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In each exercise, determine the largest positive integer \(r\) such that \(q(h)=O\left(h^{r}\right) .\) [Hint: Determine the first nonvanishing term in the Maclaurin expansion of \(q .\) ] \(q(h)=e^{h}-(1+h)\)

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Answer: 2

Step by step solution

01

Determine the Maclaurin expansion of \(q(h)\)

In order to find the Maclaurin expansion of \(q(h)\), we will first remind the Maclaurin series for \(e^h\), which is given by: $$e^h = \sum_{k=0}^{\infty}\frac{h^k}{k!} = 1 + h + \frac{h^2}{2!} + \frac{h^3}{3!} + \dots$$ Now, subtracting \((1+h)\) from this series, we obtain the Maclaurin series for \(q(h)\): $$q(h) = e^h - (1+h) = \left(1 + h + \frac{h^2}{2!} + \frac{h^3}{3!} + \dots\right) - (1+h)$$
02

Determine the first nonvanishing term in the Maclaurin expansion of \(q(h)\)

By subtracting \((1+h)\) from the Maclaurin series of \(e^h\), we can identify the remaining terms as: $$q(h) = \frac{h^2}{2!} + \frac{h^3}{3!} + \dots$$ Because everything summand in the series of q is positive for h>0, \(\frac{h^2}{2!}\) or \(\frac{1}{2} h^2\) is the first nonvanishing term in the Maclaurin expansion of \(q(h)\).
03

Identify the largest positive integer r

We determined that the first nonvanishing term in the Maclaurin expansion of \(q(h)\) is \(\frac{1}{2}h^2\). This term corresponds to the power \(r=2\). Therefore, the largest positive integer \(r\) such that \(q(h) = O(h^r)\) is \(r=2\).

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Key Concepts

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

Differential Equations
Differential equations are mathematical tools used to describe various phenomena in engineering, physics, biology, and many other fields. The general form of a differential equation represents a relationship between a function and its derivatives. They can be classified into different types based on their characteristics including order, linearity, and boundary conditions.

Understanding Differential Equations


Differential equations can range from simple linear equations to complex nonlinear ones. The solutions of these equations can be functions or sets of functions. Some differential equations can be solved exactly in a closed form, while others are only solvable through numerical methods or series approximations like the Maclaurin series. Ideally, students are expected to be familiar with basic methods of solving various types of differential equations, such as separation of variables and integrating factors, and understand concepts like particular and homogeneous solutions.
Boundary Value Problems
Boundary value problems (BVPs) arise when you are dealing with differential equations that specify conditions (boundary values) not just at a single point, but over some range or at multiple points.

Importance of Boundary Values


Such problems require the solution not only to satisfy the differential equation but to also meet the boundary conditions. BVPs are essential in the study of physical systems where initial conditions may not suffice, such as in the study of steady-state heat distribution or vibrations of a drumhead. Solution techniques vary based on whether the BVP is linear or nonlinear, and whether it is defined on a finite or infinite domain. Numerical methods often come into play when analytical solutions are intractable.
Big-O Notation
Big-O notation is a mathematical notation that describes the limiting behavior of a function when the argument tends towards a particular value or infinity. It is a member of a family of notations invented by Paul Bachmann, Edmund Landau, and others, collectively called Bachmann-Landau or asymptotic notation.

Application in Error Analysis


In the context of Maclaurin series and differential equations, Big-O notation plays a critical role in error analysis, indicating the rate at which the remainder (error term) approaches zero as the series progresses. When we say that a function is within the bound of 'Big-O of something', for example, having error terms of the form \(O(h^r)\), it provides a roof over how the error behaves, allowing one to understand the efficiency and accuracy of approximations in numerical methods. Understanding Big-O notation is crucial for analyzing algorithmic complexity in computer science and error estimation in numerical solutions.

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Most popular questions from this chapter

For the given initial value problem, an exact solution in terms of familiar functions is not available for comparison. If necessary, rewrite the problem as an initial value problem for a first order system. Implement one step of the fourth order Runge-Kutta method (14), using a step size \(h=0.1\), to obtain a numerical approximation of the exact solution at \(t=0.1\). \(y^{\prime \prime \prime}-t y=0, \quad y(0)=1, \quad y^{\prime}(0)=0, \quad y^{\prime \prime}(0)=-1\)

In each exercise, (a) Find the exact solution of the given initial value problem. (b) As in Example 1, use a step size of \(h=0.05\) for the given initial value problem. Compute 20 steps of Euler's method, Heun's method, and the modified Euler's method. Compare the numerical values obtained at \(t=1\) by calculating the error \(\left|y(1)-y_{20}\right|\). \(y^{\prime}+2 y=4, \quad y(0)=3\)

$$ \theta^{\prime \prime}+\sin \theta=0, \quad \theta(0)=0, \quad \theta^{\prime}(0)=2 ; \quad 0 \leq t \leq 20 . $$ This problem models pendulum motion when the pendulum is initially in the vertically downward position with an initial angular velocity of \(2 \mathrm{rad} / \mathrm{s}\). For this conservative system, it was shown in Chapter 6 that \(\left(\theta^{\prime}\right)^{2}-2 \cos \theta=2\). Therefore, the initial conditions have been chosen so that the pendulum will rotate upward in the positive (counterclockwise) direction, slowing down and approaching the vertically upward position as \(t \rightarrow \infty\). The phase-plane solution point is moving on the separatrix; thus, loosely speaking, the exact solution is "moving on a knife's edge." If the initial velocity is slightly less, the pendulum will not reach the upright position but will reach a maximum value less than \(\pi\) and then proceed to swing back and forth. If the initial velocity is slightly greater, the pendulum will pass through the vertically upright position and continue to rotate counterclockwise. What happens if we solve this problem numerically? Plot the numerical solutions for \(\theta(t)\) and \(\theta^{\prime}(t)\). Interpret in simple terms what the numerical solution is saying about the pendulum motion on the time interval considered. Does the numerical solution conserve energy?

In each exercise, (a) Find the exact solution of the given initial value problem. (b) As in Example 1, use a step size of \(h=0.05\) for the given initial value problem. Compute 20 steps of Euler's method, Heun's method, and the modified Euler's method. Compare the numerical values obtained at \(t=1\) by calculating the error \(\left|y(1)-y_{20}\right|\). \(y^{\prime}=-\frac{t}{y}, \quad y(0)=3\)

In each exercise, (a) Solve the initial value problem analytically, using an appropriate solution technique. (b) For the given initial value problem, write the Heun's method algorithm, $$ y_{n+1}=y_{n}+\frac{h}{2}\left[f\left(t_{n}, y_{n}\right)+f\left(t_{n+1}, y_{n}+h f\left(t_{n}, y_{n}\right)\right)\right] . $$ (c) For the given initial value problem, write the modified Euler's method algorithm, $$ y_{n+1}=y_{n}+h f\left(t_{n}+\frac{h}{2}, y_{n}+\frac{h}{2} f\left(t_{n}, y_{n}\right)\right) . $$ (d) Use a step size \(h=0.1\). Compute the first three approximations, \(y_{1}, y_{2}, y_{3}\), using the method in part (b). (e) Use a step size \(h=0.1\). Compute the first three approximations, \(y_{1}, y_{2}, y_{3}\), using the method in part (c). (f) For comparison, calculate and list the exact solution values, \(y\left(t_{1}\right), y\left(t_{2}\right), y\left(t_{3}\right)\). \(y^{\prime}=-y+t, \quad y(0)=0\)

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