Solve the differential equations by the Frobenius method; observe that you get only one solution. (Note, also, that the two values of \(s\) are equal or differ by an integer, and in the latter case the larger \(s\) gives the one solution.) Show that the conditions of Fuchs's theorem are satisfied. Knowing that the second solution is \(\ln x\) times the solution you have, plus another Frobenius series, find the second solution. $$4 x^{2}(x+1) y^{\prime \prime}-4 x^{2} y^{\prime}+(3 x+1) y=0$$

Short Answer

Expert verified
The general solution is given by \ y = C_1 x + C_2 x \text{ln} x.\

Step by step solution

01

Identify the differential equation form

The given differential equation is \[ 4 x^{2}(x+1) y^{\text{{''}}}-4 x^{2} y^{\text{'}}+(3 x+1) y=0.\] Recognize that this is in the form of a second-order linear differential equation.
02

Convert to standard form

Divide the entire differential equation by \(x^2(x+1)\) to achieve: \[ y^{\text{{''}}} - \frac{1}{x+1} y^{\text{'}} + \frac{(3x + 1)}{4x^2(x+1)} y=0.\]
03

Find the Indicial Equation

Assume a solution of the form \[ y = x^{s} \] and substitute it into the differential equation. This process helps to find the Indicial equation by looking at the lowest power of \(x\). The terms involving \(s\) give us the indicial equation, which we solve for \(s\).
04

Solve the Indicial Equation

For the indicial equation associated with this differential equation, solve \[ s(s-1) = 0.\] The roots are \( s = 0 \) and \( s = 1 \). Both roots are real and differ by an integer.
05

Verify Fuchs's theorem conditions

Ensure the given differential equation satisfies Fuchs's theorem conditions. Since the differential equation is already in a standard form suitable for Frobenius method, and its coefficients have singularities at the origin, it confirms Fuchs's conditions are satisfied.
06

Determine the general solution for the larger root

Given that the larger root \( s = 1 \) leads to one solution, find \[ y_1 = x. \]In these cases, a second solution typically takes a form involving \(\textrm{ln}(x) \).
07

Find the second solution

Knowing that the second solution takes a form involving \( y_1 = x \), find the second solution as: \[ y_2 = y_1 \text{ln} x + A x = x \text{ln} x.\]

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Key Concepts

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

second-order linear differential equations
Second-order linear differential equations are equations involving a function, its first derivative, and its second derivative. These equations are significant in various fields of science and engineering. The general form looks like this: \[ a(x) y'' + b(x) y' + c(x) y = d(x). \]\Here, the functions \(a(x)\), \(b(x)\), \(c(x)\), and \(d(x)\) can vary, but most commonly, \(d(x) = 0\), making the equation homogeneous. In our example equation is: \[ 4 x^{2}(x+1) y'' - 4 x^{2} y' + (3 x + 1) y = 0. \]To solve these, you typically bring the equation into a standard form by dividing all terms by \(a(x)\). In our case: \[ y'' - \frac{1}{x+1} y' + \frac{3x + 1}{4x^2(x+1)} y = 0. \]\br\ Understanding how to manipulate these coefficients is key to solving and understanding second-order linear differential equations.
indicial equation
The indicial equation arises when we apply the Frobenius method to solve differential equations. This method assumes a power series solution of the form \(y = x^s\).\br\ When we plug this assumed solution into the differential equation, we look at the lowest power of \(x\) to form the indicial equation.\br\ For our example: \[ 4 x^{2}(x+1) y'' - 4 x^{2} y' + (3 x + 1) y = 0, \]\assuming \(y = x^s\), we substitute into the equation and find the indicial equation: \[ s(s-1) = 0. \]\br\ This gives the roots \( s = 0 \) and \( s = 1 \). Both roots are real and differ by an integer, so only one solution initially emerges.
Fuchs's theorem
Fuchs's theorem is essential in understanding the solutions of differential equations around singular points. It states that if a point is a regular singular point of a second-order linear differential equation, then you can use techniques like the Frobenius method to find solutions.\br\ Conditions of Fuchs's theorem include: \[ a(x), \]\br\ is a standard form where \(a(x) e 0\) but it must be expandable into a Laurent series around the singular point \(x = 0\).\br\ In our example: \[ 4 x^{2}(x + 1) y'' - 4 x^{2} y' + (3 x + 1) y = 0, \] The singularity is at \( x = 0 \). Because the equation is in Frobenius standard form and the coefficients are expandable as a series, it confirms that conditions of Fuchs's theorem are satisfied. This assures us that a Frobenius series solution is applicable.
series solution
A series solution involves expressing the solution of a differential equation as an infinite sum of terms (usually power series). For the Frobenius method, we assume a solution in the form of: \[ y = x^s \sum_{n=0}^{\infty} a_n x^n, \] where \(a_0 eq 0\).\br\ Substituting this into the differential equation, we equate coefficients of equal powers of \(x\) to solve for \(a_n\) terms.\br\ For our example equation: \[ 4 x^{2}(x+1) y'' - 4 x^{2} y' + (3 x + 1) y = 0, \] we determined the roots \( s = 0 \) and \( s = 1 \).\br\ For \(s = 1\), we get the primary solution \( y_1 = x \).\br\ To find the second solution, knowing it involves \( \text{ln} x \), we get: \[ y_2 = y_1 \text{ln} x + A x = x \text{ln} x. \] Combining these solutions gives us a comprehensive understanding of the behavior around the singularity.

