Binomial Expansion (Arfken/Weber/Harris 1.3.9)

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Homework Help Overview

The problem involves the relativistic sum of two velocities in the same direction, expressed in terms of a variable α. The task is to find the expression for w/c in powers of α up to the third order, utilizing the binomial expansion.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to substitute and expand the given expression for w/c but expresses confusion regarding the convergence of the series and the form of the final expression.
  • Some participants question the correctness of the denominator used in the expansion and suggest adjusting the expansion point to improve convergence.
  • Others propose a different approach to the expansion, emphasizing the importance of selecting an appropriate variable for convergence.

Discussion Status

Participants have provided feedback on the original poster's approach, suggesting corrections and alternative methods for expansion. There is a productive exchange of ideas regarding the convergence of series and the proper setup for the binomial expansion.

Contextual Notes

There is an emphasis on the constraints of the variable α, particularly its range and implications for the series expansion. Participants note the potential divergence of the series at certain values of α and discuss the implications for the problem's setup.

CJ2116
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Hi everyone,

I'm currently working through Mathematical Methods for Physicists 7th ed. by Arfken/Weber/Harris and there's one question that's been giving me some difficulty. I would appreciate any feedback if possible.

Thanks!

Chris

Homework Statement


The relativistic sum w of two velocities u and v in the same direction is given by
$$\frac{w}{c}= \frac{u/c+v/c}{1+uv/c^2}$$
If
$$\frac{v}{c}=\frac{u}{c}=1-\alpha,$$
where ##0\le\alpha\le 1##, find w/c in powers through terms in ##\alpha^3##

Homework Equations


Binomial Expansion:
$$\left(1+x\right)^m=1+mx+\frac{m(m-1)x^2}{2!}+\frac{m(m-1)(m-2)x^3}{3!}$$

The Attempt at a Solution


This seems like a straightforward substitution and expansion:
$$\frac{w}{c}= \frac{u/c+v/c}{1+uv/c^2}=\frac{(1-\alpha)+(1-\alpha)}{1+(1-\alpha)^2}=2(1-\alpha)\left(1+(1-\alpha)^2\right)^{-1}$$
Now, expanding the last term I'm getting
$$\frac{w}{c}=2(1-\alpha)\left(1-(1-\alpha)^2+\frac{-1(-1-1)(1-\alpha)^4}{2!}+\frac{-1(-1-1)(-1-2)(1-\alpha)^6}{3!}+...\right)$$
$$\Rightarrow \frac{w}{c}=2(1-\alpha)\left(1-(1-\alpha)^2+(1-\alpha)^4-(1-\alpha)^6+...\right)$$

I'm noticing two things with this that make me think I'm doing something stupid. The first is that ##0\le\alpha\le 1## and at ##\alpha=0## this series diverges.

The second is that this is giving an infinite number of polynomials to expand and I'm not seeing how to get something of the form ##1+a_1\alpha+a_2\alpha^2+a_3\alpha^3...##, which is what I assume the problem is asking.

Can anybody see something wrong with my assumptions or calculations?
 
Last edited:
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Why do you have ##1+\alpha## in the denominator and not ##1-\alpha## ?
 
Adjusting for what fresh_42 said:

You seem to be using the expansion for ##1/(1+x)## for ##x = (1-\alpha)^2##, indicating that you are expanding around ##(1-\alpha)^2 = 0##, i.e., ##\alpha = 1##. The radius of convergence for the expansion of ##1/(1+x)## is 1 and so you actually should expect something that does not converge at ##\alpha = 0##. Try expanding around ##\alpha = 0## instead.
 
Sorry, fixed it. That's what I get for copying and pasting a typo!
 
The denominator should be ## 1+(1-\alpha)^2 =2-2 \alpha+\alpha^2=2(1-\alpha+\frac{\alpha^2}{2}) ##. You want to do the expansions with ## x=- \alpha +\frac{\alpha^2}{2} ##. ## \\ ## If you expand ## \frac{1}{1+x} =1-x+x^2-x^3+... ## with ## x>1 ##, the series diverges.## \\ ## (If you use ## x=(1-\alpha)^2 ##, the series is so close to diverging (radius of convergence =1), that it basically will not give any useful result. You can plug in a small value for ## \alpha ##, but the expression for ## \frac{1}{1+x} ## with the ## x=(1-\alpha)^2 ## converges far too slowly=it almost diverges=so that you might need a couple hundred terms to get anything close to the answer. If you choose ## x ## properly, the series converges rapidly for small ## \alpha ##).
 
Last edited:
Excellent, thanks for the responses!

With this I'm now getting:
$$\frac{w}{c}= \frac{2(1-\alpha)}{\left(1+(1-\alpha)^2\right)}=\frac{2(1-\alpha)}{\left(2-2\alpha+\alpha^2\right)}=\frac{(1-\alpha)}{\left(1-\alpha+\alpha^2/2\right)}$$
$$\Rightarrow \frac{w}{c}=(1-\alpha)\left(1-(-\alpha+\alpha^2/2)+(-\alpha+\alpha^2/2)^2-(-\alpha+\alpha^2/2)^3+O(\alpha^4)\right)$$
Ignoring anything above order 4:
$$\frac{w}{c}=(1-\alpha)\left(1+\alpha-\alpha^2/2+\alpha^2-\alpha^3+\alpha^3\right)=(1-\alpha)\left(1+\alpha+\alpha^2/2\right)$$
$$\frac{w}{c}=1+\alpha+\alpha^2/2-\alpha-\alpha^2-\alpha^3/2=1-\alpha^2/2-\alpha^3/2$$

Looks like that did it! Thanks Again!

Chris
 
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