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Use the method of Problem 11 to transform the given equation into the form \(\left[p(x) y^{\prime}\right]'+q(x) y=0\) $$ \left(1-x^{2}\right) y^{\prime \prime}-x y^{\prime}+\alpha^{2} y=0, \quad \text { Chebyshev equation } $$

Short Answer

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Question: Transform the given Chebyshev equation into the form \((p(x)y^{'})'+q(x)y=0\): Given equation: \(\left(1-x^{2}\right) y^{\prime \prime}-x y^{\prime}+\alpha^{2} y=0\) Answer: The transformed equation is \([(1-x^{2})y''] + [(-2x-x)y'] + \alpha^{2}y = 0\), with \(p(x) = 1-x^2\) and \(q(x) = \alpha^2\).

Step by step solution

01

Finding \(p(x)\) and \(q(x)\)

In our given equation, \(p(x) = 1-x^2\) and \(q(x) = \alpha^2\). Now we need to find expressions for \(y'\) and \(y''\).
02

Differentiating \(p(x)y'\)

To find the expression for \((p(x) y^{'})'\), we need to differentiate \(p(x)y'\) with respect to \(x\): $$ \frac{d}{dx}(p(x)y') = \frac{d}{dx}((1-x^2)y') $$
03

Applying Product Rule of Differentiation

Using the product rule of differentiation, \(\frac{d}{dx}(fg) = f'g+fg'\), we differentiate \((1-x^2)y'\): $$ \frac{d}{dx}((1-x^2)y') = (-2x)y' + (1-x^2)y'' $$ Now, the given equation can be reformulated using the expression found in Step 3:
04

Rearrange the Equation

Substitute the expression from Step 3 into the Chebyshev equation: $$ (-2x)y' + (1-x^2)y'' - xy' + \alpha^2y = 0 $$ Now collect terms with \(y'\) and \(y\): $$ [(1-x^{2})y''] + [(-2x-x)y'] + \alpha^{2}y = 0 $$ We have now transformed the given Chebyshev equation into the desired form: $$ \left[p(x) y^{\prime}\right]'+q(x) y=0 $$ With \(p(x) = 1-x^2\), and \(q(x) = \alpha^2\).

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Key Concepts

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

Differential Equations
Differential equations are mathematical equations that describe the relationship between a function and its derivatives. They are crucial in modeling the behavior of various physical systems, such as the motion of celestial bodies, the flow of fluids, and electrical circuits.

At their core, differential equations express how a quantity changes as it depends on other quantities. For example, the rate at which a population grows may be dependent on its current size, or the speed of a car might depend on the force applied to it and the resistance it encounters.

The Chebyshev equation, \( (1-x^{2}) y^{\'\'} - x y^{\'\text{ }}+ \text{ }\alpha^{2} y=0 \) is a specific type of differential equation with significant applications in mathematical physics and engineering. In this context, the exercise focuses on transforming the Chebyshev equation into a more general form that is easier to analyze and solve.
Boundary Value Problems
Boundary value problems (BVPs) are a class of differential equations where the solution is determined not just by the equation itself but also by conditions, known as boundary conditions, that are applied to the boundaries of the domain in which the solution is sought.

These problems arise naturally in many practical contexts—thermal conduction, wave mechanics, and static potentials, to name a few. Solving a BVP involves determining a function that satisfies not only the differential equation but also meets predefined criteria at the boundaries of the domain.

The Chebyshev equation from our exercise could lead into such a boundary value problem, depending on the conditions applied at the endpoints of an interval. These conditions often reflect physical constraints or symmetry properties in the system being modeled.
Product Rule of Differentiation
The product rule of differentiation is a fundamental calculus technique used to find the derivative of the product of two functions. It can be expressed as \( (fg)^\text{'} = f^\text{'}g + fg^\text{'} \), where \( f \) and \( g \) are functions of \( x \) and \( f^\text{'} \) and \( g^\text{'} \) are their respective derivatives.

This rule is essential when dealing with compound expressions in differential equations, where a function and its derivative are multiplied together. In the case of the Chebyshev equation exercise, the rule is applied to differentiate the term \( (1-x^2)y^\text{'} \) properly, resulting in the correct transformation of the equation into a standard form from which solutions can be more readily obtained.

