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Show that the general solution of the Euler equation \(t^{2} y^{\prime \prime}-2 t y^{\prime}+2 y=0\) is \(y(t)=c_{1} t+c_{2} t^{2}, t>0\)

Short Answer

Expert verified
Answer: The general solution of the Euler equation \(t^2y''-2ty'+2y=0\) is \(y(t) = c_1 t + c_2 t^2\), for \(t>0\).

Step by step solution

01

Substitute \(x=\ln{t}\) and \(y(t)=z(x)\)

To solve this Euler equation, we will first perform a change of variables. Let \(x = \ln{t}\) and \(y(t) = z(x)\). Therefore, \(t = e^x\). Now, we need to find expressions for \(y'\) and \(y''\) in terms of \(z\) and its derivatives.
02

Find \(y'\) and \(y''\) in terms of \(z'\) and \(z''\)

Differentiating \(y(t) = z(x)\) with respect to \(t\), we get: \(y' = \dfrac{dz}{dx}\cdot\dfrac{dx}{dt} = z'(x) \cdot \frac{1}{t}\) And differentiating again with respect to \(t\) gives us: \(y'' = \dfrac{d^2z}{dx^2} \cdot \left(\dfrac{dx}{dt}\right)^2 + \dfrac{dz}{dx}\cdot\dfrac{d^2x}{dt^2} = \frac{z''(x)}{t^2}-\frac{z'(x)}{t^2}\) Now, substitute these expressions for \(y'\) and \(y''\) back into the given Euler equation.
03

Plug \(y'\) and \(y''\) back into the Euler equation and simplify

Substituting the expressions for \(y'\) and \(y''\) into the Euler equation, we get: \(t^2\left(\frac{z''(x)}{t^2}-\frac{z'(x)}{t^2}\right) - 2t \left(z'(x) \cdot \frac{1}{t}\right) + 2z(x) = 0\) This simplifies to: \(z''(x) - z'(x) - 2z'(x) + 2z(x) = 0\) Now, we have an equation involving only derivatives of \(z(x)\), which is simpler to solve.
04

Solve the second-order linear homogeneous equation for \(z(x)\)

The equation we obtained is a second-order linear homogeneous equation with constant coefficients: \(z''(x) - 3z'(x) + 2z(x) = 0\) The characteristic equation is: \(r^2 - 3r + 2 = 0\) Factoring the equation, we get: \((r-1)(r-2) = 0\) The roots are \(r_1 = 1\) and \(r_2 = 2\). Therefore, the general solution of this equation is: \(z(x) = c_1 e^{x} + c_2 e^{2x}\)
05

Convert back to the original variables

Now, we must substitute back for \(y(t)\) and \(x = \ln{t}\): \(y(t) = z(x) = c_1 e^{\ln{t}} + c_2 e^{2\ln{t}}\) Simplifying the expression, we get the general solution for the original Euler equation: \(y(t) = c_1 t + c_2 t^2\) Thus, the general solution of the given Euler equation \(t^2y''-2ty'+2y=0\) is \(y(t) = c_1 t + c_2 t^2\), for \(t>0\).

