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Cross Product |
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| Jan31-13, 02:59 PM | #1 |
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Cross Product
What is the cross product of a constant and a vector? I know that the cross product between two vectors is the area of the parallelogram those two vectors form. My intuition tells me that since a constant is not a vector, it would only be multiplying with a vector when in a cross product with one. Since the vector will only grow larger in magnitude, there would be zero area in the paralleogram formed because there is no paralleogram.
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| Jan31-13, 03:02 PM | #2 |
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The cross product is only defined between vectors of [itex]\mathbb{R}^3[/itex]. The cross of a constant and a vector is not defined.
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| Jan31-13, 03:47 PM | #3 |
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So if I had an equation that contains a term that has a cross product of a constant and a vector, do I just cross it out of the equation? ( it is in an adding term so crossing it out would be okay). That's an awesome joke(:
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| Jan31-13, 04:03 PM | #4 |
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Cross Product |
| Jan31-13, 04:26 PM | #5 |
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Sure! An equation like F=π[hXh+cXh] where h is a vector and c is a constant.
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| Jan31-13, 04:41 PM | #6 |
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| Jan31-13, 04:47 PM | #7 |
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F is a vector.
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| Jan31-13, 04:55 PM | #8 |
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F=π[hXh+cXh] Sorry about not adding the equality.
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| Jan31-13, 05:33 PM | #9 |
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Would the term containing the cross product of the constant c and vector h in the above equation just be zero? Or am I able to take cross it out of the above equation?
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| Jan31-13, 05:35 PM | #10 |
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| Jan31-13, 05:43 PM | #11 |
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Damn that stinks. Even if the c was a constant?
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| Jan31-13, 05:52 PM | #12 |
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| Jan31-13, 06:09 PM | #13 |
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Well I made it up haha. Im sorry. I'm new at this. Do you think you can make an equation that makes sense? Like the one I attempted but failed at.
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| Jan31-13, 06:54 PM | #14 |
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What were you attempting to do?? What lead you to this particular equation? |
| Jan31-13, 07:16 PM | #15 |
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Well, the h is a vector that represents a magnetic field strength. In the definition of a current, I=dq/dt, multiplying both sides by a small length ds would give the magnetic field produced my a moving charge. (dq/dt)ds turns into dq(ds/dt) which turns into vdq where dq is a small piece of charge and v is the velocity of the total charge. Integrating both sides to I ds=vdq would give the total magnetic field. For a constant velocity, the right side of the above equation turns into vq+ c, where c is some constant. Now I get the equation h=vq+c. Solving for qv gives me h-c=qv. In the equation for magnetic force on a moving charge, F=qvxB. I substituted h-c for qv in the above force equation. B turns into uh where u is the permeability of free space. I substitute uh for B in the magnetic force equation and get F=u[hxh-cxh]. I want the cxh term to go away.
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| Jan31-13, 07:18 PM | #16 |
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Does that sort of help?
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| Jan31-13, 07:26 PM | #17 |
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I don't understand any of what you said, but my physics is very bad. I'll move this to the physics section for you.
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