/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 11 Calculations of this sort may be... [FREE SOLUTION] | 91Ó°ÊÓ

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Calculations of this sort may be used to evaluate limits that we might otherwise try to find through laborious use of I'Hôpital's Rule. Find the following: (a) \(\lim _{x \rightarrow 0} \frac{e^{x}-1-x-\frac{1}{2} x^{2}}{x-\sin x}=\lim _{x \rightarrow 0} \frac{N(x)}{D(x)}.\) Hint: First find \(P_{3,0, N}(x)\) and \(P_{3,0, D}(x)\) for the numerator and denominator \(N(x)\) and \(D(x)\) (b) \(\lim _{x \rightarrow 0} \frac{\frac{e^{x}}{1+x}-1-\frac{1}{2} x^{2}}{x-\sin x}.\) Hint: For the term \(e^{x} /(1+x),\) first write \(1 /(1+x)=1-x+x^{2}-x^{3}+\cdots\) (c) \(\lim _{x \rightarrow 0}\left(\frac{1}{\sin ^{2} x}-\frac{1}{x^{2}}\right).\) (d) \(\lim _{x \rightarrow 0} \frac{1-\cos \left(x^{2}\right)}{x^{2} \sin ^{2} x}.\) (e) \(\lim _{x \rightarrow 0} \frac{1}{\sin ^{2} x}-\frac{1}{\sin \left(x^{2}\right)}.\) (f) \(\lim _{x \rightarrow 0} \frac{(\sin x)(\arctan x)-x^{2}}{1-\cos \left(x^{2}\right)}.\)

Short Answer

Expert verified
Limits: (a) 1, (b) 0, (c) 1/3, (d) 1/2, (e) 0, (f) -1.

Step by step solution

01

Identify the Problem

The problem is to evaluate the given limits as x approaches 0 using possible approximations and simplifications.
02

Solve Part (a)

Given the limit, \ \ \ \ \( \lim_{x \to 0} \frac{e^x - 1 - x - \frac{1}{2} x^2}{x - \sin x} \), use the Taylor series expansions. \ \ \ \ For the numerator, we have: \ \ \ \ \(e^x = 1 + x + \frac{x^2}{2} + \frac{x^3}{6} + \mathcal{O}(x^4) \ \ 1 + x + \frac{x^2}{2} = 1 + x + \frac{x^2}{2} \ \ N(x) = (\frac{x^3}{6} + \mathcal{O}(x^4))\). \ \ \ \ For the denominator, we use the Taylor series for sine: \ \ \( \sin x = x - \frac{x^3}{6} + \mathcal{O}(x^5) \). \ \ \ \ Thus, \( D(x) = x - \sin x = \frac{x^3}{6} + \mathcal{O}(x^5)\). \ \ \ \ Therefore, the limit becomes: \ \ \( \lim_{x \to 0} \frac{\frac{x^3}{6} + \mathcal{O}(x^4)}{\frac{x^3}{6} + \mathcal{O}(x^5)} = 1\).
03

Solve Part (b)

Given the limit, \ \ \(\lim_{x \to 0} \frac{ \frac{e^x}{1+x} - 1 - \frac{1}{2} x^2 }{ x - \sin x }\). \ \ Rewrite \( \frac{e^x}{1+x} \) using the hint: \( \frac{1}{1+x} = 1 - x + x^2 - x^3 + \cdots \). \ \ Hence, \( \frac{e^x}{1+x} \approx (1 + x + \frac{x^2}{2} + \frac{x^3}{6}) (1 - x + x^2 - x^3) \approx 1 + x + \frac{x^2}{2} - x + \frac{x^2}{2} = 1 + x^2 + \mathcal{O}(x^3) \). \ \ Thus, the numerator simplifies to: \ \ \( N(x) \approx (1 + x^2) - 1 - \frac{x^2}{2} = \frac{x^2}{2} \). \ \ For the denominator, using the previous result, \( D(x) \approx \frac{x^3}{6} \). \ \ Therefore, the limit becomes: \ \ \( \lim_{x \to 0} \frac{ \frac{x^2}{2} }{ \frac{x^3}{6} } = \lim_{x \to 0} \frac{3}{x} = 0 \).
04

Solve Part (c)

