There is no proof per se of the vector product. It's a definition; not a theorem. It's defined because doing so and using it simplifies many equations in physics.
2006-12-25 06:26:45
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answer #1
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answered by pollux 4
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Pollux is right.
When I spotted this question I was eager to point out that it's a definition not a theorem.
It main usefulness, and original motivation, comes from physics, If you've ever twisted a wrench then you've generated a vector quatity, torque, by using the cross product of force and distance. If you've used a cheater bar on a wrench then you've increased the distance vector to increase the torque vector while using the same force vector.
A right handed coordinate system is one in which X cross Y = Z,
where X,Y,Z are vectors. It's also the right hand rule.
So, vector cross products are used big time in physics.
2006-12-25 07:01:59
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answer #2
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answered by modulo_function 7
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I expect that your question will be answered by knowing the historical derivation of vector algebra.
Why did the inventors of vector algebra make the definitions that we use today?
The mathmetician Hamilton figured out how to make an algebra to describe rotations in three dimensional space.
He defined quantities i, j, k that had the folllowing propertities.
i * i = j * j = k * k = -1
i * j = k ; j * k = i ; k * i = j
j * i = -k ; k * j = -i ; i * k = - j
This algebra, developed by Hamilton, and called quaterions,
has evolved into vector algebra and the original quaterion multiplication has been split into dot product and cross product.
i . i = j . j = k . j = 1
i . j = j . k = k . i = 0
i x i = j x j = k x k = 0
i x j = k ; j x k = i ; k x i = j
j x i = -k ; k x j = -i ; i x j = - j
2006-12-25 13:49:01
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answer #4
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answered by kermit1941 2
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this is basically a definition used via mathematicians and physicists. a x b = moda. modb. sintheta. n(hat) is the axiom somebody invented some years in the past it quite is sensible for some problems. extra problems upward thrust up while one realises that a x b isn't possibly a real vector yet a pseudo-vector yet this would not subject many human beings!
2016-11-23 16:41:08
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answer #5
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answered by Anonymous
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Yes, it is definition; Let
vector A=Ax*i + 0*j +0*k and
vector B= Bx*i +By*j +0*k = |B|*cos(phi)*i +|B|*sin(phi)*j,
where: –180
then according to definition cross-product C = [A*B] =
|``i`````j`````k|
|Ax````0````0| = Ax*By*k = Ax*|B|*sin(phi)*k,
|Bx```By```0|
hence dot products (C*A)=0 and (C*B)=0;
thus C is normal to both A and B; and |C| = |A|*|B|*sin(phi), where 0<=phi<180;
2006-12-25 09:17:52
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answer #6
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answered by Anonymous
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it is the outer product you mean
for the result of v = a x b
v is perpendicular to a and b
you can see this by the orthogonal projection of v onto the space spanned by axb
the projection will have only one point, thus _|_
2006-12-25 17:14:46
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answer #7
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answered by gjmb1960 7
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The Vector Product of two vectors is:
Z = DET(i,j,k; x1,x2,x3; y1,y2,y3) =
(x2·y3-y2·x3, y1·x3-x1·y3, x1·y2-y1·x2)
z is perpendicular to x?
= x1(x2·y3-y2·x3)
+x2(y1·x3-x1·y3)
+x3(x1·y2-y1·x2)
= 0
Implies z is perp. to x.
z is perpendicular to y?
= y1(x2·y3-y2·x3)
+y2(y1·x3-x1·y3)
+y3(x1·y2-y1·x2)
= 0
Implies z is perp. to y and x and,
therefore, to the plane.
2006-12-25 08:08:29
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answer #8
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answered by Stan L 2
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