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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. $$y^{\prime \prime}-4 x y^{\prime}+\left(4 x^{2}-2\right) y=0$$

Short Answer

Expert verified
Assume a series solution, derive the recurrence relation, then solve the differential equation by an elementary method and compare both solutions.

Step by step solution

01

- Assume Series Solution

Assume a solution of the form \[ y = \sum_{n=0}^{\infty} a_n x^n \]
02

- Find First and Second Derivatives

Calculate \[ y' = \sum_{n=1}^{\infty} a_n n x^{n-1} \]and \[ y'' = \sum_{n=2}^{\infty} a_n n (n-1) x^{n-2} \].
03

- Substitute into ODE

Substitute the series forms of \( y \), \( y' \), and \( y'' \) into the differential equation \[ y'' - 4xy' + (4x^2 - 2)y = 0 \].
04

- Equate Coefficients

Combine and compare coefficients of like powers of \( x \) to obtain a recurrence relation for the coefficients \( a_n \). Solve the recurrence relation to determine the series terms.
05

- Find Elementary Solution

Solve the differential equation using an elementary method, such as the method of undetermined coefficients or variation of parameters.
06

- Compare Solutions

Compare the solution obtained from the series method with the one obtained from the elementary method to verify that they match.
07

- Verification by Computer

Using a mathematical software or computer algebra system (like WolframAlpha, MATLAB, or Mathematica), check if both solutions satisfy the original differential equation.

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Key Concepts

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

Ordinary Differential Equations
Ordinary Differential Equations (ODEs) are equations involving a function and its derivatives. In our exercise, the ODE given is of the second order, as it involves the second derivative of the function y(x). The general form of a second-order ODE is typically written as: f(x, y, y', y'') = 0.
A common example is Newton's second law of motion. Solving an ODE means finding a function y(x) that satisfies the equation within a certain domain. Methods like separation of variables, integrating factors, or using power series can help find solutions.
Power Series
A power series is a series of the form: y = Σ n=0^ ∞. a_.n x^.n
In step 1 of our solution, we assume y(x) can be expressed as a power series. This helps us convert the differential equation into an algebraic form. We calculate the derivatives, which simplifies substitution back into the original ODE. By comparing the coefficients of different powers of x, we get a recurrence relation to find the coefficients a_.n_.
Power series expansions are powerful tools for approximating solutions near a point.
Recurrence Relation
A recurrence relation is an equation that defines a sequence based on previous terms. In our problem, after substituting the power series into the ODE (Step 3), we compare the coefficients of like powers of x. This gives us a recurrence relation for the coefficients a_.n: a_.n = n(n-1) a_n - 4 n x^(n-1) a_n + (4 x^2 - 2) a_n = 0.
Solving this recurrence helps us find the coefficients needed to build the power series solution for y(x). Recurrence relations are essential for understanding the structure of solutions.
Elementary Methods of Solving Differential Equations
Elementary methods for solving differential equations include techniques like separation of variables, integrating factors, undetermined coefficients, and variation of parameters. In step 5, we use such an elementary method to solve our ODE.
For instance, the method of undetermined coefficients involves guessing a solution form and determining the coefficients that satisfy the ODE.
By solving with an elementary method and comparing it to the series solution, we ensure our solutions are correct and confirm our understanding of both approaches.
These methods are useful in solving differential equations analytically, providing clear insights into the behavior of the system.

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Most popular questions from this chapter

Solve the following differential equations by the method of Frobenius (generalized power series). Remember that the point of doing these problems is to learn about the method (which we will use later), not just to find a solution. You may recognize some series [as we did in (11.6)] or you can check your series by expanding a computer answer. $$2 x y^{\prime \prime}-y^{\prime}+2 y=0$$

Consider each of the following problems as illustrations showing that, in a power series solution, we must be cautious about using the general recursion relation between the coefficients for the first few terms of the series. Solve \(y^{\prime \prime}+y^{\prime} / x^{2}=0\) by power series to find the relation $$a_{n+1}=-\frac{n(n-1)}{n+1} a_{n}.$$ If, without thinking carefully, we test the series \(\sum_{n=0}^{\infty} a_{n} x^{n}\) for convergence by the ratio test, we find $$\lim _{n \rightarrow \infty} \frac{\left|a_{n+1} x^{n+1}\right|}{\left|a_{n} x^{n}\right|}=\infty\quad (Show this.)$$ Thus we might conclude that the series diverges and that there is no power series solution of this equation. Show why this is wrong, and that the power series solution is \(y=\) const.

(a) The generating function for Bessel functions of integral order \(p=n\) is $$ \Phi(x, h)=e^{(1 / 2) x\left(h-h^{-1}\right)}=\sum_{n=-\infty}^{\infty} h^{n} J_{n}(x) $$ By expanding the exponential in powers of \(x\left(h-h^{-1}\right)\) show that the \(n=0\) term is \(J_{0}(x)\) as claimed. (b) Show that $$ x^{2} \frac{\partial^{2} \Phi}{\partial x^{2}}+x \frac{\partial \Phi}{\partial x}+x^{2} \Phi-\left(h \frac{\partial}{\partial h}\right)^{2} \Phi=0 $$ Use this result and \(\Phi(x, h)=\sum_{n=-\infty}^{\infty} h^{n} J_{n}(x)\) to show that the functions \(J_{n}(x)\) satisfy Bessel's equation. By considering the terms in \(h^{n}\) in the expansion of \(e^{(1 / 2) x\left(h-h^{-1}\right)}\) in part (a), show that the coefficient of \(h^{n}\) is a series starting with the term \((1 / n !)(x / 2)^{n}\). (You have then proved that the functions called \(J_{n}(x)\) in the expansion of \(\Phi(x, h)\) are indeed the Bessel functions of integral order previously defined by (12.9) and (13.1) with \(p=n\).)

(a) Make the change of variables \(z=e^{x}\) in the differential equation \(y^{\prime \prime}+e^{2 x} y=0\) and so find a solution of the differential equation in terms of Bessel functions. (b) Make the change of variables \(z=e^{x^{2} / 2}\) in the differential equation \(x y^{\prime \prime}-y^{\prime}+\) \(x^{3}\left(e^{x^{2}}-p^{2}\right) y=0,\) and solve the equation in terms of Bessel functions.

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. $$x^{2} y^{\prime \prime}-3 x y^{\prime}+3 y=0$$

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