Faili:Quadruple pendulum normal modes.gif

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Muhtasari

Maelezo
English: A quadruple pendulum has 4 degrees of freedom and thus 4 "orthogonal" modes. If the system was linear, those modes would be truly orthogonal and wouldn't interact. But since this is a non-linear system, the modes are coupled and can exchange energy.
Tarehe
Chanzo https://twitter.com/j_bertolotti/status/1493969051659517956
Mwandishi Jacopo Bertolotti
Ruhusa
(Kutumia faili tena)
https://twitter.com/j_bertolotti/status/1030470604418428929

Mathematica 13.0 code

npendula = 4; (*In principle the code can run with any number of pendula, but some minor adjustments might be needed here and there to be sure to select the right frequencies etc.*)
\[Theta] = ToExpression[ StringJoin["\[Theta]", #] & /@ Evaluate[ToString /@ Range[npendula]]];
l = ToExpression[StringJoin["l", #] & /@ Evaluate[ToString /@ Range[npendula]]];
 m = ToExpression[StringJoin["m", #] & /@ Evaluate[ToString /@ Range[npendula]]];
 g =.;
p = {0, 0};
pos = Reap[For[j = 1, j <= npendula, j++,
    p = p + l[[j]] {Sin[\[Theta][[j]][t]], -Cos[\[Theta][[j]][t]]};
    Sow[p];
    ]][[2, 1]];
vel = D[#, t] & /@ pos;
T = FullSimplify[Sum[m[[j]]/2 (vel[[j, 1]]^2 + vel[[j, 2]]^2), {j, 1, npendula}] ];
V = g Sum[m[[j]] *pos[[j, 2]], {j, 1, npendula}];
L = T - V; (*Lagrangian of the system*)
eq = Flatten[Table[
    FullSimplify[
     (D[D[L, Evaluate[D[\[Theta][[j]][t], t]] ], t] - 
        D[L, \[Theta][[j]][t] ]) == 0
     ]
    , {j, 1, npendula}] ] /. {Join[{ g -> 1}, 
    Table[l[[j]] -> 1, {j, 1, npendula}], 
    Table[m[[j]] -> 1, {j, 1, npendula}]]}; (*Equations of motion*)
L1 = (Normal@Series[(L /. Flatten@Join[
         Table[{\[Theta][[j]][t] -> \[Epsilon] \[Theta][[j]][t]}, {j, 
           1, npendula}]
         ,
         Table[{\[Theta][[j]]'[
             t] -> \[Epsilon] \[Theta][[j]]'[t]}, {j, 1, npendula}]
         ]), {\[Epsilon], 0, 2}]) /. {\[Epsilon] -> 1}; (*Linearized Lagrangian*)
eq1 = Table[
   FullSimplify[
    (D[D[L1, \[Theta][[j]]'[t] ], t] - D[L1, \[Theta][[j]][t] ]) == 0
    ]
   , {j, 1, npendula}] // Flatten; (*Linearized equations of motion*)
f\[Theta] = 
  ToExpression[
   StringJoin["f\[Theta]", #] & /@ 
    Evaluate[ToString /@ Range[npendula]]]; (*Dummy variables*)
M = Normal@CoefficientArrays[Table[
      eq1[[j]] /. 
       Join[Table[\[Theta][[j]][t] -> f\[Theta][[j]], {j, 1, 
          npendula}],
        Table[\[Theta][[j]]'[t] -> I \[Omega] f\[Theta][[j]], {j, 1, 
          npendula}],
        Table[\[Theta][[j]]''[t] -> - \[Omega]^2 f\[Theta][[j]], {j, 
          1, npendula}] ]
      , {j, 1, npendula}], f\[Theta]][[2]];
naturalfreq1 = 
 N@Solve[Det[(M /. 
       Join[{g -> 1}, Table[l[[j]] -> 1, {j, 1 npendula}], 
        Table[m[[j]] -> 1, {j, 1 npendula}]])] == 0, \[Omega]]; (*Natural frequencies. Selecting the correct ones is probably the biggest thing to check if you use a odd number of pendula.*)
e = ToExpression[ StringJoin["e", #] & /@ Evaluate[ToString /@ Range[npendula]]]; (*Dummy variables*)
modes = Table[
  FullSimplify@ Solve[(M /. Join[{\[Omega] -> naturalfreq1[[2*j, 1, 2]], g -> 1}, Table[l[[j]] -> 1, {j, 1 npendula}], Table[m[[j]] -> 1, {j, 1 npendula}]]) . e == Table[0, {j, 1, npendula}], e]
  , {j, 1, npendula}];
orthogonalmodes = Simplify@Table[e/e1 /. modes[[j, 1]], {j, 1, npendula}]
metric = Normal@CoefficientArrays[eq1, Table[\[Theta][[j]]''[t], {j, 1, npendula}]][[2]]; (*If you are changing the number of pendula, make sure you are selecting the correct matrix.*)
metric1 = (metric /. {Join[{ g -> 1},  Table[l[[j]] -> 1, {j, 1, npendula}], Table[m[[j]] -> 1, {j, 1, npendula}]]})[[1]];
eq = Flatten[Table[
     FullSimplify[
      (D[D[L, Evaluate[D[\[Theta][[j]][t], t]] ], t] - 
