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APPENDIX A


           Fractals







             The term “fractal” was coined by Mandelbrot (1967) for
           objects or sets of fractional dimension. For want of a gener-
           ally accepted definition of fractals, I will characterize them
           by listing essential properties and examining some classic
           examples. We will then proceed to methods for determining
           the fractal dimension and the fractal character of natural
           phenomena. For more information, the reader is referd to
           Falconer (1990) for mathematical background, Schroeder
           (1991) for a discipline-crossing overview of fractals, and to
           Turcotte (1997) and Hergarten (2002) for overviews directed
           to earth scientists.


             What is a fractal?
           A fractal is an object or set of objects that
             ➤ is self-similar, i.e. looks the same at all scales,
             ➤ has a fine structure,
             ➤ has a fractal dimension larger than its topological di-
               mension.

           The topological dimension is, for most practical purposes,
           equal to the Euclidean dimension. Several different formu-
           las are used to calculate the fractal dimension; all of them
           quantify the fine structure of the fractal, for instance by mea-
           suring the degree to which a wiggly curve fills an area, or a
           series of aligned dots starts to form a one-dimensional line.
             For natural scientists, it is important to recognize the dif-
           ference between abstract fractals and natural fractals. Fig.
           A.1 shows an example of an abstract fractal conceived in  Fig. A.1.— The Koch curve – a geometric fractal. It is gener-
           1904 by the Swedish mathematician H. von Koch. It is cre-  ated by erecting an equilateral triangle over the middle third of a
           ated by erecting an equilateral triangle over the middle third  line segment and repeating the operation at smaller and smaller
           of a straight line segment and repeating this operation with  segments to infinity. After Falconer (1990), modified.
           smaller and smaller line segments to infinity. The result is a
           wiggly curve that looks the same at all scales. This means
           that any part of the curve properly enlarged looks like the
           whole. The curve is self-similar because of its fine structure
           and has a fractal dimension between 1 and 2, between the
           Euclidean dimension of a line and that of an area. We may
           say that the curve is so wiggly that it starts to fill part of an
           area. The topological dimension of the curve is one. Topol-
           ogy is also known as “rubber-sheet geometry”. If the Koch
           curve in Fig. A.1 were made of a rubber string then it would
           be possible to change it by continuous transformation with-
                                                                   Fig. A.2.— The Cantor bar (or Cantor set) – a mathematical frac-
           out any cutting or pasting into a straight line or any other
                                                                  tal well known in stratigraphy. The initiating step is a line segment.
           smooth curve.                                          In the generating step, the middle third of the line is removed and
             Fig. A.2 shows another mathematical fractal – the Cantor  this operation is repeated to infinity. After Schroeder (1991), modi-
           set, also called Cantor bar, conceived by the German mathe-  fied.

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