/*! 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 8 Solve the given differential equ... [FREE SOLUTION] | 91Ó°ÊÓ

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Solve the given differential equation by separation of variables. $$e^{x} y \frac{d y}{d x}=e^{-y}+e^{-2 x-y}$$

Short Answer

Expert verified
By separating variables and integrating, we find the implicit solution: \( \frac{y^2}{2} = -e^{-x-y} - \frac{1}{2}e^{-2x-y} + C \).

Step by step solution

01

Rewrite the Differential Equation

Starting with the given differential equation: \[ e^x y \frac{dy}{dx} = e^{-y} + e^{-2x-y} \]We want to separate variables, so rewrite it by factoring out terms involving only \( y \) and only \( x \). The equation becomes:\[ y \frac{dy}{dx} = e^{-y-x} + e^{-2x-y-x} \]
02

Bring Like Terms Together

We notice that both terms on the right have a common factor of \( e^{-y-x} \). So we can factor that out:\[ y \frac{dy}{dx} = e^{-y-x}(1 + e^{-x}) \]Now, rearrange terms to group all \( y \)-dependent terms on one side and all \( x \)-dependent terms on the other side.\[ y \cdot dy = \frac{e^{-y-x}(1 + e^{-x})}{e^x} \cdot dx \]
03

Simplify the Equation

Simplify the expression by simplifying the right side:\[ y \cdot dy = e^{-y}(e^{-x} + e^{-2x}) \cdot dx \]Now, ensure like variable terms are on the same side of the equation.
04

Separate the Variables

Separate variables completely so that all \( y \) terms (including \( dy \)) and all \( x \) terms (including \( dx \)) are on opposite sides of the equation:\[ y \cdot dy = (e^{-y})dx \cdot (e^{-x} + e^{-2x}) \]Convert terms further so it's clear:\[ y \cdot dy = dx \cdot (e^{-x-y} + e^{-2x-y}) \]Thus, the equation becomes:\[ \int y \cdot dy = \int (e^{-y-x} + e^{-2x-y}) \cdot dx \]
05

Integrate Both Sides

Integrate both sides of the equation:\[ \int y \cdot dy = \int e^{-y}(e^{-x} + e^{-2x}) \cdot dx \]The left side becomes:\[ \frac{y^2}{2} + C_1 \]For the right side:Break down into parts for easier integration:\[ \int e^{-x-y} dx + \int e^{-2x-y} dx \]Each integral can be solved using the exponent rules, yielding:\[ -e^{-x-y} - \frac{1}{2}e^{-2x-y} + C_2 \]
06

Solve for y if Possible or Leave Implicit

Combine constants into a single constant \( C \):\[ \frac{y^2}{2} = -e^{-x-y} - \frac{1}{2}e^{-2x-y} + C \]This equation represents the implicit solution. Further solutions would require initial conditions or additional constraints. This format may suffice unless a specific form is requested.

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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 equations that relate a function to its derivatives. These equations come in handy when modeling phenomena where the rate of change is an essential aspect, such as physics, engineering, and other applied sciences. In our exercise, we have a differential equation with the main goal being to find the function, typically denoted as \( y(x) \), that satisfies the equation. This is done by solving the equation which may involve rearranging and simplifying terms to make the equation manageable and solvable. The given differential equation in the exercise, \( e^x y \frac{dy}{dx} = e^{-y} + e^{-2x-y} \), showcases a relationship between the function \( y \) and its derivative \( \frac{dy}{dx} \). At first glance, it might seem complex, but using separation of variables is an effective approach to isolate the function \( y \) and the independent variable \( x \) on both sides of the equation.
Implicit Solutions
An implicit solution to a differential equation is a solution where the function \( y(x) \) is not expressed explicitly in terms of \( x \). Instead, the relationship between \( x \) and \( y \) remains intertwined in the solution form. Implicit solutions are important when it's challenging to express \( y \) solely as a function of \( x \) due to complex interactions in the differential equation. In the solved exercise, the result \( \frac{y^2}{2} = -e^{-x-y} - \frac{1}{2}e^{-2x-y} + C \) is an implicit solution. The expression involves both \( x \) and \( y \) mixed together, and unless additional conditions like initial values are provided, the solution remains implicit. Finding an explicit form may not always be crucial unless otherwise specified. Implicit solutions often give a comprehensive overview of the relationship and can be invaluable when solving or approximating real-world problems.
Integration Techniques
Integration is a fundamental process in solving differential equations, especially when we separate variables. In our exercise, after separating the terms involving \( y \) and \( x \), the next step is to integrate both sides. This process requires sound integration skills, as many integration techniques could be needed.The integration on the left side of \( \int y \cdot dy \) results in \( \frac{y^2}{2} \). It demonstrates the basic power rule of integration where \( \int y^n \cdot dy = \frac{y^{n+1}}{n+1} \). On the right side, we handle the integrals \( \int e^{-x-y} dx \) and \( \int e^{-2x-y} dx \). These are solved using the properties of exponents and basic integration rules for exponential functions.Breakdown of these integrals gives \( -e^{-x-y} \) and \( -\frac{1}{2}e^{-2x-y} \) respectively. Such techniques are pivotal in achieving the solutions of complex differential equations and often involve a blend of algebraic manipulation and strategic integration techniques.

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Most popular questions from this chapter

Use a technique of integration or a substitution to find an explicit solution of the given differential equation or initial value problem. $$\frac{d y}{d x}=y^{2 / 3}-y$$

Consider the concept of an integrating factor used in Problems \(29-38 .\) Are the two equations \(M d x+N d y=0\) and \(\mu M d x+\mu N d y=0\) necessarily equivalent in the sense that a solution of one is also a solution of the other? Discuss.

Falling Chain A portion of a uniform chain of length 8 ft is loosely coiled around a peg at the edge of a high horizontal platform, and the remaining portion of the chain hangs at rest over the edge of the platform. See Figure \(2.4 .2 .\) Suppose that the length of the overhanging chain is \(3 \mathrm{ft}\), that the chain weighs \(2 \mathrm{lb} / \mathrm{ft}\), and that the positive direction is downward. Starting at \(t=0\) seconds, the weight of the overhanging portion causes the chain on the table to uncoil smoothly and to fall to the floor. If \(x(t)\) denotes the length of the chain overhanging the table at time \(t>0\), then \(v=d x / d t\) is its velocity. When all resistive forces are ignored, it can be shown that a mathematical model relating \(v\) to \(x\) is given by $$x v \frac{d v}{d x}+v^{2}=32 x$$ (a) Rewrite this model in differential form. Proceed as in Problems \(31-36\) and solve the DE for \(v\) in terms of \(x\) by finding an appropriate integrating factor. Find an explicit solution \(v(x)\) (b) Determine the velocity with which the chain leaves the platform.

Find the general solution of the given differential equation. Give the largest interval \(I\) over which the general solution is defined. Determine whether there are any transient terms in the general solution. $$\left(x^{2}-1\right) \frac{d y}{d x}+2 y=(x+1)^{2}$$

Show that an implicit solution of $$2 x \sin ^{2} y d x-\left(x^{2}+10\right) \cos y d y=0$$ is given by \(\ln \left(x^{2}+10\right)+\csc y=c .\) Find the constant solutions, if any, that were lost in the solution of the differential equation.

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