Twi-Phi

Here’s a pentagon:

Stage #1


And here’s the pentagon with smaller pentagons on its vertices:

Stage #2


And here’s more of the same:

Stage #3


Stage #4


Stage #5


Stage #6


Stage #7


Stage #8


Animated fractal


At infinity, the smaller pentagons have reached out like arms to exactly fill the gaps between themselves without overlapping. But how much smaller is each set of smaller pentagons than its mother-pentagon when the gaps are exactly filled? Well, if the radius of the mother-pentagon is r, then the radius of each daughter-pentagon is r * 1/(φ^2) = r * 0·38196601125…

But what happens if the radius relationship of mother to daughter is r * 1/φ = r * 0·61803398874 = r * (φ-1)? Then you get this fractal:

Stage #1


Stage #2


Stage #3


Stage #4


Stage #5


Stage #6


Stage #7


Stage #8


Stage #9


Animated fractal


Delta Skelta

“When I get to the bottom I go back to the top of the slide,
Where I stop and I turn and I go for a ride
Till I get to the bottom and I see you again.” — The Beatles, “Helter Skelter” (1968)


First stage of fractal #1











Animated fractal #1


First stage of fractal #2













Animated fractal #2

Middlemath

Suppose you start at the middle of a triangle, then map all possible ways you can jump eight times half-way towards one or another of the vertices of the triangle. At the end of the eight jumps, you mark your final position with a dot. You could jump eight times towards the same vertex, or once towards vertex 1, once towards vertex 2, and once again towards vertex 1. And so on. If you do this, the record of your jumps looks something like this:


The shape is a fractal called the Sierpiński triangle. But if you try the same thing with a square — map all possible jumping-routes you can follow towards one or another of the four vertices — you simply fill the interior of the square. There’s no interesting fractal:


So you need a plan with a ban. Try mapping all possible routes where you can’t jump towards the same vertex twice in a row. And you get this:

Ban on jumping towards same vertex twice in a row, v(t) ≠ v(t-1)


If you call the current vertex v(t) and the previous vertex v(t-1), the ban says that v(t) ≠ v(t-1). Now suppose you can’t jump towards the vertex one place clockwise of the previous vertex. Now the ban is v(t)-1 ≠ v(t-1) or v(t) ≠ v(t-1)+1 and this fractal appears:

v(t) ≠ v(t-1)+1


And here’s a ban on jumping towards the vertex two places clockwise (or counterclockwise) of the vertex you’ve just jumped towards:

v(t) ≠ v(t-1)+2


And finally the ban on jumping towards the vertex three places clockwise (or one place counterclockwise) of the vertex you’ve just jumped towards:

v(t) ≠ v(t-1)+3 (a mirror-image of v(t) ≠ v(t-1)+1, as above)


Now suppose you introduce a new point to jump towards at the middle of the square. You can create more fractals, but you have to adjust the kind of ban you use. The central point can’t be included in the ban or the fractal will be asymmetrical. So you continue taking account of the vertices, but if the previous jump was towards the middle, you ignore that jump. At least, that’s what I intended, but I wonder whether my program works right. Anyway, here are some of the fractals that it produces:

v(t) ≠ v(t-1) with central point (wcp)


v(t) ≠ v(t-1)+1, wcp


v(t) ≠ v(t-1)+2, wcp


And here are some bans taking account of both the previous vertex and the pre-previous vertex:

v(t) ≠ v(t-1) & v(t) ≠ v(t-2), wcp


v(t) ≠ v(t-1) & v(t-2)+1, wcp


v(t) ≠ v(t-1)+2 & v(t-2), wcp


v(t) ≠ v(t-1) & v(t-2)+1, wcp


v(t) ≠ v(t-1)+1 & v(t-2)+1, wcp


v(t) ≠ v(t-1)+2 & v(t-2)+1, wcp


v(t) ≠ v(t-1)+3 & v(t-2)+1, wcp


v(t) ≠ v(t-1) & v(t-2)+2, wcp


v(t) ≠ v(t-1)+1 & v(t-2)+2, wcp


v(t) ≠ v(t-1)+2 & v(t-2)+2, wcp


Now look at pentagons. They behave more like triangles than squares when you map all possible jumping-routes towards one or another of the five vertices. That is, a fractal appears:

