平均速度，作者：Chris King

"非吸引盆地和花瓣的離散速度：計算未逃逸點的平均離散速度軌跡：" ^[1]^[2]

 $\left\vert z_{n+1}-z_{n}\right\vert$

演算法

在動態平面，可以觀察到

填充的 Julia 集的外部（藍色），用等高線法著色，
Julia 集的內部，顯示無理流動（綠色），用速度的正弦著色

對於未逃逸的點，計算軌跡的平均離散速度

$\upsilon ={\frac {S_{n}}{n}}$

其中

$S_{n}=\sum _{n=1}^{n_{max}}d_{n}=\sum _{n=1}^{n_{max}}|Z_{n+1}-Z_{n}|$

在 Octave 中，它看起來像

# octave code
 d=0;
 iter = 0;

 while (iter < maxiter) && (abs(z)<ER)
   h=z; # previous point = z_(n)
   z=z*z+c; # next point = z_(n+1)
   iter = iter+1;
   d=d+abs(z-h); # sum of distances along orbit
 end

 if iter < maxiter  # exterior 
    measure = iter;
    myflag=3; # escaping to infinity 
             
    else # iter==maxiter ( inside filled julia set )
      measure=20*d/iter; # average distance (d/iter) = 0.5

在 Chris King 的 Maple 程式碼中，這種離散速度僅透過點之間距離的總和來測量

 $S_{n}=\sum _{n=1}^{n_{max}}d_{n}=\sum _{n=1}^{n_{max}}|Z_{n+1}-Z_{n}|$

因為

來自 Julia 集內部的所有正向軌跡都落入 Siegal 圓盤
在 Siegal 圓盤內部，點繞其中心（無差異週期點）旋轉

所以距離是衡量點落入哪個 Siegal 軌道的一個很好的指標

使用週期函式（sin，cos）建立帶狀結構 ^[3]，顯示 Julia 集內部的動態（Siegal 圓盤及其前像）。

Matlab 原始碼

% code by Chris King
% http://www.dhushara.com/DarkHeart/Viewers/source/siegel.m
function siegel();
nx = 480;
ny = 480;
ColorMset = zeros(nx,ny,3);
magc=0.65;
xmin = -1/magc;
xmax = 1/magc;
ymin = -1/magc;
ymax = 1/magc;
maxiter = 1200;
wb = waitbar(0,'Please wait...');
for iy = 1:ny
  cy = ymin + iy*(ymax - ymin)/(ny - 1);
  for ix= 1:nx
    cx = xmin + ix*(xmax - xmin)/(nx - 1);
    [k myfl] = Mlevel(cy,cx,maxiter);
    if myfl==2  
        ColorMset(ix,iy,2) = abs(sin(5*k/10+pi/4));
    else
        if myfl==1
            ColorMset(ix,iy,1) = abs(sin(2*k/10));
        else
            %ColorMset(ix,iy,2) = abs(sin(2*k/10+pi/4));
            ColorMset(ix,iy,3) = abs(cos(2*k/10));
        end
    end
  end
  waitbar(iy/ny,wb)
end
close(wb);
image(ColorMset);
imwrite(ColorMset,'siegel.jpg','jpg','Quality',100);
 
function [potential myfl] = Mlevel(cx,cy,maxiter)
z = complex(cx,cy);
th=pi*(-1+sqrt(5));
d=exp(complex(0,th));
d=d/2-d*d/4;
%e=(1-sqrt(1-4*d))/2;
%e=0;
%a=complex(0,sqrt(3));
%a=sqrt(3);
a=4;
ang=0;
iter = 0;
while (iter < maxiter)&&(abs(z) > 0.001)&&(abs(z)<20)
   h=z;
   %z=d*z*z*(z-a)/(1-a*z);
   z=z*z+d;
     hh=abs(z-h)*(z-h);
     if iter>maxiter/2
       ang=ang+hh;
    end
   iter = iter+1;
end
if iter < maxiter
    potential = iter;
    if abs(z)>=20
        myfl=0;
    else
        myfl=1;
    end
else
    %potential = -(ang-floor(ang));
    potential=abs(ang);
    myfl=2;
end

