Chapter 3: Problem 35
Solve the following differential equations by using integrating factors. $$ y^{\prime}+\ln x=\frac{y}{x} $$
Short Answer
Expert verified
The solution to the differential equation is \( y(x) = -\frac{x}{2} (\ln x)^2 + Cx \).
Step by step solution
01
Rewrite the Equation in the Standard Form
We start with the given differential equation \( y' + \ln x = \frac{y}{x} \). The goal is to rewrite it in the standard linear form \( y' + P(x)y = Q(x) \). First, simplify the equation by rearranging it as \( y' - \frac{y}{x} = -\ln x \). Here, we can see that \( P(x) = -\frac{1}{x} \) and \( Q(x) = -\ln x \).
02
Find the Integrating Factor
The integrating factor \( \mu(x) \) is given by the formula \( e^{\int P(x) \, dx} \). In this case, \( \int P(x) \, dx = \int -\frac{1}{x} \, dx = -\ln x \). Therefore, the integrating factor is \( \mu(x) = e^{-\ln x} = \frac{1}{x} \).
03
Multiply the Equation by the Integrating Factor
Multiply the entire differential equation \( y' - \frac{y}{x} = -\ln x \) by the integrating factor \( \frac{1}{x} \), obtaining \( \frac{y'}{x} - \frac{y}{x^2} = -\frac{\ln x}{x} \). This step ensures that the left-hand side becomes the derivative of the product \( \frac{y}{x} \).
04
Write the Left Side as a Derivative
The left-hand side of the equation \( \frac{y'}{x} - \frac{y}{x^2} \) can now be written as \( \frac{d}{dx} \left( \frac{y}{x} \right) \). Thus, our equation becomes \( \frac{d}{dx} \left( \frac{y}{x} \right) = -\frac{\ln x}{x} \).
05
Integrate Both Sides
Integrate both sides with respect to \( x \): \( \int \frac{d}{dx} \left( \frac{y}{x} \right) \, dx = \int -\frac{\ln x}{x} \, dx \). The left-hand side simplifies to \( \frac{y}{x} \). The integral of \( -\frac{\ln x}{x} \) can be solved using integration by parts, yielding \( \frac{y}{x} = -\frac{1}{2} (\ln x)^2 + C \), where \( C \) is the constant of integration.
06
Solve for \( y \)
To find \( y \), multiply both sides of the equation \( \frac{y}{x} = -\frac{1}{2} (\ln x)^2 + C \) by \( x \): \( y(x) = -\frac{x}{2} (\ln x)^2 + Cx \). This expression for \( y \) is the solution to the original differential equation.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Integrating Factors
When given a linear first-order differential equation, one powerful tool we use is the integrating factor. This technique simplifies solving the equation by transforming it into a format that's easier to manage. The goal is to multiply the entire differential equation by a carefully chosen function, known as the integrating factor.
- The integrating factor is derived using the formula \( \mu(x) = e^{\int P(x) \ dx} \), where \( P(x) \) is a function from the rearranged form of the differential equation.
- In our exercise, once the equation was rearranged to \( y' - \frac{y}{x} = -\ln x \), we identified \( P(x) = -\frac{1}{x} \).
- Finding the integral \( \int -\frac{1}{x} \ dx \) resulted in \( -\ln x \), leading to an integrating factor \( \mu(x) = e^{- \ln x} = \frac{1}{x} \).
Linear Differential Equations
Linear differential equations are a type of differential equation where the unknown function and its derivatives appear linearly (i.e., not multiplied together or raised to a power). These equations are crucial in mathematical modeling since they appear frequently in many applications, such as physics and engineering.
- The standard form of a linear first-order differential equation is \( y' + P(x)y = Q(x) \).
- In the given exercise, after rearranging, the equation became \( y' - \frac{y}{x} = -\ln x \), fitting the linear equation form with \( P(x) = -\frac{1}{x} \) and \( Q(x) = -\ln x \).
- By working through the standard form and applying the integrating factor, the solution is systematically derived, allowing effective use of calculus tools.
Integration by Parts
Integration by parts is a technique used in calculus to integrate the product of two functions. It is derived from the product rule of differentiation and is a valuable tool when dealing with more complex integrals.
- The formula for integration by parts is \( \int u \ dv = uv - \int v \ du \), where \( u \) and \( dv \) are parts of the original integral being solved.
- In our differential equation exercise, we used integration by parts to solve \( \int -\frac{\ln x}{x} \ dx \).
- This step resulted in the integral solution: \( -\frac{1}{2} (\ln x)^2 \). Here, \( u = \ln x \) and \( dv = -\frac{1}{x} \ dx \) were chosen, leading to an easier integration process.