Vector Product and dot product identity: Levi-Civita symbols
$begingroup$
I want to prove that $vec{a}cdot(vec{b}timesvec{c}) = (vec{c} times vec{a})cdotvec{b}$ using the Levi-Civita symbols, however, I am not $100$% sure if my proof is correct.
Please see attached my proof, see the image
Or see the (using MathJax) equations below
$$vec{a}cdot(vec{b}times vec{c}) = a_i(vec{b}timesvec{c})_i = a_iepsilon_{ijk}b_jc_ke_i = -epsilon_{jik}a_ib_jc_ke_i = -(vec{a}timesvec{c})cdotvec{b} = (vec{c}timesvec{a})cdotvec{b}$$
My main concern is that when I change the indices for epsilon from $(i,j,k)$ to $(j,i,k)$, should I also change the index for $e$ vector from $i$ to $j$ as well? It's just in my proof I assume that $b_je_i$ gives vector $b$ and I do not know if I can state that given the different indices.
Thank you in advance and I hope this all does not sound too confusing.
proof-verification vectors tensors
$endgroup$
add a comment |
$begingroup$
I want to prove that $vec{a}cdot(vec{b}timesvec{c}) = (vec{c} times vec{a})cdotvec{b}$ using the Levi-Civita symbols, however, I am not $100$% sure if my proof is correct.
Please see attached my proof, see the image
Or see the (using MathJax) equations below
$$vec{a}cdot(vec{b}times vec{c}) = a_i(vec{b}timesvec{c})_i = a_iepsilon_{ijk}b_jc_ke_i = -epsilon_{jik}a_ib_jc_ke_i = -(vec{a}timesvec{c})cdotvec{b} = (vec{c}timesvec{a})cdotvec{b}$$
My main concern is that when I change the indices for epsilon from $(i,j,k)$ to $(j,i,k)$, should I also change the index for $e$ vector from $i$ to $j$ as well? It's just in my proof I assume that $b_je_i$ gives vector $b$ and I do not know if I can state that given the different indices.
Thank you in advance and I hope this all does not sound too confusing.
proof-verification vectors tensors
$endgroup$
$begingroup$
Well one issue I see is too many of the index i, there are three which makes the product ambiguous as which pair are summed over (since summing happens in pairs). You can fix this by omitting the unit vector as this is how the dot product works
$endgroup$
– Triatticus
Oct 20 '16 at 17:13
$begingroup$
Or you can represent the dot product part as a tensor operation through use of the Kronecker Delta, that is $acdot b = a_i b_j delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:16
$begingroup$
Then you can write your product as $a cdot (btimes c) = a_i (b times c)_j delta_{ij} = a_i (epsilon_{jkl}hat{e}_j b_k c_l) delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:22
$begingroup$
you should look at the problem of calculate the det[a.(bxc)] and compare
$endgroup$
– janmarqz
Oct 20 '16 at 20:31
add a comment |
$begingroup$
I want to prove that $vec{a}cdot(vec{b}timesvec{c}) = (vec{c} times vec{a})cdotvec{b}$ using the Levi-Civita symbols, however, I am not $100$% sure if my proof is correct.
Please see attached my proof, see the image
Or see the (using MathJax) equations below
$$vec{a}cdot(vec{b}times vec{c}) = a_i(vec{b}timesvec{c})_i = a_iepsilon_{ijk}b_jc_ke_i = -epsilon_{jik}a_ib_jc_ke_i = -(vec{a}timesvec{c})cdotvec{b} = (vec{c}timesvec{a})cdotvec{b}$$
My main concern is that when I change the indices for epsilon from $(i,j,k)$ to $(j,i,k)$, should I also change the index for $e$ vector from $i$ to $j$ as well? It's just in my proof I assume that $b_je_i$ gives vector $b$ and I do not know if I can state that given the different indices.
Thank you in advance and I hope this all does not sound too confusing.
proof-verification vectors tensors
$endgroup$
I want to prove that $vec{a}cdot(vec{b}timesvec{c}) = (vec{c} times vec{a})cdotvec{b}$ using the Levi-Civita symbols, however, I am not $100$% sure if my proof is correct.
