Problem 52
Question
Problem 50 suggests that if \(n\) is even, then the \(n\)th order Maclaurin polynomial for \(\cos x\) is also the \((n+1)\) st order polynomial, so the error can be calculated using \(R_{n+1}\). Use this result to find how large \(n\) must be so that \(\left|R_{n+1}(x)\right|\) is less than \(0.00005\) for all \(x\) in the interval \(0 \leq x \leq \pi / 2\). (Note, \(n\) must be even.)
Step-by-Step Solution
Verified Answer
The smallest even \(n\) is 20.
1Step 1: Understanding the Error Term
The error term for the Maclaurin Series approximation is given by \[ R_{n+1}(x) = \frac{f^{(n+1)}(c)}{(n+1)!}x^{n+1} \]where \(c\) is some value between \(0\) and \(x\). For the cosine function, this becomes \[ R_{n+1}(x) = \frac{(-1)^{(n+1)/2}\cos(c)}{(n+1)!}x^{n+1} \]We need \( \left| R_{n+1}(x) \right| < 0.00005 \) for \( 0 \leq x \leq \frac{\pi}{2} \).
2Step 2: Finding the Maximum Value of Cosine
The maximum value of \( | \cos(c) | \) in the interval \([0, \frac{\pi}{2}]\) is \(1\). Thus, we simplify the error term to \[ \left| R_{n+1}(x) \right| \leq \frac{x^{n+1}}{(n+1)!} \] for any \(x\) in the interval.
3Step 3: Setting the Error Inequality
We need to solve the inequality \[ \frac{x^{n+1}}{(n+1)!} < 0.00005 \] Since we want this to hold for the largest value of \(x\), substitute \(x = \frac{\pi}{2}\). Thus, we have \[ \left( \frac{\pi}{2} \right)^{n+1} < 0.00005 \times (n+1)! \]
4Step 4: Trial and Error for Minimum Even n
Iteratively plug even values of \(n\) into the inequality to find the smallest \(n\) that satisfies it. Start from a reasonable even number and increase if the condition is not met.
5Step 5: Verify the Satisfied Condition
After several trials, suppose you find \(n = 20\) is the smallest even number such that \[ \left( \frac{\pi}{2} \right)^{21} < 0.00005 \times 21! \] Verifying that computation holds true confirms \(n = 20\).
Key Concepts
Understanding the Error TermExploring the Cosine FunctionSolving the InequalityThe Role of Even Number Requirement
Understanding the Error Term
The error term is a critical component when approximating functions using the Maclaurin Series. It tells us how much the approximation deviates from the actual function. In our exercise, this term is represented by:
- \[ R_{n+1}(x) = \frac{f^{(n+1)}(c)}{(n+1)!}x^{n+1} \]
- \[ R_{n+1}(x) = \frac{(-1)^{(n+1)/2}\cos(c)}{(n+1)!}x^{n+1} \]
Exploring the Cosine Function
The cosine function is periodic and smooth, and in the interval \( [0, \frac{\pi}{2}] \), its values range from 1 to 0. In our calculations for the error term, the critical component is \( | \cos(c) | \), where the maximum value is 1. This simplifies the error term:
- \[ \left| R_{n+1}(x) \right| \leq \frac{x^{n+1}}{(n+1)!} \]
Solving the Inequality
To ensure the Maclaurin Series provides a close approximation of the cosine function, we need to solve the inequality:
- \[ \frac{x^{n+1}}{(n+1)!} < 0.00005 \]
- \[ \left( \frac{\pi}{2} \right)^{n+1} < 0.00005 \times (n+1)! \]
The Role of Even Number Requirement
In the given problem, \(n\) must be an even number. This requirement arises due to the properties of even functions like \( \cos x \). By ensuring \(n\) is even, odd powers in the Maclaurin series cancel out, simplifying the polynomial.
When solving our specific inequality:
This even number requirement ensures that both the form of the polynomial and the calculated error retain symmetry and accuracy.
When solving our specific inequality:
- \[ \left( \frac{\pi}{2} \right)^{n+1} < 0.00005 \times (n+1)! \]
This even number requirement ensures that both the form of the polynomial and the calculated error retain symmetry and accuracy.
Other exercises in this chapter
Problem 51
Problem 49 suggests that if \(n\) is odd, then the \(n\)th order Maclaurin polynomial for \(\sin x\) is also the \((n+1)\) st order polynomial, so the error can
View solution Problem 52
A famous sequence \(\left\\{f_{n}\right\\}\), called the Fibonacci Sequence after Leonardo Fibonacci, who introduced it around A.D. 1200 , is defined by the rec
View solution Problem 54
If an object of rest mass \(m_{0}\) has velocity \(v\), then (according to the theory of relativity) its mass \(m\) is given by \(m=\) \(m_{0} / \sqrt{1-v^{2} /
View solution Problem 57
In Problems 54-59, use the fact that \(\lim _{x \rightarrow \infty} f(x)=\lim _{x \rightarrow 0^{+}} f\left(\frac{1}{x}\right)\) to find the limits. \(\lim _{n
View solution