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Some sample computations

Here we give a few hints on computing a few fractal dimensions. Exercise V.1.1 of Barnsley [Bar93] asks the reader to compute the fractal dimension of a point. For any tex2html_wrap_inline7376 , the number tex2html_wrap_inline7634 of balls of radius tex2html_wrap_inline7570 necessary to cover a point is (drum roll, please) just 1. So

displaymath7732

and the dimension is just 0. Exercise V.1.3 then asks for the dimension of a set of three points. What is tex2html_wrap_inline7634 in that case? You may not be able to precisely determine tex2html_wrap_inline7634 , but you can give a very precise upper bound tex2html_wrap_inline7738 that allows you to solve the problem.

Now suppose S=[0,1], the unit line segment. Again we may not be able to exactly determine tex2html_wrap_inline7634 for each tex2html_wrap_inline5748 , but that is not necessary. We will show how to use the ``squeezing theorem'' of calculus to evaluate the fractal dimension. The width of a disk of radius tex2html_wrap_inline5748 is tex2html_wrap_inline7584 . Thus, if N disks of radius tex2html_wrap_inline7570 cover S, we must have tex2html_wrap_inline7756 . On the other hand, if tex2html_wrap_inline7758 , we can in fact produce a covering by laying the disks down in a row with only a very slight overlap. This proves that

displaymath7760

Then

displaymath7762

since tex2html_wrap_inline7764 is an increasing function. Dividing by tex2html_wrap_inline7766 (which is positive for small tex2html_wrap_inline5748 ), we get

displaymath7770

Here we are giving lower and upper bounds for the quotient in the middle. The upper and lower bounds are somewhat complicated; however, we only need to apply the basic facts from calculus about limits to evaluate the limits as tex2html_wrap_inline7772 . It's better to set tex2html_wrap_inline7774 and consider the limits as tex2html_wrap_inline7776 . The lower bound is

align1831

Since tex2html_wrap_inline7778 as tex2html_wrap_inline7776 , the limit of our lower bound is 1 as tex2html_wrap_inline7782 . The reader may show by the same sort of algebra that the upper bound has the same limit. The squeezing theorem then says

displaymath7784

There are several other worthwhile exercises of this type in Barnsley (see this list). For the numerical computations from pictures, it is very useful to have a piece of fine engineering graph paper that may be laid over the picture. Then you can count the boxes of various sizes of the graph paper that touch the fractal.

Finally, we shall sketch an example that shows a weakness in the definition of fractal dimension, which is the reason that for theoretical purposes its big brother Hausdorff-Besicovitch dimension is more commonly used. Consider the set

displaymath7786

This is a sequence of points together with its one limit point 0. It is both closed and bounded, and therefore compact. We will show that the fractal dimension is at least 1/2, which contradicts our intuition that such a scant sequence of points should be 0-dimensional.

Choose a positive integer n>1 and choose tex2html_wrap_inline5748 to lie in the following interval:

displaymath7794

The outer expressions are the distances between tex2html_wrap_inline7796 and tex2html_wrap_inline7798 and between tex2html_wrap_inline7800 and tex2html_wrap_inline7798 . Then there is no way for a disk of radius tex2html_wrap_inline5748 to cover two of the points 1, tex2html_wrap_inline7808 , tex2html_wrap_inline7810 tex2html_wrap_inline7798 , since any pair of these points are more than tex2html_wrap_inline7584 apart. Thus,

displaymath7816

for this choice of tex2html_wrap_inline5748 . Hence,

align1877

using properties of logarithms. The last expression tends to 1/2 as tex2html_wrap_inline4974 , proving our claim that the fractal dimension is at least 1/2. In fact, we leave it to the reader to find an upper bound that proves that the fractal dimension is exactly 1/2.


next up previous contents
Next: Iterated Function Systems Up: Dynamical Systems and Fractal Previous: Dimension computed by growth

David J. Wright
Mon Aug 19 17:21:15 CDT 1996