Please see attached my proof, see the image
Or see the (using MathJax) equations below
$$vec{a}cdot(vec{b}times vec{c}) = a_i(vec{b}timesvec{c})_i = a_iepsilon_{ijk}b_jc_ke_i = -epsilon_{jik}a_ib_jc_ke_i = -(vec{a}timesvec{c})cdotvec{b} = (vec{c}timesvec{a})cdotvec{b}$$
My main concern is that when I change the indices for epsilon from $(i,j,k)$ to $(j,i,k)$, should I also change the index for $e$ vector from $i$ to $j$ as well? It's just in my proof I assume that $b_je_i$ gives vector $b$ and I do not know if I can state that given the different indices.
Thank you in advance and I hope this all does not sound too confusing.
proof-verification vectors tensors
proof-verification vectors tensors
edited Feb 20 '17 at 2:19
Rafael Wagner
1,8332923
1,8332923
asked Oct 20 '16 at 17:05
LiNXOLiNXO
958
958
$begingroup$
Well one issue I see is too many of the index i, there are three which makes the product ambiguous as which pair are summed over (since summing happens in pairs). You can fix this by omitting the unit vector as this is how the dot product works
$endgroup$
– Triatticus
Oct 20 '16 at 17:13
$begingroup$
Or you can represent the dot product part as a tensor operation through use of the Kronecker Delta, that is $acdot b = a_i b_j delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:16
$begingroup$
Then you can write your product as $a cdot (btimes c) = a_i (b times c)_j delta_{ij} = a_i (epsilon_{jkl}hat{e}_j b_k c_l) delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:22
$begingroup$
you should look at the problem of calculate the det[a.(bxc)] and compare
$endgroup$
– janmarqz
Oct 20 '16 at 20:31
add a comment |
$begingroup$
Well one issue I see is too many of the index i, there are three which makes the product ambiguous as which pair are summed over (since summing happens in pairs). You can fix this by omitting the unit vector as this is how the dot product works
$endgroup$
– Triatticus
Oct 20 '16 at 17:13
$begingroup$
Or you can represent the dot product part as a tensor operation through use of the Kronecker Delta, that is $acdot b = a_i b_j delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:16
$begingroup$
Then you can write your product as $a cdot (btimes c) = a_i (b times c)_j delta_{ij} = a_i (epsilon_{jkl}hat{e}_j b_k c_l) delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:22
$begingroup$
you should look at the problem of calculate the det[a.(bxc)] and compare
$endgroup$
– janmarqz
Oct 20 '16 at 20:31
$begingroup$
Well one issue I see is too many of the index i, there are three which makes the product ambiguous as which pair are summed over (since summing happens in pairs). You can fix this by omitting the unit vector as this is how the dot product works
$endgroup$
– Triatticus
Oct 20 '16 at 17:13
$begingroup$
Well one issue I see is too many of the index i, there are three which makes the product ambiguous as which pair are summed over (since summing happens in pairs). You can fix this by omitting the unit vector as this is how the dot product works
$endgroup$
– Triatticus
Oct 20 '16 at 17:13
$begingroup$
Or you can represent the dot product part as a tensor operation through use of the Kronecker Delta, that is $acdot b = a_i b_j delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:16
$begingroup$
Or you can represent the dot product part as a tensor operation through use of the Kronecker Delta, that is $acdot b = a_i b_j delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:16
$begingroup$
Then you can write your product as $a cdot (btimes c) = a_i (b times c)_j delta_{ij} = a_i (epsilon_{jkl}hat{e}_j b_k c_l) delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:22
$begingroup$
Then you can write your product as $a cdot (btimes c) = a_i (b times c)_j delta_{ij} = a_i (epsilon_{jkl}hat{e}_j b_k c_l) delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:22
$begingroup$
you should look at the problem of calculate the det[a.(bxc)] and compare
$endgroup$
– janmarqz
Oct 20 '16 at 20:31
$begingroup$
you should look at the problem of calculate the det[a.(bxc)] and compare
$endgroup$
– janmarqz
Oct 20 '16 at 20:31
add a comment |
2 Answers
2
active
oldest
votes
$begingroup$
For the Levi-Civita symbols we have that, for two vectors $vec{a}$ and $vec{b}$,
$vec{a}cdotvec{b} = sum_ia_ib_i$
and using Einstein notation convention we can just wright $vec{a}cdotvec{b} = a_ib^i$, or, we can just use that $(vec{a}cdotvec{b} )_i = a_ib_i$. We also have that
$(vec{a}timesvec{b})_i = sum_j sum_k epsilon_{ijk}a_jb_k$
Or just $(vec{a}timesvec{b})_i = epsilon_{ijk}a_jb_k$. So using that you can prove the relation as you did:
$$(vec{a}cdot(vec{b}timesvec{c})) = sum_ia_i(vec{b}timesvec{c})_i = sum_isum_jsum_ka_iepsilon_{ijk}b_jc_k = sum_isum_jsum_kepsilon_{jki}c_ka_ib_j = sum_j(vec{c}timesvec{a})_jb_j = (vec{b}cdot(vec{c}timesvec{a}))$$
Then this is what I think was your doubt.
