Reduction of order

#math

$$y''+ p(x)y' + q(x)y = 0 \tag{6}$$

If we know one non-zero solution y1(x) somehow, then we can find the other LI solution y2(x)
that forms a basis.

We assume that y2=v(x)y1, where v(x) is some arbitrary function.
Using the fact that y1 and y2 are solutions of (6), we plug it into the equation, $$y_{1}v'' + (2y_{1}' + py_{1})v' = 0$$
Dividing by y1 and writing v=U, $$U' + \left( \frac{2y_{1}'}{y_{1}} + p\right)U = 0$$
Since this is a linear equation, $$U = \frac{1}{y_{1}^2}e^{-\int pdx}$$and after substituting v=U, $$v = \int \frac{1}{y_{1}^2}e^{-\int pdx}$$
Thus the general solution of (6) can be written as $$y_{i}(x) = Cy_{1}(x) + Dy_{1}(x)\int \frac{1}{y_{1}^2}e^{-\int pdx}$$

Example 8

Solve $$ x y'' + (2x + 1)y' + (x + 1)y = 0$$

Solution

At x=0, the equation becomes singular, so we solve it for x0.
Without loss of generality, assume x>0.
Clearly,$$y_1(x) = e^{-x}$$is a solution.
Divide the entire equation by x:$$y'' + \left(2 + \frac{1}{x}\right)y' + \frac{x+1}{x}y = 0$$
Thus,$$p(x) = 2 + \frac{1}{x}$$
Using reduction of order, let$$y_2(x) = v(x) y_1(x)$$
Then$$v(x) = \int \frac{1}{y_1^2(x)} \exp\left(-\int p(x),dx\right) dx$$
Compute each part:$$y_1^2 = e^{-2x}$$

p(x)dx=(2+1x)dx=2x+lnx

So,$$\exp\left(-\int p(x),dx\right)= \exp(-2x - \ln x) = \frac{e^{-2x}}{x}$$
Therefore, $$v(x) = \int \frac{1}{e^{-2x}} \cdot \frac{e^{-2x}}{x},dx = \int \frac{1}{x},dx = \ln x$$
Hence, $$ y_2(x) = e^{-x} \ln x $$
The general solution (for x>0) is $$ y(x) = e^{-x}\left(C_1 + C_2 \ln x\right) $$

What About x<0?

The correct general antiderivative is $$\int \frac{1}{x},dx = \ln |x|$$
So for x<0, we obtain $$v(x) = \ln |x|$$
and therefore $$ y_2(x) = e^{-x} \ln |x| $$
Thus, for x0, the general solution is $$y(x) = e^{-x}\left(C_1 + C_2 \ln |x|\right)$$
Note: Since x=0 is a singular point, solutions are valid separately on the intervals (,0) and (0,).

How to guess a solution

Consider the homogeneous 2nd order linear differential $$y'' + p(x)y' + q(x)y = 0 \tag{7} $$then,

  1. if m2+mp(x)+q(x)=0 for all x then emx will be a solution of (7)
  2. if m(m1)+mxp(x)+x2q(x)=0 for all x, then xm will be a solution.

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