         D[L, \[Theta][[j]][t] ]) == 0
      ]
     , {j, 1, npendula}] ] /. {Join[{ g -> 1}, 
     Table[l[[j]] -> 1, {j, 1, npendula}], 
     Table[m[[j]] -> 1, {j, 1, npendula}]]};
eqbound = (Join[eq, 
     Table[\[Theta][[j]][0] == 1.*orthogonalmodes[[1, j]], {j, 1, 
       npendula}], 
     Table[\[Theta][[j]]'[0] == 0, {j, 1, npendula}]]) /. {Join[{ 
      g -> 1}, Table[l[[j]] -> 1, {j, 1, npendula}], 
     Table[m[[j]] -> 1, {j, 1, npendula}]]};
vars = Table[\[Theta][[j]][t], {j, 1, npendula}];
tmax = 150;
sol = NDSolve[eqbound, vars, {t, 0, tmax}, Method -> {"EquationSimplification" -> "Residual"}] (*Solve the equations of motion.*)
solpos = (pos /. Table[l[[j]] -> 1, {j, 1, npendula}]) /. sol;
frames = Table[
   modepos = 
    Table[(pos /. Table[l[[j]] -> 1, {j, 1, npendula}]) /. 
      Table[\[Theta][[j]][t] -> orthogonalmodes[[k, j]]*
         Simplify[
           orthogonalmodes[[k]] . metric1 . 
            Evaluate[((Table[\[Theta][[j]][t], {j, 1, npendula}] /. 
                  sol) /. {t -> \[Tau]})[[1]] ] ]/(orthogonalmodes[[
             k]] . metric1 . orthogonalmodes[[k]])
       , {j, 1, npendula}], {k, 1, npendula}];
   GraphicsGrid[{{
      Graphics[{
        Line[Join[{{0, 0}}, Table[solpos[[1, j]], {j, 1, npendula}]] ],
        Disk[{0, 0}, 0.075], 
        Table[Disk[solpos[[1, j]], 0.1], {j, 1, npendula}],
        Text[
         Style["Quadruple pendulum", Bold, FontSize -> 14], {0, 3.5}]
        }, 
       PlotRange -> 
        1.1 {{-npendula, npendula}, {-npendula, npendula}}
       ]
      , SpanFromLeft,
      Graphics[{
        Line[
         Join[{{0, 0}}, Table[modepos[[1, j]], {j, 1, npendula}]] ],
        Disk[{0, 0}, 0.075], 
        Table[Disk[modepos[[1, j]], 0.1], {j, 1, npendula}],
        Text[
         Style["\!\(\*SuperscriptBox[\(1\), \(st\)]\) mode", Bold, 
          FontSize -> 14], {0, 3.5}]
        }, 
       PlotRange -> 
        1.1 {{-npendula, npendula}, {-npendula, npendula}}
       ]
      ,
      Graphics[{
        Line[
         Join[{{0, 0}}, Table[modepos[[2, j]], {j, 1, npendula}]] ],
        Disk[{0, 0}, 0.075], 
        Table[Disk[modepos[[2, j]], 0.1], {j, 1, npendula}],
        Text[
         Style["\!\(\*SuperscriptBox[\(2\), \(nd\)]\) mode", Bold, 
          FontSize -> 14], {0, 3.5}]
        }, 
       PlotRange -> 
        1.1 {{-npendula, npendula}, {-npendula, npendula}}
       ]
      }, {SpanFromAbove, SpanFromBoth,
      Graphics[{
        Line[
         Join[{{0, 0}}, Table[modepos[[3, j]], {j, 1, npendula}]] ],
        Disk[{0, 0}, 0.075], 
        Table[Disk[modepos[[3, j]], 0.1], {j, 1, npendula}],
        Text[
         Style["\!\(\*SuperscriptBox[\(3\), \(rd\)]\) mode", Bold, 
          FontSize -> 14], {0, 3.5}]
        }, 
       PlotRange -> 
        1.1 {{-npendula, npendula}, {-npendula, npendula}}
       ]
      ,
      Graphics[{
        Line[
         Join[{{0, 0}}, Table[modepos[[4, j]], {j, 1, npendula}]] ],
        Disk[{0, 0}, 0.075], 
        Table[Disk[modepos[[4, j]], 0.1], {j, 1, npendula}],
        Text[
         Style["\!\(\*SuperscriptBox[\(4\), \(th\)]\) mode", Bold, 
          FontSize -> 14], {0, 3.5}]
        }, 
       PlotRange -> 
        1.1 {{-npendula, npendula}, {-npendula, npendula}}
       ]
      }}, Frame -> All, ImageSize -> 600]
   , {t, 0, tmax/1, 0.3}];
ListAnimate[frames] (*Plot everything.*)

Hatimiliki

I, the copyright holder of this work, hereby publish it under the following license:
Creative Commons CC-Zero 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.

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Motion of a quadruple pendulum prjected on its normal modes.

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16 Februari 2022

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