Re: resolve to perpendicular components, because they are independent


"FrediFizzx" <fredifizzx@xxxxxxxxxxx> wrote in message
news:43gpcpF1nr999U1@xxxxxxxxxxxxxxxxx
> "Ken S. Tucker" <dynamics@xxxxxxxxxxxx> wrote in message
> news:1137871786.842707.317150@xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx
> |
> | FrediFizzx wrote:
> | > "Ken S. Tucker" <dynamics@xxxxxxxxxxxx> wrote in message
> | > news:1137804799.742330.45120@xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx
> | > |
> | > | FrediFizzx wrote:
> | > | > "Ken S. Tucker" <dynamics@xxxxxxxxxxxx> wrote in message
> | > | > news:1137800854.404588.75250@xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx
> | > | > |
> | > | > | Timo Nieminen wrote:
> | > | > | > On Fri, 20 Jan 2006, Ken S. Tucker wrote:
> | > | > | >
> | > | > | > > I find nonorthogonal axes easier than orthogonal,
> | > | > | >
> | > | > | > Then you must be some kind of bizarre freak of nature!!!
> | > | > |
> | > | > | Not really, as in Chess, solving problems in mathematical
> | > | > | physics consists of keeping your options open, to be
> | > | > | closed by physical principle, and certainly not by an aprior
> | > | > | preceived convenience. It's well known "orthogonality" is
> | > | > | at best an approximation in a g-field, but Reimann and his
> | > | > | "gang" evolved quite a nice "tensor" analysis notation that
> | > | > | is easier to use than clunky "ijk" unit vectors.
> | > | > |
> | > | > | > > indeed a Curl
> | > | > | > > becomes A_u,v - A_v,u (== &A_u/&x^v - &A_v/&x^u), because
> | > | > | > > manipulating equations in tensors is streamlined by
> notation.
> | > | > | >
> | > | > | > Can't you just do that with orthogonal metrics too? (Mixing
> | > | > covariant and
> | > | > | > contravariant is just a naughty little trick to hide the
> metric
> | > | > tensor!)
> | > | > |
> | > | > | If your intrinsic dimensionality differs from an integer, i.e
> | > | > | let n= intrinsic dimensionality =2.9, then how the heck do
> | > | > | you expect to squeeze 3 orthogonals into that?
> | > | >
> | > | > Hmm... I wonder if that would apply to what Lisa Randall is
> calling
> | > | > "Warped Passages"?
> | > |
> | > | LOL, ok, how about a link, Randall is super-pop, so
> | > | I know you're not jokin...
> | >
> | > "Discretizing Gravity in Warped Spacetime"
> | > http://www.arxiv.org/abs/hep-th/0507102
> | >
> | > I haven't read this yet but maybe it has something. I was mainly
> | > referring to something she was saying in her new book (did you get
> it
> | > yet? ;-) ). I didn't make the connection at the time I was reading
> it
> | > until you brought this up (forgot what you call it) again.
> | > FrediFizzx
> |
> | Here's an interesting quicky...
> |
> | http://en.wikipedia.org/wiki/Fractional_calculus
> |
> | that demo's a departure from our usual "integer" thinking, we
> | commonly apply to both calculus and so to dimensionality.
> |
> | Recall that when we integrate a line like "x" by
> |
> | $ x dx = x^2/2 == area
> |
> | we go from 1D "x" to 2D "x^2" , but what the link above shows
> | is that integration (and differentiation) can be a continuous thing,
> | and so can dimensionality.
> |
> | Is that where we're going?
>
> Yep, I am really thinking that this is what she is talking about with
> "warped" spacetime. Now what is that particular name you had for this?
> Sheesh... I can't believe I forgot it!

Warped mind, perhaps?
Have some curved spacetime:
http://ww2010.atmos.uiuc.edu/(Gh)/guides/mtr/fw/crls.rxml
Hexenmeister.


.

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