$endgroup$
add a comment |
$begingroup$
That's almost right, but there are some inconsistencies in your notation.
- In the first step $acdot(btimes c)$, you have a scalar. Nothing wrong here. But note that since you begin with a scalar, you should have scalars in all the next steps.
- In the second step $a_{i}cdot(btimes c)_{i}$ you use a dot ($cdot$) between components. That is illegal. Components are numbers, and you can only use dot product between vectors. Hence, the second step should read just $a_{i}(btimes c)_{i}$
- Since $(btimes c)_{i} = epsilon_{ijk}b_{j}c_{k}$, in step three you should have just $a_{i}epsilon_{ijk}b_{j}c_{k}$, without the vectors $e_{i}$. This resonates with the note in (1), where I remarked you should have just scalars and not vector expressions. Also note that this goes against the summation convention, where it is only valid to sum over pairs of indices.
- The switch of indices and switch of sign is correct. Since, as mentioned in (3), you shouldn't write the vectors $e_i$, your concern about the index $i$ is just out of the question.
Steps 5 and 6 are indeed correct.
So, the correct derivation (with a pair of extra steps) is
$$acdot(btimes c) = a_{i}(btimes c)_{i} = a_{i}epsilon_{ijk}b_{j}c_{k} = -a_{i}epsilon_{jik}b_{j}c_{k} \= -epsilon_{jik}a_{i}c_{k}b_{j} = -(atimes c)_{j}b_{j} = -(atimes c)cdot b = (ctimes a)cdot b$$
$endgroup$
add a comment |
Your Answer
StackExchange.ifUsing("editor", function () {
return StackExchange.using("mathjaxEditing", function () {
StackExchange.MarkdownEditor.creationCallbacks.add(function (editor, postfix) {
StackExchange.mathjaxEditing.prepareWmdForMathJax(editor, postfix, [["$", "$"], ["\\(","\\)"]]);
});
});
}, "mathjax-editing");
StackExchange.ready(function() {
var channelOptions = {
tags: "".split(" "),
id: "69"
};
initTagRenderer("".split(" "), "".split(" "), channelOptions);
StackExchange.using("externalEditor", function() {
// Have to fire editor after snippets, if snippets enabled
if (StackExchange.settings.snippets.snippetsEnabled) {
StackExchange.using("snippets", function() {
createEditor();
});
}
else {
createEditor();
}
});
function createEditor() {
StackExchange.prepareEditor({
heartbeatType: 'answer',
autoActivateHeartbeat: false,
convertImagesToLinks: true,
noModals: true,
showLowRepImageUploadWarning: true,
reputationToPostImages: 10,
bindNavPrevention: true,
postfix: "",
imageUploader: {
brandingHtml: "Powered by u003ca class="icon-imgur-white" href="https://imgur.com/"u003eu003c/au003e",
contentPolicyHtml: "User contributions licensed under u003ca href="https://creativecommons.org/licenses/by-sa/3.0/"u003ecc by-sa 3.0 with attribution requiredu003c/au003e u003ca href="https://stackoverflow.com/legal/content-policy"u003e(content policy)u003c/au003e",
allowUrls: true
},
noCode: true, onDemand: true,
discardSelector: ".discard-answer"
,immediatelyShowMarkdownHelp:true
});
}
});
Sign up or log in
StackExchange.ready(function () {
StackExchange.helpers.onClickDraftSave('#login-link');
});
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Post as a guest
Required, but never shown
StackExchange.ready(
function () {
StackExchange.openid.initPostLogin('.new-post-login', 'https%3a%2f%2fmath.stackexchange.com%2fquestions%2f1977486%2fvector-product-and-dot-product-identity-levi-civita-symbols%23new-answer', 'question_page');
}
);
Post as a guest
Required, but never shown
2 Answers
2
active
oldest
votes
2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
$begingroup$
For the Levi-Civita symbols we have that, for two vectors $vec{a}$ and $vec{b}$,
$vec{a}cdotvec{b} = sum_ia_ib_i$
and using Einstein notation convention we can just wright $vec{a}cdotvec{b} = a_ib^i$, or, we can just use that $(vec{a}cdotvec{b} )_i = a_ib_i$. We also have that
$(vec{a}timesvec{b})_i = sum_j sum_k epsilon_{ijk}a_jb_k$
Or just $(vec{a}timesvec{b})_i = epsilon_{ijk}a_jb_k$. So using that you can prove the relation as you did:
$$(vec{a}cdot(vec{b}timesvec{c})) = sum_ia_i(vec{b}timesvec{c})_i = sum_isum_jsum_ka_iepsilon_{ijk}b_jc_k = sum_isum_jsum_kepsilon_{jki}c_ka_ib_j = sum_j(vec{c}timesvec{a})_jb_j = (vec{b}cdot(vec{c}timesvec{a}))$$
Then this is what I think was your doubt.
