Question #50743

Solve the following ODE using the power series method: (1 - X^2) y" - 2xy' + 2 y = 0

Expert's answer

Answer on Question #50743 – Math – Differential Calculus | Equations

Solve the following ODE using the power series method:


(1X2)y2xy+2y=0(1 - X ^ {\wedge} 2) y'' - 2 x y' + 2 y = 0

Solution

Ordinary differential equation


(1x2)y2xy+2y=0(1 - x^2) y'' - 2 x y' + 2 y = 0


is equivalent to


y2x1x2y+21x2y=0.y'' - \frac{2x}{1 - x^2} y' + \frac{2}{1 - x^2} y = 0.


Let


y=n=0anxn=a0+a1x+a2x2+a3x3+,y=n=1nanxn1,y=n=2n(n1)anxn2y = \sum_{n=0}^{\infty} a_n x^n = a_0 + a_1 x + a_2 x^2 + a_3 x^3 + \cdots, \quad y' = \sum_{n=1}^{\infty} n a_n x^{n-1}, \quad y'' = \sum_{n=2}^{\infty} n(n-1) a_n x^{n-2}


Substitute x=0x = 0 into y=n=0anxny = \sum_{n=0}^{\infty} a_n x^n, which results in y(0)=a0=0y(0) = a_0 = 0.

Substitute x=0x = 0 into y=n=1nanxn1y = \sum_{n=1}^{\infty} n a_n x^{n-1}, which results in y(0)=a1=1y'(0) = a_1 = 1.

We are searching for two linearly independent solutions of differential equation, so let the first one be such that y(0)=0,y(0)=1y(0) = 0, y'(0) = 1, hence a0=0a_0 = 0, a1=1a_1 = 1.

Substitute y=n=0anxny = \sum_{n=0}^{\infty} a_n x^n, y=n=1nanxn1y' = \sum_{n=1}^{\infty} n a_n x^{n-1}, y=n=2n(n1)anxn2y'' = \sum_{n=2}^{\infty} n(n-1) a_n x^{n-2}, into initial differential equation (1x2)y2xy+2y=0(1 - x^2) y'' - 2 x y' + 2 y = 0, which results in


n=2n(n1)anxn2n=2n(n1)anxn2n=1nanxn+2n=0anxn=0\sum_{n=2}^{\infty} n(n-1) a_n x^{n-2} - \sum_{n=2}^{\infty} n(n-1) a_n x^n - 2 \sum_{n=1}^{\infty} n a_n x^n + 2 \sum_{n=0}^{\infty} a_n x^n = 0n=0(n+1)(n+2)an+2xnn=2n(n1)anxn2n=1nanxn+2n=0anxn=0\sum_{n=0}^{\infty} (n + 1)(n + 2)a_{n+2}x^n - \sum_{n=2}^{\infty} n(n - 1)a_nx^n - 2\sum_{n=1}^{\infty} na_nx^n + 2\sum_{n=0}^{\infty} a_nx^n = 0n=2[(n+1)(n+2)an+2n(n1)an2nan+2an]xn+2a2+6a3x2a1x+2a0+2a1x=0\sum_{n=2}^{\infty} [(n + 1)(n + 2)a_{n+2} - n(n - 1)a_n - 2na_n + 2a_n]x^n + 2a_2 + 6a_3x - 2a_1x + 2a_0 + 2a_1x = 0n=2[(n+1)(n+2)an+2n(n1)an2nan+2an]xn+2a2+6a3x+2a0=0\sum_{n=2}^{\infty} [(n + 1)(n + 2)a_{n+2} - n(n - 1)a_n - 2na_n + 2a_n]x^n + 2a_2 + 6a_3x + 2a_0 = 0


Plug x=0x = 0 and a0=0a_0 = 0 into the last equation, obtain a2=0a_2 = 0. Rewrite the series as


n=2[(n+1)(n+2)an+2n(n1)an2nan+2an]xn+6a3x=0\sum_{n=2}^{\infty} [(n + 1)(n + 2)a_{n+2} - n(n - 1)a_n - 2na_n + 2a_n]x^n + 6a_3x = 0


Divide both sides by x0x \neq 0 and obtain


n=2[(n+1)(n+2)an+2n(n1)an2nan+2an]xn1+6a3=0\sum_{n=2}^{\infty} [(n + 1)(n + 2)a_{n+2} - n(n - 1)a_n - 2na_n + 2a_n]x^{n-1} + 6a_3 = 0


Plug x=0x = 0 into the last equation, obtain 6a3=06a_3 = 0, hence a3=0a_3 = 0.