Given the limit: \ \ \(\lim_{x \to 0} \left( \frac{1}{\sin^2 x} - \frac{1}{x^2} \right) = \lim_{x \to 0} \frac{x^2 - \sin^2 x}{x^2 \sin^2 x} \). \ \ Use the Taylor series expansion for \( \sin x \approx x - \frac{x^3}{6} + \mathcal{O}(x^5) \): \ \ \( \sin^2 x \approx x^2 - \frac{x^4}{3} + \mathcal{O}(x^6) \). \ \ Therefore, \( x^2 - \sin^2 x \approx x^2 - (x^2 - \frac{x^4}{3}) = \frac{x^4}{3} \). \ \ Hence the limit becomes: \ \ \( \lim_{x \to 0} \frac{ \frac{x^4}{3} }{ x^2 \sin^2 x } = \lim_{x \to 0} \frac{ x^2 }{ 3 \sin^2 x } = \lim_{x \to 0} \frac{x^2}{3 x^2} = \frac{1}{3} \).
05

Solve Part (d)

Given the limit: \ \ \(\lim_{x \to 0} \frac{1 - \cos (x^2)}{x^2 \sin^2 x} \). \ \ Use the Taylor series expansion for \( 1 - \cos y \approx \frac{y^2}{2} \) where \( y = x^2 \). \ \ Thus, \( 1 - \cos (x^2) \approx \frac{(x^2)^2}{2} = \frac{x^4}{2} \). \ \ Therefore, \( \lim_{x \to 0} \frac{ \frac{x^4}{2} }{ x^2 \sin^2 x } = \lim_{x \to 0} \frac{x^2}{2 \sin^2 x} = \lim_{x \to 0} \frac{x^2}{2 x^2} = \frac{1}{2} \).
06

Solve Part (e)

Given the limit: \ \ \(\lim_{x \to 0} \frac{1}{\sin^2 x} - \frac{1}{\sin(x^2)} \). \ \ We use the Taylor series expansions: \ \ \( \sin x \approx x - \frac{x^3}{6} \) and \( \sin (x^2) \approx x^2 - \frac{x^6}{6} \). \ \ Therefore, \( \frac{1}{\sin^2 x} \approx \frac{1}{x^2 (1 - \frac{x^2}{6})^2} \) and \( \frac{1}{\sin (x^2)} \approx \frac{1}{x^2 (1 - \frac{x^2}{6} + \mathcal{O}(x^4))^2} \). \ \ Simplifying these, both terms have \(\frac{1}{x^2}\) and the remaining terms go to 0 as \(x \to 0\). \ \ Hence, the limit is 0.
07

Solve Part (f)

Given the limit: \ \ \(\lim_{x \to 0} \frac{(\sin x)(\arctan x) - x^2}{1 - \cos (x^2)} \). \ \ Use Taylor series expansions: \ \ \(\sin x \approx x - \frac{x^3}{6} \), \(\arctan x \approx x - \frac{x^3}{3} \), and \(1 - \cos (x^2) \approx \frac{x^4}{2} \). \ \ Therefore, the numerator: \ \ \( (\sin x)(\arctan x) - x^2 \approx (x - \frac{x^3}{6})(x - \frac{x^3}{3}) - x^2 \approx x^2 - \frac{x^4}{6} - \frac{x^4}{3} - x^2 = -\frac{x^4}{2} + \mathcal{O}(x^6) \). \ \ Thus, \( \lim_{x \to 0} \frac{-\frac{x^4}{2}}{\frac{x^4}{2}} = -1 \).

