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Mathematical Methods for Physicists: A concise introduction - Site Map

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TAYLOR'S EXPANSION<br />

where f 0 …† means that f …x† has been di€erentiated and then we have put x ˆ ;<br />

and by f 00 …† we mean that we have found f 00 …x† and then put x ˆ , and so on.<br />

Substituting these into (A1.8) we obtain<br />

f …x† ˆf …†‡f 0 …†…x †‡ 1 2! f 00 …†…x † 2 ‡‡ 1 n! f …n† …†…x † n ‡:<br />

…A1:9†<br />

This is the Taylor series <strong>for</strong> f …x† about x ˆ . The Maclaurin series <strong>for</strong> f …x† is the<br />

Taylor series about the origin. Putting ˆ 0 in (A1.9), we obtain the Maclaurin<br />

series <strong>for</strong> f …x†:<br />

f …x† ˆf …0†‡f 0 …0†x ‡ 1 2! f 00 …0†x 2 ‡ 1 3! f F…0†x3 ‡‡ 1 n! f …n† …0†x n ‡:<br />

…A1:10†<br />

Example A1.15<br />

Find the Maclaurin series expansion of the exponential function e x .<br />

Solution: Here f …x† ˆe x . Di€erentiating, we have f …n† …0† ˆ1 <strong>for</strong> all<br />

n; n ˆ 1; 2; 3 .... Then, by Eq. (A1.10), we have<br />

e x ˆ 1 ‡ x ‡ 1 2! x2 ‡ 1 3! x3 ‡ ˆX1 x n<br />

; 1< x < 1:<br />

n!<br />

The following series are frequently employed in practice:<br />

…1† sin x ˆ x x3<br />

3! ‡ x5<br />

5! x7<br />

x 2n1<br />

7! ‡…1†n1 ‡;<br />

…2n 1†!<br />

1< x < 1:<br />

…2† cos x ˆ 1 x2<br />

2! ‡ x4<br />

4! x6<br />

x 2n2<br />

6! ‡…1†n1 ‡;<br />

…2n 2†!<br />

1 < x < 1:<br />

…3† e x ˆ 1 ‡ x ‡ x2<br />

2! ‡ x3 xn1<br />

‡‡ ‡; 1 < x < 1:<br />

3! …n 1†!<br />

…4† lnj…1 ‡ xj ˆx x2<br />

2 ‡ x3<br />

3 x4<br />

x n<br />

4 ‡…1†n1 ‡;<br />

n<br />

1 < x 1:<br />

…5† 1 2 ln 1 ‡ x<br />

1 x 3 ‡ x5<br />

5 ‡ x7 x2n1<br />

‡‡ ‡;<br />

7 2n 1<br />

1 < x < 1:<br />

…6† tan 1 x ˆ x x3<br />

3 ‡ x5<br />

5 x7<br />

x 2n1<br />

7 ‡…1†n1 ‡; 1 x 1:<br />

2n 1<br />

…7† …1 ‡ x† p ˆ 1 ‡ px ‡<br />

nˆ0<br />

p…p 1†<br />

x 2 ‡‡<br />

2!<br />

525<br />

p…p 1†…p n ‡ 1†<br />

x n ‡:<br />

n!

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