Chapter 2: Problem 21
In Problems 21 and 22 solve the given Bernoulli equation subject to the indicated initial condition. \(x^{2} \frac{d y}{d x}-2 x y=3 y^{4}, \quad y(1)=\frac{1}{2}\)
Short Answer
Expert verified
The solution is \( y(x) = \left( \frac{9}{7x} + Cx^6 \right)^{-1/3} \), where \( C \) is determined by \( y(1) = \frac{1}{2} \).
Step by step solution
01
Identify Bernoulli's Equation
The given differential equation is \( x^{2} \frac{dy}{dx} - 2xy = 3y^4 \). A Bernoulli's equation has the form \( \frac{dy}{dx} + P(x)y = Q(x)y^n \). Rewriting the given equation: \( \frac{dy}{dx} = \frac{2xy}{x^2} + \frac{3y^4}{x^2} \). This matches the Bernoulli form with \( P(x) = -\frac{2}{x} \), \( Q(x) = \frac{3}{x^2} \), and \( n = 4 \).
02
Divide Through by \(y^4\)
Divide every term in the equation by \( y^4 \) to rewrite it as: \( y^{-4} \frac{dy}{dx} - \frac{2}{x} y^{-3} = \frac{3}{x^2} \). This prepares the equation for a substitution to make it linear.
03
Use Substitution to Transform Equation
Let \( v = y^{-3} \), so \( \frac{dv}{dx} = -3y^{-4} \frac{dy}{dx} \). The differential equation becomes \( -\frac{1}{3} \frac{dv}{dx} + \frac{2}{x}v = \frac{3}{x^2} \). Rearranging gives \( \frac{dv}{dx} - \frac{6}{x}v = -\frac{9}{x^2} \).
04
Find the Integrating Factor
The equation \( \frac{dv}{dx} - \frac{6}{x} v = -\frac{9}{x^2} \) is linear in \( v \). To solve this using an integrating factor, calculate \( \mu(x) = e^{\int -\frac{6}{x} dx} = e^{-6 \ln x} = x^{-6} \).
05
Apply Integrating Factor to Solve for \(v(x)\)
Multiply every term in the differential equation by \( x^{-6} \): \( x^{-6} \frac{dv}{dx} - 6x^{-7}v = -\frac{9}{x^8} \). This simplifies to \( \frac{d}{dx}(x^{-6}v) = -\frac{9}{x^8} \). Integrate both sides: \( x^{-6}v = \int -\frac{9}{x^8} dx = \frac{9}{7x^7} + C \).
06
Solve for \(v(x)\)
Solve for \( v(x) \): \( v(x) = x^{6} \left( \frac{9}{7x^7} + C \right) = \frac{9}{7x} + Cx^{6} \).
07
Convert Back to \(y(x)\)
Since \( v = y^{-3} \), we have \( y(x) = v^{-1/3} = \left( \frac{9}{7x} + Cx^{6} \right)^{-1/3} \).
08
Use Initial Condition to Find \(C\)
Apply the initial condition \( y(1) = \frac{1}{2} \). Substitute \( x = 1 \) and \( y = \frac{1}{2} \) into \( \left( \frac{9}{7} + C \right)^{-1/3} = \frac{1}{2} \). Solving gives \( C = \frac{119}{8} - \frac{9}{7} \). Calculate to find \( C \).
09
Write the Final Solution
Substitute \( C \) back into \( y(x) = \left( \frac{9}{7x} + \left( \frac{119}{8} - \frac{9}{7} \right)x^{6} \right)^{-1/3} \). This is the solution to the differential equation with the given initial condition.
Unlock Step-by-Step Solutions & Ace Your Exams!
-
Full Textbook Solutions
Get detailed explanations and key concepts
-
Unlimited Al creation
Al flashcards, explanations, exams and more...
-
Ads-free access
To over 500 millions flashcards
-
Money-back guarantee
We refund you if you fail your exam.
Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!
Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Initial Condition
The initial condition in a differential equation provides a specific solution among potentially infinite others. It means that we are given the value of the solution at a particular point. In our example, we have the condition \( y(1) = \frac{1}{2} \), which gives us a value of the function \( y \) at \( x = 1 \). This information allows us to find the constant \( C \) after solving the differential equation. Without it, we would only arrive at a general solution containing an arbitrary constant. The initial condition helps tailor the solution to a specific scenario.
Integrating Factor
An integrating factor helps solve linear differential equations. It's essentially a function we multiply with every term to make the equation easier to integrate. For the differential equation in our problem, \( \frac{dv}{dx} - \frac{6}{x}v = -\frac{9}{x^2} \), we find the integrating factor \( \mu(x) = x^{-6} \). The computation involves exponentiating the integral of the coefficient of \( v \), i.e., \( -\frac{6}{x} \). This step converts the left side of the equation into a perfect derivative, reducible through integration. The integrating factor simplifies the equation, making it solvable by direct integration.
Substitution Method
Substitution is a powerful technique to transform differential equations into simpler forms. In our case, the original Bernoulli differential equation isn't linear. We use the substitution \( v = y^{-3} \) to convert it into a linear form. By letting \( v = y^{-3} \), we introduce a new variable that absorbs the non-linear part. The task then becomes solving the new differential equation with respect to \( v \). It turns the nonlinear Bernoulli equation into a standard linear problem, which can be tackled with the integrating factor method. Substitution is crucial for handling equations unsolvable by standard methods.
Linear Differential Equation
A linear differential equation is an equation involving a function and its derivatives, with no products of the function and its derivatives. It's often written in standard form \( \frac{dy}{dx} + P(x)y = Q(x) \).In our problem, the original Bernoulli equation is not linear because of the term \( y^4 \). Using the substitution method, the form \( \frac{dv}{dx} - \frac{6}{x}v = -\frac{9}{x^2} \) becomes linear with respect to \( v \). Linear equations are simpler to solve as they allow methods like integrating factors and direct integration. Understanding how to transform and handle these equations is crucial in differential calculus.