Calculus (3rd Edition)

Published by W. H. Freeman
ISBN 10: 1464125260
ISBN 13: 978-1-46412-526-3

Chapter 11 - Infinite Series - 11.7 Taylor Series - Exercises - Page 588: 47

Answer

(a) Five terms are needed. (b) Using a computer algebra system, we get: ${F_4}\left( 1 \right) \approx 0.747487$, ${\ \ \ \ \ }$ $F\left( 1 \right) \approx 0.7468244$ Hence, it is verified that $\left| {F\left( 1 \right) - {F_4}\left( 1 \right)} \right| \approx 0.00066264 \lt 0.001$.

Work Step by Step

From Table 2: ${{\rm{e}}^x} = \mathop \sum \limits_{n = 0}^\infty \dfrac{{{x^n}}}{{n!}} = 1 + x + \dfrac{{{x^2}}}{{2!}} + \dfrac{{{x^3}}}{{3!}} + \dfrac{{{x^4}}}{{4!}} + \cdot\cdot\cdot$, ${\ \ \ }$ converges for all $x$. Substituting $ - {t^2}$ for $x$ in the series above gives ${{\rm{e}}^{ - {t^2}}} = \mathop \sum \limits_{n = 0}^\infty \dfrac{{{{\left( { - {t^2}} \right)}^n}}}{{n!}} = \mathop \sum \limits_{n = 0}^\infty \dfrac{{{{\left( { - 1} \right)}^n}{t^{2n}}}}{{n!}} = 1 - {t^2} + \dfrac{{{t^4}}}{{2!}} - \dfrac{{{t^6}}}{{3!}} + \dfrac{{{t^8}}}{{4!}} + \cdot\cdot\cdot$, converges for all $t$. Next, we express the function $F\left( x \right) = \mathop \smallint \limits_0^x {{\rm{e}}^{ - {t^2}}}{\rm{d}}t$ using the series above: $F\left( x \right) = \mathop \smallint \limits_0^x {{\rm{e}}^{ - {t^2}}}{\rm{d}}t = \mathop \sum \limits_{n = 0}^\infty \mathop \smallint \limits_0^x \dfrac{{{{\left( { - 1} \right)}^n}{t^{2n}}}}{{n!}}{\rm{d}}t$ $ = \mathop \sum \limits_{n = 0}^\infty \left[ {\dfrac{{{{\left( { - 1} \right)}^n}{t^{2n + 1}}}}{{\left( {2n + 1} \right)n!}}} \right]_0^x = \mathop \sum \limits_{n = 0}^\infty \dfrac{{{{\left( { - 1} \right)}^n}{x^{2n + 1}}}}{{\left( {2n + 1} \right)n!}}$ Thus, $F\left( x \right) = \mathop \smallint \limits_0^x {{\rm{e}}^{ - {t^2}}}{\rm{d}}t = \mathop \sum \limits_{n = 0}^\infty \dfrac{{{{\left( { - 1} \right)}^n}{x^{2n + 1}}}}{{\left( {2n + 1} \right)n!}}$. (a) For $x=1$, we have $F\left( 1 \right) = \mathop \sum \limits_{n = 0}^\infty \dfrac{{{{\left( { - 1} \right)}^n}}}{{\left( {2n + 1} \right)n!}}$, where the positive terms are ${b_n} = \dfrac{1}{{\left( {2n + 1} \right)n!}}$. By Eq. (2) in Section 11.4: $\left| {F\left( 1 \right) - {F_n}\left( 1 \right)} \right| \lt {b_{n + 1}}$ We choose $n$ so that $\left| {F\left( 1 \right) - {F_n}\left( 1 \right)} \right| \lt {b_{n + 1}} \lt {10^{ - 3}}$ $\dfrac{1}{{\left( {2n + 3} \right)\left( {n + 1} \right)!}} \lt {10^{ - 3}}$ $\left( {2n + 3} \right)\left( {n + 1} \right)! \gt {10^3}$ We evaluate and list some values for $n$ in the following table: $\begin{array}{*{20}{c}} n&{}&{\left( {2n + 3} \right)\left( {n + 1} \right)!}\\ 2&{}&{42}\\ 3&{}&{216}\\ 4&{}&{1320}\\ 5&{}&{9360} \end{array}$ Using the results in the table above, we choose $N=4$ such that the approximation of the integral for $x=1$ is within an error of at most $0.001$. (b) Using a computer algebra system, we compute: ${F_4}\left( 1 \right) \approx 0.747487$, ${\ \ \ \ \ }$ $F\left( 1 \right) \approx 0.7468244$ Hence, it is verified that $\left| {F\left( 1 \right) - {F_4}\left( 1 \right)} \right| \approx 0.00066264 \lt 0.001$.
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