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use the result of Problem 27 to determine whether the given equation is exact. If so, solve the equation. $$ x^{2} y^{\prime \prime}+x y^{\prime}-y=0, \quad x>0 $$

Short Answer

Expert verified
Given equation: \(x^2y'' + xy' - y = 0\) Answer: Yes, the given equation is exact. The solution is any function, y(x).

Step by step solution

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01

Check if the equation is exact

To check if the given equation is exact, we need to find a function that satisfies the following conditions: $$ \frac{\partial F}{\partial x} = xy', \quad \frac{\partial F}{\partial y} = x^2y'' $$ Since \(y'\) appears only in the first condition, we can integrate the first equation with respect to \(x\): $$ F(x, y) = \int xy' \, dx $$ Let's call the integration constant \(G(y)\) since it depends only on \(y\). So, we have: $$ F(x, y) = \frac{1}{2}x^2y' + G(y) $$ Now, we can differentiate \(F(x, y)\) with respect to \(y\): $$ \frac{\partial F}{\partial y} = x^2y' + G'(y) $$ We want this to be equal to \(x^2y''\). Comparing the two equations, we have: $$ x^2y' = x^2y'', \quad G'(y) = -y $$ Integrating the G'(y) equation with respect to \(y\), we obtain the function G(y): $$ G(y) = -\frac{1}{2}y^2 + C $$ So, the function F(x, y) is given by: $$ F(x, y) = \frac{1}{2}x^2y' - \frac{1}{2}y^2 + C $$ As we found a function F(x, y) that satisfies both conditions, the given equation is exact.
02

Solve the exact equation

From Step 1, we have \(F(x, y) = \frac{1}{2}x^2y' - \frac{1}{2}y^2 + C = 0\). Rearranging the terms, we get: $$ y' = \frac{y}{x} $$ This is a first order linear differential equation on y. To solve this equation, we can first identify the integrating factor: $$ IF = e^{\int \frac{1}{x} \, dx} = e^{\ln{x}} = x $$ Now, we multiply the whole equation by the integrating factor and use product rule: $$ x y' + \frac{1}{x} xy = x({\frac{y}{x}}) $$ Integrating both sides of the equation with respect to \(x\), we get: $$ (xy)' = \int x\cdot \frac{y}{x} \, dx \Rightarrow xy = \int y \, dx \Rightarrow xy=y(x) \int dx $$ This states that there is a function \(y(x)=y\) whose derivative multiplied by \(x\) is equal to y. Given this, we can find out that the original equation is an identity and will be true for all functions y(x). So the solution for the given equation is any function y(x).

Key Concepts

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

Exactness Condition
When dealing with differential equations, the concept of exactness is crucial. It mainly revolves around determining whether a given differential equation can be expressed as the derivative of some function.
An equation of the form \(M(x,y) + N(x,y)\frac{dy}{dx} = 0\) is said to be exact if there exists a function \(F(x, y)\) such that:
  • \(\frac{\partial F}{\partial x} = M(x, y)\)
  • \(\frac{\partial F}{\partial y} = N(x, y)\).
The system is similar to a gradient of some potential function, which changes the equation into an exact differential.
In the given exercise, we expressed the equation as a system and managed to find such a function \(F(x, y)\), proving exactness and subsequently finding a simplified solution. Understanding exactness is essential for breaking down more complex differential equations into solvable parts.
First Order Linear Differential Equation
First order linear differential equations are among the simplest forms of differential equations that mathematics students encounter. They take the form \(\frac{dy}{dx} + P(x)y = Q(x)\).
In the original problem, once the equation \(x^2y'' + xy' - y = 0\) was reduced to \( y' = \frac{y}{x} \), it became a first order linear differential equation.
Solving such equations often involves utilizing an integrating factor or directly integrating if it's already separable. Recognizing that it can be solved by integrating directly is part of mastering the technique for these types of equations.
First order linear differential equations are powerful tools in modeling exponential growth, decay, cooling, and more.
Integrating Factor
An integrating factor is a special function used to simplify solving first order linear differential equations. This method aims to transform the equation into an easily integrable form. To find the integrating factor, \(IF\), for equations of the form \(\frac{dy}{dx} + P(x)y = Q(x)\), we use:
  • \(IF = e^{\int P(x) \, dx}\).
Multiplying the entire differential equation by this integrating factor allows the left side to become a derivative of the product \(IF \cdot y\).
In the given solution, we identified \(IF = e^{\ln{x}} = x\) to multiply throughout, turning the derivative \((xy)'\) into a much simpler form to integrate. By making the left-hand side an exact derivative, the solution becomes straightforward.
Mastery of applying integrating factors is invaluable in handling a wide array of differential equations.

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Most popular questions from this chapter

try to transform the given equation into one with constant coefficients by the method of Problem 34. If this is possible, find the general solution of the given equation. $$ t y^{\prime \prime}+\left(t^{2}-1\right) y^{\prime}+t^{3} y=0, \quad 0

Show that the solution of the initial value problem $$ L[y]=y^{\prime \prime}+p(t) y^{\prime}+q(t) y=g(t), \quad y\left(t_{0}\right)=y_{0}, \quad y^{\prime}\left(t_{0}\right)=y_{0}^{\prime} $$ can be written as \(y=u(t)+v(t)+v(t),\) where \(u\) and \(v\) are solutions of the two initial value problems $$ \begin{aligned} L[u] &=0, & u\left(t_{0}\right)=y_{0}, & u^{\prime}\left(t_{0}\right)=y_{0}^{\prime} \\ L[v] &=g(t), & v\left(t_{0}\right)=0, & v^{\prime}\left(t_{0}\right) &=0 \end{aligned} $$ respectively. In other words, the nonhomogeneities in the differential equation and in the initial conditions can be dealt with separately. Observe that \(u\) is easy to find if a fundamental set of solutions of \(L[u]=0\) is known.

A mass of \(20 \mathrm{g}\) stretches a spring \(5 \mathrm{cm}\). Suppose that the mass is also attached to a viscous damper with a damping constant of \(400 \mathrm{dyne}\) -sec/cm. If the mass is pulled down an additional \(2 \mathrm{cm}\) and then released, find its position \(u\) at any time \(t .\) Plot \(u\) versus \(t .\) Determine the quasi frequency and the quasi period. Determine the ratio of the quasi period to the period of the corresponding undamped motion. Also find the time \(\tau\) such that \(|u(t)|<0.05\) \(\mathrm{cm}\) for all \(t>\tau\)

determine \(\omega_{0}, R,\) and \(\delta\) so as to write the given expression in the form \(u=R \cos \left(\omega_{0} t-\delta\right)\) $$ u=-\cos t+\sqrt{3} \sin t $$

Deal with the initial value problem $$ u^{\prime \prime}+0.125 u^{\prime}+u=F(t), \quad u(0)=2, \quad u^{\prime}(0)=0 $$ (a) Plot the given forcing function \(F(t)\) versus \(t\) and also plot the solution \(u(t)\) versus \(t\) on the same set of axes. Use a \(t\) interval that is long enough so the initial transients are substantially eliminated. Observe the relation between the amplitude and phase of the forcing term and the amplitude and phase of the response. Note that \(\omega_{0}=\sqrt{k / m}=1\). (b) Draw the phase plot of the solution, that is, plot \(u^{\prime}\) versus \(u .\) \(F(t)=3 \cos 3 t\)

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