Chapter 9: Problem 26
Find the general solution. $$ \left(D^{2}+4 D+4\right) y=-x^{-2} e^{-2 x} $$
Short Answer
Expert verified
The general solution is \( y(x) = C_1 e^{-2x} + C_2 x e^{-2x} + y_p(x) \) with \( y_p(x) \) from the particular solution calculation.
Step by step solution
01
Identify the Differential Operator and Solve for the Complementary Solution
Firstly, observe that the left-hand side is the operator \( L(D) = D^2 + 4D + 4 \). To find the complementary solution \( y_c \), solve the characteristic equation of the homogeneous differential equation \( L(D) y = 0 \). This is given by \( m^2 + 4m + 4 = 0 \).
02
Find the Roots of the Characteristic Equation
The characteristic equation \( m^2 + 4m + 4 = 0 \) can be factored as \( (m+2)^2 = 0 \), which implies a repeated root \( m = -2 \).
03
Write the Complementary Solution
Since we have a repeated root \( m = -2 \), the complementary solution is \( y_c(x) = C_1 e^{-2x} + C_2 x e^{-2x} \), where \( C_1 \) and \( C_2 \) are constants.
04
Find the Particular Solution Using Variation of Parameters
To find the particular solution \( y_p \), use the variation of parameters method since the right-hand side \(-x^{-2} e^{-2x} \) is not a polynomial. Assume \( y_p = u_1(x) e^{-2x} + u_2(x) x e^{-2x} \). Compute \( u_1(x) \) and \( u_2(x) \) using the Wronskian and the given functions.
05
Set Up Wronskian and Solve for u1 and u2
The Wronskian of the functions \( e^{-2x} \) and \( x e^{-2x} \) is \( \begin{vmatrix} e^{-2x} & x e^{-2x} \ -2e^{-2x} & (1-2x) e^{-2x} \end{vmatrix} = e^{-4x} \). Using this, find \( u_1(x) \) and \( u_2(x) \) from the system:\[ \begin{aligned} u_1' &= \frac{-xe^{-2x}}{e^{-4x}}, \ u_2' &= \frac{e^{-2x}}{e^{-4x}}, \end{aligned} \]and solve these integrals.
06
Compute Integrals for u1 and u2
Integrate to find:\[ \begin{aligned} u_1(x) &= \int -x e^{2x} \, dx, \ u_2(x) &= \int e^{2x} \, dx. \end{aligned} \] These integrals yield expressions for \( u_1(x) \) and \( u_2(x) \) to be used in computing \( y_p \).
07
Combine Complementary and Particular Solution
After solving the integrals for \( u_1(x) \) and \( u_2(x) \), substitute back into the equation \( y_p = u_1(x) e^{-2x} + u_2(x) x e^{-2x} \). Finally, the general solution is the sum of the complementary and particular solutions: \( y(x) = y_c(x) + y_p(x) \).
08
Finalize and Simplify the General Solution
Combine the expressions for \( y_c \) and \( y_p \) to write the general solution in its simplest form. The full form is:\[ y(x) = C_1 e^{-2x} + C_2 x e^{-2x} + y_p(x) \] where \( y_p(x) \) is computed based on \( u_1(x) \) and \( u_2(x) \) obtained in previous steps.
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.
Differential Equations
Differential equations are mathematical equations that relate a function with its derivatives. They are crucial in modeling various physical, natural, and engineering processes. A differential equation involves unknown functions and their derivatives. The order of the equation is determined by the highest derivative present. In our problem, we deal with a second-order linear differential equation given by: \[ (D^2 + 4D + 4)y = -x^{-2}e^{-2x} \]. This equation is linear because it only involves the first power of the derivative terms. Solving such equations typically involves finding solutions to both homogeneous and non-homogeneous forms of the differential equation. This involves finding a complementary solution (for the homogeneous part) and a particular solution (for the non-homogeneous part), which when combined give the general solution. Differential equations have widespread applications ranging from physics to finance.
Complementary Solution
The complementary solution, often symbolized as \( y_c(x) \), is a part of the general solution of a differential equation that solves its homogeneous form. The homogeneous part of our differential equation ignores the right-hand side driving function and is expressed as: \[ (D^2 + 4D + 4)y = 0 \].To find \( y_c(x) \), we must solve the characteristic equation which is extracted by replacing the derivatives (like \(D^2\)) with corresponding powers of an unknown \( m \), resulting in: \[ m^2 + 4m + 4 = 0 \]. Finding the roots of this characteristic equation helps us to determine the form of the complementary solution. In this problem, the repeated root \( m = -2 \) means the complementary solution takes the form: \[ y_c(x) = C_1 e^{-2x} + C_2 x e^{-2x} \]. This kind of solution arises due to the multiplicity of the roots and is common in second-order linear differential equations.
Wronskian
The Wronskian is a determinant used in the study of differential equations to assess the linear independence of solutions. Particularly, it plays a pivotal role in the variation of parameters method. When finding a particular solution with this method, we require two linearly independent solutions from the complementary solution, here \( e^{-2x} \) and \( x e^{-2x} \). The Wronskian of these solutions is given by: \[ W(e^{-2x}, x e^{-2x}) = \begin{vmatrix} e^{-2x} & xe^{-2x} \ -2e^{-2x} & (1-2x)e^{-2x} \end{vmatrix} = e^{-4x} \].A non-zero Wronskian confirms that the solutions \( e^{-2x} \) and \( x e^{-2x} \) are linearly independent, making them valid for constructing a particular solution using the variation of parameters. This involves setting up equations based on the Wronskian to solve for unknown functions \( u_1(x) \) and \( u_2(x) \), which are then integrated to form the particular solution of the differential equation. Thus, the Wronskian is an essential tool in the solution process.