Curl of a vector using indicial notation

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The discussion focuses on demonstrating that the expression ε_{ijk}A_{k,j} represents the curl of the vector A_k in indicial notation. The original poster has successfully computed the cross product but struggles with transforming it into the alternating tensor form. Participants suggest explicitly writing out the components of both the curl and the tensor expression to verify their equivalence. Clarifications are provided regarding the meaning of free and dummy indices, as well as the definitions of ε_{ijk} and A_{k,j}. The conversation emphasizes the importance of understanding these concepts to solve the problem effectively.
jbrisby
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Homework Statement



A.) Show that \epsilon_{ijk}A_{k,j} represents the curl of vector A_k

B.) Write the expression in indicial nottation:
\triangledown \cdot \triangledown \times A


2. The attempt at a solution
I'm hoping that if I can get help on part A.) it will shed light on part B.) I have several more of these to do but not going to ask all of them here. For A.) I have done the cross product easily enough:
\begin{bmatrix}<br /> i &amp;j &amp;k \\ <br /> \frac{\partial }{\partial x_i} &amp;\frac{\partial }{\partial x_j} &amp;\frac{\partial }{\partial x_k} \\ <br /> A_1&amp;A_2 &amp;A_3 <br /> \end{bmatrix} = i(\frac{\partial A_3 }{\partial x_j}-\frac{\partial A_2 }{\partial x_k})-j(\frac{\partial A_3 }{\partial x_i}-\frac{\partial A_1 }{\partial x_k})+k(\frac{\partial A_2 }{\partial x_i}-\frac{\partial A_1 }{\partial x_j})

I'm having problems transforming this into the alternating tensor form. Everything I've found for the problem just states that the product can be expressed as \epsilon_{ijk}A_{k,j} without any mention of how that happens. If someone could break down the transformation for me it would be greatly appreciated.
 
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First of all, note that your ##i,j,k## mean different things in different equations. This could lead to some confusion.

Either way, I guess they want you to write out each component of ##\nabla \times \mathbf{A}## and ##\epsilon_{ijk}A_{k,j}## explicitly and verify that they are equal. Can you do that?
 
I edited the equation so maybe it'll make more sense. I'm not sure how to show that the cross product is transformed into the alternating tensor form.
 
As I said, write out each component of both expressions explicitly. You have more or less done so for ##\nabla \times \mathbf{A}##. It is probably more convenient to use ##\mathbf{e}_1, \mathbf{e}_2, \mathbf{e}_3## rather than ##\mathbf{i}, \mathbf{j},\mathbf{k}##.

Can you write out each component of ##\epsilon_{ijk}A_{k,j}## explicitly, i.e., do you know what the expression actually means?
 
I'm not sure that I have the grasp on the meaning of it, which is why I'm having the problem. I think that the components of the alternating tensor look like \begin{bmatrix}<br /> \epsilon_{111}A_{1,1} &amp;\epsilon_{112}A_{1,2} &amp;\epsilon_{113}A_{3,1} \\ <br /> \epsilon_{121}A_{1,2} &amp;\epsilon_{122}A_{2,2} &amp;\epsilon_{123}A_{3,2} \\ <br /> \epsilon_{131}A_{1,3} &amp;\epsilon_{132}A_{3,2} &amp;\epsilon_{133}A_{3,3}<br /> \end{bmatrix}

(I'm sure my notation is sloppy)
 
Do you know what a free index and a dummy index is?

How is ##\epsilon_{ijk}## defined?

What does ##A_{k,j}## look like?

If you are having trouble answering these questions, I suggest that you read up on it in your textbook or lecture notes.
 
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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