There is always the classical lecture notes by Dolgachev on this. https://dept.math.lsa.umich.edu/~idolga/physicsbook.pdf
Physics for Mathematicians – Introduction
51–60 of 63 posts
Re: Physics for Mathematicians – Introduction
#52Earlier quoted context omitted.
Unfortunately, even though it is said to be a "generalization" of these things, mathematical measure theory has nothing to do with physical units of measure or dimensional analysis.
Why?
Re: Physics for Mathematicians – Introduction
#53Hi, this is the author. I've been coming back to this project off and on over the past few years but I often think of these articles as mostly something I'm writing for myself, so I'm really happy to see that some other people might be getting something out of them! I'd definitely love to hear if anyone knows anything I got wrong or can think of a way any particular explanation might be made better. I should also tak…
If you have a Patreon or similar account, let us know!
PS: The Rieman zeta function page seems to be missing a few enclosing tags leading to non-typeset latex formulae after "This gives us a nice way to pick out terms from a Dirichlet series..." and also after the Von Mangoldt function.
Re: Physics for Mathematicians – Introduction
#54Re: Physics for Mathematicians – Introduction
#55Hi, this is the author. I've been coming back to this project off and on over the past few years but I often think of these articles as mostly something I'm writing for myself, so I'm really happy to see that some other people might be getting something out of them! I'd definitely love to hear if anyone knows anything I got wrong or can think of a way any particular explanation might be made better. I should also tak…
Thanks a lot for this effort! As someone wanting to learn physics from a math background, this seems to be at the right level for discussing critical high-level ideas mathematically. The article format is great as I get distracted reading book-length treatments whether they are written by physicists or mathematicians. If you have a Patreon or similar account, let us know! PS: The Rieman zeta function page seems to be…
I appreciate the heads up about the typesetting --- it looks like it's due to some macros that the web-based TeX typesetter I'm using hasn't implemented. I usually go over the PDF versions more carefully than the automatically generated web versions, and I guess this is the price I pay.
EDIT: Should be fixed now!
Re: Physics for Mathematicians – Introduction
#56Skimmed some of the articles, particularly those nearer to my field. Seems like a generally good set of informal notes. Random comments: >when the states evolve in time and the observables don’t we are using Liouville’s picture; when the observables evolve in time and the states don’t we are using Hamilton’s picture. I have never heard this terminology, I have only heard Schrodinger's picture vs. Heisenberg's picture…
> I have never heard this terminology, I have only heard Schrodinger's picture vs. Heisenberg's picture. I wrote the QM article a very long time ago at this point, and I actually can't reconstruct at the moment why I used those two names! I've also heard Schrodinger and Heisenberg much more frequently. Might be worth an edit.
Re: Physics for Mathematicians – Introduction
#57Earlier quoted context omitted.
IMHO that is the result of Gibbs style vectors and the cross product only being validated in R^3 Lie groups and geometric algebra remove a lot of problems. It also applies to differential calculus and ML methods like back propagation and gradient decent. Gibbs style vectors and the cross are convenient as they tend to match our visual intuitions. But lots of the 'physics isn't real math' claims just don't understand…
Could you explain what you think Gibbs style vectors have to do with Banach-Tarski or the axiom of choice? As an aside, I'd like to emphasise that geometric algebra gives exactly the same physics outcomes as doing the maths with vectors or tensors or whatever else you like. The difference is essentially just notation. Some things look prettier.
GA gets rid of the external conventions for coordinate and chirality and also uses SU(2) which is simply connected vs SO(3) which is not. Rotors in GA can be used as elements of the algebra like any number avoiding the complexity of Euler angles, gimbal lock, etc....
GA's rotors are geometrically intuitive and can do rotations around an arbitrary axis, where quaternions are limited to an axis through the origin.
As Banach-Tarski is not physically realizable and because physics uses the computable reals, rationals and other aleph naught numbers it doesn't cause a problem there.
Lots of important work resulted _from_ the Banach-Tarski paradox but really it is just a cautionary tail about ZF+AC and on-measurable sets as far as physics goes.
What I was talking about is tools about building intuitions on why it arises.
Note that the maths aren't exactly the same, as an example Maxwells equations require four separate formula to express in Vector Calculus vs just one in GA. I don't think I fully comprehended the connection before learning GA.
This is also digging deep into the implications of your chosen groups and resulting algebra but as an example:
A Tensor can't represent a spinor but an even multivector can. A pure grade multivector can only completely represent antisymmetric tensors.
You can look into Dirac's belt trick as a physical example showing that SO(3) isn't simply connected but it arises in E(3) in that particular case too.
I wish this site had latex support, so I apologize for the above which is probably of little value in reality.
Re: Physics for Mathematicians – Introduction
#58This introduction must assume that the reader already understands physics deeply, right? For instance, the page on Hamiltonian mechanics stated that force is the derivative of momentum with respect to time. I can't imagine how one will understand the intuition behind the definition without having already learned at least college-level physics.
If you know F=ma, p=mv, and by calculus that a=v', all of which is high school level, then the time derivative of momentum is clearly force.
Re: Physics for Mathematicians – Introduction
#59Hi, this is the author. I've been coming back to this project off and on over the past few years but I often think of these articles as mostly something I'm writing for myself, so I'm really happy to see that some other people might be getting something out of them! I'd definitely love to hear if anyone knows anything I got wrong or can think of a way any particular explanation might be made better. I should also tak…
Thanks a lot for this effort! As someone wanting to learn physics from a math background, this seems to be at the right level for discussing critical high-level ideas mathematically. The article format is great as I get distracted reading book-length treatments whether they are written by physicists or mathematicians. If you have a Patreon or similar account, let us know! PS: The Rieman zeta function page seems to be…
Re: Physics for Mathematicians – Introduction
#60Hi, this is the author. I've been coming back to this project off and on over the past few years but I often think of these articles as mostly something I'm writing for myself, so I'm really happy to see that some other people might be getting something out of them! I'd definitely love to hear if anyone knows anything I got wrong or can think of a way any particular explanation might be made better. I should also tak…