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For the following alternating series, \(\sum_{n=1}^{\infty} a_{n}=1-\frac{1}{10}+\frac{1}{100}-\frac{1}{1000}+\ldots\) how many terms do you have to go for your approximation (your partial sum) to be within 1e-07 from the convergent value of that series?

Short Answer

Expert verified
7 terms

Step by step solution

01

- Identify the general term of the series

The general term of the series can be written as \(a_n = \frac{(-1)^{n+1}}{10^{n-1}}\).
02

- Apply the Alternating Series Error Estimation Theorem

The theorem states that for an alternating series, the error after \(n\) terms is less than or equal to the absolute value of the \((n+1)\)-th term, \(|a_{n+1}|\). Set this less than 1e-07: \(|a_{n+1}| < 1 \times 10^{-7}\).
03

- Solve for n to find the smallest term that fits the error criterion

From the inequality \(\left| \frac{(-1)^{(n+1)}}{10^n} \right| < 1 \times 10^{-7}\), we get \(\frac{1}{10^n} < 1 \times 10^{-7}\). Solving for \(n\), we take logarithms to get: \(n > \log_{10}(10^7) = 7\).
04

- Conclusion

Since \(n\) must be greater than 7, we need to include at least 7 terms. Therefore, the partial sum of the first 7 terms will be within the required error margin.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Alternating Series
An alternating series is a series in which the signs of the terms alternate between positive and negative. It is typically written in the form \sum_{n=1}^{\infty} (-1)^{n} b_{n}, where \(b_{n}\) is a sequence of positive terms. One well-known example is the alternating harmonic series:\ 1 - \frac{1}{2} + \frac{1}{3} - \frac{1}{4} + \ldots.\ Alternating series are interesting because they often converge even when the similar series with all positive terms would diverge. This makes them useful in approximating functions and values. Moreover, the behavior of alternating series is governed by the Alternating Series Test, ensuring the series converges if the terms \(b_{n}\) are decreasing and approach zero.
Error Approximation
When working with alternating series, we often want to know how close a partial sum is to the full sum of the series. This is called error approximation. The Alternating Series Error Estimation Theorem helps us find this error. For an alternating series, the error after summing the first \(n\) terms is less than or equal to the absolute value of the next term, or \(|a_{n+1}|\). This means that if you stop at the nth term, your error is no more than the size of the (n+1)th term. Understanding error approximation is crucial for practical applications, because it tells us how good our approximation is.
Convergence of Series
The convergence of a series refers to whether the sum of its terms approaches a finite limit as more terms are added. For alternating series, the Alternating Series Test (or Leibniz's criterion) is a simple way to check this. An alternating series \sum_{n=1}^{\infty} (-1)^{n} b_{n} converges if two conditions are met: (1) The magnitude of the terms \(b_{n}\) decreases monotonically (each term is smaller than the one before). (2) The limit of \(b_{n}\) as \(n\) approaches infinity is zero. When these conditions are satisfied, the series is guaranteed to converge, and you can use partial sums to approximate its value accurately.
Logarithmic Inequality
Logarithmic inequality involves using the properties of logarithms to solve inequalities. In the context of this exercise, we need to solve \(\frac{1}{10^n} < 1 \times 10^{-7}\). To solve for \(n\), we can use logarithms. First, rewrite the inequality as \(10^{-n} < 10^{-7}\). Taking the logarithm base 10 of both sides, we obtain: \(-n < -7\) or simply \(n > 7\). This tells us that \(n\) must be greater than 7 for the partial sum to be within the error margin. Thus, logarithmic inequality helps in finding out how many terms are needed to meet a specific accuracy when working with series.

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Most popular questions from this chapter

Determine the sum of the following series. $$ \sum_{n=1}^{\infty}\left(\frac{3^{n}+5^{n}}{9^{n}}\right) $$

Suppose you drop a golf ball onto a hard surface from a height \(h\). The collision with the ground causes the ball to lose energy and so it will not bounce back to its original height. The ball will then fall again to the ground, bounce back up, and continue. Assume that at each bounce the ball rises back to a height \(\frac{3}{4}\) of the height from which it dropped. Let \(h_{n}\) be the height of the ball on the \(n\) th bounce, with \(h_{0}=h .\) In this exercise we will determine the distance traveled by the ball and the time it takes to travel that distance. a. Determine a formula for \(h_{1}\) in terms of \(h\). b. Determine a formula for \(h_{2}\) in terms of \(h\). c. Determine a formula for \(h_{3}\) in terms of \(h\). d. Determine a formula for \(h_{n}\) in terms of \(h\). e. Write an infinite series that represents the total distance traveled by the ball. Then determine the sum of this series. f. Next, let's determine the total amount of time the ball is in the air. i) When the ball is dropped from a height \(H,\) if we assume the only force acting on it is the acceleration due to gravity, then the height of the ball at time \(t\) is given by $$ H-\frac{1}{2} g t^{2} $$ Use this formula to determine the time it takes for the ball to hit the ground after being dropped from height \(H\). ii) Use your work in the preceding item, along with that in (a)-(e) above to determine the total amount of time the ball is in the air.

