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a. Find the nth-order Taylor polynomials for the following functions centered at the given point a, for \(n=0,1,\) and 2 b. Graph the Taylor polynomials and the function. $$f(x)=e^{x}, a=\ln 2$$

Short Answer

Expert verified
Answer: The 0th, 1st, and 2nd order Taylor polynomials for the function \(f(x) = e^x\) centered at \(a = \ln 2\) are as follows: 1. \(P_0(x) = 2\) 2. \(P_1(x) = 2 + 2(x - \ln 2)\) 3. \(P_2(x) = 2 + 2(x - \ln 2) + (x - \ln 2)^2\) When graphed alongside the original function \(f(x) = e^x\), the Taylor polynomials show how well they approximate the function around the point \(a = \ln 2\). With increasing order, the Taylor polynomials more accurately approximate the function in a larger region around the point \(a\).

Step by step solution

01

Calculate derivatives of the function

To calculate up to the second-order derivatives of \(f(x) = e^x\), we will sequentially differentiate the function. 1. \(f(x) = e^x\) 2. \(f'(x) = e^x\) 3. \(f''(x) = e^x\) The derivatives of \(e^x\) are all equal to \(e^x\).
02

Evaluate the derivatives at the point \(a = \ln 2\)

Now, we will evaluate the derivatives at point \(a = \ln 2\). 1. \(f(\ln 2) = e^{\ln 2} = 2\) 2. \(f'(\ln 2) = e^{\ln 2} = 2\) 3. \(f''(\ln 2) = e^{\ln 2} = 2\) Each of these evaluations simplifies to \(2\).
03

Calculate the Taylor polynomials

Now, we will calculate the Taylor polynomials for \(n = 0, 1,\) and \(2\). - For \(n = 0\), the Taylor polynomial is given by: $$P_0(x) = \frac{f^{(0)}(\ln 2)}{0!}(x - \ln 2)^0 = 2$$ - For \(n = 1\), the Taylor polynomial is given by: $$P_1(x) = \frac{f^{(0)}(\ln 2)}{0!}(x - \ln 2)^0 + \frac{f^{(1)}(\ln 2)}{1!}(x - \ln 2)^1 = 2 + 2(x - \ln 2)$$ - For \(n = 2\), the Taylor polynomial is given by: $$P_2(x) = \frac{f^{(0)}(\ln 2)}{0!}(x - \ln 2)^0 + \frac{f^{(1)}(\ln 2)}{1!}(x - \ln 2)^1 + \frac{f^{(2)}(\ln 2)}{2!}(x - \ln 2)^2 = 2 + 2(x - \ln 2) + (x - \ln 2)^2$$
04

Graph the Taylor polynomials and the function

To complete the exercise, graph the Taylor polynomials \(P_0(x), P_1(x),\) and \(P_2(x)\) alongside the original function \(f(x) = e^x\). To do this, use a graphing tool like Desmos, GeoGebra, or any other software of your choice. 1. Graph the function \(f(x) = e^x\). 2. Graph the nth-order Taylor polynomials: a. \(P_0(x) = 2\) b. \(P_1(x) = 2 + 2(x - \ln 2)\) c. \(P_2(x) = 2 + 2(x - \ln 2) + (x - \ln 2)^2\) This will allow you to see the approximation of the original function given by each Taylor polynomial visually.

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Key Concepts

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

Derivatives
Derivatives are fundamental in calculus as they represent the rate at which a function is changing at any given point. They are essential for finding the slope of a tangent to the function's curve at a particular point. In the context of Taylor polynomials, derivatives play a crucial role because they help in approximating functions locally around a point.

When you calculate derivatives for a function like the exponential function, which is given by \(f(x) = e^x\), you will find that all its derivatives are surprisingly the same: \(f'(x) = e^x\), \(f''(x) = e^x\), and so on. This is one of the reasons why exponential functions are so elegant — their behavior is predictable based on their derivatives. For the exercise mentioned, the derivatives of \(e^x\) are evaluated at \(a = \ln 2\), resulting in \(e^{\ln 2} = 2\). By using these derivatives, Taylor polynomials offer a powerful tool to approximate \(f(x) = e^x\) near the point \(a = \ln 2\).
Exponential Functions
Exponential functions are a significant category of functions where the variable appears in the exponent, such as \(f(x) = e^x\). These functions are extremely important in mathematics due to their unique properties and their prevalence in modeling real-world phenomena, such as population growth and radioactive decay.

