Summation Convention – Substitution Rule

Click For Summary
SUMMARY

The forum discussion centers on the proof of the substitution rule for the Kronecker delta, specifically the equation δij δjk = δik. Participants clarify that when substituting indices, only the dummy index 'j' should be replaced with numerical values, while 'i' and 'k' remain unchanged. The discussion emphasizes the relationship between the Kronecker delta and the identity matrix, illustrating that the equation holds true through matrix multiplication principles. Ultimately, the proof is established by recognizing that the Kronecker delta effectively evaluates expressions at specific indices.

PREREQUISITES
  • Understanding of Cartesian Tensors
  • Familiarity with the Kronecker delta notation
  • Knowledge of matrix multiplication
  • Proficiency in the Einstein summation convention
NEXT STEPS
  • Study the properties of the Kronecker delta in linear algebra
  • Learn about the Einstein summation convention and its applications
  • Explore matrix multiplication and its implications in tensor calculus
  • Investigate Cartesian tensors and their role in computational fluid dynamics (CFD)
USEFUL FOR

PhD students in mathematics or engineering, researchers in computational fluid dynamics, and anyone interested in advanced tensor analysis and its applications in physics and engineering.

FluidStu
Messages
25
Reaction score
3
Hello. I'm new to this forum. I'm starting a PhD – it's going to be a big long journey through the jungle that is CFD. I would like to arm myself with some tools before entering. The machete is Cartesian Tensors.

I know the rules regarding free suffix's and dummy suffixes, but I'm having trouble proving the substitution rule:
δi j δj k = δi k

Assuming a range of 3 for each component, I will choose that the free suffix's have the following values: i=3, k=1. Therefore, using the implicit summation rule for the dummy index:
δi j δj k = δ3 1 δ1 1 + δ3 2 δ2 1 + δ3 3 δ3 1 = ?

Is my expansion correct?

Many thanks.
 
Last edited by a moderator:
Physics news on Phys.org
FluidStu said:
I know the rules regarding free suffix's and dummy suffixes, but I'm having trouble proving the substitution rule:
δi j δj k = δi k
You can visualize this equation by remembering that kronecker delta symbol actually represents the matrix elements of an identity matrix.
 
FluidStu said:
Hello. I'm new to this forum. I'm starting a PhD – it's going to be a big long journey through the jungle that is CFD. I would like to arm myself with some tools before entering. The machete is Cartesian Tensors.

I know the rules regarding free suffix's and dummy suffixes, but I'm having trouble proving the substitution rule:
δi j δj k = δi k

Assuming a range of 3 for each component, I will choose that the free suffix's have the following values: i=3, k=1. Therefore, using the implicit summation rule for the dummy index:
δi j δj k = δ3 1 δ1 1 + δ3 2 δ2 1 + δ3 3 δ3 1 = ?

Is my expansion correct?
No, It is not because, since "i" and "k" are NOT repeated your result should have "i" and "k" in it, only "j" is replaced by numbers:
δijδjk= δi1δ1k+ δi2δ2k+ δi3δ3k

FluidStu said:
Many thanks.
 
HallsofIvy said:
No, It is not because, since "i" and "k" are NOT repeated your result should have "i" and "k" in it, only "j" is replaced by numbers:
δijδjk= δi1δ1k+ δi2δ2k+ δi3δ3k
Ok, that makes sense (since the index which appears once simultaneously represents all the possible values of that index).

However, from your expansion, I do not understand how one could end up with δik. This was really the point in my question – I would like to see step-wise how δijδjk = δik.
 
FluidStu said:
However, from your expansion, I do not understand how one could end up with δik. This was really the point in my question – I would like to see step-wise how δijδjk = δik.
What do you get when multiplying an identity matrix with another identity matrix?
 
blue_leaf77 said:
What do you get when multiplying an identity matrix with another identity matrix?
I * I = I
 
Now, imagine you have a 3x3 matrices ##A##, ##B##, and ##C## such that ##AB=C##. How do you write the element ##c_{ik}## of ##C## in terms of the elements of ##A## and ##B##?
 
blue_leaf77 said:
Now, imagine you have a 3x3 matrices ##A##, ##B##, and ##C## such that ##AB=C##. How do you write the element ##c_{ik}## of ##C## in terms of the elements of ##A## and ##B##?
cik = aiibik + aijbjk + aikbkk
 
FluidStu said:
cik = aiibik + aijbjk + aikbkk
Almost, just that the index to be summed must be written as numbers, not as indices as you did there.
 