All possible jumping-routes towards the vertices of a pentagon


But the pentagonal-jump fractals get more interesting when you introduce jump-bans:

v(t) ≠ v(t-1)


v(t) ≠ v(t-1)+1


v(t) ≠ v(t-1)+2


v(t) ≠ v(t-1) & v(t-2)


v(t) ≠ v(t-1)+2 & v(t-2)


v(t) ≠ v(t-1)+1 & v(t-2)+1


v(t) ≠ v(t-1)+3 & v(t-2)+1


v(t) ≠ v(t-1)+1 & v(t-2)+2


v(t) ≠ v(t-1)+2 & v(t-2)+2


v(t) ≠ v(t-1)+3 & v(t-2)+2


Finally, here are some pentagonal-jump fractals using a central point:








Post-Performative Post-Scriptum

I’m not sure if I’ve got the order of some bans right above. For example, should v(t) ≠ v(t-1)+1 & v(t-2)+2 really be v(t) ≠ v(t-1)+2 & v(t-2)+1? I don’t know and I’m not going to check. But the idea of jumping-point bans is there and that’s all you need if you want to experiment with these fractal methods for yourself.

Back to Drac’ #2

Boring, dull, staid, stiff, everyday, ordinary, unimaginative, unexceptional, crashingly conventional — the only interesting thing about squares is the number of ways you can say how uninteresting they are. Unlike triangles, which vary endlessly and entertainingly, squares are square in every sense of the word.

And they don’t get any better if you tilt them, as here:

Sub-squares from gray square (with corner-numbers)


Nothing interesting can emerge from that set of squares. Or can it? As I showed in Curvous Energy, it can. Suppose that the gray square is dividing into the colored squares like a kind of amoeba. And suppose that the colored squares divide in their turn. So square divides into sub-squares and sub-squares divide into sub-sub-squares. And so on. And all the squares keep the same relative orientation.

What happens if the gray square divides into sub-squares sq2 and sq9? And then sq2 and sq9 each divide into their own sq2 and sq9? And so on. Something very unsquare-like happens:

Square-split stage #1


Stage #2


Square-split #3


Square-split #4


Square-split #5


Square-split #6


Square-split #7


Square-split #8


Square-split #9


Square-split #10


Square-split #11


Square-split #12


Square-split #13


Square-split #14


Square-split #15


Square-split #16


Square-split (animated)


The square-split creates a beautiful fractal known as a dragon-curve:

Dragon-curve


Dragon-curve (red)


And dragon-curves, at various angles and in various sizes, emerge from every other possible pair of sub-squares:

Lots of dragon-curves


And you get other fractals if you manipulate the sub-squares, so that the corners are rotated or reverse-rotated:

Rotation = 1,2 (sub-square #1 unchanged, in sub-square #2 corner 1 becomes corner 2, 2 → 3, 3 → 4, 4 → 1)


rot = 1,2 (animated)


rot = 1,2 (colored)


rot = 1,5 (in sub-square #2 corner 1 stays the same, 4 → 2, 3 stays the same, 2 → 4)


rot = 1,5 (anim)


rot = 4,7 (sub-square #2 flipped and rotated)


rot = 4,7 (anim)


rot = 4,7 (col)


rot = 4,8


rot = 4,8 (anim)


rot = 4,8 (col)


sub-squares = 2,8; rot = 5,6


sub-squares = 2,8; rot = 5,6 (anim)


sub-squares = 2,8; rot = 5,6 (col)


Another kind of dragon-curve — rot = 3,2


rot = 3,2 (anim)


rot = 3,2 (col)


sub-squares = 4,5; rot = 3,9


sub-squares = 4,5; rot = 3,9 (anim)


sub-squares = 4,5; rot = 3,9 (col)


Elsewhere other-accessible…

Curvous Energy — a first look at dragon-curves
Back to Drac’ — a second look at dragon-curves

Think Inc #2

In a pre-previous post called “Think Inc”, I looked at the fractals created by a point first jumping halfway towards the vertex of a square, then using a set of increments to decide which vertex to jump towards next. For example, if the inc-set was [0, 1, 3], the point would jump next towards the same vertex, v[i]+0, or the vertex immediately clockwise, v[i]+1, or the vertex immediately anti-clockwise, v[i]+3. And it would trace all possible routes using that inc-set. Then I added refinements to the process like giving the point extra jumping-targets half-way along each side.

