Chapter 3: Problem 27
Solve the given initial-value problem. Use a graphing utility to graph the solution curve. $$ x^{2} y^{\prime \prime}+x y^{\prime}+y=0, y(1)=1, y^{\prime}(1)=2 $$
Short Answer
Expert verified
The solution is \( y(x) = x^{-1/2} ( \cos(\frac{\sqrt{3}}{2} \ln x) + 2\sqrt{3} \sin(\frac{\sqrt{3}}{2} \ln x) ) \).
Step by step solution
01
Identify the Type of Differential Equation
The given differential equation is \( x^2 y'' + x y' + y = 0 \). This is a second-order linear differential equation with variable coefficients. Recognizing this form, we can explore solution methods such as the Cauchy-Euler equation form.
02
Apply a Suitable Method
Given the structure \( x^2 y'' + x y' + y = 0 \), recognize it as a Cauchy-Euler equation, often solved using a substitution such as \( y = x^m \), leading to a characteristic equation.
03
Find the Characteristic Equation
Substitute \( y = x^m \) into the differential equation: \( m(m-1)x^m + mx^m + x^m = 0 \). Simplify to \( m^2 x^m = 0 \), giving the characteristic equation \( m^2 + m + 1 = 0 \).
04
Solve the Characteristic Equation
The characteristic equation is \( m^2 + m + 1 = 0 \). Solving this, use the quadratic formula: \( m = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \), where \( a = 1 \), \( b = 1 \), and \( c = 1 \). Calculate the discriminant: \( 1^2 - 4 \times 1 \times 1 = -3 \). Thus, roots are \( m = \frac{-1 \pm \sqrt{-3}}{2} = \frac{-1 \pm i \sqrt{3}}{2} \).
05
Form the General Solution
For complex roots \( a \pm bi \), the general solution is \( y(x) = x^a (C_1 \cos(b \ln x) + C_2 \sin(b \ln x)) \). Here, \( a = -\frac{1}{2} \) and \( b = \frac{\sqrt{3}}{2} \), so the general solution is \( y(x) = x^{-1/2}(C_1 \cos(\frac{\sqrt{3}}{2} \ln x) + C_2 \sin(\frac{\sqrt{3}}{2} \ln x)) \).
06
Apply Initial Conditions
Use initial conditions \( y(1) = 1 \) and \( y'(1) = 2 \) to find \( C_1 \) and \( C_2 \). First, apply \( y(1) = 1 \): \( 1^{-1/2}(C_1 \cos(0) + C_2 \sin(0)) = 1 \) leading to \( C_1 = 1 \).
07
Use Derivative for Second Initial Condition
Differentiate the general solution for \( y' \), then use \( y'(1) = 2 \). Differentiating gives a general formula, evaluated at \( x = 1 \); solve for \( C_2 \) to satisfy the second initial condition, resulting in \( C_2 = 2 \sqrt{3} \).
08
Final Solution with Constants
Substitute \( C_1 = 1 \) and \( C_2 = 2\sqrt{3} \) back into the general solution: \( y(x) = x^{-1/2} ( \cos(\frac{\sqrt{3}}{2} \ln x) + 2\sqrt{3} \sin(\frac{\sqrt{3}}{2} \ln x) ) \).
09
Graph the Solution
Use a graphing utility like Desmos or Python's matplotlib to visually confirm the behavior of the solution curve. Input the derived equation and plot \( y(x) = x^{-1/2} ( \cos(\frac{\sqrt{3}}{2} \ln x) + 2\sqrt{3} \sin(\frac{\sqrt{3}}{2} \ln x) ) \) within a suitable range of \( x \).
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Understanding Second-Order Linear Differential Equations
Second-order linear differential equations are essential in various fields, including physics and engineering. These equations involve an unknown function and its derivatives, specifically the second derivative. The standard form of a second-order linear differential equation is \(a(x)y'' + b(x)y' + c(x)y = 0\). In our exercise, the coefficients are functions of \(x\), making it a Cauchy-Euler equation.
These equations have important properties that simplify finding their solutions:
These equations have important properties that simplify finding their solutions:
- Linearity: The equation is linear in terms of the function and its derivatives.
- Order: The highest derivative is the second derivative.
- Variable Coefficients: The coefficients \(a(x), b(x), c(x)\) often follow specific patterns, simplifying analysis.
Defining the Initial Value Problem
An initial value problem (IVP) is a differential equation coupled with specified values at a particular point. The purpose of initial conditions is to ensure a unique solution among the infinitely many possible solutions of a differential equation.
In our case, the initial value problem is given by the equation \( x^{2} y^{\prime \prime}+x y^{\prime}+y=0 \) with conditions \( y(1)=1 \) and \( y^{\prime}(1)=2 \). Here’s why initial conditions matter:
In our case, the initial value problem is given by the equation \( x^{2} y^{\prime \prime}+x y^{\prime}+y=0 \) with conditions \( y(1)=1 \) and \( y^{\prime}(1)=2 \). Here’s why initial conditions matter:
- They provide specific values for the solution and its derivative at \(x = 1\).
- They help determine the constants in the solution that appear after solving the differential equation itself.
Exploring the Characteristic Equation
The characteristic equation is a crucial step in solving second-order linear differential equations. For Cauchy-Euler equations, this is derived by assuming a solution of the form \(y = x^m\). Substituting this into the differential equation allows us to derive what is called the characteristic equation.
In this exercise, we derived the characteristic equation as \(m^2 + m + 1 = 0\) by substituting \(y = x^m\). Key points include:
In this exercise, we derived the characteristic equation as \(m^2 + m + 1 = 0\) by substituting \(y = x^m\). Key points include:
- These equations are typically polynomial equations in terms of \(m\).
- The roots of the characteristic polynomial reveal the form of the general solution.
Handling Complex Roots Solution
Complex roots in the characteristic equation signal a particular behavior in the solution of differential equations. When solving \(m^2 + m + 1 = 0\), we found the roots \(m = \frac{-1 \pm i\sqrt{3}}{2}\). These complex roots yield solutions that involve trigonometric functions along with the powers of \(x\).
For this scenario, the general solution is structured using:
For this scenario, the general solution is structured using:
- Real part \(a\) translates into exponentiation: \(x^a\).
- Imaginary part \(b\) introduces oscillatory behavior: \(C_1\cos(b\ln x) + C_2\sin(b\ln x)\).