What Are the Mathematical Foundations of the Dipole Approximation?

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center o bass
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Homework Statement


I'm referring to http://hyperphysics.phy-astr.gsu.edu/hbase/electric/dipole.html and the approximation [tex]r_1 - r_2 \approx = d \cos \theta[/tex]. I see that it is correct if I draw it up, but I wondered if there were any "more mathematical" ways to see this?

Where does these kind of approximations come from? Is this just a special case or is it often used? I don't think I've seen this kind before.
 
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center o bass said:

Homework Statement


I'm referring to http://hyperphysics.phy-astr.gsu.edu/hbase/electric/dipole.html and the approximation [tex]r_1 - r_2 \approx = d \cos \theta[/tex]. I see that it is correct if I draw it up, but I wondered if there were any "more mathematical" ways to see this?

Where does these kind of approximations come from? Is this just a special case or is it often used? I don't think I've seen this kind before.

The only approximation you need is that [itex]d \ll r[/itex], i.e. the dipole is very small compared to the distance(s) from its center at which you are interested in measuring the field or potential.

To see how this approximation implies that [itex]|\textbf{r}_{+}-\textbf{r}_{-}|\approx d\cos\theta[/itex], you simply use the standard rules for vector addition/subtraction and calculate the magnitude of [itex]|\textbf{r}_{+}-\textbf{r}_{-}|[/itex], then Taylor expand it for small [itex]\frac{d}{r}[/itex].