Is Aijxi/xk a Contravariant Tensor of Rank 3?

  • Thread starter peripatein
  • Start date
  • Tags
    Tensors
In summary, the student attempted to solve a problem statement that was incorrect, and then attempted to solve it again using the chain rule and the correct product. The student was not able to solve the problem using the correct product.
  • #1
peripatein
880
0
Hi,

Homework Statement


Given that Aij is a contravariant tensor of rank 2, is the following a contravariant tensor of rank 3: Aijxi/xk?

The Attempt at a Solution


Using the chain rule, I have found xi/xk to be a contravariant tensor of rank 1:
[itex]\bar{x}[/itex]i/[itex]\bar{x}[/itex]k = [itex]\bar{x}[/itex]i/xl * xl/[itex]\bar{x}[/itex]k
Is that correct? Does the above product indeed yield a contravariant tensor of rank 3?
 
Physics news on Phys.org
  • #2
That doesn't look correct. How and why did you use the chain rule?

I think you should just try to determine what ##A^{ij}x_i/x_k## transforms to.
 
  • #3
May this be a better attempt?
Following your advice, I got:
∂[itex]\bar{q}[/itex]i/∂ql * ∂[itex]\bar{q}[/itex]j/∂qp * ∂qt/∂[itex]\bar{q}[/itex]s * ∂[itex]\bar{q}[/itex]a/∂qr
Hence, a composite tensor of rank 4? :S
 
  • #4
I don't understand what you're doing. Why is there no A, no k, and no division in that result? And why is there an i in it?

By the way, are you sure the problem statement is correct? You can tell immediately from the fact that there are only two free indices that it can't be a rank-3 tensor.
 
  • #5
peripatein said:
May this be a better attempt?
Following your advice, I got:
∂[itex]\bar{q}[/itex]i/∂ql * ∂[itex]\bar{q}[/itex]j/∂qp * ∂qt/∂[itex]\bar{q}[/itex]s * ∂[itex]\bar{q}[/itex]a/∂qr
Hence, a composite tensor of rank 4? :S

There was no division as I multiplied by the inverse. May I not do so?
The 'i' stems from the contravariant component of A.
'a' should have been 'k', sorry for that.
Should it have been:
[∂[itex]\bar{q}[/itex]i/∂ql * ∂[itex]\bar{q}[/itex]j/∂qp * ∂qt/∂[itex]\bar{q}[/itex]s * ∂[itex]\bar{q}[/itex]k/∂qr]Alpxtxr)?
 
  • #6
If this is wrong, I am then not really sure how to proceed.
I am not sure how to transform the original expression and was merely trying to infer based on what I have been hitherto taught.
 
  • #7
Since repeated indices are summed over, i is a dummy variable in the original expression. ##A^{ij}x_i/x_k## can also be written as ##A^{mj}x_m/x_k##. This expression may or may not denote the ##{}^j_k## component of a tensor. So it's natural to check what the ##{}^j_k## component is in another coordinate system. That's why I don't expect to find a free ##i## in the final result.

You seem to be handling j and the first i correctly. I don't understand the rest of what you're doing. In particular I don't understand the comment about why there's no division. The transformation of the denominator is going to look something like this:
$$\frac{1}{\bar x_k} =\frac{1}{M_k^px_p}.$$ Here M is the matrix defined by writing the transformation of the basis vectors as ##\bar e_i=M_i^j e_j##. I don't see a way to rewrite this so that there's no division.
 
  • #8
Fredrik said:
Since repeated indices are summed over, i is a dummy variable in the original expression. ##A^{ij}x_i/x_k## can also be written as ##A^{mj}x_m/x_k##. This expression may or may not denote the ##{}^j_k## component of a tensor. So it's natural to check what the ##{}^j_k## component is in another coordinate system. That's why I don't expect to find a free ##i## in the final result.

You seem to be handling j and the first i correctly. I don't understand the rest of what you're doing. In particular I don't understand the comment about why there's no division. The transformation of the denominator is going to look something like this:
$$\frac{1}{\bar x_k} =\frac{1}{M_k^px_p}.$$ Here M is the matrix defined by writing the transformation of the basis vectors as ##\bar e_i=M_i^j e_j##. I don't see a way to rewrite this so that there's no division.

Could I write the division thus:
1/[itex]\bar{x}[/itex]k = 1/(∂qs/∂[itex]\bar{x}[/itex]k)?
 
  • #9
What's q? And what's s? You could write this:
$$\frac{1}{\bar x_k}=\frac{1}{\displaystyle\frac{\partial x^p}{\partial\bar x^k}x_p}.$$ By the way, I think a notation like this makes it easier to do the calculation:
\begin{align}
M^p_k &=\frac{\partial x^p}{\partial\bar x^k}\\
(M^{-1})^p_k & =\frac{\partial\bar x^p}{\partial x^k}
\end{align}
 
  • #10
So I would get:
∂[itex]\bar{q}[/itex]i/∂ql * ∂[itex]\bar{q}[/itex]j/∂qp * Alp*$$\frac{1}{\displaystyle\frac{\partial x^p}{\partial\bar x^k}x_p}.$$
Right?
 
  • #11
You're getting closer, but what happened to the ##x_i## that you had in the original expression? Also, I would recommend to not use the same dummy index for two different summations in the same expression. (There are four p's in that expression).
 
