/*! 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 9 For \(y^{\prime}-\frac{1}{x} y=x... [FREE SOLUTION] | 91Ó°ÊÓ

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For \(y^{\prime}-\frac{1}{x} y=x \sin x\) an integrating factor is \(e^{-\int(1 / x) d x}=\frac{1}{x}\) so that \(\frac{d}{d x}\left[\frac{1}{x} y\right]=\sin x\) and \(y=c x-x \cos x\) for \(0< x<\infty\).

Short Answer

Expert verified
The integrating factor solution to the differential equation is \( y = Cx - x \cos x \).

Step by step solution

01

Identify the Differential Equation

The given differential equation is \[ y^{\prime} - \frac{1}{x} y = x \sin x \] which is a first-order linear differential equation.
02

Determine the Integrating Factor

For a differential equation of the form \( y^{\prime} + P(x)y = Q(x) \), the integrating factor is given by \[ e^{\int P(x)\,dx} \]In this problem, \( P(x) = -\frac{1}{x} \), so the integrating factor is: \[ e^{-\int \frac{1}{x}\,dx} = e^{\ln x^{-1}} = \frac{1}{x} \] as provided in the problem.
03

Multiply Through by the Integrating Factor

Multiply every term in the differential equation by the integrating factor \( \frac{1}{x} \) to get \[ \frac{1}{x} y^{\prime} - \frac{1}{x^2} y = \sin x \] which simplifies to \[ \frac{d}{dx} \left( \frac{1}{x} y \right) = \sin x \].
04

Integrate Both Sides

Integrate both sides with respect to \(x\): \[ \int \frac{d}{dx} \left( \frac{1}{x} y \right) \, dx = \int \sin x \, dx \] This implies: \[ \frac{1}{x} y = -\cos x + C \] where \(C\) is the constant of integration.
05

Solve for \( y \)

Multiply both sides by \(x\) to solve for \(y\): \[ y = -x \cos x + Cx \]Thus, the general solution is: \[ y = Cx - x \cos x \].

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Key Concepts

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

Integrating Factor
An integrating factor is a mathematical tool used in solving first-order linear differential equations like the one given in the exercise: \[ y^{\prime} - \frac{1}{x} y = x \sin x \]When you see a differential equation in the standard linear form, which is \( y^{\prime} + P(x)y = Q(x) \), your first task is to determine the integrating factor. The integrating factor is a function, typically denoted as \( \,\mu(x) \), that you multiply through the entire differential equation to simplify it. Here’s a quick guide to finding and applying the integrating factor:
  • Identify \( P(x) \) from your equation. In our example, \( P(x) = -\frac{1}{x} \).
  • The integrating factor, \( \,\mu(x) \), is \( e^{\int P(x) \, dx} \).
  • For \( P(x) = -\frac{1}{x} \), the integral \( \int -\frac{1}{x} \, dx \) results in \( -\ln x \), so the integrating factor is \( e^{-\ln x} = \frac{1}{x} \).
  • Multiply the original differential equation by this integrating factor to transform it into a simpler form.
This transformation allows the equation to express the left-hand side as the derivative of a product, making it much easier to integrate and solve.
Constant of Integration
The constant of integration, often denoted as \( C \), plays a crucial role in solving indefinite integrals in calculus, particularly when finding the general solution to differential equations. Let's connect this concept with the exercise at hand:After integrating both sides of the simplified differential equation, we have:\[\frac{1}{x}y = -\cos x + C\]The constant of integration \( C \) appears as a result of performing the integration process. Since the integration of a function can yield infinitely many antiderivatives, the constant \( C \) accounts for all these possible solutions.
  • Every time you solve an indefinite integral, remember to add \( C \), because the derivative of a constant is zero and it does not appear in the differentiation process.
  • In the context of differential equations, this constant ensures that the solution represents the family of all possible solutions.
  • To find a particular solution, more information like initial conditions would be needed to determine the specific value of \( C \).
Including the constant \( C \) ensures that our solution captures all the possibilities that satisfy the original differential equation.
General Solution
A general solution to a differential equation encompasses all possible solutions. In the context of first-order linear differential equations, once an intercepting factor simplifies the process, we aim to obtain this general solution by integrating and applying the constant of integration.In the provided exercise:\[ y = Cx - x \cos x\]This example illustrates the overall solution taking the following components into consideration:
  • The solution incorporates the particular integral or specific function satisfying the non-homogeneous part of the differential equation, which is \(-x \cos x\) here.
  • It also includes the homogeneous part of the solution reflecting the general behavior without the specific non-homogeneous factor, expressed as \(Cx\).
  • The parameter \( C \) allows for the representation of all solutions to the differential equation without specific boundary or initial conditions.
The general solution presents a complete family of functions that satisfy the differential equation, with each specific \( C \) value providing a unique function that solves the equation under certain conditions. This is essential in understanding the flexibility and breadth of potential solutions.

