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Determine the general solution of the given differential equation that is valid in any interval not including the singular point. \((x-1)^{2} y^{\prime \prime}+8(x-1) y^{\prime}+12 y=0\)

Short Answer

Expert verified
Answer: The general solution is \(y(x)= C_1 e^{r_1 (x - 1)} + C_2 e^{r_2 (x - 1)}\), where \(r_1\) and \(r_2\) are the roots of the characteristic equation.

Step by step solution

01

Perform substitution

Replace \(x-1\) with \(t\). So we have, \(t^{2} y^{\prime \prime}+8t y^{\prime}+12 y=0\).
02

Write the characteristic equation

Convert the given second-order linear differential equation to its corresponding characteristic equation. This is done by replacing \(y^{\prime \prime}\) with \(r^2\), \(y^{\prime}\) with \(r\), and \(y\) with 1 in the original differential equation to obtain: \(t^2r^2 + 8tr + 12 = 0\).
03

Solve for r

To find the roots of the characteristic equation, we first divide the equation by \(t^2\) to give: \(r^2 + 8r + \frac{12}{t^2} = 0\). Now, use the quadratic formula to find the roots of the equation: \(r = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}\), where \(a=1\), \(b = 8\), and \(c = \frac{12}{t^2}\). So, we have: \(r = \frac{-8 \pm \sqrt{64 - \frac{48}{t^2}}}{2}\).
04

Find the general form of the solution

Since the differential equation has two different real roots, the general form of the solution is: \(y(t)=C_1 e^{r_1 t} + C_2 e^{r_2 t}\), where \(C_1\) and \(C_2\) are constants and \(r_1\) and \(r_2\) are the roots of the characteristic equation.
05

Substitute back to find the solution in terms of x

Recall that we have \(t = x - 1\). So we can write the general form of the solution in terms of x as follows: \(y(x)= C_1 e^{r_1 (x - 1)} + C_2 e^{r_2 (x - 1)}\), where \(r_1\) and \(r_2\) are the roots from Step 3. Thus, the general solution of the given differential equation that is valid in any interval not including the singular point is \(y(x)= C_1 e^{r_1 (x - 1)} + C_2 e^{r_2 (x - 1)}\).

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Key Concepts

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

Second-Order Linear Differential Equation
Understanding the second-order linear differential equation is fundamental for solving many problems in mathematics and physics. These equations are characterized by the highest derivative being second-order and the equation itself being linear in the unknown function and its derivatives.

In the given exercise, we have the second-order linear differential equation \( (x-1)^{2} y''+8(x-1) y'+12 y=0 \). The coefficients of \( y'' \) and \( y' \) are functions of \( x \) and are non-zero when \( x eq 1 \)—making \( x=1 \) a singular point. In intervals where \( x eq 1 \) the equation can be tackled effectively by simplification techniques such as substitution, which help transform it into a more standard form where known solution methods can be applied.
Characteristic Equation
The characteristic equation is a key aspect of solving linear differential equations with constant coefficients. It is an algebraic equation obtained by substituting the unknown function with an exponential trial solution.

In our exercise, once we perform the substitution suggested in the step-by-step solution (\( x-1 \) with \( t \)), we replace \( y'' \) with \( r^2 \) and \( y' \) with \( r \) for the corresponding characteristic equation: \(t^2r^2 + 8tr + 12 = 0\). This transformation paves the way for determining the roots which in turn define the general solution of the differential equation.
Roots of Characteristic Equation
Finding the roots of the characteristic equation is a pivotal step in solving second-order linear differential equations. These roots indicate the nature of the solutions to the differential equation. They can be real and distinct, real and repeated, or complex conjugates.

In our example, after simplifying the characteristic equation, the quadratic formula is used to find the roots \( r \). The solutions \( r_1 \) and \( r_2 \) are then used to construct the general solution of the original differential equation. The quadratic equation's discriminant (\( b^2 - 4ac \) in the quadratic formula) determines if the roots are real and distinct, or if they are complex.
Singular Points in Differential Equations
Singular points, or singularities, in differential equations are values of the independent variable at which the coefficients of the highest derivatives become either zero or undefined, leading to complications in finding a solution.

Our exercise highlights the singular point at \( x=1 \) because the coefficient \( (x-1)^2 \) of \( y'' \) would be zero, which invalidates the standard form of a second-order linear differential equation. It is crucial to exclude such singular points from the interval of solution as they are points where the behavior of the solution may change fundamentally. Near singular points, special techniques or a separate analysis may be needed to understand the solutions.

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Most popular questions from this chapter

Show that $$ (\ln x) y^{\prime \prime}+\frac{1}{2} y^{\prime}+y=0 $$ has a regular singular point at \(x=1 .\) Determine the roots of the indicial equation at \(x=1\) Determine the first three nonzero terms in the series \(\sum_{n=0}^{\infty} a_{n}(x-1)^{r+n}\) corresponding to the larger root. Take \(x-1>0 .\) What would you expect the radius of convergence of the series to be?

The Chebyshev equation is $$ \left(1-x^{2}\right) y^{\prime \prime}-x y^{\prime}+\alpha^{2} y=0 $$ where \(\alpha\) is a constant; see Problem 10 of Section 5.3 . (a) Show that \(x=1\) and \(x=-1\) are regular singular points, and find the exponents at each of these singularities. (b) Find two linearly independent solutions about \(x=1\)

In several problems in mathematical physics (for example, the Schrödinger equation for a hydrogen atom) it is necessary to study the differential equation $$ x(1-x) y^{\prime \prime}+[\gamma-(1+\alpha+\beta) x] y^{\prime}-\alpha \beta y=0 $$ where \(\alpha, \beta,\) and \(\gamma\) are constants. This equation is known as the hypergeometric equation. (a) Show that \(x=0\) is a regular singular point, and that the roots of the indicial equation are 0 and \(1-\gamma\). (b) Show that \(x=1\) is a regular singular point, and that the roots of the indicial equation are 0 and \(\gamma-\alpha-\beta .\) (c) Assuming that \(1-\gamma\) is not a positive integer, show that in the neighborhood of \(x=0\) one solution of (i) is $$ y_{1}(x)=1+\frac{\alpha \beta}{\gamma \cdot 1 !} x+\frac{\alpha(\alpha+1) \beta(\beta+1)}{\gamma(\gamma+1) 2 !} x^{2}+\cdots $$ What would you expect the radius of convergence of this series to be? (d) Assuming that \(1-\gamma\) is not an integer or zero, show that a second solution for \(0

Find all the regular singular points of the given differential equation. Determine the indicial equation and the exponents at the singularity for each regular singular point. \(x^{2} y^{\prime \prime}+3(\sin x) y^{\prime}-2 y=0\)

First Order Equations. The series methods discussed in this section are directly applicable to the first order linear differential equation \(P(x) y^{\prime}+Q(x) y=0\) at a point \(x_{0}\), if the function \(p=Q / P\) has a Taylor series expansion about that point. Such a point is called an ordinary point, and further, the radius of convergence of the series \(y=\sum_{n=0}^{\infty} a_{n}\left(x-x_{0}\right)^{n}\) is at least as large as the radius of convergence of the series for \(Q / P .\) In each of Problems 16 through 21 solve the given differential equation by a series in powers of \(x\) and verify that \(a_{0}\) is arbitrary in each case. Problems 20 and 21 involve nonhomogeneous differential equations to which series methods can be easily extended. Where possible, compare the series solution with the solution obtained by using the methods of Chapter 2 . $$ y^{\prime}-x y=0 $$

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