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> if it would be possible to make proteins that fold into knots and he pointed out (correctly) that entropy makes it very unlikely this would happen

This is exactly the opposite argument I'd make from entropy:

https://www.npr.org/sections/bryantpark/2008/01/knot_theory_...

There's many ways that a string can be knotted and only one way it can not be knotted.




Note I am talking about entropy of "folding" as a verb- the process by which a fold is adopted. Not the entropy of the final state (which is confusing called a "fold" by some practioners, although that habit is decreasing).

the argument is that the folding process would require the protein to go through an intermediate: forming a loop and then getting one end to go through the loop requires a very specific set of conformations, and reducing the number of conformations has an "entropic cost". Note also that the final post-folding form of a knotted protein isn't really a continuum of many different conformations, but probably one "locked" one which means there really is only a small set of conformations the protein can adopt once locked into the folded, knotted state.

In protein folding, there is not "only one way it can not be knotted"; you have to include all the degrees of freedom in the backbone available in the unfolded state (I am ignoring hydrophobicity and other important sources of entropy which help proteins fold rapidly to the "correct" final state). We already know this pretty well from more basic polymer physics,

but, entropy being subtle, I'm sure there are many different forces at play.


I think with proteins the ways it can be "not knotted" are basically infinite. Topologically-speaking, yeah, it's just a deformed ring. But the deformations (folds) are the huge thing that makes a protein do its job.

So there are tons of folding configurations, and entering a knotted state restricts a lot of the freedom-to-fold a protein would have


Topology gets its utility from collapsing lots of degrees of freedom into a small number of equivalence classes. That's great for reasoning about topological properties, where those degrees of freedom are not relevant, but it doesn't mean those degrees of freedom just go away.




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