Earlier quoted context omitted.
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.
Specific to building _intuitions_ for why the Banach-Tarski arises in ZF+AC. 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 arbi…
Physics for Mathematicians – Introduction
61–63 of 63 posts
Re: Physics for Mathematicians – Introduction
#62This is really cool. Can also serve as a Rosetta Stone for physicists wanting to better understand the language of mathematicians.
Re: Physics for Mathematicians – Introduction
#63Earlier quoted context omitted.
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.
Specific to building _intuitions_ for why the Banach-Tarski arises in ZF+AC. 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 arbi…
To answer some of the other points
1. No physicist is particuarly confused by Euler angles, and gimbal lock is not a problem in physics.
2. I'm not sure I agree that physics even uses computable reals or rationals. I would say in reality we use fuzzy confidence intervals mostly and not exact numbers.
3. Maxwell's equations look different when written in geometric algebra style, you get one neat looking equation rather than the traditional 4, but its just a difference of notation, the same stuff is happening just written in a slightly different way.
4. A tensor can represent a spinor if you let it transform under the correct transformation rule. A basic spinor just looks like (https://en.wikipedia.org/wiki/Dirac_spinor) a complex vector which you let the Clifford algebra act on.
More generally everything I've seen from Geometric Algebra enthusiasts is just a weird way of doing fairly standard stuff in special cases of Clifford algebras in slightly weird old-fashioned notation. Pretty much everyone I've seen doing real work just does stuff in the Clifford algebra.