Problem 19
Question
Find the Maclaurin series for the functions. \(\cosh x=\frac{e^{x}+e^{-x}}{2}\)
Step-by-Step Solution
Verified Answer
\( \cosh x = \sum_{n=0}^{\infty} \frac{x^{2n}}{(2n)!} \) is the Maclaurin series for \( \cosh x \).
1Step 1: Recall the Definition of Maclaurin Series
The Maclaurin series is a Taylor series expansion around the point zero. The general formula for the Maclaurin series of a function \( f(x) \) is given by:\[f(x) = f(0) + f'(0)x + \frac{f''(0)x^2}{2!} + \frac{f'''(0)x^3}{3!} + \cdots \]
2Step 2: Determine the Derivatives of \( \cosh x \)
Calculate the successive derivatives of the function \( \cosh x = \frac{e^x + e^{-x}}{2} \). - \( f(x) = \cosh x = \frac{e^x + e^{-x}}{2} \)- \( f'(x) = \sinh x = \frac{e^x - e^{-x}}{2} \)- \( f''(x) = \cosh x = \frac{e^x + e^{-x}}{2} \)- \( f'''(x) = \sinh x = \frac{e^x - e^{-x}}{2} \)Notice the alternating pattern of derivatives.
3Step 3: Evaluate the Derivatives at \( x = 0 \)
Substitute \( x = 0 \) into the derivatives:- \( f(0) = \cosh 0 = 1 \)- \( f'(0) = \sinh 0 = 0 \)- \( f''(0) = \cosh 0 = 1 \)- \( f'''(0) = \sinh 0 = 0 \)This pattern continues for higher derivatives, with even derivatives evaluated at zero yielding 1, and odd derivatives yielding 0.
4Step 4: Construct the Series
Using the values obtained, plug them into the Maclaurin series formula:\[\cosh x = 1 + 0 \cdot x + \frac{1 \cdot x^2}{2!} + 0 \cdot x^3 + \frac{1 \cdot x^4}{4!} + \cdots\]This simplifies to:\[\cosh x = 1 + \frac{x^2}{2!} + \frac{x^4}{4!} + \frac{x^6}{6!} + \cdots\]
5Step 5: Write the General Formula
Recognize the pattern where the non-zero terms occur only at even powers of \( x \):\[\cosh x = \sum_{n=0}^{\infty} \frac{x^{2n}}{(2n)!}\]This is the Maclaurin series for \( \cosh x \).
Key Concepts
Taylor series expansionhyperbolic cosine functionderivativesseries evaluation
Taylor series expansion
The Taylor series is a powerful tool used to express a function as an infinite sum of terms. Each term is derived from the values of the function's derivatives at a single point. A Maclaurin series is a type of Taylor series expansion centered at zero, which makes calculating the series terms easier for many functions. The general formula for a Maclaurin series of a function \( f(x) \) is:
\[ f(x) = f(0) + f'(0)x + \frac{f''(0)x^2}{2!} + \frac{f'''(0)x^3}{3!} + \cdots \]
This formula highlights how each term in the series uses the derivatives evaluated at zero, multiplied by a power of \( x \) and divided by a factorial. Factoring in the derivatives and their corresponding factorial helps ensure the approximation works well, even for complex functions.
\[ f(x) = f(0) + f'(0)x + \frac{f''(0)x^2}{2!} + \frac{f'''(0)x^3}{3!} + \cdots \]
This formula highlights how each term in the series uses the derivatives evaluated at zero, multiplied by a power of \( x \) and divided by a factorial. Factoring in the derivatives and their corresponding factorial helps ensure the approximation works well, even for complex functions.
hyperbolic cosine function
The hyperbolic cosine function, \( \cosh x \), is defined as:
\[ \cosh x = \frac{e^x + e^{-x}}{2} \]
This function is similar in form to the trigonometric cosine function but uses exponential functions with base \( e \) instead. The hyperbolic functions, including \( \cosh x \), have interesting identities and properties that make them useful in various mathematical and physics applications.
\[ \cosh x = \frac{e^x + e^{-x}}{2} \]
This function is similar in form to the trigonometric cosine function but uses exponential functions with base \( e \) instead. The hyperbolic functions, including \( \cosh x \), have interesting identities and properties that make them useful in various mathematical and physics applications.
- Unlike trigonometric functions, hyperbolic functions are defined for all real numbers.
- They have properties akin to the trigonometric functions but differ in their nature and periodicity.
- The graph of \( \cosh x \) shows symmetry about the y-axis, making it an even function.
derivatives
Derivatives play a vital role in constructing the Taylor series for any function. They help us approximate the function around a specific point. For the hyperbolic cosine function, \( \cosh x \), calculating derivatives is made easier due to the repeating nature of its terms:
- \( f(x) = \cosh x = \frac{e^x + e^{-x}}{2} \)
- \( f'(x) = \sinh x = \frac{e^x - e^{-x}}{2} \)
- \( f''(x) = \cosh x = \frac{e^x + e^{-x}}{2} \)
- \( f'''(x) = \sinh x = \frac{e^x - e^{-x}}{2} \)
series evaluation
Evaluating the series involves substituting the derivatives' values into the Maclaurin series formula. For the hyperbolic cosine function, this means recognizing the terms in the formula:
\[ \cosh x = 1 + \frac{x^2}{2!} + \frac{x^4}{4!} + \frac{x^6}{6!} + \cdots \]
These series terms capture the behavior of \( \cosh x \), especially near \( x = 0 \). The even powers reflect the even function nature of \( \cosh x \), leading to the concise format:
\[ \cosh x = \sum_{n=0}^{\infty} \frac{x^{2n}}{(2n)!} \]
This formula not only presents \( \cosh x \) as an infinite sum but also provides a useful approximation tool for practical calculations.
- \( f(0) = \cosh 0 = 1 \)
- \( f'(0) = \sinh 0 = 0 \)
- \( f''(0) = \cosh 0 = 1 \)
- \( f'''(0) = \sinh 0 = 0 \)
\[ \cosh x = 1 + \frac{x^2}{2!} + \frac{x^4}{4!} + \frac{x^6}{6!} + \cdots \]
These series terms capture the behavior of \( \cosh x \), especially near \( x = 0 \). The even powers reflect the even function nature of \( \cosh x \), leading to the concise format:
\[ \cosh x = \sum_{n=0}^{\infty} \frac{x^{2n}}{(2n)!} \]
This formula not only presents \( \cosh x \) as an infinite sum but also provides a useful approximation tool for practical calculations.
Other exercises in this chapter
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