Problem 9
Question
Find the Maclaurin series for \(f(x)\) using the definition of a Maclaurin series. [Assume that \(f\) has a power series expansion. Do not show that \(R_{n}(x) \rightarrow 0 . ]\) Also find the associated radius of convergence. $$f(x)=\sinh x$$
Step-by-Step Solution
Verified Answer
The Maclaurin series for \(\sinh x\) is \(\sum_{n=0}^{\infty} \frac{x^{2n+1}}{(2n+1)!}\) with an infinite radius of convergence.
1Step 1: Understanding Maclaurin Series
A Maclaurin series is a Taylor series expansion of a function about 0. It is given by the formula: \\[ f(x) = \sum_{n=0}^{\infty} \frac{f^{(n)}(0)}{n!} x^n \] \where \(f^{(n)}(0)\) is the \(n\)-th derivative of \(f(x)\) evaluated at \(x=0\).
2Step 2: Calculate Derivatives of \( \sinh x \)
The hyperbolic sine function is defined as \( \sinh x = \frac{e^x - e^{-x}}{2} \). We need to calculate the derivatives at \( x = 0 \).\1. \( f(x) = \sinh x \). So, \( f(0) = \sinh(0) = 0 \).2. \( f'(x) = \cosh x \), calculate \( f'(0) = \cosh(0) = 1 \).3. \( f''(x) = \sinh x \), calculate \( f''(0) = \sinh(0) = 0 \).4. \( f'''(x) = \cosh x \), calculate \( f'''(0) = \cosh(0) = 1 \).5. Continue alternating derivatives for pattern.
3Step 3: Construct Maclaurin Series
Substituting the derivatives into the Maclaurin series formula:\[f(x) = \sum_{n=0}^{\infty} \frac{f^{(n)}(0)}{n!} x^n = 0 + \frac{1}{1!} x + 0 \frac{x^2}{2!} + \frac{1}{3!}x^3 + 0 \frac{x^4}{4!} + \frac{1}{5!}x^5 + \cdots\]This simplifies to \\[\sinh x = \sum_{n=0}^{\infty} \frac{x^{2n+1}}{(2n+1)!}\]
4Step 4: Radius of Convergence
The radius of convergence \( R \) of a power series can be found using the ratio test. In this series, every term is \(\frac{x^{2n+1}}{(2n+1)!}\). Applying the ratio test, we find:\[\lim_{n \to \infty} \left| \frac{x^{2n+3}}{(2n+3)!} \cdot \frac{(2n+1)!}{x^{2n+1}} \right| = \lim_{n \to \infty} \frac{x^2}{(2n+2)(2n+3)} = 0\]For any finite \(x\), this approaches 0 as \(n \to \infty\), thus the series converges for all \(x\). Consequently, the radius of convergence is \( R = \infty \).
Key Concepts
Taylor seriesHyperbolic functionsRadius of convergence
Taylor series
The Taylor series is a powerful way to express a wide variety of functions as an infinite sum of terms, calculated from the values of their derivatives at a particular point. This allows us to approximate complex functions with polynomials, making them easier to work with under various conditions.The general formula for the Taylor series of a function \( f(x) \) about a point \( a \) is:
- \( f(x) = \sum_{n=0}^{\infty} \frac{f^{(n)}(a)}{n!} (x-a)^n \)
- \( f(x) = \sum_{n=0}^{\infty} \frac{f^{(n)}(0)}{n!} x^n \)
Hyperbolic functions
Hyperbolic functions are analogs of the trigonometric functions, but they are based on hyperbolas rather than circles. The most common hyperbolic functions are the hyperbolic sine (\( \sinh \)) and cosine (\(\cosh\)).The hyperbolic sine function, \( \sinh x \), is defined as:
- \( \sinh x = \frac{e^x - e^{-x}}{2} \)
Radius of convergence
The radius of convergence of a power series is the distance from the center of the series where the series converges, or sums to a finite value. It is vital in determining the domain of valid inputs for which the series provides an accurate representation of the function.The radius of convergence is commonly determined through the ratio test or the root test, both of which are methods to determine the convergence behavior of series terms as the number of terms approach infinity.For the Maclaurin series of \( \sinh x \), the power series we derived has the form:
- \( \sum_{n=0}^{\infty} \frac{x^{2n+1}}{(2n+1)!} \)
Other exercises in this chapter
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