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Key Concepts

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

Taylor Series Expansion
Taylor series expansions allow us to approximate complex functions with polynomials, making it easier to work with them analytically. For example, the exponential function can be approximated as: \ \( e^x ≈ 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \dots \).
Similarly, for trigonometric functions like sine and cosine, the expansions are: \ \( \sin x ≈ x - \frac{x^3}{3!} + \frac{x^5}{5!} - \dots \) and \( \cos x ≈ 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \dots \), respectively.
In the given exercise, we used Taylor series to simplify both the numerator and the denominator to evaluate the limit. For instance, we expanded: \ \( e^x - 1 - x - \frac{1/2 x^2} \) and \( x - \sin x \) to approximate these to simpler polynomial expressions.
This approximation helps us directly compute the limit without relying solely on L'Hôpital's Rule which can be more complex and time-consuming.
L'Hôpital's Rule
L'Hôpital's Rule is a powerful tool in calculus for evaluating limits, especially when working with indeterminate forms like \( \frac{0}{0} \) or \( \frac{\infty}{\infty} \). The rule states that if \( \lim_{x \to c} \frac{f(x)}{g(x)} \) leads to an indeterminate form, then: \ \( \lim_{x \to c} \frac{f(x)}{g(x)} = \lim_{x \to c} \frac{f'(x)}{g'(x)} \), provided the limit on the right side exists.
In the given exercise, instead of repeatedly applying L'Hôpital's Rule, we used the Taylor series expansion to simplify our functions. It reduced the problem to evaluating simpler rational expressions.
For instance, part (a)'s limit of \( \lim_{x \to 0} \frac{e^x - 1 - x - \frac{1}{2} x^2}{x - \sin x} \) could potentially involve multiple applications of L'Hôpital's Rule. Instead, by expanding and simplifying, we saw the limit approached 1 almost directly.
Evaluating Limits
Evaluating limits in calculus often involves simplifying complex expressions. Key strategies include:
  • Using algebraic manipulation
  • Applying Taylor series expansions
  • Implementing L'Hôpital's Rule
Limits determine the behavior of functions as they approach specific points. In the exercise, we found the limits as \( x \) approached 0 for various given expressions.
In part (b), we rewrote \( \frac{e^x}{1+x} \) using series expansion of the denominator to evaluate: \ \( \lim_{x \to 0} \frac{ \frac{e^x}{1+x} - 1 - \frac{1}{2} x^2 }{ x - \sin x} \) by simplifying the numerator and existing Taylor series for \( x - \sin x \). This gave us a straightforward method to compute the limit.
Each limit we evaluated in the steps took advantage of these techniques to simplify the expression and avoid more complicated differentiation procedures.
Trigonometric Functions
Trigonometric functions like sine and cosine are common in calculus problems involving limits. They are periodic and have useful Taylor series expansions, which help in simplifying expressions. For instance:
  • \( \sin x \approx x - \frac{x^3}{3!} + \dots \)
  • \( \cos x \approx 1 - \frac{x^2}{2!} + \dots \)
  • \(1 - \,\cos (x^2) \approx \frac{x^4}{2} \)

These expansions simplify the calculations when \( x \) approaches specific values, like 0. For example, in part (c), to find \( \lim_{x \to 0} \left( \frac{1}{\sin^2 x} - \frac{1}{x^2} \right) \), we expanded \( \sin x \) and derived a rational expression which simplified the limit.
Trigonometric limits are fundamental in problems dealing with oscillatory motion or wave behavior in physics and engineering.

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Most popular questions from this chapter

(a) Prove that the Taylor polynomial of \(f(x)=\sin \left(x^{2}\right)\) of degree \(4 n+2\) at 0 $$x^{2}-\frac{x^{6}}{3 !}+\frac{x^{10}}{5 !}-\cdots+(-1)^{n} \frac{x^{4 n+2}}{(2 n+1) !}.$$ Hint: If \(P\) is the Taylor polynomial of degree \(2 n+1\) for \(\sin\) at \(0 .\) then \(\sin x=P(x)+R(x),\) where \(\lim R(x) / x^{2 n+1}=0 .\) What does this imply about \(\lim _{x \rightarrow 0} R\left(x^{2}\right) / x^{4 n+2} ?\) (b) Find \(f^{(k)}(0)\) for all \(k\). (c) In general, if \(f(x)=g\left(x^{m}\right)\), find \(f^{(k)}(0)\) in terms of the derivatives of \(g\) at 0. The ideas in this problem can be extended significantly, in ways that are explored in the next three problems.

Prove that if \(x \leq 0,\) then the remainder term \(R_{n, 0}\) for \(e^{x}\) satisfies $$\left|R_{n, 0}\right| \leq \frac{|x|^{n+1}}{(n+1) !}.$$

Suppose that \(a_{i}\) and \(b_{i}\) are the coefficients in the Taylor polynomials at \(a\) of \(f\) and \(g,\) respectively. In other words, \(a_{i}=f^{(i)}(a) / i !\) and \(b_{i}=g^{(i)}(a) / i ! .\) Find the cocficients \(c_{i}\) of the Taylor polynomials at \(a\) of the following functions, in terms of the \(a_{i}\) 's and \(b_{i}\) 's. (i) \(\quad f+g\). (ii) \(\quad f g\). (iii) \(\quad f^{\prime}\). (iv) \(\quad h(x)=\int_{a}^{x} f(t) d t\). (v) \(\quad k(x)=\int_{0}^{x} f(t) d t\).

Use the Taylor polynomial \(P_{1, a, f},\) together with the remainder, to prove a weak form of Theorem 2 of the Appendix to Chapter 11: If \(f^{\prime \prime}>0,\) then the graph of \(f\) always lies above the tangent line of \(f,\) except at the point of contact.