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Most popular questions from this chapter

A straight wire clamped vertically at its lower end stands vertically if it is short, but bends under its own weight if it is long. It can be shown that the greatest length for vertical equilibrium is \(l,\) where \(k l^{3 / 2}\) is the first zero of \(J_{-1 / 3}\) and $$k=\frac{4}{3 r^{2}} \sqrt{\frac{\rho g}{\pi Y}},$$ \(r=\) radius of the wire, \(\rho=\) linear density, \(g=\) acceleration of gravity, \(Y=\) Young's modulus. Find \(l\) for a steel wire of radius \(1 \mathrm{mm}\); for a lead wire of the same radius.

Solve the following differential equations by series and also by an elementary method and verify that your solutions agree. Note that the goal of these problems is not to get the answer (that's easy by computer or by hand) but to become familiar with the method of series solutions which we will be using later. Check your results by computer. $$\left(x^{2}+2 x\right) y^{\prime \prime}-2(x+1) y^{\prime}+2 y=0$$

Prove the least squares approximation property of Legendre polynomials [see (9.5) and (9.6)] as follows. Let \(f(x)\) be the given function to be approximated. Let the functions \(p_{l}(x)\) be the normalized Legendre polynomials, that is, $$p_{l}(x)=\sqrt{\frac{2 l+1}{2}} P_{l}(x) \quad \text { so that } \quad \int_{-1}^{1}\left[p_{l}(x)\right]^{2} d x=1$$ Show that the Legendre series for \(f(x)\) as far as the \(p_{2}(x)\) term is $$f(x)=c_{0} p_{0}(x)+c_{1} p_{1}(x)+c_{2} p_{2}(x) \quad \text { with } \quad c_{l}=\int_{-1}^{1} f(x) p_{l}(x) d x$$ Write the quadratic polynomial satisfying the least squares condition as \(b_{0} p_{0}(x)+\) \(b_{1} p_{1}(x)+b_{2} p_{2}(x)\) (by Problem 5.14 any quadratic polynomial can be written in this form). The problem is to find \(b_{0}, b_{1}, b_{2}\) so that $$I=\int_{-1}^{1}\left[f(x)-\left(b_{0} p_{0}(x)+b_{1} p_{1}(x)+b_{2} p_{2}(x)\right)\right]^{2} d x$$ is a minimum. Square the bracket and write \(I\) as a sum of integrals of the individual terms. Show that some of the integrals are zero by orthogonality, some are 1 because the \(p_{t}\) 's are normalized, and others are equal to the coefficients \(c_{l}\). Add and subtract \(c_{0}^{2}+c_{1}^{2}+c_{2}^{2}\) and show that $$I=\int_{-1}^{1}\left[f^{2}(x)+\left(b_{0}-c_{0}\right)^{2}+\left(b_{1}-c_{1}\right)^{2}+\left(b_{2}-c_{2}\right)^{2}-c_{0}^{2}-c_{1}^{2}-c_{2}^{2}\right] d x$$ Now determine the values of the \(b\) 's to make \(I\) as small as possible. (Hint: The smallest value the square of a real number can have is zero.) Generalize the proof to polynomials of degree \(n\).

Expand the following functions in Legendre series. $$f(x)=\left\\{\begin{array}{rr} -1, & -1

Let \(\alpha\) be the first positive zero of \(J_{1}(x)\) and let \(\beta_{n}\) be the zeros of \(J_{0}(x) .\) In terms of \(\alpha\) and \(\beta_{n},\) find the values of \(x\) at the maximum and minimum points of the function \(y=x J_{1}(\alpha x) .\) By computer or tables, find the needed zeros and compute the coordinates of the maximum and minimum points on the graph of \(y(x)\) for \(x\) between 0 and \(5 .\) Computer plot \(y\) from \(x=0\) to 5 and compare your computed maximum and minimum points with what the plot shows.

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