$endgroup$
add a comment |
$begingroup$
For the Levi-Civita symbols we have that, for two vectors $vec{a}$ and $vec{b}$,
$vec{a}cdotvec{b} = sum_ia_ib_i$
and using Einstein notation convention we can just wright $vec{a}cdotvec{b} = a_ib^i$, or, we can just use that $(vec{a}cdotvec{b} )_i = a_ib_i$. We also have that
$(vec{a}timesvec{b})_i = sum_j sum_k epsilon_{ijk}a_jb_k$
Or just $(vec{a}timesvec{b})_i = epsilon_{ijk}a_jb_k$. So using that you can prove the relation as you did:
$$(vec{a}cdot(vec{b}timesvec{c})) = sum_ia_i(vec{b}timesvec{c})_i = sum_isum_jsum_ka_iepsilon_{ijk}b_jc_k = sum_isum_jsum_kepsilon_{jki}c_ka_ib_j = sum_j(vec{c}timesvec{a})_jb_j = (vec{b}cdot(vec{c}timesvec{a}))$$
Then this is what I think was your doubt.
$endgroup$
add a comment |
$begingroup$
For the Levi-Civita symbols we have that, for two vectors $vec{a}$ and $vec{b}$,
$vec{a}cdotvec{b} = sum_ia_ib_i$
and using Einstein notation convention we can just wright $vec{a}cdotvec{b} = a_ib^i$, or, we can just use that $(vec{a}cdotvec{b} )_i = a_ib_i$. We also have that
$(vec{a}timesvec{b})_i = sum_j sum_k epsilon_{ijk}a_jb_k$
Or just $(vec{a}timesvec{b})_i = epsilon_{ijk}a_jb_k$. So using that you can prove the relation as you did:
$$(vec{a}cdot(vec{b}timesvec{c})) = sum_ia_i(vec{b}timesvec{c})_i = sum_isum_jsum_ka_iepsilon_{ijk}b_jc_k = sum_isum_jsum_kepsilon_{jki}c_ka_ib_j = sum_j(vec{c}timesvec{a})_jb_j = (vec{b}cdot(vec{c}timesvec{a}))$$
Then this is what I think was your doubt.
$endgroup$
For the Levi-Civita symbols we have that, for two vectors $vec{a}$ and $vec{b}$,
$vec{a}cdotvec{b} = sum_ia_ib_i$
and using Einstein notation convention we can just wright $vec{a}cdotvec{b} = a_ib^i$, or, we can just use that $(vec{a}cdotvec{b} )_i = a_ib_i$. We also have that
$(vec{a}timesvec{b})_i = sum_j sum_k epsilon_{ijk}a_jb_k$
Or just $(vec{a}timesvec{b})_i = epsilon_{ijk}a_jb_k$. So using that you can prove the relation as you did:
$$(vec{a}cdot(vec{b}timesvec{c})) = sum_ia_i(vec{b}timesvec{c})_i = sum_isum_jsum_ka_iepsilon_{ijk}b_jc_k = sum_isum_jsum_kepsilon_{jki}c_ka_ib_j = sum_j(vec{c}timesvec{a})_jb_j = (vec{b}cdot(vec{c}timesvec{a}))$$
Then this is what I think was your doubt.
answered Feb 20 '17 at 2:29
Rafael WagnerRafael Wagner
1,8332923
1,8332923
add a comment |
add a comment |
$begingroup$
That's almost right, but there are some inconsistencies in your notation.
