24. Applications of Taylor Series
b. Derivatives
Recall the Taylor series formula: \[\begin{aligned} f\,(x) &=\sum_{n=0}^\infty \dfrac{f\,^{(n)}(a)}{n!}(x-a)^n \\ &=f\,(a)+f'(a)(x-a)+\dfrac{f''(a)}{2}(x-a)^2 \\[2 pt] &\quad+\dfrac{f\,^{(3)}(a)}{3!}(x-a)^3 +\cdots+\dfrac{f\,^{(n)}(a)}{n!}(x-a)^n+\cdots \end{aligned}\] In the chapter on Taylor series, we used this formula to find the power series about \(x=a\) for a given function \(f\,(x)\). However, if you already know the power series for a given function, then you can turn the Taylor series around and use it to compute \(f\,^{(n)}(a)\), the \(n^\text{th}\) derivative of \(f\,(x)\) evaluated at \(x=a\).
If \(f\,(x)=\ln(1-x^2)\), compute
- \(f\,^{(14)}(0)\), the \(14^\text{th}\) derivative of \(f\,(x)\) evaluated at \(x=0\).
- \(f\,^{(15)}(0)\), the \(15^\text{th}\) derivative of \(f\,(x)\) evaluated at \(x=0\).
Since we want derivatives evaluated at \(x=0\), we need a Taylor series for \(\ln(1-x^2)\) centered at \(x=0\). We substitute \(x\to-x^2\) into the known series \[ \ln(1+x)=\sum_{n=1}^\infty \dfrac{(-1)^{n-1}}{n}x^n =x-\dfrac{1}{2}x^2+\dfrac{1}{3}x^3-\dfrac{1}{4}x^4+\cdots \] to get \[\begin{aligned} \ln(1-x^2) &=\sum_{n=1}^\infty \dfrac{(-1)^{n-1}}{n}(-x^2)^n \\ &=(-x^2)-\dfrac{1}{2}(-x^2)^2 +\dfrac{1}{3}(-x^2)^3-\dfrac{1}{4}(-x^2)^4+\cdots \end{aligned}\] and simplify to get the specific series: \[ \ln(1-x^2)=\sum_{n=1}^\infty \dfrac{-1}{n}x^{2n}=-x^2-\dfrac{1}{2}x^4-\dfrac{1}{3}x^6-\dfrac{1}{4}x^8+\cdots \] We now compare this with the general Maclaurin series (Taylor series centered at \(x=0\)): \[\begin{aligned} f\,(x) &=\sum_{n=0}^\infty \dfrac{f\,^{(n)}(0)}{n!}x^n \\ &=f\,(0)+f'(0)x+\dfrac{f''(0)}{2}x^2 +\dfrac{f\,^{(3)}(0)}{3!}x^3+\cdots+\dfrac{f\,^{(n)}(0)}{n!}x^n+\cdots \end{aligned}\] Caution: Notice that \(n\) has a different meaning in the two series. In the specific series, the power of \(x\) is \(2n\). In the general series, the power of \(x\) is just \(n\).
- To find \(f\,^{(14)}(0)\), we note that in the general series the coefficient of \(x^{14}\) is \(\dfrac{f\,^{(14)}(0)}{14!}\). In the specific series for \(\ln(1-x^2)\), the term with an \(x^{14}\) has \(n=7\) and its coefficient is \(-\dfrac{1}{7}\). We equate these terms and solve for \(f\,^{(14)}(0)\): \[ \dfrac{f\,^{(14)}(0)}{14!}x^{14}=-\dfrac{1}{7}x^{14} \qquad \Longrightarrow \] \[ f\,^{(14)}(0)=-\dfrac{14!}{7}=-2\cdot13! \]
- To find \(f\,^{(15)}(0)\), we note that in the general series the coefficient of \(x^{15}\) is \(\dfrac{f\,^{(15)}(0)}{15!}\). In the specific series for \(\ln(1-x^2)\), there are no odd powers of \(x\). So the coefficient \(x^{15}\) is \(0\). We equate these terms and solve for \(f\,^{(15)}(0)\): \[ \dfrac{f\,^{(15)}(0)}{15!}x^{15}=0 \qquad \Longrightarrow \qquad f\,^{(15)}(0)=0 \]
Notice that computing the \(14^\text{th}\) derivative of \(\ln(1-x^2)\) directly would be a long, tedious process.
If \(g(x)=\sin(x^2)\), compute
- \(g^{(16)}(0)\), the \(16^\text{th}\) derivative of \(g(x)\) evaluated at \(x=0\).
- \(g^{(18)}(0)\), the \(18^\text{th}\) derivative of \(g(x)\) evaluated at \(x=0\).
Remember \[ \sin(x)=\sum_{n=0}^\infty \dfrac{(-1)^n}{(2n+1)!}x^{2n+1} =x-\dfrac{x^3}{3!}+\dfrac{x^5}{5!}-\cdots \]
\(g^{(16)}(0)=0\) \(g^{(18)}(0)=\dfrac{18!}{9!}\)
To find the specific series for \(\sin(x^2)\) we substitute \(x\to x^2\) into the series \[ \sin(x)=\sum_{n=0}^\infty \dfrac{(-1)^n}{(2n+1)!}x^{2n+1} =x-\dfrac{x^3}{3!}+\dfrac{x^5}{5!}-\cdots \] to get \[ \sin(x^2)=\sum_{n=0}^\infty \dfrac{(-1)^n}{(2n+1)!}x^{4n+2} =x^2-\dfrac{x^6}{3!}+\dfrac{x^{10}}{5!}-\cdots \] We compare this to the general Maclaurin series: \[\begin{aligned} g(x) &=\sum_{n=0}^\infty \dfrac{g^{(n)}(0)}{n!}x^n \\ &=g(0)+g'(0)x+\dfrac{g''(0)}{2}x^2 \\ &\quad+\dfrac{g^{(3)}(0)}{3!}x^3+\cdots+\dfrac{g^{(n)}(0)}{n!}x^n+\cdots \end{aligned}\]
- To find \(g^{(16)}(0)\), we note that in the general series the coefficient of \(x^{16}\) is \(\dfrac{g^{(16)}(0)}{16!}\). In the specific series for \(\sin(x^2)\), the power of \(x\) is \(4n+2\). When is this \(16\)? Never! So the coefficient of \(x^{16}\) is \(0\) and \(g^{(16)}(0)=0\).
- To find \(g^{(18)}(0)\), we note that in the general series the coefficient of \(x^{18}\) is \(\dfrac{g^{(18)}(0)}{18!}\). In the specific series for \(\sin(x^2)\), the power of \(x\) is \(4n+2\). When is this \(18\)? When \(n=4\). We equate these terms and solve for \(g^{(18)}(0)\): \[ \dfrac{g^{(18)}(0)}{18!}x^{18}=\dfrac{(-1)^4}{9!}x^{18} \] \[ \Longrightarrow \qquad g^{(18)}(0)=\dfrac{18!}{9!} \]
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