Proving the Vector Triple Product Identity: A x (B x C) = (A x C)B - (A x B)C

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The discussion revolves around proving the vector triple product identity A x (B x C) = (A x C)B - (A x B)C using index notation and the Levi-Civita symbol. Participants express confusion about handling indices and the proper application of summation rules. There is emphasis on distinguishing between free and bound indices, and the importance of correctly applying the contraction of epsilon tensors. A suggestion is made to explicitly write out components to clarify the proof process. The conversation highlights the complexity of tensor notation and the need for careful manipulation of indices to achieve the desired result.
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I have to prove the above equation.
I tried:
$$\bigl[ A\times ( B\times C) \bigr]_i=\sum_{jk} \varepsilon_{ijk}A_j\biggl[ \sum_{ij}\varepsilon_{ijk}B_iC_j\biggr]$$
In order to reach the k'th member of (BxC) but i tested it with i=1 and saw that in the member:
$$\biggl[ \sum_{ij}\varepsilon_{ijk}B_iC_j\biggr]=\biggl[ \sum_{1j}B_1C_j\biggr]$$
And it can't be that B1 is inside the sum since it has to receive also other values.
Then i tried:
$$\bigl[ A\times ( B\times C) \bigr]_i=\sum_{jk} \varepsilon_{ijk}A_j\biggl[ \sum_{ij}\varepsilon_{ijk}B_iC_j\biggr]_k$$
But it doesn't enable me to open the [] brackets, or does it? i am new to this
 
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The first approach is confusing i and k.
The second approach is better, but you still have to rename indices to remove the brackets (j is used twice).
 
Karol said:
I have to prove the above equation.
I tried:
$$\bigl[ A\times ( B\times C) \bigr]_i=\sum_{jk} \varepsilon_{ijk}A_j\biggl[ \sum_{ij}\varepsilon_{ijk}B_iC_j\biggr]$$

You have to be careful about distinguishing between bound (or "dummy") indices and free indices. Your expression is wrong because on the left-hand side is a free index, i, but on the right-hand side, there is no free index.

I think that you would be better off just brute-forcing this. Just write out explicitly:

(A \times (B \times C))_1 = A_2 (B \times C)_3 - A_3 (B \times C)_2
(B \times C)_2 = B_3 C_1 - B_1 C_3
(B \times C)_3 = B_1 C_2 - B_2 C_1
 
$$\bigl[ A\times ( B\times C) \bigr]_i=\sum_{jk} \varepsilon_{ijk}A_j \sum_{lm}\varepsilon_{klm}B_lC_m=\sum_{jk} \varepsilon_{ijk}A_j \varepsilon_{klm}\sum_{lm}B_lC_m$$
I try i=1:
$$\bigl[ A\times ( B\times C) \bigr]_i=\varepsilon_{123}\varepsilon_{312}A_2 B_1 C_2$$
And i stopped substituting since i don't know if i am allowed to change the indices outside the second summation symbol. i now want to substitute l=2 and m=1 but ##\varepsilon_{klm}## is outside of ##\sum_{lm}\varepsilon_{klm}B_lC_m##, its:
$$...\varepsilon_{klm}\sum_{lm}B_lC_m$$
 
The second equation is not right. The component 1 is not a single term but a double sum.
By using the contraction of the epsilons you reduce these sums to two terms.
 
nasu said:
The second equation is not right. The component 1 is not a single term but a double sum.
By using the contraction of the epsilons you reduce these sums to two terms.
Yes, i know that it's not a single term, you didn't understand my question. i could complete the other terms:
$$\bigl[ A\times ( B\times C) \bigr]_i=\varepsilon_{123}\varepsilon_{312}A_2 B_1 C_2+\varepsilon_{132}\varepsilon_{213}A_3 B_1 C_3+\varepsilon_{123}\varepsilon_{321}A_2 B_2 C_1+\varepsilon_{132}\varepsilon_{231}A_3 B_3 C_1$$
The last 3 members have their l and m indices changed while they can be changed only inside the ##\sum_{lm}##, no? the member ##\varepsilon_{klm}## is outside the sum
 
