| d²y | + P | dy | + Qy = R, |
| dx² | dx |
where P, Q, R are functions of x only. There is no method always effective; the main general result for such a linear equation is that if any particular function of x, say y1, can be discovered, for which
| d²y1 | + P | dy1 | + Qy1 = 0, |
| dx² | dx |
then the substitution y = y1η in the original equation, with R on the right side, reduces this to a linear equation of the first order with the dependent variable dη/dx. In fact, if y = y1η we have
| dy | = y1 | dη | + η | dy1 | and | d²y | = y1 | d²η | + 2 | dy1 | dη | + η | d²y1 | , |
| dx | dx | dx | dx² | dx² | dx | dx | dx² |
and thus
| d²y | + P | dy | + Qy = y1 | d²η | + (2 | dy1 | + Py1) | dη | + ( | d²y1 | + P | dy1 | + Qy1)η; | |
| dx² | dx | dx² | dx | dx | dx² | dx |
if then
| d²y1 | + P | dy1 | + Qy1 = 0, |
| dx² | dx |
and z denote dη/dx, the original differential equation becomes