Agnes Scott College
Larry Riddle, Agnes Scott College
flowsnake100

Flowsnake


Description

motif2

Start with a pattern of seven regular hexagons. Eight vertices are connected as shown above to create the basic red motif. The red line segments are oriented by the arrows. Now replace each red line segment by a copy of the motif scaled by r = \(1/ \sqrt 7 \) such that the copy lies to the left of the oriented edge it is replacing. Notice that this will place the copy of the motif inside the hexagon containing that edge. This recursive procedure is continued and in the limit will produce the image the flowsnake.

Iterated
Function
System

 
 
 
 

Animation

With the hexagons and motif located as shown above, we get the following IFS where \(A = \arcsin \left( {\frac{{\sqrt 3 }}{{2\sqrt 7 }}} \right) \approx {19.1066^ \circ }\) [Details].
 
\({f_1}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { -1/ \sqrt 14} & {3\sqrt 3 /14 } \\ {-3\sqrt 3 /14} & { -1/ \sqrt 14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {1/14 } \\ {3\sqrt 3 /14} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A-120°
 
\({f_2}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { 5/14} & {- \sqrt 3 / 14} \\ { \sqrt 3 / 14} & { 5/14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {1/14 } \\ {3\sqrt 3 /14} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A
 
\({f_3}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { 5/14} & {- \sqrt 3 / 14} \\ { \sqrt 3 / 14} & { 5/14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {3/7} \\ {2 \sqrt 3 / 7} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A
 
\({f_4}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { -1/ \sqrt 14} & {3\sqrt 3 /14 } \\ {-3\sqrt 3 /14} & { -1/ \sqrt 14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {11/14} \\ {5 \sqrt 3 / 14} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A-120°
 
\({f_5}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { 5/14} & {- \sqrt 3 / 14} \\ { \sqrt 3 / 14} & { 5/14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {5/14} \\ {\sqrt 3 /14} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A
 
\({f_6}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { -2/7} & {- \sqrt 3 /7} \\ { \sqrt 3 /7} & { -2/7} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {9/14} \\ {- \sqrt 3 / 14} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A+120°
 
\({f_7}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { 5/14} & {- \sqrt 3 / 14} \\ { \sqrt 3 / 14} & { 5/14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {9/14} \\ {- \sqrt 3 / 14} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A
 

IFSflowsnake4thStage
4th Iteration

 

hexagons

There is an another way to get the flowsnake by working with hexagons directly instead of line segments. In this case start with a hexagon as shown in the figure to the right, make 7 copies scaled by r = \(1 / \sqrt 7\), rotate them by \(A = \arcsin \left( {\frac{{\sqrt 3 }}{{2\sqrt 7 }}} \right) \approx {19.1066^ \circ }\), then translate so that six of them exactly surround the seventh. This yields the following IFS [Details].

 
 
 
 

Animation

\({f_1}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { 5/ 14} & {-\sqrt 3 /14 } \\ {\sqrt 3 /14} & { 5/ 14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {\sqrt 3 /14 } \\ {9 /14} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A
 
\({f_2}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { 5/ 14} & {-\sqrt 3 /14 } \\ {\sqrt 3 /14} & { 5/ 14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {5 \sqrt 3 /14} \\ {3 /14} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A
 
\({f_3}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { 5/ 14} & {-\sqrt 3 /14 } \\ {\sqrt 3 /14} & { 5/ 14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {2 \sqrt 3 /7} \\ {-3/ 7} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A
 
\({f_4}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { 5/ 14} & {-\sqrt 3 /14 } \\ {\sqrt 3 /14} & { 5/ 14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {- \sqrt 3/14} \\ {-9/ 14} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A
 
\({f_5}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { 5/ 14} & {-\sqrt 3 /14 } \\ {\sqrt 3 /14} & { 5/ 14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {-5 \sqrt 3 /14} \\ {-3 /14} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A
 