Octave 原始碼

# http://www.dhushara.com/DarkHeart/DarkHeart.htm
# it is Octave m-file
# converted from matlab m-file by Chris King
# http://www.dhushara.com/DarkHeart/Viewers/source/siegel.m
#

# ------------- load packages ------------------------
pkg load image;
pkg load miscellaneous; # waitbar

# --------- definitions ------------------------------
 
function [potential myfl] = Mlevel(zx,zy,c,maxiter)
 ER=2.0; # escape radius = bailout value 
 z = complex(zx,zy);
 ang=0;
 iter = 0;

 while (iter < maxiter) && (abs(z) > 0.001) && (abs(z)<ER)
   h=z; # previous point = z_(n)
   z=z*z+c; # next point = z_(n+1)
   

     # for the points that don''t escape compute 
     #  the average discrete velocity  on the orbit = abs( z_(n+1) - z_n ) 
     if iter>maxiter/2 # ???
       zh=z-h; 
       hh=abs(zh)*zh;
       ang=ang+hh;
    endif;

   iter = iter+1;
 end

 if iter < maxiter 
    potential = iter;
    if abs(z)>=ER  myfl=3; # escaping to infinity 
             else  myfl=1; # ??? falling into Siegel disc
    end
 else # iter==maxite ( inside filled julia set )
    potential=abs(ang);
    myfl=2;
 end
endfunction; # Mlevel

# ------------- const ------------------------------

# integer ( screen ) coordinate 
iSide=1000
nx = iSide;
ny = iSide;

# image as a 2D matrix of 24 bit colors coded from 0.0 to 1.0 
MyImage = zeros(ny,nx,3); # matrix filled with 0

# world ( float) coordinate - dynamical (Z) plane 
magc=0.65;
dSide=1/magc
Zxmin = -dSide;
Zxmax = dSide;
Zymin = -dSide;
Zymax = dSide;

stepy = (Zymax - Zymin)/(ny - 1); # pixel height
stepx = (Zxmax - Zxmin)/(nx - 1); # pixel width

maxiter = 2000

# fc(z) = z*z + c 
# rotation number or internal angle
t = (-1+sqrt(5))/2
th=2*pi*t;  # from turns to radians
d=exp(complex(0,th)); # 
c =d/2-d*d/4 # point on boundary of main cardioid


pi4=pi/4;

# --------------- main : 2 loops ---------------------

waitbar(0,'Please wait...'); # info 

# scan all pixels of image and comput color 
for iy = 1:ny
  Zy = Zymax - iy*stepy; # invert y axis
  for ix= 1:nx
    Zx = Zxmin + ix*stepx; # map from screen to world coordinate

    [k myfl] = Mlevel(Zx,Zy,c, maxiter);
    # color 
    switch (myfl)
     case 1 MyImage(iy,ix,1) = abs(sin(2*k/10)); # ?? Julia set in red
     case 2 MyImage(iy,ix,2) = abs(sin(5*k/10 + pi4)); # irrational flow (green) by the sine of the velocity.
     case 3 MyImage(iy,ix,3) = abs(cos(2*k/10)); # Exterior (blue) by level sets of escape time
    endswitch;
   
   # check plane orientation
   # first quadrant should be in upper right position
   # if(Zy>0 && Zx>0)  
   # MyImage(iy,ix,2)=1.0-MyImage(iy,ix,2);
   # endif;
  endfor; # for ix
  
  waitbar(iy/ny);
endfor; # for iy

# image 

image(MyImage); # display image
imwrite(MyImage,'si-test.png');  # save image to file
# this requires the ImageMagick "convert" utility.

包含原始碼的影像（參見 Commons 頁面）

灰色 Siegal 圓盤
彩色 Siegal 圓盤

參考文獻

[1] Chris King 合併的 Julia 集繪製方法

[2] 爆破混沌的黑暗之心 Chris King 2009 年 3 月 - 2016 年 7 月奧克蘭大學數學系

[3] 維基百科: 色帶

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