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- Xref: sparky sci.math:18794 sci.physics:23533
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- From: mcirvin@husc8.harvard.edu (Matt McIrvin)
- Newsgroups: sci.math,sci.physics
- Subject: Re: Vectors Question
- Message-ID: <mcirvin.728078636@husc.harvard.edu>
- Date: 26 Jan 93 20:03:56 GMT
- Article-I.D.: husc.mcirvin.728078636
- References: <93025.223136A54SI@CUNYVM.BITNET>
- Lines: 28
- Nntp-Posting-Host: husc8.harvard.edu
-
- <A54SI@CUNYVM.BITNET> writes:
-
- > Let us set c = a cross b. In my mind, if a and b are both polar or they are
- > both axial then c is axial. I do this by picturing reflections performed on
- > the vectors, and I am fairly certain of this result. If we try to cross two
- > vectors of different types, then the c vectors before and after the
- > reflection (c and c') differ in magnitude as well as direction and so
- > I feel that it's impossible to cross different type vectors. Be that as it
- > it may you won't get a polar vector by crossing a polar with and axial
- > (Unless my mental pictures are totally wrong.)
-
- I think you will, actually. The terms axial and polar don't refer to
- mirror reflections, exactly; they refer to how the vector transforms under
- the transformation x -> -x, where x is a position vector. In general
- that's equivalent to a mirror reflection combined with some rotation; you
- can think of it as mirror reflection through *all three* coordinate planes.
- Under this space inversion a polar vector reverses direction and an
- axial vector doesn't.
-
- Now suppose a is axial and b is polar. The product a x b points in
- a direction given by the right hand rule, of course, and its magnitude
- is given by |a||b| sin theta where theta is the angle between the two
- vectors. a is unchanged and b goes to -b. This leaves theta unchanged,
- as well as |a| and |b|; all that changes is the direction given by the
- right-hand rule. Therefore the product reverses direction and is a
- polar vector.
- --
- Matt McIrvin
-