Thus we have a1=1a_1 = 1, a0=a2=a3=0a_0 = a_2 = a_3 = 0.

Rewrite the series as


n=2[(n+1)(n+2)an+2n(n1)an2nan+2an]xn1=0.\sum_{n=2}^{\infty} [(n + 1)(n + 2)a_{n+2} - n(n - 1)a_n - 2na_n + 2a_n]x^{n-1} = 0.


A power series is identically equal to zero if and only if all of its coefficients are equal to zero.

Hence


(n+1)(n+2)an+2n(n1)an2nan+2an=0an+2=n2+n2(n+1)(n+2)an=n1n+1an\begin{array}{l} (n + 1)(n + 2) a_{n+2} - n(n - 1) a_n - 2 n a_n + 2 a_n = 0 \rightarrow \\ \rightarrow \quad a_{n+2} = \frac{n^2 + n - 2}{(n + 1)(n + 2)} a_n = \frac{n - 1}{n + 1} a_n \end{array}


Read the recurrence relation for the case n=0n = 0: a2=a0a_2 = -a_0. Reading off the recurrence relation for n=1n = 1 yields a3=0a_3 = 0.

Notice that because a2=a3=0a_2 = a_3 = 0, all rest coefficients must be zero. Therefore the first linear independent solution is y=xy = x.

Points x=1x = 1 and x=1x = -1 are singular points of equation


y2x1x2y+21x2y=0.y'' - \frac{2x}{1 - x^2} y' + \frac{2}{1 - x^2} y = 0.


The first linearly independent solution is found.

To obtain the second linearly independent solution, the next formula is used:


F=f1f2dx=2x1x2dx=d(1x2)1x2dx=ln1x2,F = \int \frac{f_1}{f_2} dx = \int \frac{-2x}{1 - x^2} dx = \int \frac{d(1 - x^2)}{1 - x^2} dx = \ln |1 - x^2|,


general solution can be represented as


y=y1(C1+C2eFy12dx)=x(C1+C2eln1x2x2dx),y = y_1 \left(C_1 + C_2 \int \frac{e^{-F}}{y_1^2} dx\right) = x \left(C_1 + C_2 \int \frac{e^{-ln|1 - x^2|}}{x^2} dx\right),


where C1C_1 and C2C_2 are arbitrary real constants.

Let 1<x<1-1 < x < 1, then


y=y1(C1+C2eFy12dx)=x(C1+C2eln(1x2)x2dx)=y = y_1 \left(C_1 + C_2 \int \frac{e^{-F}}{y_1^2} dx\right) = x \left(C_1 + C_2 \int \frac{e^{-ln(1 - x^2)}}{x^2} dx\right) ==x(C1+C2dx(1x2)x2)=x(C1C2dx(x21)x2)=x(C1C2(1x211x2)dx)=x(C1C2(12lnx1x+1+1x))=x(C1C2(lnx1x+1+1x))\begin{array}{l} = x \left(C _ {1} + C _ {2} \int \frac {d x}{(1 - x ^ {2}) x ^ {2}}\right) = x \left(C _ {1} - C _ {2} \int \frac {d x}{(x ^ {2} - 1) x ^ {2}}\right) \\ = x \left(C _ {1} - C _ {2} \int \left(\frac {1}{x ^ {2} - 1} - \frac {1}{x ^ {2}}\right) d x\right) \\ = x \left(C _ {1} - C _ {2} \left(\frac {1}{2} \ln \left| \frac {x - 1}{x + 1} \right| + \frac {1}{x}\right)\right) \\ = x \left(C _ {1} - C _ {2} \left(\ln \sqrt {\left| \frac {x - 1}{x + 1} \right|} + \frac {1}{x}\right)\right) \\ \end{array}


Other method is to search for the second linearly independent solution in the form


y=n=0anxn+r.y = \sum_ {n = 0} ^ {\infty} a _ {n} x ^ {n + r}.


www.AssignmentExpert.com


Need a fast expert's response?

Submit order

and get a quick answer at the best price

for any assignment or question with DETAILED EXPLANATIONS!

LATEST TUTORIALS
APPROVED BY CLIENTS