Understanding Index Notation and Tensor Operations in Vector Calculus

Niles
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Homework Statement


Hi

I have a vector v. According to my book, the following is valid:
<br /> \frac{1}{2}\nabla v^2-v\cdot \nabla v = v\times \nabla \times v <br />
I disagree with this, because the first term on the LHS I can write as (partial differentiation)
<br /> \frac{1}{2}\partial_i v_jv_j = v_j\partial_i v_j <br />
which is just v\cdot \nabla v. So IMO it should equal 0.

What is wrong here?
 
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Niles said:

Homework Statement


Hi

I have a vector v. According to my book, the following is valid:
<br /> \frac{1}{2}\nabla v^2-v\cdot \nabla v = v\times \nabla \times v <br />

I disagree with this, because the first term on the LHS I can write as (partial differentiation)
<br /> \frac{1}{2}\partial_i v_jv_j = v_j\partial_i v_j <br />
which is just v\cdot \nabla v. So IMO it should equal 0.

What is wrong here?

v_j \partial_i v_j \neq v_j \partial_j v_i = (v \cdot \nabla) v_i

Note that on the left the index on the derivative is i (a free index), but on the right the index on the derivative is j (a dummy index).
 
Thanks. I hope there is omething else you can help me with (you seem to have experience with this kind of notation). Is the following always true for some vector u?

<br /> \nabla \cdot (\nabla u) = \nabla (\nabla \cdot u)<br />
 
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