Here are some more variations on the inc-set theme using two and three extra jumping-targets along each side of the square. First of all, try two extra jumping-targets along each side and a set of three increments:

inc = 0, 1, 6


inc = 0, 2, 6


inc = 0, 2, 8


inc = 0, 3, 6


inc = 0, 3, 9


inc = 0, 4, 8


inc = 0, 5, 6


inc = 0, 5, 7


inc = 1, 6, 11


inc = 2, 6, 10


inc = 3, 6, 9


Now try two extra jumping-targets along each side and a set of four increments:

inc = 0, 1, 6, 11


inc = 0, 2, 8, 10


inc = 0, 3, 7, 9


inc = 0, 4, 8, 10


inc = 0, 5, 6, 7


inc = 0, 5, 7, 8


inc = 1, 6, 7, 9


inc = 1, 4, 6, 11


inc = 1, 5, 7, 11


inc = 2, 4, 8, 10


inc = 3, 5, 7, 9


And finally, three extra jumping-targets along each side and a set of three increments:

inc = 0, 3, 13


inc = 0, 4, 8


inc = 0, 4, 12


inc = 0, 5, 11

inc = 0, 6, 9


inc = 0, 7, 9


Previously Pre-Posted

Think Inc — an earlier look at inc-set fractals

Think Inc

This is a T-square fractal:

T-square fractal


Or you could say it’s a T-square fractal with the scaffolding taken away, because there’s nothing to show how it was made. And how is a T-square fractal made? There are many ways. One of the simplest is to set a point jumping 1/2 of the way towards one or another of the four vertices of a square. If the point is banned from jumping towards the vertex two places clockwise (or counter-clockwise) of the vertex, v[i=1..4], it’s just jumped towards, you get a T-square fractal by recording each spot where the point lands.

You also get a T-square if the point is banned from jumping towards the vertex most distant from the vertex, v[i], it’s just jumped towards. The most distant vertex will always be the diagonally opposite vertex, or the vertex, v[i+2], two places clockwise of v[i]. So those two bans are functionally equivalent.

But what if you don’t talk about bans at all? You can also create a T-square fractal by giving the point three choices of increment, [0,1,3], after it jumps towards v[i]. That is, it can jump towards v[i+0], v[i+1] or v[i+3] (where 3+2 = 5 → 5-4 = 1; 3+3 = 6 → 2; 4+1 = 5 → 1; 4+2 = 6 → 2; 4+3 = 7 → 3). Vertex v[i+0] is the same vertex, v[i+1] is the vertex one place clockwise of v[i], and v[i+3] is the vertex two places clockwise of v[i].

So this method is functionally equivalent to the other two bans. But it’s easier to calculate, because you can take the current vertex, v[i], and immediately calculate-and-use the next vertex, without having to check whether the next vertex is forbidden. In other words, if you want speed, you just have to Think Inc!

Speed becomes important when you add a new jumping-target to each side of the square. Now the point has 8 possible targets to jump towards. If you impose several bans on the next jump, e.g the point can’t jump towards v[i+2], v[i+3], v[i+5], v[i+6] and v[i+7], you will have to check for five forbidden targets. But using the increment-set [0,1,4] you don’t have to check for anything. You just inc-and-go:

inc = 0, 1, 4


Here are more fractals created with the speedy inc-and-go method:

inc = 0, 2, 3


inc = 0, 2, 5


inc = 0, 3, 4


inc = 0, 3, 5


inc = 1, 4, 7


inc = 2, 4, 7


inc = 0, 1, 4, 7


inc = 0, 3, 4, 5


inc = 0, 3, 4, 7


inc = 0, 4, 5, 7


inc = 1, 2, 6, 7


With more incs, there are more possible paths for the jumping point and the fractals become more “solid”:

inc = 0, 1, 2, 4, 5


inc = 0, 1, 2, 6, 7


inc = 0, 1, 3, 5, 7


Now try applying inc-and-go to a pentagon:

inc = 0, 1, 2

(open in new window if blurred)


inc = 0, 2, 3


And add a jumping-target to each side of the pentagon:

inc = 0, 2, 5


inc = 0, 3, 6


inc = 0, 3, 7


inc = 1, 5, 9


inc = 2, 5, 8


inc = 5, 6, 9


And add two jumping-targets to each side of the pentagon:

inc = 0, 1, 7


inc = 0, 2, 12


inc = 0, 3, 11


inc = 0, 3, 12


inc = 0, 4, 11


inc = 0, 5, 9


inc = 0, 5, 10


inc = 2, 7, 13


inc = 2, 11, 13


inc = 3, 11, 13


After the pentagon comes the hexagon:

