- #1

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Yes, no?

- Thread starter Rockazella
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- #1

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Yes, no?

- #2

Alexander

That is why magnetic force is such "twisted" force - because it is the result of existence of such "twisted" object as a vector product.

- #3

Hurkyl

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Vectors are used to represent directions. They are good at representing a single direction, such as pointing along a line... however they are somewhat clumsy at representing a multidimensional direction, such as describing a plane.

The "natural" way to describe a planar direction is with something called a bivector. Just like a vector points along a direction and has a size, a bivector points along a planar direction and has a size. There is something called a "wedge product" that allows you to multiply two vectors to yield a bivector that contains them and has the appropriate size.

Now, it is somewhat more complicated to deal with bivectors, because they are a more complicated concept. However, in three dimensional space, we can simplify them via using a complementary space. Instead of using the bivector which describes a planar direction, we use the normal vector which describes the direction perpendicular to the planar direction. That is what the cross product computes.

- #4

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All true but I get the impression that the original poster wasn't really at this stage, so at the risk of being simplistic:Originally posted by Hurkyl

Cross products seem abstract because they are aredualto the concept they actually describe.

The cross-product appears whenever there is rotation or a tendancy for something to try to rotate.

Think of a whirlpool - the water can rotate clockwise or anti-clockwise about the centre. To allow us to perform calculations with both cases, we assign one a positive sign and the other a negative sign. If we're looking down on the pool from above, we take anticlockwise as positive and clockwise as negative. We can then describe the anticlockwise rotation by an arrow pointing upwards and whose length is proportional to the speed of rotation. Clockwise rotation is represented by a vector pointing downwards. So, the speed and direction of the rotation is represented by a vector normal to the surface.

Now consider a force F acting at some distance r from a central point; this produces a turning moment M about the centre, the magnitude of M is F.r.sin(w) (where w is the angle between F and r) and M is either clockwise or anticlockwise depending on the direction of F. Both of these cases are contained in the cross product:

M = r x F.

Beware: this only works in 3-D space, the only space in which there is one and only one axis (which may point up or down) at right angles to a plane.

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- #5

Alexander

Actually an element (portion) of surface or of plane IS a vector. Recall Gauss law (=scalar product of area with field).Originally posted by Hurkyl

Vectors are used to represent directions. They are good at representing a single direction, such as pointing along a line... however they are somewhat clumsy at representing a multidimensional direction, such as describing a plane.

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- #6

chroot

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Actually, it is not -- which is the reason Hurkyl posted what he did. The only manifold in which you can get away with describing a plane with a vector is R^3. In general, you cannot use a vector to describe a plane; you'd use the wedge products of two vectors. In normal Euclidean 3-space R^3, the wedge product is the 'same' as a cross product. (Omitting the 'trivial' detail of chriality when demoting a 2-form to a 1-form.)Originally posted by Alexander

Actually an element (portion) of surface or of plane IS a vector. Recall Gauss law (=scalar product of area with field).

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