] - Sqrt[ rs^2 - 1], rs Sin[\[Theta]1[t]] Sin[\[Phi]1[t]], rs Cos[\[Theta]1[t]]} /. sols][[1]] /. {t -> \[Tau]}, 1], Cyan, Sphere[ Evaluate[{rs Cos[\[Phi]2[t]] Sin[\[Theta]2[t]] - Sqrt[ rs^2 - 1], rs Sin[\[Theta]2[t]] Sin[\[Phi]2[t]], rs Cos[\[Theta]2[t]]} /. sols][[1]] /. {t -> \[Tau]}, 1] }] , ParametricPlot3D[ Evaluate[{rs Cos[\[Phi]1[t]] Sin[\[Theta]1[t]] - Sqrt[rs^2 - 1], rs Sin[\[Theta]1[t]] Sin[\[Phi]1[t]], rs Cos[\[Theta]1[t]]} /. sols][[1]], {t, 0.01, \[Tau]}, PlotStyle -> {Opacity[0.5], Orange}] , ParametricPlot3D[ Evaluate[{rs Cos[\[Phi]2[t]] Sin[\[Theta]2[t]] - Sqrt[rs^2 - 1], rs Sin[\[Theta]2[t]] Sin[\[Phi]2[t]], rs Cos[\[Theta]2[t]]} /. sols][[1]], {t, 0.01, \[Tau]}, PlotStyle -> {Opacity[0.5], Cyan}] , ViewVector -> {{20, -20, 20}, {0, 0, 0}}, ViewAngle -> 50*Degree ] , {\[Tau], 0, 100, 1}]; ListAnimate[Join[p0, p1, p2, p3]]
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http://creativecommons.org/publicdomain/zero/1.0/deed.enCC0Creative Commons Zero, Public Domain Dedicationfalsefalse |
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