  • #10
blue_leaf77 said:
Almost, just that the index to be summed must be written as numbers, not as indices as you did there.
Do you mean:

cik = a11b13 + a12b23 + a13b33 ?
 
  • #11
FluidStu said:
Do you mean:

cik = a11b13 + a12b23 + a13b33 ?
No. The left most and right most indices in each term in right hand side should be equal to the indices in the left hand side, which is ##ik##. Only the two two middle indices changes due to the summation.
Having fixed this, you should be able to see how that equation becomes of when ##A=B=C=I##.
 
  • #12
FluidStu said:
Ok, that makes sense (since the index which appears once simultaneously represents all the possible values of that index).

However, from your expansion, I do not understand how one could end up with δik. This was really the point in my question – I would like to see step-wise how δijδjk = δik.
I presume this is the "Kronecker delta"- \delta_{ii}= 1, \delta_{ij}= 0 if i\ne j.
Then \delta_{ij}\delta_{jk}= \delta_{i1}\delta_{1k}+ \delta_{i2}\delta_{2j}+ \delta_{i3}\delta_{3j}
If i= 1, k= 1, then only the first term is non-zero and it is 1: \delta_{11}= 1+ 0+ 0= 1[/quote].<br /> If i= 1, k= 2, then at least one of the factors in every term is 0: \delta_{12}= 0+ 0+ 0= 0[/quote].&lt;br /&gt; If i= 1, k= 3, then at least one of the factors in every term is 0: \delta_{13}= 0+ 0+ 0= 0.&amp;lt;br /&amp;gt; &amp;lt;br /&amp;gt; If i= 2, k= 2, then only the second term is non-zero and it is 1: \delta_{22}= 0+ 1+ 0= 1.&amp;amp;lt;br /&amp;amp;gt; etc.
 
  • Like
Likes FluidStu
  • #13
blue_leaf77 said:
No. The left most and right most indices in each term in right hand side should be equal to the indices in the left hand side, which is ##ik##. Only the two two middle indices changes due to the summation.
Having fixed this, you should be able to see how that equation becomes of when ##A=B=C=I##.

Ok, so then cik = ai1b1k + ai2b2k + ai3b3k?

In this way I can see that A=B=C=I. However, I still don't see how this leads to the proof that δijδjk= δik. If you want to expand on this for others visiting the thread, feel free. However, I can see it clearly from this:

HallsofIvy said:
Then δijδjk=δi1δ1k+δi2δ2j+δi3δ3jδijδjk=δi1δ1k+δi2δ2j+δi3δ3j\delta_{ij}\delta_{jk}= \delta_{i1}\delta_{1k}+ \delta_{i2}\delta_{2j}+ \delta_{i3}\delta_{3j}

In all the cases where i = k, we end up with 1, while in all the cases where i ≠ k, we end up with 0. In other words, we end up with δik. Very good, thank you both for your help.
 
  • #14
FluidStu said:
However, I still don't see how this leads to the proof that δijδjk= δik.
That the Kronecker delta is defined as ##\delta_{ik}=1## for ##i=k## and zero for ##i\neq k##, doesn't it remind you of the elements of the identity matrix?
 
  • #15
blue_leaf77 said:
That the Kronecker delta is defined as ##\delta_{ik}=1## for ##i=k## and zero for ##i\neq k##, doesn't it remind you of the elements of the identity matrix?

Yes, it does. I can see that the Kronecker Delta in matrix form is simply an identity matrix. But how does this help me to prove:
FluidStu said:
δijδjk= δik
?
 
  • #16
$$\delta_{ij}\delta_{jk} = \delta_{i1}\delta_{1k} + \delta_{i2}\delta_{2k} + \delta_{i3}\delta_{3k} = \delta_{ik}$$
Now you already have
FluidStu said:
cik = ai1b1k + ai2b2k + ai3b3k
for the matrix equation ##AB=C##. If A=B=C=I, you will only need to replace ##a##, ##b##, and ##c## with ##\delta## in that quoted equation.
 