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Most popular questions from this chapter

Assume that \(d T / d t=k(T-5)\) so that \(T=5+c e^{k t} .\) If \(T(1)=55^{\circ}\) and \(T(5)=30^{\circ}\) then \(k=-\frac{1}{4} \ln 2\) and \(c=59.4611\) so that \(T(0)=64.4611^{\circ}\).

(a) The equilibrium solutions \(y(x)=2\) and \(y(x)=-2\) satisfy the initial conditions \(y(0)=2\) and \(y(0)=-2\) respectively. Setting \(x=\frac{1}{4}\) and \(y=1\) in \(y=2\left(1+c e^{4 x}\right) /\left(1-c e^{4 x}\right)\) we obtain $$1=2 \frac{1+c e}{1-c e}, \quad 1-c e=2+2 c e, \quad-1=3 c e, \quad \text { and } \quad c=-\frac{1}{3 e}$$. (b) Separating variables and integrating yields \\[ \begin{aligned} \frac{1}{4} \ln |y-2|-\frac{1}{4} \ln |y+2|+\ln c_{1} &=x \\ \ln |y-2|-\ln |y+2|+\ln c &=4 x \\ \ln \left|\frac{c(y-2)}{y+2}\right| &=4 x \\ c \frac{y-2}{y+2} &=e^{4 x}.\end{aligned}\\] Solving for \(y\) we get \(y=2\left(c+e^{4 x}\right) /\left(c-e^{4 x}\right) .\) The initial condition \(y(0)=-2\) implies \(2(c+1) /(c-1)=-2\) which yields \(c=0\) and \(y(x)=-2 .\) The initial condition \(y(0)=2\) does not correspond to a value of \(c,\) and it must simply be recognized that \(y(x)=2\) is a solution of the initial-value problem. Setting \(x=\frac{1}{4}\) and \(y=1\) in \(y=2\left(c+e^{4 x}\right) /\left(c-e^{4 x}\right)\) leads to \(c=-3 e .\) Thus, a solution of the initial-value problem is $$y=2 \frac{-3 e+e^{4 x}}{-3 e-e^{4 x}}=2 \frac{3-e^{4 x-1}}{3+e^{4 x-1}}.$$

From \(\frac{1}{1+(2 y)^{2}} d y=\frac{-x}{1+\left(x^{2}\right)^{2}} d x\) we obtain \(\frac{1}{2} \tan ^{-1} 2 y=-\frac{1}{2} \tan ^{-1} x^{2}+c \quad\) or \(\quad \tan ^{-1} 2 y+\tan ^{-1} x^{2}=c_{1}\). Using \(y(1)=0\) we find \(c_{1}=\pi / 4\). Thus, an implicit solution of the initial-value problem is \(\tan ^{-1} 2 y+\tan ^{-1} x^{2}=\pi / 4 .\) Solving for \(y\) and using a trigonometric identity we get $$\begin{aligned} 2 y &=\tan \left(\frac{\pi}{4}-\tan ^{-1} x^{2}\right) \\ y &=\frac{1}{2} \tan \left(\frac{\pi}{4}-\tan ^{-1} x^{2}\right) \\ &=\frac{1}{2} \frac{\tan \frac{\pi}{4}-\tan \left(\tan ^{-1} x^{2}\right)}{1+\tan \frac{\pi}{4} \tan \left(\tan ^{-1} x^{2}\right)} \\ &=\frac{1}{2} \frac{1-x^{2}}{1+x^{2}}. \end{aligned}$$

(a) Integrating \(d^{2} s / d t^{2}=-g\) we get \(v(t)=d s / d t=-g t+c .\) From \(v(0)=300\) we find \(c=300,\) and we are given \(g=32,\) so the velocity is \(v(t)=-32 t+300\). (b) Integrating again and using \(s(0)=0\) we get \(s(t)=-16 t^{2}+300 t .\) The maximum height is attained when \(v=0,\) that is, at \(t_{a}=9.375 .\) The maximum height will be \(s(9.375)=1406.25 \mathrm{ft}\).

For \(0 \leq t \leq 20\) the differential equation is \(20 d i / d t+2 i=120 .\) An integrating factor is \(e^{t / 10},\) so \((d / d t)\left[e^{t / 10} i\right]=\) \(6 e^{t / 10}\) and \(i=60+c_{1} e^{-t / 10} .\) If \(i(0)=0\) then \(c_{1}=-60\) and \(i=60-60 e^{-t / 10} .\) For \(t>20\) the differential equation is \(20 d i / d t+2 i=0\) and \(i=c_{2} e^{-t / 10} .\) At \(t=20\) we want \(c_{2} e^{-2}=60-60 e^{-2}\) so that \(c_{2}=60\left(e^{2}-1\right)\). Thus $$i(t)=\left\\{\begin{array}{ll} 60-60 e^{-t / 10}, & 0 \leq t \leq 20 \\ 60\left(e^{2}-1\right) e^{-t / 10}, & t>20 \end{array}\right.$$

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