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Physical significance would be nice, and cartesian components if possible. Perhaps there's an identity I'm missing that would shed some light on the situation.

2006-09-05 12:01:48 · 3 answers · asked by Sean43243234 1 in Science & Mathematics Physics

3 answers

The other answerers aren't considering something.

In the following I will use a '.' to represent the dot product.

So if:
(A . Del)B = A . Del(B) as he suggests, you would be taking the gradiant of a vector, which is not a vector (it's not well defined in strictly vector algebra - but can be in more advanced stuff). So that's not a well-defined equation. You either need to get into carternians or tensors, or just tensor notation. I'm sure that's not what you want to do. But sometimes you do in a physical application, which is why you really need parenthesis uses right.

What it really means is (A . Del) operating on vector B. (notice A . Del does not equal Del . A, so this is not a commutative process). (A . Del) gives you a scalar, not a vector. So when you operate it on B you're going from a vector to a vector since each component of B gets operated on by (A . Del) .

What that means physically depends on your application. I'm not sure if I can come up with a conceptual explanation. Maybe someone else can? I just know it shows up a lot in Physics.

After thinking about it, I'd say it tells you how each component of B changes with position in the A direction.

2006-09-05 13:21:15 · answer #1 · answered by Davon 2 · 0 0

I think, A (dot DEL) B is the dot product of vector A and (del B).

Which means the component of A in the direction of (del B).

Hey, if it is not the correct answer pls let me know the correct answer when you get it. Good Luck.

2006-09-05 12:17:41 · answer #2 · answered by muggle_puff 2 · 0 0

One place I've seen this used is in the convective time derivative of hydrodynamics. If A is fluid velocity, it gives the total time derivative of B when added to the partial time derivative of B.

2006-09-05 15:30:00 · answer #3 · answered by Dr. R 7 · 0 0

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