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Most popular questions from this chapter

Solve the given problem by means of an eigenfunction expansion. $$ y^{\prime \prime}+2 y=-x, \quad y^{\prime}(0)=0, \quad y^{\prime}(1)+y(1)=0 ; \quad \text { see Section } 11.2, \text { Problem } 11 $$

The differential equations in Problems 19 and 20 differ from those in previous problems in that the parameter \(\lambda\) multiplies the \(y^{\prime}\) term as well as the \(y\) term. In each of these problems determine the real eigenvalues and the corresponding eigenfunctions. $$ \begin{array}{l}{y^{\prime \prime}+y^{\prime}+\lambda\left(y^{\prime}+y\right)=0} \\ {y^{\prime}(0)=0, \quad y(1)=0}\end{array} $$

Let \(L\) be a second order linear differential operator. Show that the solution \(y=\phi(x)\) of the problem $$ \begin{array}{c}{L[y]=f(x)} \\ {a_{1} y(0)+a_{2} y^{\prime}(0)=\alpha, \quad b_{1} y(1)+b_{2} y^{\prime}(1)=\beta}\end{array} $$ can be written as \(y=u+v,\) where \(u=\phi_{1}(x)\) and \(v=\phi_{2}(x)\) are solutions of the problems $$ \begin{aligned} L[u]=0 & \\ a_{1} u(0)+a_{2} u^{\prime}(0)=\alpha, & b_{1} u(1)+b_{2} u^{\prime}(1)=\beta \end{aligned} $$ and $$ \begin{aligned} L_{L}[v] &=f(x) \\ a_{1} v(0)+a_{2} v^{\prime}(0) &=0, \quad b_{1} v(1)+b_{2} v^{\prime}(1)=0 \end{aligned} $$ respectively.

In this problem we consider a higher order eigenvalue problem. In the study of transverse vibrations of a uniform elastic bar one is led to the differential equation $$ y^{\mathrm{w}}-\lambda y=0 $$ $$ \begin{array}{l}{\text { where } y \text { is the transverse displacement and } \lambda=m \omega^{2} / E I ; m \text { is the mass per unit length of }} \\\ {\text { the rod, } E \text { is Young's modulus, } I \text { is the moment of inertia of the cross section about an }} \\ {\text { axis through the centroid perpendicular to the plane of vibration, and } \omega \text { is the frequency of }} \\ {\text { vibration. Thus for a bar whose material and geometric properties are given, the eigenvalues }} \\ {\text { determine the natural frequencies of vibration. Boundary conditions at each end are usually }} \\ {\text { one of the following types: }}\end{array} $$ $$ \begin{aligned} y=y^{\prime} &=0, \quad \text { clamped end } \\ y=y^{\prime \prime} &=0, \quad \text { simply supported or hinged end, } \\ y^{\prime \prime}=y^{\prime \prime \prime} &=0, \quad \text { free end } \end{aligned} $$ $$ \begin{array}{l}{\text { For each of the following three cases find the form of the eigenfunctions and the equation }} \\ {\text { satisfied by the eigenvalues of this fourth order boundary value problem. Determine } \lambda_{1} \text { and }} \\ {\lambda_{2}, \text { the two eigenvalues of smallest magnitude. Assume that the eigenvalues are real and }} \\ {\text { positive. }}\end{array} $$ $$ \begin{array}{ll}{\text { (a) } y(0)=y^{\prime \prime}(0)=0,} & {y(L)=y^{\prime \prime}(L)=0} \\ {\text { (b) } y(0)=y^{\prime \prime}(0)=0,} & {y(L)=y^{\prime \prime}(L)=0} \\ {\text { (c) } y(0)=y^{\prime}(0)=0,} & {y^{\prime \prime}(L)=y^{\prime \prime \prime}(L)=0 \quad \text { (cantilevered bar) }}\end{array} $$

Use the method of Problem 11 to transform the given equation into the form \(\left[p(x) y^{\prime}\right]'+q(x) y=0\) $$ x^{2} y^{\prime \prime}+x y^{\prime}+\left(x^{2}-v^{2}\right) y=0, \quad \text { Bessel equation } $$

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