  • #12
My bad :). So I would get:
(∂[itex]\bar{q}[/itex]i/∂ql)(∂[itex]\bar{q}[/itex]j/∂qp)(Alp)(∂qn/∂[itex]\bar{q}[/itex]i)(xn)($$\frac{1}{\frac{\partial x^b}{\partial\bar x^k}x_b}$$)
Right?
 
  • #13
What is q? Shouldn't it be x? If yes, then you're finally getting the result I'm getting. It can be simplified a bit because of the two i's.

I'm going to bed, so I probably won't post again tonight.

Did you see my question in post #4 (my second post)? I doubt that the problem statement is OK, since we don't actually have to do any of these calculations to see that we're not dealing with a tensor of rank 3. All we have to do is to count the number of free indices and see that it's not 3.
 
  • #14
Yes, it should have been x. But why is the use of the q's in the beginning legit (in the transformation of A)? That is, why was I "allowed" to use q's for transforming A itself whereas I could only use x's to transform x? Is it because q's denote the vectors spanning A?
Isn't that a composite tensor of rank 4 then?
 
  • #15
I thought that q was just an alternative notation, i.e. sometimes you denote the coordinate by q and sometimes by x. In that case, you should pick one of the symbols and stick to it. In this case, I assume that ##x_k## denotes the ##k##th coordinate of a point in space. If that's the case, then the problem has already chosen the notation for us: You have to use x.

Since there are only two free indices, this is either a tensor of rank 2 or not a tensor at all. That's why I suspect that you got the problem statement wrong. It's immediately obvious that it can't be a tensor of rank 3. No calculations necessary.

You should try to simplify your result.
 
Last edited:
  • #16
Would you please care to explain why there are only two free indices? In other words, which are the two?
 
  • #17
j and k. See the first sentence in post #7.
 
  • #18
Okay, I understand. BUT -
1) What do l,p,n and b denote (in the transformation)? Are they dummy as well?
2) By what means at this point may it be determined then whether this is at all a tensor?
 
  • #19
peripatein said:
Okay, I understand. BUT -
1) What do l,p,n and b denote (in the transformation)? Are they dummy as well?
Every index that appears twice is summed over, and is therefore a dummy index.

peripatein said:
2) By what means at this point may it be determined then whether this is at all a tensor?
Simplify the expression. Then compare your formula for ##\bar A^{ij}\bar x_i/\bar x_k## with the tensor transformation law for rank-2 tensors. If it looks exactly the same, then we're dealing with a tensor. If it doesn't, then we almost certainly aren't. It's a bit tricky to make absolutely sure. You would have to evaluate your result and the result you get from the tensor transformation law in a specific coordinate system and see if they're the same. It's possible that you have to repeat this procedure with several different coordinate systems. The first coordinate system you try may tell you something like "if this is a tensor, then the 11 component is 0". If you keep trying with other coordinate systems, you may find that this is a tensor only if all the components are 0.
 

1. What is a contravariant tensor of rank 3?

A contravariant tensor of rank 3 is a mathematical object that represents the relationship between three sets of vectors, where the transformation rules for the components of the tensor involve a change in direction of the vectors. It is a type of tensor that is commonly used in physics and engineering to describe the properties of physical systems.

2. How is Aijxi/xk related to a contravariant tensor of rank 3?

Aijxi/xk is a notation used to represent the components of a contravariant tensor of rank 3. The indices i, j, and k correspond to the three sets of vectors that the tensor relates. The notation Aijxi/xk indicates that the component A has an index i that relates to the first set of vectors, an index j that relates to the second set of vectors, and an index k that relates to the third set of vectors.

3. What is the significance of the indices in Aijxi/xk?

The indices in Aijxi/xk represent the direction of the vectors that the tensor relates. For example, the index i could represent the x-direction, the index j the y-direction, and the index k the z-direction. This notation allows us to easily keep track of the direction of the vectors and their relationship to each other.

4. Why is the rank of a tensor important?

The rank of a tensor is important because it tells us the number of sets of vectors that the tensor relates. In the case of a contravariant tensor of rank 3, it relates three sets of vectors. The rank also determines the number of indices needed to represent the components of the tensor, which is important for performing mathematical operations on the tensor.

5. How is a contravariant tensor of rank 3 different from a covariant tensor of rank 3?

A contravariant tensor of rank 3 and a covariant tensor of rank 3 are different in how they transform under coordinate transformations. In a contravariant tensor, the transformation rules involve a change in direction of the vectors, while in a covariant tensor, the transformation rules involve a change in magnitude of the vectors. This distinction is important in physics and engineering, as it determines how the tensors are used to describe physical systems.

Similar threads

  • Calculus and Beyond Homework Help
Replies
2
Views
2K
  • Calculus and Beyond Homework Help
Replies
2
Views
2K
  • Advanced Physics Homework Help
Replies
5
Views
2K
  • Calculus and Beyond Homework Help
Replies
3
Views
2K
  • Calculus and Beyond Homework Help
Replies
1
Views
3K
  • General Math
Replies
1
Views
1K
  • Special and General Relativity
Replies
1
Views
1K
  • Special and General Relativity
Replies
11
Views
1K
  • Calculus and Beyond Homework Help
Replies
1
Views
1K
  • Calculus and Beyond Homework Help
Replies
5
Views
2K
Back
Top