General Relativity - Index Notation

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The discussion focuses on solving a homework problem related to General Relativity using index notation. Participants analyze the matrix element M_{ij}, correcting initial errors in the calculation of the second derivative and the application of the Kronecker delta. They clarify that M_{ij} should incorporate terms that account for both cases where indices are equal and not equal. The conversation emphasizes the importance of using explicit expressions for clarity and ensuring proper indexing in calculations. The final consensus is that x^j is indeed an eigenvector of M_{ij}, and further exploration of the remaining parts is encouraged.
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Homework Statement



(a) Find matrix element ##M_{ij}##
(b) Show that ##x^j## is an eigenvector of ##M_{ij}##
(c) Show any vector orthogonal to ##x^j## is also an eigenvector of ##M_{ij}##
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Homework Equations

The Attempt at a Solution



Part(a)
[/B]
\frac{\partial^2 \Phi}{\partial x^i x^j} = -\frac{2GM_i}{(x^i)^3} \delta_{ij}Part(b)

M_{ij}x_j = \frac{-2GM_i}{(x^i)^2}

How do I show it is an eigenvector? It is clearly not..
 
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Hi. What you obtain in (a) is wrong: the double derivative should give you two terms, the denominator should be a power of r and the index on M is probably a typo...
 
Goddar said:
Hi. What you obtain in (a) is wrong: the double derivative should give you two terms, the denominator should be a power of r and the index on M is probably a typo...
Sorry I don't quite follow..
 
Can you detail your calculation of Mij so maybe i can tell you what goes wrong?
 
Goddar said:
Can you detail your calculation of Mij so maybe i can tell you what goes wrong?

Part(a)
M_{ij} = \frac{\partial^2}{\partial x^j x^i} GM(x^i x^i)^{-\frac{1}{2}} = -GM \frac{\partial}{\partial x^j} x^i (x^i x^i)^{-\frac{3}{2}} = 3GMx^i x^j (x^i x^i)^{-\frac{5}{2}} \delta_{ij}

Part (b)

M_{ij} x^j = 3GMx^i (x^j)^2 (x^i x^i)^{-\frac{5}{2}} \delta_{ij} = 3GM (x^i x^i)^{-2}
 
Ok. First i would recommend you actually expand r in terms of x,y and z instead of using summation convention: it will be less confusing and you'll see what's going on more clearly.
But if you want to use it, you have to pick a different index for your denominator (not i or j)!
Then you will see that in the second derivative you wrongfully assigned a Kronecker delta to 3GMxixj/r5,
while you're forgetting a term for the case where i = j (so that this second term does come with a Kronecker delta!).
If you do all that you'll see how part (b) comes out as expected.
 
Goddar said:
Ok. First i would recommend you actually expand r in terms of x,y and z instead of using summation convention: it will be less confusing and you'll see what's going on more clearly.
But if you want to use it, you have to pick a different index for your denominator (not i or j)!
Then you will see that in the second derivative you wrongfully assigned a Kronecker delta to 3GMxixj/r5,
while you're forgetting a term for the case where i = j (so that this second term does come with a Kronecker delta!).
If you do all that you'll see how part (b) comes out as expected.
Oh I think I got it now. I should have used a dummy index for ##r##.

Part(a)

<br /> M_{ij} = \frac{\partial^2}{\partial x^j x^i} GM(x^l x^l)^{-\frac{1}{2}} = -GM \frac{\partial}{\partial x^j} x^i (x^l x^l)^{-\frac{3}{2}} = -GM \left[ \frac{\partial}{\partial x^i} x^i (x^l x^l)^{-\frac{3}{2}} + \frac{\partial}{\partial x^{j \neq i}} x^i (x^l x^l)^{-\frac{3}{2}} \right]<br />

<br /> M_{ij} = -GM \left[ (x^l x^l)^{-\frac{3}{2}} -3 (x^i)^2 (x^l x^l)^{-\frac{5}{2}} -3 x^i x^j (x^l x^l)^{-\frac{5}{2}} \delta_{ij} \right]<br />

Part (b)

<br /> M_{ij} x^j = GM \left[ x^j (x^l x^l)^{-\frac{3}{2}} -3 x^j (x^i)^2 (x^l x^l)^{-\frac{5}{2}} -3 x^i (x^j)^2 (x^l x^l)^{-\frac{5}{2}} \delta_{ij} \right]<br />

Using the kronecker delta,
<br /> M_{ij} x^j = GM (x^l x^l)^{-\frac{3}{2}} x^j<br />
 
Last edited:
You're getting there but there's still a mistake in your second derivative (again it would probably appear more clearly if you used explicit expressions of x,y,z):
1 - you obtain 3 terms while there should be only two because the xj in the denominator gets a derivative whether or not j = i
2 - the first term you obtain should be the one carrying a Kronecker delta since it is the one corresponding solely to the case where j = i
 
Goddar said:
You're getting there but there's still a mistake in your second derivative (again it would probably appear more clearly if you used explicit expressions of x,y,z):
1 - you obtain 3 terms while there should be only two because the xj in the denominator gets a derivative whether or not j = i
2 - the first term you obtain should be the one carrying a Kronecker delta since it is the one corresponding solely to the case where j = i

You're right, I'm complicating things. Here's what it should be:

Part(a)

<br /> M_{ij} = \frac{\partial^2}{\partial x^j x^i} GM(x^l x^l)^{-\frac{1}{2}} = -GM \frac{\partial}{\partial x^j} x^i (x^l x^l)^{-\frac{3}{2}} = -GM \left[ \delta_{ij}(x^l x^l)^{-\frac{3}{2}} -3 x^j x^i (x^l x^l)^{-\frac{5}{2}}\right]<br />

Part (b)

<br /> M_{ij} x^j = -GM \left[ \delta_{ij} x^j (x^l x^l)^{-\frac{3}{2}} -3 (x^j x^j) x^i (x^l x^l)^{-\frac{5}{2}} \right] = -GM \left[ \delta_{ij} x^j (x^l x^l)^{-\frac{3}{2}} -3 x^i (x^l x^l)^{-\frac{3}{2}} \right] = 2 GM (x^l x^l)^{-\frac{3}{2}} x^j<br />
 
Last edited:
  • #10
Yep. Now you can express again the denominator as r-3, so it's obvious that xj is an eigenvector...
 
  • #11
Goddar said:
Yep. Now you can express again the denominator as r-3, so it's obvious that xj is an eigenvector...
Thanks man! I will try out the remaining parts and update it here
 

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