inc = 0, 1, 2


inc = 0, 1, 5


inc = 0, 3, 4


inc = 0, 3, 5


inc = 1, 3, 5


inc = 2, 3, 4


Add a jumping-target to each side of the hexagon:

inc = 0, 2, 5


inc = 0, 2, 9


inc = 0, 6, 11


inc = 0, 3, 6


inc = 0, 3, 8


inc = 0, 3, 9


inc = 0, 4, 7


inc = 0, 4, 8


inc = 0, 5, 6


inc = 0, 5, 8


inc = 1, 5, 9


inc = 1, 6, 10


inc = 1, 6, 11


inc = 2, 6, 8


inc = 2, 6, 10


inc = 3, 5, 7


inc = 3, 6, 9


inc = 6, 7, 11


Boole(b)an #3

In the posts “Boole(b)an #1″ and “Boole(b)an #2” I looked at fractals created by certain kinds of ban on a point jumping (quasi-)randomly towards the four vertices, v=1..4, of a square. For example, suppose the program has a vertex-history of 2, that is, it remembers two jumps into the past, the previous jump and the pre-previous jump. There are sixteen possible combinations of pre-previous and previous jumps: [1,1], [1,2], 1,3] … [4,2], [4,3], [4,4].

Let’s suppose the program bans 4 of those 16 combinations by reference to the current possible jump. For example, it might ban [0,0]; [0,1]; [0,3]; [2,0]. To see what that means, let’s suppose the program has to decide at some point whether or not to jump towards v=3. It will check whether the combination of pre-previous and previous jumps was [3+0,3+0] = [3,3] or [3+0,3+1] = [3,4] or [3+0,3+3] = [3,2] or [3+2,3+0] = [1,3] (when the sum > 4, v = sum-4). If the previous combination is one of those pairs, it bans the jump towards v=3 and chooses another vertex; otherwise, it jumps towards v=3 and updates the vertex-history. This is the fractal that appears when those bans are used:

ban = [0,0]; [0,1]; [0,3]; [2,0]


And here are more fractals using a vertex-history of 2 and a ban on 4 of 16 possible combinations of pre-previous and previous jump:

ban = [0,0]; [0,1]; [0,3]; [2,2]


ban = [0,0]; [0,2]; [1,0]; [3,0]


ban = [0,0]; [0,2]; [1,1]; [3,3]


ban = [0,0]; [0,2]; [1,3]; [3,1]


ban = [0,0]; [1,0]; [2,2]; [3,0]


ban = [0,0]; [1,1]; [1,2]; [3,2]

Continue reading “Boole(b)an #3”…


Elsewhere other-engageable

Boole(b)an #1
Boole(b)an #2

This Charming Dis-Arming

One of the charms of living in an old town or city is finding new routes to familiar places. It’s also one of the charms of maths. Suppose a three-armed star sprouts three half-sized arms from the end of each of its three arms. And then sprouts three quarter-sized arms from the end of each of its nine new arms. And so on. This is what happens:

Three-armed star


3-Star sprouts more arms


Sprouting 3-Star #3


Sprouting 3-Star #4


Sprouting 3-Star #5


Sprouting 3-Star #6


Sprouting 3-Star #7


Sprouting 3-Star #8


Sprouting 3-Star #9


Sprouting 3-Star #10


Sprouting 3-Star #11 — the Sierpiński triangle


Sprouting 3-star (animated)


The final stage is a famous fractal called the Sierpiński triangle — the sprouting 3-star is a new route to a familiar place. But what happens when you trying sprouting a four-armed star in the same way? This does:

Four-armed star #1


Sprouting 4-Star #2


Sprouting 4-Star #3


Sprouting 4-Star #4


Sprouting 4-Star #5


Sprouting 4-Star #6


Sprouting 4-Star #7


Sprouting 4-Star #8


Sprouting 4-Star #9


Sprouting 4-Star #10


Sprouting 4-star (animated)


There’s no obvious fractal with a sprouting 4-star. Not unless you dis-arm the 4-star in some way. For example, you can ban any new arm sprouting in the same direction as the previous arm:

Dis-armed 4-star (+0) #1


Dis-armed 4-Star (+0) #2


Dis-armed 4-Star (+0) #3


Dis-armed 4-Star (+0) #4


Dis-armed 4-Star (+0) #5


Dis-armed 4-Star (+0) #6


Dis-armed 4-Star (+0) #7


Dis-armed 4-Star (+0) #8


Dis-armed 4-Star (+0) #9


Dis-armed 4-Star (+0) #10


Dis-armed 4-star (+0) (animated)


Once again, it’s a new route to a familiar place (for keyly committed core components of the Overlord-of-the-Über-Feral community, anyway). Now try banning an arm sprouting one place clockwise of the previous arm:

Dis-armed 4-Star (+1) #1


Dis-armed 4-Star (+1) #2


Dis-armed 4-Star (+1) #3


Dis-armed 4-Star (+1) #4


Dis-armed 4-Star (+1) #5


Dis-armed 4-Star (+1) #6


Dis-armed 4-Star (+1) #7


Dis-armed 4-Star (+1) #8


Dis-armed 4-Star (+1) #9


Dis-armed 4-Star (+1) #10


Dis-armed 4-Star (+1) (animated)


Again it’s a new route to a familiar place. Now trying banning an arm sprouting two places clockwise (or anti-clockwise) of the previous arm:

Dis-armed 4-Star (+2) #1


Dis-armed 4-Star (+2) #2


Dis-armed 4-Star (+2) #3


Dis-armed 4-Star (+2) #4


Dis-armed 4-Star (+2) #5


Dis-armed 4-Star (+2) #6


Dis-armed 4-Star (+2) #7


Dis-armed 4-Star (+2) #8


Dis-armed 4-Star (+2) #9


Dis-armed 4-Star (+2) #10


Dis-armed 4-Star (+2) (animated)


Once again it’s a new route to a familiar place. And what happens if you ban an arm sprouting three places clockwise (or one place anti-clockwise) of the previous arm? You get a mirror image of the Dis-armed 4-Star (+1):

Dis-armed 4-Star (+3)


Here’s the Dis-armed 4-Star (+1) for comparison:

Dis-armed 4-Star (+1)


Elsewhere other-accessible

Boole(b)an #2 — other routes to the fractals seen above

Boole(b)an #2

In “Boole(b)an”, I looked at some of the things that happen when you impose bans of different kinds on a point jumping half-way towards a randomly chosen vertex of a square. If the point can’t jump towards the same vertex twice (or more) in a row, you get the fractal below (or rather, you get a messier version of the fractal below, because I’ve used an algorithm that finds all possible routes to create the fractals in this post):

ban = v(i) + 0


If the point can’t jump towards the vertex one place clockwise of the point it has just jumped towards, you get this fractal:

ban = v(i) + 1


If the point can’t jump towards the vertex two places clockwise (or anti-clockwise) of the point it has just jumped towards, you get this fractal:

ban = v(i) + 2


Finally, you get a mirror-image of the one-place-clockwise fractal when the ban is on jumping towards the vertex three places clockwise (or one place anti-clockwise) of the previous vertex:

ban = v(i) + 3


Now let’s introduce the concept of “vertex-history”. The four fractals above use a vertex-history of 1, vh = 1, because they look one step into the past, at the previously chosen vertex. Because there are four vertices, there are four possible previous vertices. But when vh = 2, you’re taking account of both the previous vertex, v(i), and what you might call the pre-previous vertex, v(i-1). There are sixteen possible combinations of previous vertex and pre-previous vertex (16 = 4 x 4).

Now, suppose the jump-ban is imposed when one of two conditions is met: the vertex is 1) one place clockwise of the previous vertex and the same as the pre-previous vertex; 2) three places clockwise of the previous chosen vertex and the same as the pre-previous vertex. So the boolean test is (condition(1) AND condition(2)) OR (condition(3) AND condition(4)). When you apply the test, you get this fractal:

ban = v(i,i-1) + [0,1] or v(i,i-1) + [0,3]


The fractal looks more complex, but I think it’s a blend of some combination of the four classic fractals shown at the beginning of this post. Here are more multiple-ban fractals using vh = 2 and bani = 2:

ban = [0,1] or [1,1]


ban = [0,2] or [2,0]


ban = [0,2] or [2,2]


ban = [1,0] or [3,0]


ban = [1,1] or [3,3]


ban = [1,2] or [2,2]


ban = [1,2] or [3,2]


ban = [1,3] or [2,0]


ban = [1,3] or [3,1]


ban = [2,0] or [2,2]


ban = [2,1] or [2,3]