Conditionally convergent series exhibit interesting and unexpected behavior. In this exercise we examine the conditionally convergent alternating harmonic series \(\sum_{k=1}^{\infty} \frac{(-1)^{k+1}}{k}\) and discover that addition is not commutative for conditionally convergent series. We will also encounter Riemann's Theorem concerning rearrangements of conditionally convergent series. Before we begin, we remind ourselves that $$ \sum_{k=1}^{\infty} \frac{(-1)^{k+1}}{k}=\ln (2) $$ a fact which will be verified in a later section.a. First we make a quick analysis of the positive and negative terms of the alternating harmonic series. i. Show that the series \(\sum_{k=1}^{\infty} \frac{1}{2 k}\) diverges. ii. Show that the series \(\sum_{k=1}^{\infty} \frac{1}{2 k+1}\) diverges. iii. Based on the results of the previous parts of this exercise, what can we say about the sums \(\sum_{k=C}^{\infty} \frac{1}{2 k}\) and \(\sum_{k=C}^{\infty} \frac{1}{2 k+1}\) for any positive integer \(C ?\) Be specific in your explanation. b. Recall addition of real numbers is commutative; that is $$ a+b=b+a $$ for any real numbers \(a\) and \(b\). This property is valid for any sum of finitely many terms, but does this property extend when we add infinitely many terms together? The answer is no, and something even more odd happens. Riemann's Theorem (after the nineteenth-century mathematician Georg Friedrich Bernhard Riemann) states that a conditionally convergent series can be rearranged to converge to any prescribed sum. More specifically, this means that if we choose any real number \(S\), we can rearrange the terms of the alternating harmonic series \(\sum_{k=1}^{\infty} \frac{(-1)^{k+1}}{k}\) so that the sum is \(S\). To understand how Riemann's Theorem works, let's assume for the moment that the number \(S\) we want our rearrangement to converge to is positive. Our job is to find a way to order the sum of terms of the alternating harmonic series to converge to \(S\). i. Explain how we know that, regardless of the value of \(S\), we can find a partial sum \(P_{1}\) $$ P_{1}=\sum_{k=1}^{n_{1}} \frac{1}{2 k+1}=1+\frac{1}{3}+\frac{1}{5}+\cdots+\frac{1}{2 n_{1}+1} $$ of the positive terms of the alternating harmonic series that equals or exceeds \(S\). Let $$ S_{1}=P_{1} $$ii. Explain how we know that, regardless of the value of \(S_{1}\), we can find a partial sum \(N_{1}\) $$ N_{1}=-\sum_{k=1}^{m_{1}} \frac{1}{2 k}=-\frac{1}{2}-\frac{1}{4}-\frac{1}{6}-\cdots-\frac{1}{2 m_{1}} $$ so that $$ S_{2}=S_{1}+N_{1} \leq S $$ iii. Explain how we know that, regardless of the value of \(S_{2}\), we can find a partial sum \(P_{2}\) $$ P_{2}=\sum_{k=n_{1}+1}^{n_{2}} \frac{1}{2 k+1}=\frac{1}{2\left(n_{1}+1\right)+1}+\frac{1}{2\left(n_{1}+2\right)+1}+\cdots+\frac{1}{2 n_{2}+1} $$ of the remaining positive terms of the alternating harmonic series so that $$ S_{3}=S_{2}+P_{2} \geq S $$iv. Explain how we know that, regardless of the value of \(S_{3}\), we can find a partial sum $$ N_{2}=-\sum_{k=m_{1}+1}^{m_{2}} \frac{1}{2 k}=-\frac{1}{2\left(m_{1}+1\right)}-\frac{1}{2\left(m_{1}+2\right)}-\cdots-\frac{1}{2 m_{2}} $$ of the remaining negative terms of the alternating harmonic series so that $$ S_{4}=S_{3}+N_{2} \leq S $$ v. Explain why we can continue this process indefinitely and find a sequence \(\left\\{S_{n}\right\\}\) whose terms are partial sums of a rearrangement of the terms in the alternating harmonic series so that \(\lim _{n \rightarrow \infty} S_{n}=S\).

We can use known Taylor series to obtain other Taylor series, and we explore that idea in this exercise, as a preview of work in the following section. a. Calculate the first four derivatives of \(\sin \left(x^{2}\right)\) and hence find the fourth order Taylor polynomial for \(\sin \left(x^{2}\right)\) centered at \(a=0\) b. Part (a) demonstrates the brute force approach to computing Taylor polynomials and series. Now we find an easier method that utilizes a known Taylor series. Recall that the Taylor series centered at 0 for \(f(x)=\sin (x)\) is $$ \sum_{k=0}^{\infty}(-1)^{k} \frac{x^{2 k+1}}{(2 k+1) !} $$ i. Substitute \(x^{2}\) for \(x\) in the Taylor series \((8.5 .7) .\) Write out the first several terms and compare to your work in part (a). Explain why the substitution in this problem should give the Taylor series for \(\sin \left(x^{2}\right)\) centered at \(0 .\) ii. What should we expect the interval of convergence of the series for \(\sin \left(x^{2}\right)\) to be? Explain in detail.

We can use power series to approximate definite integrals to which known techniques of integration do not apply. We will illustrate this in this exercise with the definite integral \(\int_{0}^{1} \sin \left(x^{2}\right) d s\) a. Use the Taylor series for \(\sin (x)\) to find the Taylor series for \(\sin \left(x^{2}\right) .\) What is the interval of convergence for the Taylor series for \(\sin \left(x^{2}\right) ?\) Explain. b. Integrate the Taylor series for \(\sin \left(x^{2}\right)\) term by term to obtain a power series expansion for \(\int \sin \left(x^{2}\right) d x\) c. Use the result from part (b) to explain how to evaluate \(\int_{0}^{1} \sin \left(x^{2}\right) d x\). Determine the number of terms you will need to approximate \(\int_{0}^{1} \sin \left(x^{2}\right) d x\) to 3 decimal places.

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