In the last subunit, I introduced the self-similarity dimension and we calculated the self-similarity dimension for three different fractals. The fractals snowflake, the Sierpienski triangle and the Koch curve. In this subunit, I’ll make a number of other remarks about fractals including thinking about what self-similarity means and what it means to say something is scale-free. And also I’ll try to address a question. It’s a quite likely on your mind which is what’s up with non-integer dimensions, how can it make sense for an object to have dimension that’s not 1 or 2 but it’s something in between. How can we even think about that? So to begin addressing that get some new ways to think about this we’re gonna start by asking the question how long is the Koch curve. So the question before I say is how long is the Koch curve. Reminder you calculated its dimension in the previous section. Here are the steps and its construction. So what I’m gonna do is come up with an expression for the length of zero step, the initial step. And then after 1 step, 2 step, 3 step and so on. And we’ll see what happens. So I’m gonna say, let’s call this initial length 1. Just for a convenience say Let’s say this is a meter or something. So I’m gonna fill out this table here, so it is step 0 initially how long is each line segment but there was only one segment and it has length 1. So the total length is 1. There is one line segment of length 1, the total length is 1. Ok, what about at the first step, now there are 4 line segments, 1, 2, 3, 4. And each line segment is one third the length of the original line segment. So step 1, length of each line segment is a third, the number of line segments is 4, and if we have four things each of which have a length of a third, the total length is four third. Right, what about the step 2? Well, the process repeats. If I just look at this section here, I go from one line segment, 1,2,3,4,.. four line segments. But that same story happens here, here and here. So there are now 16, …1,2,3,4,5,6,7,8 and so on line segments. Right, so step 2, there are 16 line segments, by the way 16 is 4 squared. I have 4 segments here and then 1,2,3,4, shape like that 4 times 4 is 16. Ok, so now this length is a third. This length then into the other lengths is a third of third. So that’ s nine. So that’s 1/9 which is a third of third which is also a third squared. So if I had 16 things each of which have a length of a ninth, and the total lengths, length is 16 over 9 which happens to be 4 third squared. Right, probably see the pattern that’s taking shape here. Let’s do step 3 quickly, so if I just focus on this little piece here, I go from this length to this length, And I now have 4 times as many segments as I did before and every step the number of line segments goes up by a factor 4, it’s multiplied by 4. So now I am gonna have, that’s step 3, 4 times 4 times 4, which is 4 cubed. At each step, the length of the line segment was down by a third. This is one. This is third. This is a third of third. This a third of a third of a third. That’s a third cubed. So let’s say that third cubed. So if I have 4 cubed things each of which has a length of a third cubed, then the total length is going to be 4 third cubed. Notice by the way that the length is getting longer and that’s pretty easy to see. This is length 1, now I added the detour. It’s clearly this path with the bend in it is longer than this. Every time I add a bend in a path, I am adding length. So the length is getting larger and larger. We can generalize this, we see the pattern now. At the nth step, each line segments has been cut in third n times, and every step the number of line segments is multiplied by 4. So that the total length is 4 third to the n. So now the question is what happens as n gets larger and larger and larger. And you can see what’s happening here. This number is getting larger and larger and larger. 4 third multiplied by itself again and again and again. It’s always getting larger you are adding 33 percent every time. So as n gets larger and larger, the total length also gets larger and larger. Say that it goes to infinity. So here is a picture of the Koch curve. This, I did in computer, ought to I think 16 steps. The resolution wouldn’t let me go any farther. We wouldn’t see it. And so as we continue the iteration process at every step adding a bend and every line then the length of this curve becomes infinite. So this curve here it’s gonna have infinite length. So if we have a curve it's infinitely long but it’s clearly contained a finite area. I can draw a circle around it. The area in here is definitely finite. This is just some little oval on my paper. It’s about size of my hand. Nevertheless I can fit one of these wiggly Koch curves in here. That actually has infinite length. So one of things about fractals is that they combine quality is of finite and infinite in interesting way. And in fact, that was some of the original motivation for these constructions in the early 1900. Mathematicians were looking at set theory and trying to think about different properties of inifinities. So in any event the Koch curve has an infinite length, although clearly you can fit that infinite length in a finite area. So now let’s think about the dimension of the Koch curve. Recall that we found previously that is dimension log4 over log3 which is approximately 1.262 so it’s in between in 1 and 2 dimensions. So one way of think about this is that objects with this sort of dimensions between 1 and 2 have some features of qualities of 1 dimensional and some therein two-dimensional. So it’s one-dimensional in that it’s made up out of lines. Remember in our construction we started with a line and put a wiggle in it, put a bump in it, put bumps in it, put bumps on the bums and so on, so on and so on. And we end it up with a shape. So it’s one-dimensional in a sense or it has one dimensional qualities because it started as a line. However it has so many bumps in it. And the shape becomes so jagged so many teeth teeth on teeth on teeth and bumps and bumps and bumps and that it starts a bump up, sort of push up into the second dimension. It’s not fully two-dimensional, like an area. It doesn’t really take up space. But the line becomes so bumpy that it has some sort of two-dimensional features. That’s not a precise argument by any means but just qualitatively it’s a way to think about this non-integer dimension. They combine so something that’s between dimensions one and two, is sort of one-dimensional, sort of two-dimensional. So another thing to think about with a Koch curve is as we said in a finite area, it has an infinite length. So that would be really beneficial if this was may be a part of along or something some organ of structure that was trying to exchange that wanted to have a large surface area. May be this is a shape that’s trying to dissipate heat, so it could be something physical, it doesn’t have to be biological. So this large surface area would be i.e. this large long perimeter of this large length would be really beneficial. Because that will be a large length to cross which the heat could dissipate, or oxygen could be exchanged or something. So that’s another interesting feature of these sorts of fractals so said before they combined finite and infinite and they could have some real structural advantages depending on the particular application.