/*! 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 40 Consider the concept of an integ... [FREE SOLUTION] | 91Ó°ÊÓ

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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.

Short Answer

Expert verified
Yes, they are equivalent if \(\mu \neq 0 \).

Step by step solution

01

Understanding the Problem

We are given two differential equations: \( M\,dx + N\,dy = 0 \) and \( \mu M\,dx + \mu N\,dy = 0 \). We want to determine if solving one equation implies solving the other. The idea is that applying an integrating factor \( \mu \) should not change the set of solutions of the equation.
02

Introducing the Integrating Factor

An integrating factor \( \mu \) is a function used to make a non-exact differential equation exact. This means that \( \mu(M\,dx + N\,dy) \) becomes exact, allowing us to find a potential function \( f \) such that \( df = \mu M\,dx + \mu N\,dy = 0 \). If \( \mu \) satisfies this requirement, it is an integrating factor for the equation.
03

Equivalent Solutions

To determine if these equations are equivalent, assume \( (x_0, y_0) \) is a solution to \( M\,dx + N\,dy = 0 \). Then \( x(t) \) and \( y(t) \) satisfy \( M\frac{dx}{dt} + N\frac{dy}{dt} = 0 \). Multiplying through by \( \mu \), we have \( \mu M\frac{dx}{dt} + \mu N\frac{dy}{dt} = 0 \), which suggests \( (x(t), y(t)) \) is also a solution to \( \mu M\,dx + \mu N\,dy = 0 \).
04

Validity of the Integrating Factor

An important condition is that the integrating factor \( \mu \) must not be zero. If \( \mu(x, y) \equiv 0 \), multiplying any equation by zero gives the trivial equation 0=0, which is not useful for finding solutions to the original equations. Therefore, the suitability of \( \mu \) as an integrating factor ensures the equivalence of the solutions.
05

Conclusion

The equations \( M\,dx + N\,dy = 0 \) and \( \mu M\,dx + \mu N\,dy = 0 \) are equivalent in the sense that a solution to one is a solution to the other, provided that \( \mu eq 0 \).

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Key Concepts

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

Exact Differential Equations
In mathematics, exact differential equations are equations that can be expressed in a specific form that allows the solution process to be relatively straightforward. An exact differential equation takes the form \( M\,dx + N\,dy = 0 \). For an equation to be considered exact, there must exist a potential function \( f(x, y) \) such that the differential of \( f \) is exactly this equation.

This means that \( \frac{\partial f}{\partial x} = M \) and \( \frac{\partial f}{\partial y} = N \). If these conditions hold, the differential equation can be directly integrated, as the potential function acts much like an anti-derivative does in basic calculus.

Being able to determine exactness allows us to find closed-form solutions efficiently, but not all differential equations meet this criterion, leading us to our next concept.
Non-exact Differential Equations
Non-exact differential equations are those where the conditions for exactness are not satisfied. This means that there are no potential functions \( f(x, y) \) for which \( M\,dx + N\,dy = 0 \) directly corresponds to \( df \). These equations cannot be solved as easily as exact equations because they cannot be integrated directly using simple calculus concepts.

Fortunately, we have a tool called an "integrating factor" which can transform a non-exact equation into an exact one. The integrating factor is a function, often denoted by \( \mu(x, y) \), that when multiplied with the non-exact equation, results in an equation that becomes exact.

The process of finding an integrating factor is sometimes complex, but once found, it greatly simplifies solving the differential equation.
Solutions of Differential Equations
The solution of a differential equation is a function or a set of functions that satisfy the equation. For instance, in our context, if \( M\,dx + N\,dy = 0 \) is exact, there exists a potential function \( f(x, y) \) such that \( df = 0 \). Solving this leads us to \( f(x, y) = C \), where \( C \) is an integration constant. This expression represents a family of solutions that define curves on a plane.

Using the integrating factor technique for non-exact differential equations involves identifying the factor \( \mu(x, y) \) that can transform the equation into an exact form. This allows us to apply the same solution process as for exact differential equations. Hence, an integrating factor expands the solvability of differential equations significantly.

It is crucial that the integrating factor never equals zero, as this would render the equation unsolvable in the traditional sense.
Potential Function
A potential function is integral to solving exact differential equations. It is a function \( f(x, y) \) whose existence guarantees that a differential equation is exact. When dealing with an exact equation, \( M\,dx + N\,dy = 0 \), the potential function \( f \) fulfills \( df = M\,dx + N\,dy \).

Finding the potential function involves partial integration of the components \( M \) and \( N \). This process links calculus to differential equations, specifically showcasing how we can solve them when they represent the derivative of some function.

Understanding potential functions offers a conceptual insight into how changing the perspective on a differential equation—from viewing it as a relation between derivatives to viewing it as a differential of a single function—can drastically simplify solving it.

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Most popular questions from this chapter

Radioactive Decay Series The following system of differential equations is encountered in the study of the decay of a special type of radioactive series of elements: $$\begin{aligned} &\frac{d x}{d t}=-\lambda_{1} x\\\ &\frac{d y}{d t}=\lambda_{1} x-\lambda_{2} y. \end{aligned}$$ where \(\lambda_{1}\) and \(\lambda_{2}\) are constants. Discuss how to solve this system subject to \(x(0)=x_{0}, y(0)=y_{0} .\) Carry out your ideas.

Solve the given initial-value problem. $$\left(\frac{3 y^{2}-t^{2}}{y^{5}}\right) \frac{d y}{d t}+\frac{t}{2 y^{4}}=0, \quad y(1)=1$$

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.

Solve the given differential equation by using an appropriate substitution. $$\frac{d y}{d x}=\sin (x+y)$$

Solve the given initial-value problem. Give the largest interval \(I\) over which the solution is defined. $$y \frac{d x}{d y}-x=2 y^{2}, \quad y(1)=5$$

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