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Key Concepts

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

Second-Order Linear Homogeneous Equation
A second-order linear homogeneous equation is a type of differential equation that involves a second derivative and can be written generally as \( a(t)y'' + b(t)y' + c(t)y = 0 \). These equations are considered linear because they only involve the linear terms of the function \(y\), its derivatives, and the coefficients \(a(t)\), \(b(t)\), and \(c(t)\) are functions of the independent variable. They are homogeneous because the equation is set to zero.
This concept is significant in the study of differential equations as it allows the use of characteristic equations to determine the solutions. In the specific Euler equation provided, you're tasked with finding solutions to \( t^2 y'' - 2t y' + 2y = 0 \). This form, typical of Euler equations, contains coefficients that are powers of the independent variable, here \(t\), which requires specialized techniques to solve.
Characteristic Equation
The characteristic equation is a tool used to solve second-order linear homogeneous equations, particularly those with constant coefficients. It is formed by substituting an assumed solution of the form \(y = e^{rt}\) into the differential equation and solving for \(r\).
In our problem, once we express the Euler equation through a change of variables, it simplifies to \( z''(x) - 3z'(x) + 2z(x) = 0 \). The corresponding characteristic equation is \( r^2 - 3r + 2 = 0 \). After solving, we find the roots \( r_1 = 1 \) and \( r_2 = 2 \). These roots indicate the form of the solution to the differential equation. The solutions are used to construct the general solution, which involves a linear combination of terms like \( e^{r_1x} \) and \( e^{r_2x} \).
Change of Variables
Changing variables is a technique used to simplify differential equations by substituting one set of variables for another. In the context of the Euler equation, the substitution \(x = \ln{t}\) transforms the problem into one with constant coefficients. This transformation is particularly useful because it takes advantage of the properties of exponential functions in differential equations.
In this exercise, let \(y(t) = z(x)\), and through differentiation, find the expressions of \( y' \) and \( y'' \) in terms of \( z' \) and \( z'' \). This substitution simplifies the Euler equation to a manageable form, allowing for the application of methods for equations with constant coefficients. It's a clever mathematical maneuver that greatly simplifies solving Euler-type differential equations.
General Solution
The general solution of a differential equation represents a family of all possible solutions that satisfy the equation. For second-order linear homogeneous equations, it typically involves two arbitrary constants, reflecting the degree of the equation.
In this example, after using the characteristic equation, the general solution in terms of \(z(x)\) was found to be \( z(x) = c_1 e^{x} + c_2 e^{2x} \). Changing back to the original variables provides the solution in terms of \(t\), giving \( y(t) = c_1 t + c_2 t^2 \).
This form indicates all possible solutions depending on the initial conditions or boundary values. It shows how the function can be expressed as a combination of these independent solutions weighted by \(c_1\) and \(c_2\), providing deep insights into the nature of the solution.

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Most popular questions from this chapter

In each exercise, (a) Show that the given two-point boundary value problem has a unique solution. (b) Solve the problem. Note that a fundamental matrix for \(\mathbf{y}^{\prime}=\left[\begin{array}{rr}1 & -2 \\ -2 & 1\end{array}\right] \mathbf{y}\) is $$ \Psi(t)=\left[\begin{array}{cc} e^{-t} & e^{3 t} \\ e^{-t} & -e^{3 t} \end{array}\right] $$ $$ \mathbf{y}^{r}=\left[\begin{array}{rr} 1 & -2 \\ -2 & 1 \end{array}\right] \mathbf{y}, \quad y_{1}(0)=1, \quad y_{2}(1)=0 $$

In each exercise, you are given boundary conditions for the two-point boundary value problem $$ \begin{aligned} &\mathbf{y}^{r}=A \mathbf{y}+\mathbf{g}(t), \quad 0

The unique solution of the boundary value problem $$ \begin{aligned} &y^{\prime \prime}+y=1 \\ &y(0)+a_{1} y^{\prime}(0)=5, \quad y(\pi / 2)+y^{\prime}(\pi / 2)=\beta \end{aligned} $$ is shown in the figure. Find the integer constants \(a_{1}\) and \(\beta\).

In each exercise, the unique solution of the boundary value problem is given. Determine the constants \(\alpha, \beta\), and \(\gamma\). $$ y^{\prime \prime}+\gamma y=2 e^{t}, \quad y(0)=\alpha, \quad y\left(\frac{\pi}{2}\right)=\beta . \quad \text { The solution is } y(t)=e^{t}+\sin t $$

These exercises explore some additional aspects of the radiative transport model presented in Section 11.1. Suppose we modify the radiative transport model solved in Example 4 to allow for a partial reflection of energy at the slab edge at \(x=l\). A portion of the energy arriving at \(x=l\) from within the slab is reflected backwards, while the rest exits the slab. To model this phenomenon, we adopt the boundary condition $$ I^{(-)}(l)=\Gamma I^{(+)}(l), $$ where \(\Gamma\), a positive constant satisfying \(0 \leq \Gamma \leq 1\), is often called a reflection coefficient. (Note that \(\Gamma=0\) is the case solved in Example 4, while the other extreme, \(\Gamma=1\), corresponds to placing a reflecting wall at \(x=l\).) The new boundary value problem becomes $$ \begin{aligned} &\frac{d}{d x}\left[\begin{array}{l} I^{(+)} \\ I^{(-)} \end{array}\right]=\beta\left[\begin{array}{ll} -1 & 1 \\ -1 & 1 \end{array}\right]\left[\begin{array}{l} I^{(+)} \\ I^{(-)} \end{array}\right], \quad 0

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