One of the remarkable characteristics of the exponential function \(e^x\) is that its rate of growth is proportional to its current value, which means no matter how large or small \(x\) is, \(e^x\) continues to grow by the same factor — specifically, the arithmetic constant \(e\), approximate value 2.718. This quality makes it an indispensable function in calculus and beyond.

In Taylor polynomials, exponential functions like \(e^x\) are quite favorable subjects for approximation because their derivatives are straightforward, as each derivative is \(e^x\) again. Therefore, the Taylor series expands into a straightforward series of terms, properly centered around a point such as \(\ln 2\), capturing the behavior of \(e^x\) efficiently.
Graphing Software
Graphing software like Desmos or GeoGebra is crucial for visualizing mathematical functions and their approximations, such as Taylor polynomials. By graphing, students can gain a deeper understanding of how these polynomials approximate a function and where the approximation holds well or begins to diverge.

Using graphing software allows students to visualize the original function \(f(x) = e^x\) along with its Taylor polynomials \(P_0(x)\), \(P_1(x)\), and \(P_2(x)\). This visual perspective can significantly enhance comprehension, as students can observe how the different order polynomials hug the curve of \(e^x\) more closely near the point \(a = \ln 2\).

When using such tools, it helps to:
  • Graph the base function first to understand its general shape.
  • Add each polynomial progressively to observe how each degree improves the approximation.
  • Zoom in around the point of interest to inspect how well the Taylor polynomial fits locally.
These steps help students grasp the power and purpose of Taylor series in approximating complex functions with simpler polynomials.

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Most popular questions from this chapter

Elliptic integrals The period of a pendulum is given by $$ T=4 \sqrt{\frac{\ell}{g}} \int_{0}^{\pi / 2} \frac{d \theta}{\sqrt{1-k^{2} \sin ^{2} \theta}}=4 \sqrt{\frac{\ell}{g}} F(k) $$ where \(\ell\) is the length of the pendulum, \(g \approx 9.8 \mathrm{m} / \mathrm{s}^{2}\) is the acceleration due to gravity, \(k=\sin \left(\theta_{0} / 2\right),\) and \(\theta_{0}\) is the initial angular displacement of the pendulum (in radians). The integral in this formula \(F(k)\) is called an elliptic integral, and it cannot be evaluated analytically. a. Approximate \(F(0.1)\) by expanding the integrand in a Taylor (binomial) series and integrating term by term. b. How many terms of the Taylor series do you suggest using to obtain an approximation to \(F(0.1)\) with an error less than \(10^{-3} ?\) c. Would you expect to use fewer or more terms (than in part (b)) to approximate \(F(0.2)\) to the same accuracy? Explain.

Compute the coefficients for the Taylor series for the following functions about the given point a and then use the first four terms of the series to approximate the given number. $$f(x)=\sqrt{x} \text { with } a=36 ; \text { approximate } \sqrt{39}$$

Summation notation Write the following power series in summation (sigma) notation. $$1-\frac{x}{2}+\frac{x^{2}}{3}-\frac{x^{3}}{4}+\dots$$

Bessel functions arise in the study of wave propagation in circular geometries (for example, waves on a circular drum head). They are conveniently defined as power series. One of an infinite family of Bessel functions is $$ J_{0}(x)=\sum_{k=0}^{\infty} \frac{(-1)^{k}}{2^{2 k}(k !)^{2}} x^{2 k} $$ a. Write out the first four terms of \(J_{0}.\) b. Find the radius and interval of convergence of the power series for \(J_{0}\) c. Differentiate \(J_{0}\) twice and show (by keeping terms through \(x^{6}\) ) that \(J_{0}\) satisfies the equation \(x^{2} y^{\prime \prime}(x)+x y^{\prime}(x)+x^{2} y(x)=0.\)

Use composition of series to find the first three terms of the Maclaurin series for the following functions. a. \(e^{\sin x}\) b. \(e^{\tan x}\) c. \(\sqrt{1+\sin ^{2} x}\)

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