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Can you send some material on port hamiltonians?
I'm reading this paper: http://www.math.rug.nl/arjan/DownloadPublicaties/ICMvanderSchaft.pdf
It looks like they get halfway to what I got:
They consider forces as inputs instead of also flows!
Aha! This is what I was talking about: they remove the necessity of having an even-dimensional symplectic manifold by considering something more general:
image.png
This paper is extremely exciting
If I can make port-Hamiltonians into an operad, I think that I will have done something important
It's a Lagrangian subspace!
Oh wait, not quite
It's not with respect to symplectic structure, it's with respect to the normal bilinear form
Interesting
OK, this guy actually wrote a more recent book on this: http://www.math.rug.nl/arjan/DownloadVarious/PHbook.pdf
Interestingly enough, he considers switched systems
Which is what I did to derive the Carnot cycle
Ah, and they even do a bit of thermodynamics in this book: http://www.math.rug.nl/arjan/DownloadVarious/PHbook.pdf
Whoops
He wrote a very recent paper (2020) on thermodynamics: https://arxiv.org/pdf/2010.04213.pdf
It's not "port hamiltonians", it's always "port-hamiltonian". "Port-" is basically a synonym for "open".
The first paper you linked to by van der Schaft is one of the good papers I was going to find for you. Equations (1-5) should remind you of things you told me about... though maybe they're a bit different?
OK, so my "flow systems" are pretty much exactly port-Hamiltonian systems, I just hadn't worked out all the details yet.
I wish you had told me about these earlier... maybe you did but I just didn't listen
OK, so making port-Hamiltonian systems into an operad algebra is almost completely trivial
I'll write it up more formally, but the short answer is that there is a PROP where the morphisms between and are the "Dirac structures" . These are similar to Lagrangian relations, but the definition is slightly different.
Then there is a lax symmetric monoidal functor from this PROP to Set that sends to the set of port-Hamiltonian systems with interface . The laxator takes the product of the state spaces of the various port-Hamiltonian systems, and adds together the Hamiltonians.
Then, we apply the same construction we did in the thermostatics paper to make an operad.
It's almost boring how easy this is
Arjan van der Schaft has done pretty much all of the necessary proofs, he just didn't know about SMCs or operads
Owen Lynch said:
I wish you had told me about these earlier... maybe you did but I just didn't listen
It's a bit hard to know what I should tell you about before it becomes clearly relevant. I believe existing port-Hamiltonian mechanics only handles systems with vector spaces as phase spaces. I'm pretty sure I told you about my paper Open systems in classical mechanics which describes an approach that can handle general symplectic manifolds. The last paragraph in the intro says:
In future work we hope to compare the present approach to the theory of port-Hamiltonian systems, an approach to open systems in classical mechanics widely used in engineering [29].
[29] is a reference to "Port-hamiltonian systems theory: an introductory overview" by van der Schaft and Jeltsema. That's a different paper than the one you're reading, right?
Chapter 3 of the book by van der Schaft handles manifolds: http://www.math.rug.nl/arjan/DownloadVarious/PHbook.pdf#chapter.3
Interesting - my friend Eugene Lerman, who is into symplectic geometry and wrote a paper with Spivak, complained that work on port-Hamiltonian systems assumed a linear phase space! I'd never seen a good nonlinear version. But my coauthor David Weisbart was working on one. (I think he's gotten distracted.)
It is not as easy (I think) to do the operad with the nonlinear version, so there may yet be opportunities for improvement
Also, my impression (which could be off; I've only skimmed the paper) is that for Open systems in classical mechanics, you compose systems by glueing together their phase spaces via pullback. In port-Hamiltonian systems, one takes the product of the phase spaces, and then equalizes forces and fluxes. So perhaps these are complementary approaches.
The fact that this paper treats intensive quantities using projective geometry feels very right to me.
https://arxiv.org/pdf/2102.05493.pdf
I wonder if the projectivization of the symplectic manifold has something to do with the fact that thermodynamics can happen at any speed.
I.e., a quasi-static process is a limit as the path taken becomes infinitely slow.
Hi Owen, I don't think so. Maybe I am also trying to tell you something that you know better than I do. The contact structure relates the thermodynamic variables (extensive and intensive) according to some generating function (say internal energy) which is called a thermodynamic potential. There are other thermodynamic potentials (Helmholtz free energy, Gibbs free energy, and enthalpy) which generate the same contact manifold and they are all related via the Legendre transformations. The potential (or the contact manifold that it generates) encodes the material behavior. However, the same material behavior could be encoded by entropy and the corresponding Legendre transformed quantities, sometimes called Massieu functions. The idea of projectivization is to encode the material behavior by (homogeneous) Hamiltonian function and a symplectic manifold. The advantage of that is that energetic and entropic representations of the material behavior are united. This might give you a lot of flexibility in choosing variables and Arjan says that some calculations are "simpler" in the symplectic realm but that might also be his preference, idk. I want to clarify that this has nothing to do whatsoever with port-Hamiltonian systems. However, Arjan and Bernhard have worked on porting the "port-cocept" to these systems, then termed "port thermodynamic systems".
Hi Markus! Thanks for popping in here; I'm not sure if I've met you before but it's always good to hear from someone else interested in thermodynamics.
Mathematically, I know that the projectivization doesn't have anything to do with the quasistatic nature; it's just a way of getting at the geometric structure in a convenient way. But one of my eventual goals is to see if contact geometry can be united with/derived from the statistical mechanics of a symplectic manifold. It is my (unfounded) intuition that time-rescaling may come into play in this derivation, and this seems connected to projectivization in my head.
We unfortunately didn't meet yet and I am not that much familiar with statistical mechanics. Although maybe not directly related, maybe you could find something interesting/inspiring in one of the following references: 2020 Montefusco Öttinger Peletier - A Framework of Nonequilibrium Statistical Mechanics ; 2017 Kraaij Azarescu Maes Peletier - Deriving GENERIC from a generalized fluctuation symmetry ; 2021 Patterson Renger Sharma - Variational structures beyond gradient flows A macroscopic fluctuation-theory perspective ; In case unfamiliar, GENERIC is in the first place a different framework for writing thermodynamic systems beyond equilibrium (i.e. with dynamics) that might appear to have less geometric structure. Yet, the equations are coordinate-independent, and GENERIC can be written based on the contact formalism.
These look very interesting! Thanks for the references!