\({f_6}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { 5/ 14} & {-\sqrt 3 /14 } \\ {\sqrt 3 /14} & { 5/ 14} \\ \end{array}} \right]{\bf{x}} + \left[ {\begin{array}{*{20}{c}} {-2 \sqrt 3/7} \\ {3/7} \\ \end{array}} \right]\)
 
   scale by \(1/ \sqrt{7} \), rotate by A
 
\({f_7}({\bf{x}}) = \left[ {\begin{array}{*{20}{c}} { 5/ 14} & {-\sqrt 3 /14 } \\ {\sqrt 3 /14} & { 5/ 14} \\ \end{array}} \right]{\bf{x}}\)
 
   scale by \(1/ \sqrt{7} \), rotate by A
 

IFSflowsnake2

L-System

The boundary of the flowsnake can be obtained through an iterative construction that replaces line segments with the following zigzag motif, where each of the three smaller segments have been scaled by \(1 / \sqrt 7 \).

boundarymotif

This boundary can therefore by obtained with the following L-system:

Angle 60
Axiom F+F+F+F+F+F+
F —> F−F+F

Here is the initial hexagon (axiom) and the first 5 iterations of the L-system. The boundary shown here is rotated from the flowsnake constructed above because the angle A is not taken into account.

lsystem0 lsystem1 lsystem2
lsystem3 lsystem4 lsystem5

Similarity
Dimension

The flowsnake is self-similar with 7 non-overlapping copies of itself, each scaled by the factor r < 1. Therefore the similarity dimension, d, of the attractor of the IFS is the solution to

\[\sum\limits_{k = 1}^7 {{r^d}} = 1 \quad \Rightarrow \quad d =\frac{{\log (1/7)}}{{\log (r)}} = \frac{{\log (1/7)}}{{\log (1/ \sqrt 7)}} = 2\]

The boundary of the flowsnake has a fractal dimension of \( \dfrac {\log(3)}{\log( \sqrt 7)} = 1.12915 \).

Special
Properties

The flowsnake is also known as the Gosper Island, a name first used by Mandelbrot. The space-filling curve that fills the flowsnake is known as the Peano-Gosper curve.

area The area of the flowsnake is the same as the area of the initial hexagon. As illustrated in the figure to the right, at the first stage of the construction of the boundary, the new zigzag line segments along each edge of the initial hexagon have as much area added outside the hexagon as area is removed from inside the hexagon. Thus this first iteration has the same area as the hexagon. At each step of the iterative construction, the number of edges will continue to increase, but the same balance of adding and subtracting areas will occur, hence the total area will never change. At the limit the area enclosed by the boundary will the exactly the same as the area of the initial hexagon.

Copies of the flowsnake will tile the plane. The figure below shows how hexagons can tile the plane. On the right we see the first stage in the construction of the flowsnake boundary and how the zigzag boundaries coming from adjacent hexagons perfectly fit together. As the construction continues, the boundaries will continue to fit together so that in the limit the flowsnakes will tile the plane.

tiling

 

References

  1. Barcellos, Anthony. "The Fractal Geometry of Mandelbrot," The College Mathematics Journal, Vol. 15, No. 2, (1984), 98-114. [Available at the MAA website]
  2. Fonn, Elvind. Construction of the Gosper Curve on YouTube, uploaded Nov. 20, 2009.
  3. Gardner, Martin. "Mathematical Games," Scientific American, December 1976, 124-129. [Reprinted in Penrose Tiles to Trapdoor Ciphers, Freeman (1977), and in Penrose Tiles to Trapdoor Ciphers: And the Return of Dr Matrix, Mathematical Association of America (1997)].
  4. Mandelbrot, Benoit. Fractals: Form, Chance, and Dimension, W. H. Freeman and Co., 1977.
  5. Mandelbrot, Benoit. The Fractal Geometry of Nature, W.H. Freeman and Co. 1983. [Preview available at Google Books]