Why is the epsilon klm outside the l-m sum? That's not right. Put the summation signs all the way to the left, then do what nasu says and collapse the epsilons into deltas using the formula in the link.
 
davidmoore63@y said:
Why is the epsilon klm outside the l-m sum? That's not right. Put the summation signs all the way to the left
$$\bigl[ A\times ( B\times C) \bigr]_i=\sum_{jk} \varepsilon_{ijk}A_j \sum_{lm}\varepsilon_{klm}B_lC_m=\sum_{jk}\sum_{lm} \varepsilon_{ijk} \varepsilon_{klm}A_jB_lC_m$$
davidmoore63@y said:
then do what nasu says and collapse the epsilons into deltas using the formula in the link.
In the link it says:
$$\sum_{k} \varepsilon_{ijk} \varepsilon_{klm}=\delta_{il}\delta_{jm}-\delta_{im}\delta_{jl}$$
But, for example, for i=l:
$$\sum_{k} \varepsilon_{ijk}\varepsilon_{imk}=\varepsilon_{ij1} \varepsilon_{im1}+\varepsilon_{ij2} \varepsilon_{im2}+\varepsilon_{ij3} \varepsilon_{im3}=$$
$$=\varepsilon_{321} \varepsilon_{231}+\varepsilon_{132} \varepsilon_{312}+\varepsilon_{213} \varepsilon_{123}=3$$
While the sum:
$$\delta_{il}\delta_{jm}-\delta_{im}\delta_{jl}$$
Can be at most ±1. i don't know to use this formula, how to fill in the indices on the right side, since they take the values 1,2,3. the left side is a summation while the right is?
 
  • #10
Karol said:
$$\bigl[ A\times ( B\times C) \bigr]_i=\sum_{jk} \varepsilon_{ijk}A_j \sum_{lm}\varepsilon_{klm}B_lC_m=\sum_{jk}\sum_{lm} \varepsilon_{ijk} \varepsilon_{klm}A_jB_lC_m$$

In the link it says:
$$\sum_{k} \varepsilon_{ijk} \varepsilon_{klm}=\delta_{il}\delta_{jm}-\delta_{im}\delta_{jl}$$
But, for example, for i=l:
$$\sum_{k} \varepsilon_{ijk}\varepsilon_{imk}=\varepsilon_{ij1} \varepsilon_{im1}+\varepsilon_{ij2} \varepsilon_{im2}+\varepsilon_{ij3} \varepsilon_{im3}=$$
$$=\varepsilon_{321} \varepsilon_{231}+\varepsilon_{132} \varepsilon_{312}+\varepsilon_{213} \varepsilon_{123}=3$$
While the sum:
$$\delta_{il}\delta_{jm}-\delta_{im}\delta_{jl}$$
Can be at most ±1. i don't know to use this formula, how to fill in the indices on the right side, since they take the values 1,2,3. the left side is a summation while the right is?

Could you please try working out a concrete example? You have:

\sum_{k} \varepsilon_{ijk}\varepsilon_{imk}=\varepsilon_{ij1} \varepsilon_{im1}+\varepsilon_{ij2} \varepsilon_{im2}+\varepsilon_{ij3} \varepsilon_{im3}

A particular example: i=3, j=2, m=2:

\sum_{k} \varepsilon_{32k}\varepsilon_{32k}=\varepsilon_{321} \varepsilon_{321}+\varepsilon_{322} \varepsilon_{322}+\varepsilon_{323} \varepsilon_{323}

That's equal to 1.
 
  • #11
When you have satisfied yourself that the formula is correct, the next step is to apply the delta symbols to the components in the following fashion (apologies no latex):

Sigma (m=1 to 3) Delta(j,m) A(m) = A(j)

It's worth persevering with this. Once mastered, the index notation is very powerful.
 
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