- In the first step $acdot(btimes c)$, you have a scalar. Nothing wrong here. But note that since you begin with a scalar, you should have scalars in all the next steps.
- In the second step $a_{i}cdot(btimes c)_{i}$ you use a dot ($cdot$) between components. That is illegal. Components are numbers, and you can only use dot product between vectors. Hence, the second step should read just $a_{i}(btimes c)_{i}$
- Since $(btimes c)_{i} = epsilon_{ijk}b_{j}c_{k}$, in step three you should have just $a_{i}epsilon_{ijk}b_{j}c_{k}$, without the vectors $e_{i}$. This resonates with the note in (1), where I remarked you should have just scalars and not vector expressions. Also note that this goes against the summation convention, where it is only valid to sum over pairs of indices.
- The switch of indices and switch of sign is correct. Since, as mentioned in (3), you shouldn't write the vectors $e_i$, your concern about the index $i$ is just out of the question.
Steps 5 and 6 are indeed correct.
So, the correct derivation (with a pair of extra steps) is
$$acdot(btimes c) = a_{i}(btimes c)_{i} = a_{i}epsilon_{ijk}b_{j}c_{k} = -a_{i}epsilon_{jik}b_{j}c_{k} \= -epsilon_{jik}a_{i}c_{k}b_{j} = -(atimes c)_{j}b_{j} = -(atimes c)cdot b = (ctimes a)cdot b$$
$endgroup$
add a comment |
$begingroup$
That's almost right, but there are some inconsistencies in your notation.
- In the first step $acdot(btimes c)$, you have a scalar. Nothing wrong here. But note that since you begin with a scalar, you should have scalars in all the next steps.
- In the second step $a_{i}cdot(btimes c)_{i}$ you use a dot ($cdot$) between components. That is illegal. Components are numbers, and you can only use dot product between vectors. Hence, the second step should read just $a_{i}(btimes c)_{i}$
- Since $(btimes c)_{i} = epsilon_{ijk}b_{j}c_{k}$, in step three you should have just $a_{i}epsilon_{ijk}b_{j}c_{k}$, without the vectors $e_{i}$. This resonates with the note in (1), where I remarked you should have just scalars and not vector expressions. Also note that this goes against the summation convention, where it is only valid to sum over pairs of indices.
- The switch of indices and switch of sign is correct. Since, as mentioned in (3), you shouldn't write the vectors $e_i$, your concern about the index $i$ is just out of the question.
Steps 5 and 6 are indeed correct.
So, the correct derivation (with a pair of extra steps) is
$$acdot(btimes c) = a_{i}(btimes c)_{i} = a_{i}epsilon_{ijk}b_{j}c_{k} = -a_{i}epsilon_{jik}b_{j}c_{k} \= -epsilon_{jik}a_{i}c_{k}b_{j} = -(atimes c)_{j}b_{j} = -(atimes c)cdot b = (ctimes a)cdot b$$
$endgroup$
add a comment |
$begingroup$
That's almost right, but there are some inconsistencies in your notation.
- In the first step $acdot(btimes c)$, you have a scalar. Nothing wrong here. But note that since you begin with a scalar, you should have scalars in all the next steps.
- In the second step $a_{i}cdot(btimes c)_{i}$ you use a dot ($cdot$) between components. That is illegal. Components are numbers, and you can only use dot product between vectors. Hence, the second step should read just $a_{i}(btimes c)_{i}$
- Since $(btimes c)_{i} = epsilon_{ijk}b_{j}c_{k}$, in step three you should have just $a_{i}epsilon_{ijk}b_{j}c_{k}$, without the vectors $e_{i}$. This resonates with the note in (1), where I remarked you should have just scalars and not vector expressions. Also note that this goes against the summation convention, where it is only valid to sum over pairs of indices.
- The switch of indices and switch of sign is correct. Since, as mentioned in (3), you shouldn't write the vectors $e_i$, your concern about the index $i$ is just out of the question.
