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Eq. 15.22 in IPMB; the ugliest equation. |
Russ Hobbie and I write
Equation 15.22 is a rather nasty equation to evaluate, particularly at low energies, because many of the terms nearly cancel.Examining the behavior of the expression in brackets at small x should be easy: just take its Taylor’s series (to review Taylor’s series, see Appendix D of IPMB). In order to get the correct answer, however, you need to keep not two terms in the expansion, or three, but four! The Taylor’s series you need are
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Three Taylor's series needed to analyze Eq. 15.22. |
Oddly, the expansion for the fourth term 4x2/3(1+2x)3 doesn’t even need one term in its expansion; it is small and doesn’t contribute to the limiting behavior. Plug these all in, and you find that the terms in x−2, x−1, and x0 all vanish. The first nonzero term is linear: 4x/3.
Out of curiosity, I evaluated each of the five terms in the expression using x = 0.01. I got
20001.9608 - 0.9900 + 9900.0192 - 0.0001 - 29900.9771 = 0.0128
The terms really do “nearly cancel.”
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