Skip to main content

Square Grids, Cylinders, Spheres, and Toruses

This is straying from the point; but if any graph can be described by canonized trees made from its subgraphs, then what are the properties of very large (regular) graphs? A grid, for example?

Starting with a square, and fusing squares together results in this situation:


two and three fused squares are similar, at the height-two tree level. With four rings, a new type c appears (b becomes b' with three rings). Beyond this point, any number of rings fused in a row like this has the same structure.

Moving to a second dimension of growth, a square grid (Gnn) has the following structure:


On the left are 'snapshots' of the advancing wave of the tree. Looks a lot like a breadth-first search, I suppose. On the right are the trees for each snapshot, with increasing heights. Although this is not shown, 8 of the 20 leaves of the third tree are duplicates. This should be clear from the third snapshot, which has only 12 (filled) circles on the 'wavefront'.

These trees can even be extended to grids wrapped around three-dimensional objects. Or, to put it another way, grids wrapped up as surfaces:

The diamond shapes with lines radiating out are the expanding trees. To the left of each surface is a very rough sketch of what the spanning tree would be like. The dashed lines indicate cutpoints where the wavefronts meet - these are duplicated on the trees. This is similar to the idea of 'gluing' surfaces in topology.

Comments

Popular posts from this blog

chalky

I wanted to show something that hints at the things that the new architecture can afford us: This is using a Java2D graphics Paint object to make it look like chalk...kindof. It's a very simplistic way of doing it by making a small image with a random number of white, gray, lightgray, and black pixels. edit: it doesn't look so good at small scales some tweaking of stroke widths and so on is essential.

1,2-dichlorocyclopropane and a spiran

As I am reading a book called "Symmetry in Chemistry" (H. H. Jaffé and M. Orchin) I thought I would try out a couple of examples that they use. One is 1,2-dichlorocylopropane : which is, apparently, dissymmetric because it has a symmetry element (a C2 axis) but is optically active. Incidentally, wedges can look horrible in small structures - this is why: The box around the hydrogen is shaded in grey, to show the effect of overlap. A possible fix might be to shorten the wedge, but sadly this would require working out the bounds of the text when calculating the wedge, which has to be done at render time. Oh well. Another interesting example is this 'spiran', which I can't find on ChEBI or ChemSpider: Image again courtesy of JChempaint . I guess the problem marker (the red line) on the N suggests that it is not a real compound? In any case, some simple code to determine potential chiral centres (using signatures) finds 2 in the cyclopropane structure, and 4 in the ...

The Gale-Ryser Theorem

This is a small aside. While reading a paper by Grüner, Laue, and Meringer on generation by homomorphism they mentioned the Gale-Ryser (GR) theorem. As it turns out, this is a nice small theorem closely related to the better known Erdős-Gallai  (EG). So, GR says that given two partitions of an integer ( p and q)  there exists a (0, 1) matrix   A  iff p*   dominates q such that the row sum vector r(A)  = p  and the column sum vector c(A) = q . As with most mathematics, that's quite terse and full of terminology like 'dominates' : but it's relatively simple. Here is an example: The partitions p  and q  are at the top left, they both sum to 10. Next, p is transposed to get p*  = [5, 4, 1] and this is compared to q at the bottom left. Since the sum at each point in the sequence is greater (or equal) for p*  than q , the former dominates. One possible matrix is at the top left with the row sum vector to the right, and th...