File:Non chaotic double pendulum.gif
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Summary
[edit]DescriptionNon chaotic double pendulum.gif |
English: Does a chaotic system always behave chaotically?
Not really, as many chaotic systems have a subset of possible initial conditions that lead to a quasi-periodic motion. As an example, below are two sets (black and orange) of 20 double pendula each, all with the same initial energy, and each group starting with very similar initial conditions. The first group (black) spread out a little bit with time, but nearby initial conditions keeps evolving into nearby dynamics, which is typical of integrable systems. On the other hand the pendula in the second group (orange) also starts with similar initial condition, but after a short transient evolve each very differently from each other, which is a mark of a chaotic system. |
Date | |
Source | https://twitter.com/j_bertolotti/status/1693998359030452310 |
Author | Jacopo Bertolotti |
Permission (Reusing this file) |
https://twitter.com/j_bertolotti/status/1030470604418428929 |
Mathematica 13.1 code
[edit]H = -2 Cos[a] - Cos[a + b] + (la^2 - 2 (1 + Cos[b]) la lb + (3 + 2 Cos[b]) lb^2)/(3 - Cos[2 b]);
qs = {a, b}; ps = {la, lb};
stateVars = Join[qs, ps]; varsToFuncs = # -> #[t] & /@ stateVars;
Brack[f_, g_] := Sum[D[f, qs[[i]]] D[g, ps[[i]]] - D[f, ps[[i]]] D[g, qs[[i]]], {i, Length@qs}]
EOMs = (#'[t] == (Brack[#, H] /. varsToFuncs)) & /@ stateVars;
laSol = FullSimplify[Solve[En == H /. {a -> 0}, la] // First, Assumptions -> {b \[Element] Reals, lb \[Element] Reals, En \[Element] Reals}];
Discrim[En_, b_, lb_] := (4 + 2 En - lb^2 + 2 Cos[b]) (-3 + Cos[2 b])
InitConds[EE_, B_, Lb_] /; Discrim[EE, B, Lb] <= 0 := {a[0] == 0, la[0] == (Re[la] /. laSol /. {En -> EE, b -> B, lb -> Lb}), b[0] == B, lb[0] == Lb};
InitConds[EE_, B_, Lb_] /; Discrim[EE, B, Lb] > 0 := {a[0] == 0, la[0] == 0, b[0] == B, lb[0] == Lb};
energy = -1.5;
initconditiontest = {{energy, 0., -0.5}, {energy, 0., 0.8}};
npendula = 20;
initial1 = Table[{0, 0, RandomReal[{-0.001, 0.001}]}, {npendula}] + Threaded@initconditiontest[[1]];
sol1 = Table[
NDSolve[{EOMs, InitConds[energy, initial1[[j, 2]], initial1[[j, 3]] ] }, {a[t], b[t], la[t], lb[t]}, {t, 0, 500}], {j, 1, npendula}];
initial2 = Table[{0, 0, RandomReal[{-0.01, 0.01}]}, {npendula}] + Threaded@initconditiontest[[2]];
sol2 = Table[
NDSolve[{EOMs, InitConds[energy, initial2[[j, 2]], initial2[[j, 3]] ] }, {a[t], b[t], la[t], lb[t]}, {t, 0, 500}], {j, 1, npendula}];
pos1[t_] := {Sin[a[t]], -Cos[a[t]]};
pos2[t_] := pos1[t] + {Sin[a[t] + b[t]], -Cos[a[t] + b[t]]}
pendulumplot[j_, color_, \[Tau]_, sol_] := (Graphics[{
Disk[{0, 0}, 0.05], Disk[pos1[t], 0.1], Disk[pos2[t], 0.1], Thick, Line[{{0, 0}, pos1[t], pos2[t]}], color, Disk[pos1[t], 0.075], Disk[pos2[t], 0.075] }, PlotRange -> 2.2 {{-1, 1}, {0.3, -1}}] /. sol[[j]] /. {t -> \[Tau]})[[1]]
frames = Table[
GraphicsRow[{Show[
Table[pendulumplot[j, Black, \[Tau], sol1], {j, 1, npendula}]
],
Show[
Table[pendulumplot[j, Orange, \[Tau], sol2], {j, 1, npendula}]
]
}]
, {\[Tau], 0.01, 200, 0.2}];
ListAnimate[frames]
Licensing
[edit]This file is made available under the Creative Commons CC0 1.0 Universal Public Domain Dedication. | |
The person who associated a work with this deed has dedicated the work to the public domain by waiving all of their rights to the work worldwide under copyright law, including all related and neighboring rights, to the extent allowed by law. You can copy, modify, distribute and perform the work, even for commercial purposes, all without asking permission.
http://creativecommons.org/publicdomain/zero/1.0/deed.enCC0Creative Commons Zero, Public Domain Dedicationfalsefalse |
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current | 10:25, 24 August 2023 | 800 × 264 (7.05 MB) | Berto (talk | contribs) | Uploaded own work with UploadWizard |
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