Simple Taylor or Multipole Expansion of Potential

Join the discussion
Registration is free. Ask a follow-up in this thread, or start your own.
1 reply · 5K views
bavaji
Messages
1
Reaction score
0
Hullo,

Somehow, I couldn't get the TeX to come out right.

I have been trying to learn scheme theory (algebraic geometry) and completely forgotten how to do this simple calculus type stuff...

Homework Statement



Let V be a potential of the form

[tex]V = \left(\frac{1}{r} + \left(\frac{1}{\left|\vec{r} - \left(\vec{r_{1}} - vec{r_{2}}\right)\right|} - \left(\frac{1}{\left|\vec{r} + \vec{r_{2}}\right|} - \left(\frac{1}{\left|\vec{r} - \vec{r_{1}}\right|} \right)[\tex]<br /> <br /> where r = [tex]\left|\vec{r}\right|[\tex].<br /> <br /> For large r >> 1 I am supposed to expand in powers of [tex]\frac{\vec{r_{i}}}{r}[\tex] to obtain the expression <br /> [tex]V \sim \frac{1}{r^3}\left(x_{1}x_{2} + y_{1}y_{2} - 2z_{1}z_{2} \right)[\tex] where higher order terms have been neglected. <br /> <br /> <h2>Homework Equations</h2><br /> <br /> <br /> <h2>The Attempt at a Solution</h2><br /> <br /> I tried using the expansion [tex]\left(\frac{1}{\left|\vec{r} + \vec{r'}\right|} = \frac{1}{r} + \frac{\vec{r}\vec{r'}}{r^3}[\tex] + terms of higher order, but somehow end up with V = 0 (up to order [tex]r^-3[\tex]. I have completely forgotten how to do this...<br /> <br /> Would be thankful for any help...<br /> <br /> Greetings from Germany, <br /> <br /> bavaji[/tex][/tex][/tex][/tex][/tex][/tex]
 
Last edited:
Physics news on Phys.org
bavaji said:
Hullo,

Somehow, I couldn't get the TeX to come out right.

While you do use "backslashes" for the special TeX characters, you need to terminate the TeX command with regular "slash" [ / tex ]:

[tex]V = \left(\frac{1}{r} + \left(\frac{1}{\left|\vec{r} - \left(\vec{r_{1}} - vec{r_{2}}\right)\right|} - \left(\frac{1}{\left|\vec{r} + \vec{r_{2}}\right|} - \left(\frac{1}{\left|\vec{r} - \vec{r_{1}}\right|} \right)[/tex]

It looks like the expression may be missing something...
 
Last edited: