How is a binomial expansion done?

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Discussion Overview

The discussion revolves around the process of binomial expansion, particularly in the context of multipole expansion in electromagnetism. Participants explore how to apply binomial expansion to approximate expressions involving powers and fractional exponents, with a focus on its relevance to a specific problem encountered in Griffiths' E&M textbook.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Homework-related

Main Points Raised

  • One participant seeks a high-level overview of binomial expansion, expressing confusion about its application in a specific context related to multipole expansion.
  • Another participant provides the general form of binomial expansion, noting its validity for non-integer exponents, and applies it to the participant's problem by substituting specific values.
  • A third participant mentions that binomial expansion is a special case of Taylor expansion, suggesting a connection between the two concepts.
  • One participant references Isaac Newton's contributions to the topic, indicating a historical perspective on binomial expansion.
  • A later reply indicates that the original poster found clarity after consulting their math professor and acknowledges the importance of Taylor Series in physics, while also expressing a need to memorize relevant expansions.

Areas of Agreement / Disagreement

Participants generally agree on the validity of binomial expansion and its connection to Taylor Series, but there is no consensus on the original poster's understanding or comfort level with the material. The discussion reflects a mix of clarification and exploration rather than a definitive resolution of the original query.

Contextual Notes

Some participants reference mathematical concepts that may depend on prior knowledge of calculus, particularly Taylor Series and binomial coefficients, which could limit understanding for those less familiar with these topics.

Who May Find This Useful

This discussion may be useful for students studying electromagnetism, particularly those preparing for exams that involve mathematical techniques like binomial and Taylor expansions.

CrosisBH
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TL;DR
Can someone give me a basic high level overview on how to do a binomial expansion?
Summary: Can someone give me a basic high level overview on how to do a binomial expansion?

I'm studying for my E&M test and going over multipole expansion. I'm particularly confused about these lines (Griffiths E&M 4th Edition)

š“‡^2_{\pm} = r^2 \left(1\mp \frac{d}{r} \cos\theta + \frac{d^2}{4r^2}\right)

We're interested in the rƩgime r>>d, so the third term in negligible, and the binomial expansion yields

\frac{1}{š“‡^2_{\pm}} \cong \frac{1}{r} \left( 1 \mp \frac{d}{r}\cos\theta\right)^{-1/2}\cong \frac{1}{r}\left(1\pm\frac{d}{2r}\cos\theta\right)

Thus

\frac{1}{š“‡^2_{+}} - \frac{1}{š“‡^2_{-}} \cong \frac{d}{r^2}\cos\theta

I understand how the first line was derived, and I understand the first half on the second line, but I don't understand how the approximation was made in the second half. It's called a binomial expansion apparently, but all my research seems to point toward expanding an integer power binomial

(a+b)^2 = a^2 + 2ab + b^2

And anything about a generalized form is written with binomial coefficients which I can't seem to wrap my head around, and right now it seems beyond my math level to understand it formally. Could someone give me a physics level rigor on how this expansion is done? This'll probably be on my next exam and I want to understand it.
 
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The general binomial expansion is:

##(1 + x)^n = 1 + nx + \frac {n(n - 1)} { 2! } x^2 + ...##

It's still valid if n = -1/2

and so in your case ## x = \frac d { 2r } cos \theta##

and so you get ##\frac 1 {r_{-}^2} = \frac 1 r (1 - \frac d { 2r } cos \theta) ##

and ##\frac 1 {r_{+}^2} =\frac 1 r (1 + \frac d { 2r } cos \theta)##

and hence you get

## \frac 1 {r_{+}^2} - \frac 1 {r_{-}^2} = \frac 1 r (1 + \frac d { 2r } cos \theta) - \frac 1 r (1 - \frac d { 2r } cos \theta) = \frac d { r^2 } cos \theta##

Does that make sense ?

https://socratic.org/questions/how-do-you-use-the-binomial-series-to-expand-1-x-1-2
 
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It is also a special case of the Taylor expansion, expand ##(1+x)^c## around x=0.
 
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That makes perfect sense. After I posted this, I consulted my current Math Professor (Diff eq and Linear Algebra) and he explained it was an infinite series but he forgot the exact equation but I should be able to find it. Then I come here and jedishrfu posted the equation I needed and went through the math, and mfb explained it was derived from the Taylor Series. I honestly haven't touched a Taylor Series since Calc 2 a year ago and I forgot they were a thing. My professor would probably give a very similar problem to this one and I should just memorize.
(1+x)^{-1/2} \cong 1-\frac{1}{2}x

I've heard that Taylor Series expansions are so common in physics so I should just start getting used to them. Thank you everyone!
 
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