Steps 5 and 6 are indeed correct.
So, the correct derivation (with a pair of extra steps) is
$$acdot(btimes c) = a_{i}(btimes c)_{i} = a_{i}epsilon_{ijk}b_{j}c_{k} = -a_{i}epsilon_{jik}b_{j}c_{k} \= -epsilon_{jik}a_{i}c_{k}b_{j} = -(atimes c)_{j}b_{j} = -(atimes c)cdot b = (ctimes a)cdot b$$
$endgroup$
That's almost right, but there are some inconsistencies in your notation.
- In the first step $acdot(btimes c)$, you have a scalar. Nothing wrong here. But note that since you begin with a scalar, you should have scalars in all the next steps.
- In the second step $a_{i}cdot(btimes c)_{i}$ you use a dot ($cdot$) between components. That is illegal. Components are numbers, and you can only use dot product between vectors. Hence, the second step should read just $a_{i}(btimes c)_{i}$
- Since $(btimes c)_{i} = epsilon_{ijk}b_{j}c_{k}$, in step three you should have just $a_{i}epsilon_{ijk}b_{j}c_{k}$, without the vectors $e_{i}$. This resonates with the note in (1), where I remarked you should have just scalars and not vector expressions. Also note that this goes against the summation convention, where it is only valid to sum over pairs of indices.
- The switch of indices and switch of sign is correct. Since, as mentioned in (3), you shouldn't write the vectors $e_i$, your concern about the index $i$ is just out of the question.
Steps 5 and 6 are indeed correct.
So, the correct derivation (with a pair of extra steps) is
$$acdot(btimes c) = a_{i}(btimes c)_{i} = a_{i}epsilon_{ijk}b_{j}c_{k} = -a_{i}epsilon_{jik}b_{j}c_{k} \= -epsilon_{jik}a_{i}c_{k}b_{j} = -(atimes c)_{j}b_{j} = -(atimes c)cdot b = (ctimes a)cdot b$$
answered Jun 2 '18 at 10:17
Jackozee HakkiuzJackozee Hakkiuz
970417
970417
add a comment |
add a comment |
Thanks for contributing an answer to Mathematics Stack Exchange!
- Please be sure to answer the question. Provide details and share your research!
But avoid …
- Asking for help, clarification, or responding to other answers.
- Making statements based on opinion; back them up with references or personal experience.
Use MathJax to format equations. MathJax reference.
To learn more, see our tips on writing great answers.
Sign up or log in
StackExchange.ready(function () {
StackExchange.helpers.onClickDraftSave('#login-link');
});
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Post as a guest
Required, but never shown
StackExchange.ready(
function () {
StackExchange.openid.initPostLogin('.new-post-login', 'https%3a%2f%2fmath.stackexchange.com%2fquestions%2f1977486%2fvector-product-and-dot-product-identity-levi-civita-symbols%23new-answer', 'question_page');
}
);
Post as a guest
Required, but never shown
Sign up or log in
StackExchange.ready(function () {
StackExchange.helpers.onClickDraftSave('#login-link');
});
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Post as a guest
Required, but never shown
Sign up or log in
StackExchange.ready(function () {
StackExchange.helpers.onClickDraftSave('#login-link');
});
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Post as a guest
Required, but never shown
Sign up or log in
StackExchange.ready(function () {
StackExchange.helpers.onClickDraftSave('#login-link');
});
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Post as a guest
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
$begingroup$
Well one issue I see is too many of the index i, there are three which makes the product ambiguous as which pair are summed over (since summing happens in pairs). You can fix this by omitting the unit vector as this is how the dot product works
$endgroup$
– Triatticus
Oct 20 '16 at 17:13
$begingroup$
Or you can represent the dot product part as a tensor operation through use of the Kronecker Delta, that is $acdot b = a_i b_j delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:16
$begingroup$
Then you can write your product as $a cdot (btimes c) = a_i (b times c)_j delta_{ij} = a_i (epsilon_{jkl}hat{e}_j b_k c_l) delta_{ij}$
$endgroup$
– Triatticus
Oct 20 '16 at 17:22
$begingroup$
you should look at the problem of calculate the det[a.(bxc)] and compare
$endgroup$
– janmarqz
Oct 20 '16 at 20:31