/*! 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 20 Define \(y=u(x) e^{x}\) so $$y... [FREE SOLUTION] | 91Ó°ÊÓ

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Define \(y=u(x) e^{x}\) so $$y^{\prime}=u e^{x}+u^{\prime} e^{x}, \quad y^{\prime \prime}=u^{\prime \prime} e^{x}+2 u^{\prime} e^{x}+u e^{x}$$ and $$y^{\prime \prime}-4 y^{\prime}+3 y=e^{x} u^{\prime \prime}-e^{x} u^{\prime}=x$$ If \(w=u^{\prime}\) we obtain the linear first-order equation \(w^{\prime}-2 w=x e^{-x}\) which has the integrating factor \(e^{-\int 2 d x}=\) \(e^{-2 x} .\) Now $$\frac{d}{d x}\left[e^{-2 x} w\right]=x e^{-3 x} \quad \text { gives } \quad e^{-2 x} w=-\frac{1}{3} x e^{-3 x}-\frac{1}{9} e^{-3 x}+c_{1}$$ Therefore \(w=u^{\prime}=-\frac{1}{3} x e^{-x}-\frac{1}{9} e^{-x}+c_{1} e^{2 x}\) and \(u=\frac{1}{3} x e^{-x}+\frac{4}{9} e^{-x}+c_{2} e^{2 x}+c_{3} .\) The general solution is $$y=u e^{x}=\frac{1}{3} x+\frac{4}{9}+c_{2} e^{3 x}+c_{3} e^{x}$$

Short Answer

Expert verified
The general solution is \( y = \frac{1}{3}x + \frac{4}{9} + c_2 e^{3x} + c_3 e^x \).

Step by step solution

01

Understanding the Problem

We are given a function in the form of a product: \( y = u(x) e^x \). We also know the derivatives \( y' \) and \( y'' \). Our task is to find the general solution \( y \) that satisfies a differential equation.
02

Set Up the Differential Equation

The differential equation provided is: \( y'' - 4y' + 3y = e^x u'' - e^x u' = x \). This can be translated into solving for \( w = u' \).
03

Transform and Simplify Equation

Introduce \( w = u' \). Transforming the equation, we get \( w' - 2w = xe^{-x} \). This is a linear first-order differential equation.
04

Find Integrating Factor

Calculate the integrating factor for the equation \( w' - 2w = xe^{-x} \). The integrating factor is \( e^{-2x} \).
05

Solve Using Integrating Factor

Using the integrating factor, derive \( \frac{d}{dx}[e^{-2x} w] = xe^{-3x} \). Integrate both sides to find: \( e^{-2x}w = -\frac{1}{3} xe^{-3x} - \frac{1}{9} e^{-3x} + c_1 \).
06

Solve for \( w \)

Multiply through by \( e^{2x} \) to isolate \( w \), resulting in \( w = u' = -\frac{1}{3} xe^{-x} - \frac{1}{9} e^{-x} + c_1 e^{2x} \).
07

Integrate to Find \( u \)

Integrate \( u' \) to find \( u \): \( u = \frac{1}{3} xe^{-x} + \frac{4}{9} e^{-x} + c_2 e^{2x} + c_3 \).
08

Find General Solution for \( y \)

Substitute \( u \) back into the expression for \( y = u e^x \), giving \( y = \frac{1}{3} x + \frac{4}{9} + c_2 e^{3x} + c_3 e^x \). This is the general solution.