Consider a function \(f\) which satisfies the differential equation $$f^{(n)}=\sum_{j=0}^{n-1} a_{j} f^{(j)}.$$ for certain numbers \(a_{0}, \ldots, a_{n-1} .\) Several special cases have already received detailed treatment, either in the text or in other problems; in particular, we have found all functions satisfying \(f^{\prime}=f,\) or \(f^{\prime \prime}+f=0,\) or \(f^{\prime \prime}-f=0 .\) The trick in Problem 18-42 enables us to find many solutions for such equations, but doesn't say whether these are the only solutions. This requires a uniqueness result, which will be supplied by this problem. At the end you will find some (necessarily sketchy) remarks about the general solution. (a) Derive the following formula for \(f^{(n+1)}\) (let us agree that " \(^{\prime \prime} a_{-1} "\) will be 0 ): $$f^{(n+1)}=\sum_{j=0}^{n-1}\left(a_{j-1}+a_{n-1} a_{j}\right) f^{(j)}.$$ (b) Deduce a formula for \(f^{(n+2)}\) The formula in part (b) is not going to be used; it was inserted only to convince you that a general formula for \(f^{(n+k)}\) is out of the question. On the other hand, as part (c) shows, it is not very hard to obtain estimates on the size of \(f^{(n+k)}(x)\). (c) Let \(N=\max \left(1,\left|a_{0}\right|, \ldots,\left|a_{n-1}\right|\right)\). Then \(\left|a_{j-1}+a_{n-1} a_{j}\right| \leq 2 N^{2} ;\) this means that $$f^{(n+1)}=\sum_{j=0}^{n-1} b_{j}^{1} f^{(j)}, \quad \text { where }\left|b_{j}^{1}\right| \leq 2 N^{2}.$$ Show that $$f^{(n+2)}=\sum_{j=0}^{n-1} b_{j}^{2} f^{(j)}, \quad \text { where }\left|b_{j}^{2}\right| \leq 4 N^{3},$$ and, more generally, $$f^{(n+k)}=\sum_{j=0}^{n-1} b_{j}^{k} f^{(j)}, \quad \text { where }\left|b_{j}^{k}\right| \leq 2^{k} N^{k+1}.$$ (d) Conclude from part (c) that, for any particular number \(x\), there is a number \(M\) such that $$\left|f^{(n+k)}(x)\right| \leq M \cdot 2^{k} N^{k+1} \quad \text { for all } k.$$ (e) Now suppose that \(f(0)=f^{\prime}(0)=\cdots=f^{(n-1)}(0)=0 .\) Show that $$|f(x)| \leq \frac{M \cdot 2^{k+1} N^{k+2}|x|^{n+k+1}}{(n+k+1) !} \leq \frac{M \cdot|2 N x|^{n+k+1}}{(n+k+1) !},$$ and conclude that \(f=0\). (f) Show that if \(f_{1}\) and \(f_{2}\) are both solutions of the differential equation $$f^{(n)}=\sum_{j=0}^{n-1} a_{j} f^{(j)},$$ and \(f_{1}^{(j)}(0)=f_{2}^{(j)}(0)\) for \(0 \leq j \leq n-1,\) then \(f_{1}=f_{2}\). In other words, the solutions of this differential equation are determined by the "initial conditions" (the values \(f^{(j)}(0)\) for \(0 \leq j \leq n-1\) ). This means that we can find all solutions once we can find enough solutions to obtain any given set of initial conditions. If the equation $$x^{n}-a_{n-1} x^{n-1}-\cdots-a_{0}=0$$ has \(n\) distinct roots \(\alpha_{1}, \ldots, \alpha_{n},\) then any function of the form $$f(x)=c_{1} e^{\alpha_{1} x}+\cdots+c_{n} e^{\alpha_{n} x}$$ is a solution, and $$\begin{aligned} f(0) &=c_{1}+\cdots+c_{n} \\ f^{\prime}(0) &=\alpha_{1} c_{1}+\cdots+\alpha_{n} c_{n} \\ \vdots & \\ f^{(n-1)}(0) &=\alpha_{1}^{n-1} c_{1}+\cdots+\alpha_{n}^{n-1} c_{n}. \end{aligned}$$ As a matter of fact, every solution is of this form, because we can obtain any set of numbers on the left side by choosing the \(c\) 's properly, but we will not try to prove this last assertion. (It is a purely algebraic fact, which you can easily check for \(n=2\) or \(3 .\) ) These remarks are also true if some of the roots are multiple roots, and even in the more general situation considered in Chapter 27.

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