  • Like
Likes FluidStu
  • #17
blue_leaf77 said:
$$\delta_{ij}\delta_{jk} = \delta_{i1}\delta_{1k} + \delta_{i2}\delta_{2k} + \delta_{i3}\delta_{3k} = \delta_{ik}$$
Now you already have

for the matrix equation ##AB=C##. If A=B=C=I, you will only need to replace ##a##, ##b##, and ##c## with ##\delta## in that quoted equation.
I see that replacing each with δ gives the required proof. But is it "ok" to replace a, b and c with δ? Aren't a, b and c simply elements of matrices? How can we just replace them with δ?
 
  • #18
At the risk of repetition: To put the essential point in one place:

Let A = (aij), B = (bij), and C = (cij) be n-dimensional matrices such that

AB = C.​

Then you know from the definition of matrix multiplication that

cij = Σ aik bkj

for any i, j in the range 1 ≤ i, j ≤ n, where the sum is over k = 1,...,n.

Specializing to the case of n = 3, for the case of A = B = C = I3 (the 3D identity matrix), and then using the repeated-index summation convention, you get

δik δkj = δij

for any i, j in the range 1 ≤ i, j ≤ 3.
 
  • Like
Likes FluidStu
  • #19
FluidStu said:
But is it "ok" to replace a, b and c with δ? Aren't a, b and c simply elements of matrices? How can we just replace them with δ?
Note that the last sentence in post #16 is a conditional statement, look what the condition is in order for the conclusion to be true.
 
  • #20
Here's an alternative proof (for which I'll abandon the summation convention):

##\Sigma_{j} \delta_{ij} \delta_{jk} = \delta_{ii} \delta_{ik} = \delta_{ik} \ \ ## (as ##\delta_{ij} = 0 \ (i \ne j)##)

Or, more laboriously:

##\Sigma_{j} \delta_{ij} \delta_{jk} = \delta_{ii} \delta_{ik} + \Sigma_{j \ne i} \delta_{ij} \delta_{jk} = \delta_{ik} + 0 \ \ ## (as ##\delta_{ii} = 1, \ \delta_{ij} = 0 \ (i \ne j)##)
 
  • Like
Likes FluidStu
  • #21
Try to get an intuitive feeling for what the Kronecker-Delta \delta_{ij} does.
Consider this sum:
\sum_{j=1}^{n} c_j = c_1 + c_2 + \dots + c_n

Now observe what happens if we multiply with the Kronecker-Delta:
\sum_{j=1}^{n} \delta_{ij} c_j = \delta_{i1} c_1 + \delta_{i2}c_2 + \dots + \delta_{ii}c_i + \dots + \delta_{in}c_n

There will be exactly one summand with j=i, that is \delta_{ii} c_i = 1 \cdot c_i = c_i.
For the remaining summands with j \neq i we have \delta_{ij} c_j = 0 \cdot c_j = 0
(by the definition of the Kronecker-Delta).

We get:
\sum_{j=1}^{n} \delta_{ij} c_j
= \delta_{i1} c_1 + \delta_{i2}c_2 + \dots + \delta_{ii}c_i + \dots + \delta_{in}c_n
= 0 \cdot c_1 + 0 \cdot c_2 + \dots + 1 \cdot c_i + \dots + 0 \cdot c_n
= c_i

With the Einstein summation convention we have \delta_{ij} c_j = c_i.
Intuitively, \delta_{ij} evaluates the expression c_j at j=i.

Now, similarly, \delta_{ij} \delta_{jk} = \delta_{ik} since
intuitively \delta_{ij} evaluates the expression \delta_{jk} at j=i.
 
  • Like
Likes FluidStu
  • #22
blue_leaf77 said:
Note that the last sentence in post #16 is a conditional statement, look what the condition is in order for the conclusion to be true.
The condition being that A=B=C=I≡ δij? Then we may replace the a, b and c with δ and the following two are equivalent:

FluidStu said:
cik = ai1b1k + ai2b2k + ai3b3k
blue_leaf77 said:
δijδjk=δi1δ1k+δi2δ2k+δi3δ3k=δik

Having this then makes it easy to see how both post #12 and #21 explain the required proof. Thanks.
 

Similar threads

  • · Replies 7 ·
Replies
7
Views
2K
Replies
5
Views
2K
Replies
3
Views
2K
Replies
27
Views
17K
Replies
12
Views
38K
Replies
40
Views
7K
Replies
6
Views
4K
  • · Replies 7 ·
Replies
7
Views
10K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K