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Key Concepts

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

Integrating Factor
The integrating factor is a crucial tool when solving linear first-order differential equations, allowing us to transform the equation into a more easily solvable form.
Understanding when and how to use it requires recognizing that you're dealing with a linear first-order differential equation, typically of the form:
\[ y' + p(x)y = q(x) \]
where \(p(x)\) and \(q(x)\) are functions of \(x\).
The integrating factor, \( \mu(x) \), is given by the exponential of the integral of \(p(x)\):
  • \( \mu(x) = e^{\int p(x)\, dx} \)
After determining this factor, you multiply through the entire differential equation, transforming it into:
  • \( \frac{d}{dx}[\mu(x) y] = \mu(x) q(x) \)
This simplification allows us to integrate both sides with respect to \(x\), ultimately solving for \(y\).
In the original exercise, the integrating factor is \(e^{-2x}\), helping to isolate and solve for \(w = u'\).
Understanding how to choose and apply an integrating factor is essential for tackling these types of equations.
Linear First-Order Differential Equations
Linear first-order differential equations are the simplest form of differential equations, involving no powers or products of the unknown function and its derivative.
These equations have the general form:
  • \( y' + p(x)y = q(x) \)
where \(y'\) represents the derivative of \(y\) with respect to \(x\), \(p(x)\) and \(q(x)\) are given functions of \(x\).
These equations describe various processes, like growth and decay, and are fundamental to understanding more complex differential systems.
The main objective is to solve for \(y\), using techniques such as identifying an integrating factor.By transforming the equation with the integrating factor, it becomes straightforward to derive the solution by integrating the transformed expression.
In the given exercise, the differential equation \( w' - 2w = xe^{-x} \) is a linear first-order differential equation, recognizable by its structure and the presence of the derivative \( w' \).
Solving this equation requires identifying and working with the integrating factor as a critical step.
General Solution
The general solution of a differential equation encompasses all possible solutions, accounting for arbitrary constants.
These constants arise from integration during the solving process, providing a family of solutions rather than a single unique one.
In the context of linear differential equations, once the solution form is identified, integrating offers the general solution containing constants that fit various initial conditions.
The aim is to express the solution in terms of known functions, such as exponential or polynomial forms.
For the exercise at hand, we obtain a general solution:
  • \( y = \frac{1}{3} x + \frac{4}{9} + c_2 e^{3x} + c_3 e^{x} \)
This expression not only solves the equation but continues to satisfy initial values set by specific conditions.
Understanding how to determine the general solution allows for adapting to a variety of real-world scenarios depicted by the equation.
Derivatives and Integration
Differentiation and integration are fundamental operations in calculus, each serving distinct purposes in analyzing functions.
The derivative measures how a function changes concerning its variable, reflecting rates of change or slopes of tangents.
Integration, on the other hand, is the inverse process of differentiation. It sums up infinitesimal changes over an interval, useful for finding areas under curves or accumulated quantities.
When solving differential equations, we frequently alternate between using derivatives to set up the problem and integrals to solve it.
Each step in the solution often involves integrating or differentiating to simplify expressions and find solutions.
In this exercise, we differentiate to transform the equation, and integrate to solve it, like in the step:
  • \( \frac{d}{dx}[e^{-2x} w] = xe^{-3x} \)
Mastering these processes is essential for effectively tackling a wide array of mathematical problems.

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Most popular questions from this chapter

The auxiliary equation $$m(m-1)(m-2)-m(m-1)-2 m+6=m^{3}-4 m^{2}+m+6=0$$ has roots \(m_{1}=-1, m_{2}=2,\) and \(m_{3}=3,\) so \(y_{c}=c_{1} x^{-1}+c_{2} x^{2}+c_{3} x^{3} .\) With \(y_{1}=x^{-1}, y_{2}=x^{2}, y_{3}=x^{3},\) and the identification \(f(x)=1 / x,\) we get from (10) of Section 4.6 in the text $$W_{1}=x^{3}, \quad W_{2}=-4, \quad W_{3}=3 / x, \quad \text { and } \quad W=12 x.$$ Then \(u_{1}^{\prime}=W_{1} / W=x^{2} / 12, u_{2}^{\prime}=W_{2} / W=-1 / 3 x, u_{3}^{\prime}=1 / 4 x^{2},\) and integration gives $$u_{1}=\frac{x^{3}}{36}, \quad u_{2}=-\frac{1}{3} \ln x, \quad \text { and } \quad u_{3}=-\frac{1}{4 x},$$ so $$y_{p}=u_{1} y_{1}+u_{2} y_{2}+u_{3} y_{3}=\frac{x^{3}}{36} x^{-1}+x^{2}\left(-\frac{1}{3} \ln x\right)+x^{3}\left(-\frac{1}{4 x}\right)=-\frac{2}{9} x^{2}-\frac{1}{3} x^{2} \ln x.$$ and $$y=y_{c}+y_{p}=c_{1} x^{-1}+c_{2} x^{2}+c_{3} x^{3}-\frac{2}{9} x^{2}-\frac{1}{3} x^{2} \ln x, \quad x > 0.$$

The thinner curve is obtained using a numerical solver, while the thicker curve is the graph of the Taylor polynomial. We look for a solution of the form \\[ y(x)=y(0)+y^{\prime}(0) x+\frac{1}{2 !} y^{\prime \prime}(0) x^{2}+\frac{1}{3 !} y^{\prime \prime \prime}(0) x^{3}+\frac{1}{4 !} y^{(4)}(0) x^{4}+\frac{1}{5 !} y^{(5)}(0) x^{5} \\] From \(y^{\prime \prime}(x)=x^{2}+y^{2}-2 y^{\prime}\) we compute \\[ \begin{aligned} y^{\prime \prime \prime}(x) &=2 x+2 y y^{\prime}-2 y^{\prime \prime} \\ y^{(4)}(x) &=2+2\left(y^{\prime}\right)^{2}+2 y y^{\prime \prime}-2 y^{\prime \prime \prime} \\ y^{(5)}(x) &=6 y^{\prime} y^{\prime \prime}+2 y y^{\prime \prime \prime}-2 y^{(4)} \end{aligned} \\] Using \(y(0)=1\) and \(y^{\prime}(0)=1\) we find \\[ y^{\prime \prime}(0)=-1, \quad y^{\prime \prime \prime}(0)=4, \quad y^{(4)}(0)=-6, \quad y^{(5)}(0)=14 \\] An approximate solution is \\[ y(x)=1+x-\frac{1}{2} x^{2}+\frac{2}{3} x^{3}-\frac{1}{4} x^{4}+\frac{7}{60} x^{5} \\]

