Taylor Expansion for rational function

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Homework Help Overview

The discussion revolves around finding the Taylor expansion of a rational function, specifically the expression for \( \frac{1}{r_{+}} \) in the limit where \( r \) is much greater than \( d \). The original poster is attempting to derive the first-order expansion in terms of \( \epsilon = \frac{d}{r} \).

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • The original poster attempts to apply the first-order Taylor expansion to the given function but questions their approach after receiving a different answer from the instructor. They explore the implications of neglecting higher-order terms and seek clarification on the application of the relevant equation.

Discussion Status

Participants have provided feedback on the original poster's reasoning, suggesting that neglecting higher-order terms is appropriate in this context. There is acknowledgment of the importance of considering the first-order approximation and the implications of the problem's constraints.

Contextual Notes

Participants note that the problem specifies a first-order expansion, which implies that terms involving squares or higher powers of \( \epsilon \) should be disregarded. There is also mention of the physical context related to electric dipoles and the significance of distance in the formulation.

KEØM
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Homework Statement


Find the taylor expansion of the following formula in the case where [tex]r > > d[/tex] to the first order in [tex]\epsilon = \frac{d}{r}[/tex]

[tex]\frac{1}{r_{+}} = \frac{1}{\sqrt{r^{2} + (\frac{d}{2})^{2} - rdcos\theta}}[/tex]



Homework Equations



[tex](1 + \epsilon)^{m} = 1+m\epsilon[/tex], where [tex]\epsilon << 1[/tex] (First order Taylor expansion)


The Attempt at a Solution


[tex]\frac{1}{r_{+}} = \frac{1}{\sqrt{r^{2}(1 + \frac{d^{2}}{4r^{2}} - \frac{d}{r}cos\theta)}}<br /> <br /> =\frac{1}{r \sqrt{1 + \frac{\epsilon^{2}}{4} - \epsilon cos\theta}}<br /> <br /> =\frac{1}{r} \left( 1 + \frac{\epsilon^{2}}{4} - \epsilon cos\theta \right)^{\frac{-1}{2}}<br /> = \frac{1}{r} \left(1 + \left(\frac{-1}{2} \right) \frac{\epsilon^{2}}{4} + \frac{1}{2}\epsilon cos\theta \right)<br /> <br /> = \frac{1}{r} \left(1 - \frac{1}{8} \left( \frac{d}{r}\right)^{2} + \frac{d}{2r} cos\theta \right)[/tex]

but the answer my instructor gives is

[tex]\frac{1}{r_{+}} = \frac{1}{r} \left( 1 + \frac{d}{2r}cos\theta \right)[/tex]

Can someone please point out where I made a mistake? Can I just assume that [tex]\left(\frac{d}{r} \right)^{2}[/tex] must be extremely close to zero because it is being squared? I also am somewhat confused on how to apply the relevant equation for an expression that has more that just 1 and epsilon being raised to the m.




Thanks in advance,

KEØM
 
Last edited:
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yes you may neglect the term you mentioned for r>>d. it's contribution will be small. shouldn't write strictly equal but approximately. note this is part of the formulation of an electric dipole. higher order moments become less significant at far distances more significant at short distances (with respect to the charge configuration).
 
For this particular problem, it is not just that "r>> d". The important point is that the problem said "to first order". That means dropping squares and higher powers.
 
Thank you both for replying. That really helps!

KEØM
 

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