Hopefully just the stupid half.
Hopefully just the stupid half.
Does fiscally conservative count? Because that's what I am![]()
That statement was really aimed more at the extreme, Glen Beck/Sarah Palin worshipers. Regular conservatives don't bother me any more than regular liberals.
One more delay away from 2012.
I'm surprised that no one has yet mentioned that today is the birthday of the father to the theories of relativity; Albert Einstein. 131 days ago today.
It's amazing how much an affect one person can have on so many fields of physics.
Been busy with basketball todayI gave my props and well wishes this morning on my FB page if that counts.
That works! I do love my astronomy calendar, so full of useful dates. Such as Saturday 20th being the anniversary of Isaac Newtons death.
Kind of a random question, but does anyone have a good place to start to learn Brownian motion that kind of gives a brief background of the stochastic calculus and sigma algebra needed to understand it. I can't seem to find any explanations or lecture notes online that don't assume that you're writing a dissertation on the subject. I'm more interested in the option pricing theory behind it, but even a model used to describe particle movement would be great if it's slightly simplified.
Have you tried a statistical mechanics textbook? Or thermal physics? Something like this:
http://www.amazon.com/gp/product/157...der_1577666127
You should be able to find books like this at your school library or on demonoid or rapidshare or something.
Edit: http://www.amazon.com/Modern-Course-...der_3527407820
Another good one. But most Statistical Mechanics books will have something on brownian motion. I actually learned about brownian motion from a book on computational physics. I can't remember the exact book it was though.
Yeah I'm on spring break so I haven't checked the library at my school yet, was just seeing if anyone knew of anything online to get me started. Thanks for the suggestions though.
For internet sources I'd just go to a torrent and try to find pdf files of statistical mechanics books. But like I said, if you're good at programming, learning from a computational physics book may be a good idea. You can download those as pdf files too, but not all of them go over brownian motion. If I could remember which one I learned brownian motion from, I'd find the pdf for you.
Saw this at work today, thought it was pretty interesting
http://www.scientificamerican.com/ar...ames-webb-jwst
EDIT: URL not working right because of the = sign in it, article title is 6 Fun Facts about the James Webb Space Telescope. Neat pictures of it and the development.
What kind of space are we dealing it in relavity, and what mathematical axiom are used before we reach the s² metrics. It's never defined clearly in the book I'm using, they always jump to s² metrics without defining anything.
Numerous answers, differentiable manifold, pseudo-Riemannian manifold, such that the metric tensor need not be strictly positive definite.
Wait, lemme pull up the wiki, since I couldn't know this stuff on my own.
http://en.wikipedia.org/wiki/Pseudo-Riemannian_manifold
There ya go, from matrices to that should be simple enough.
Further into the basics: http://en.wikipedia.org/wiki/Differentiable_manifold
or further down the rabbit hole: http://en.wikipedia.org/wiki/Introdu...ral_relativity
and
http://en.wikipedia.org/wiki/Mathema...ral_relativity
Believe it or not, you can do a lot more by reading through these wiki pages, and using the heavily crosslinked nature of the articles to further investigate terms you don't recognize, than simply find stuff to copy/paste to try and appear smart.
Whoops, I assumed you meant GR, not SR, if you meant SR then these are what you're after: http://en.wikipedia.org/wiki/Minkowski_space and http://en.wikipedia.org/wiki/Riemannian_manifold for further info on the positive definite Riemannian forms.
Yeah, I already read most of these.
I was simply wondering what's the difference between euclidian R^4 and the space we use in general relativity. Is the only difference the metric/pseudo metric (and it's implication), or is there something that else I'm missing?
Basically, I had an argument with a teacher, and I'm writting a follow up e-mail. I just want to be sure of my stuff before sending it.
Yeah, it's the mapping variations between Euclidean with it's flat metric and Pseudo-Riemannian which can have variable metrics.
I believe Euclidean is isomorphic, lemme check, ah, it is isomorphic to any n-dimensional vector space, and Riemannian is at best diffeomorphic, there can be a map produced, but it can vary depending on the space it is being mapped to/from.
tl;dr, the mapping and metric are the big differences before you start applying tensor structures and shit like that.
To further check your points: http://en.wikipedia.org/wiki/Isomorphism
http://en.wikipedia.org/wiki/Homeomorphism
http://en.wikipedia.org/wiki/Diffeomorphism
Euclidean can have diffeomorphic maps produced to pseudo-Riemannian spaces, but you can't do calculus normally on said manifold as it is.
Ah, this should be what you're trying to find:
From good old: http://en.wikipedia.org/wiki/Euclidean_spaceIn modern mathematics, Euclidean spaces form the prototypes for other, more complicated geometric objects. For example, a smooth manifold is a Hausdorff topological space that is locally diffeomorphic to Euclidean space. Diffeomorphism does not respect distance and angle, so these key concepts of Euclidean geometry are lost on a smooth manifold. However, if one additionally prescribes a smoothly varying inner product on the manifold's tangent spaces, then the result is what is called a Riemannian manifold. Put differently, a Riemannian manifold is a space constructed by deforming and patching together Euclidean spaces. Such a space enjoys notions of distance and angle, but they behave in a curved, non-Euclidean manner. The simplest Riemannian manifold, consisting of Rn with a constant inner product, is essentially identical to Euclidean n-space itself.
If one alters a Euclidean space so that its inner product becomes negative in one or more directions, then the result is a pseudo-Euclidean space. Smooth manifolds built from such spaces are called pseudo-Riemannian manifolds. Perhaps their most famous application is the theory of relativity, where empty spacetime with no matter is represented by the flat pseudo-Euclidean space called Minkowski space, spacetimes with matter in them form other pseudo-Riemannian manifolds, and gravity corresponds to the curvature of such a manifold.
I didn't realize you were asking literally for the defining difference between a Euclidean and Riemannian.