The complementary function is \(y_{c}=e^{2 x}\left(c_{1} \cos 2 x+c_{2} \sin 2 x\right) .\) We assume a particular solution of the form \(y_{p}=\left(A x^{3}+B x^{2}+C x\right) e^{2 x} \cos 2 x+\left(D x^{3}+E x^{2}+F\right) e^{2 x} \sin 2 x .\) Substituting into the differential equation and using a CAS to simplify yields $$\left[12 D x^{2}+(6 A+8 E) x+(2 B+4 F)\right] e^{2 x} \cos 2 x$$ $$+\left[-12 A x^{2}+(-8 B+6 D) x+(-4 C+2 E)\right] e^{2 x} \sin 2 x$$ $$=\left(2 x^{2}-3 x\right) e^{2 x} \cos 2 x+\left(10 x^{2}-x-1\right) e^{2 x} \sin 2 x$$ This gives the system of equations $$\begin{array}{ccc} 12 D=2, & 6 A+8 E=-3, & 2 B+4 F=0 \\ -12 A=10, & -8 B+6 D=-1, & -4 C+2 E=-1 \end{array}$$ from which we find \(A=-\frac{5}{6}, B=\frac{1}{4}, C=\frac{3}{8}, D=\frac{1}{6}, E=\frac{1}{4},\) and \(F=-\frac{1}{8} .\) Thus, a particular solution of the differential equation is $$y_{p}=\left(-\frac{5}{6} x^{3}+\frac{1}{4} x^{2}+\frac{3}{8} x\right) e^{2 x} \cos 2 x+\left(\frac{1}{6} x^{3}+\frac{1}{4} x^{2}-\frac{1}{8} x\right) e^{2 x} \sin 2 x$$

We have \(y_{c}=c_{1} e^{-2 x}+e^{x}\left(c_{2} \cos \sqrt{3} x+c_{3} \sin \sqrt{3} x\right)\) and we assume \(y_{p}=A x+B+C x e^{-2 x}\). Substituting into the differential equation we find \(A=\frac{1}{4}, B=-\frac{5}{8},\) and \(C=\frac{2}{3} .\) Thus \(y=c_{1} e^{-2 x}+e^{x}\left(c_{2} \cos \sqrt{3} x+c_{3} \sin \sqrt{3} x\right)+\frac{1}{4} x-\frac{5}{8}+\frac{2}{3} x e^{-2 x}\) From the initial conditions we obtain \(c_{1}=-\frac{23}{12}, c_{2}=-\frac{59}{24},\) and \(c_{3}=\frac{17}{72} \sqrt{3},\) so $$y=-\frac{23}{12} e^{-2 x}+e^{x}\left(-\frac{59}{24} \cos \sqrt{3} x+\frac{17}{72} \sqrt{3} \sin \sqrt{3} x\right)+\frac{1}{4} x-\frac{5}{8}+\frac{2}{3} x e^{-2 x}$$

(a) When \(T(x)=x^{2}\) the given differential equation is the Cauchy-Euler equation \\[ x^{2} y^{\prime \prime}+2 x y^{\prime}+\rho \omega^{2} y=0 \\] The solutions of the auxiliary equation \\[ m(m-1)+2 m+\rho \omega^{2}=m^{2}+m+\rho \omega^{2}=0 \\] are \\[ m_{1}=-\frac{1}{2}-\frac{1}{2} \sqrt{4 \rho \omega^{2}-1} i, \quad m_{2}=-\frac{1}{2}+\frac{1}{2} \sqrt{4 \rho \omega^{2}-1} \\] when \(\rho \omega^{2}>0.25 .\) Thus \\[ y=c_{1} x^{-1 / 2} \cos (\lambda \ln x)+c_{2} x^{-1 / 2} \sin (\lambda \ln x) \\] where \(\lambda=\frac{1}{2} \sqrt{4 \rho \omega^{2}-1} .\) Applying \(y(1)=0\) gives \(c_{1}=0\) and consequently \\[ y=c_{2} x^{-1 / 2} \sin (\lambda \ln x) \\]. The condition \(y(e)=0\) requires \(c_{2} e^{-1 / 2} \sin \lambda=0 . \quad\) We obtain a nontrivial solution when \(\lambda_{n}=n \pi\) \(n=1,2,3, \ldots .\) But $$\lambda_{n}=\frac{1}{2} \sqrt{4 \rho \omega_{n}^{2}-1}=n \pi$$ Solving for \(\omega_{n}\) gives \\[ \omega_{n}=\frac{1}{2} \sqrt{\left(4 n^{2} \pi^{2}+1\right) / \rho} \\]. The corresponding solutions are \\[ y_{n}(x)=c_{2} x^{-1 / 2} \sin (n \pi \ln x) \\]. b.

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