For the fractals below, vh = 2 and bani = 3 (i.e., bans are imposed when one of three possible conditions is met). Again, I think the fractals are blends of some combination of the four classic ban-fractals shown at the beginning of this post:

ban = [0,0] or [1,2] or [3,2]


ban = [0,0] or [1,3] or [3,1]


ban = [0,0] or [2,1] or [2,3]


ban = [0,1] or [0,2] or [0,3]


ban = [0,1] or [0,3] or [1,1]


ban = [0,1] or [0,3] or [2,0]


ban = [0,1] or [0,3] or [2,2]


ban = [0,1] or [1,1] or [1,2]


ban = [0,1] or [1,1] or [3,0]


ban = [0,1] or [1,2] or [3,2]


ban = [0,2] or [1,0] or [3,0]


ban = [0,2] or [1,1] or [3,3]


ban = [0,2] or [1,2] or [2,2]


ban = [0,2] or [1,2] or [3,1]


ban = [0,2] or [1,2] or [3,2]


ban = [0,2] or [1,3] or [2,0]


ban = [0,2] or [1,3] or [3,1]


ban = [0,2] or [2,0] or [2,2]


ban = [0,2] or [2,1] or [2,3]


ban = [0,2] or [2,2] or [3,2]


ban = [0,3] or [1,0] or [2,0]


ban = [1,0] or [1,2] or [3,0]


ban = [1,0] or [2,2] or [3,0]


ban = [1,1] or [2,0] or [3,3]


ban = [1,1] or [2,1] or [3,1]


ban = [1,1] or [2,2] or [3,3]


ban = [1,1] or [2,3] or [3,3]


ban = [1,2] or [2,0] or [3,1]


ban = [1,2] or [2,0] or [3,2]


ban = [1,2] or [2,1] or [2,3]


ban = [1,2] or [2,3] or [3,2]


ban = [1,2] or [3,2] or [3,3]


ban = [1,3] or [2,0] or [2,2]


ban = [1,3] or [2,0] or [3,0]


ban = [1,3] or [2,0] or [3,1]


ban = [1,3] or [2,2] or [3,1]


ban = [2,0] or [3,1] or [3,2]


ban = [2,1] or [2,3] or [3,2]


Previously pre-posted

Boole(b)an — an early look at ban-fractals

Fink Frakt

Pre-previously on Overlord-In-Terms-of-Issues-Around-Engagement-with-the-Über-Feral, I’ve looked at various ways of creating fractals by restricting the moves of a point jumping towards the vertices of a polygon. For example, the point can be banned from jumping towards the same vertex twice in a row. This time, I want to look at fractals created not by restriction, but by compulsion. If the point jumps towards vertex v and then tries to jump towards vertex v again, it will be forced to jump towards vertex v+1 instead, and so on.

You could call vv+1 a forced increment or finc. So these are finc fractals. In some cases, restriction and compulsion create the same fractals, but I’ve found some new fractals using compulsion. Consider the fractal created by the rule v[-2]+1, v[-1] → +0,+1, where the subscripts refer to the history of jumps: v[-2] is the jump-before-last, v[-1] is the last jump. If the new vertex, v[0], chosen is the same as v[-2]+1 (e.g., v[0] = 2 = v[-2]+1 = 1+1), then the forced increment is 0, i.e., the point is allowed to choose that jump. However, if v[0] = v[-1], then the forced increment is 1 and the point must jump towards v[-1]+1.

Here is the fractal in question:

v[-2]+1, v[-1] → +0,+1 (black-and-white)


v[-2]+1, v[-1] → +0,+1 (colour)


1,0 → +0,+1 (animated)


1,0 → +1,+0 (bw)


1,0 → +1,+0 (col)


1,0 → +1,+0 (anim)


1,0 → +1,+1 (bw)


1,0 → +1,+1 (col)


1,0 → +1,+1 (animated)


0,1 → +2,+1 (anim)


0,1 → +3,+1


1,0 → +0,+1


1,0 → +1,+0


1,1 → +0,+1


1,1 → +1,+2


1,1 → +1,+3


1,1 → +2,+1


1,2 → +0,+3


1,3 → +0,+1


2,2 → +0,+1


But suppose the history of jumps records not actual jumps, but the jumps the point wanted to make instead. In some cases, the jump made will be the same as the jump originally chosen, but in other cases it won’t. Here are some fractals using this method:

0 → +2


0 → +3


2 → +1


2 → +2