Given a Second-Order Ordinary Differential Equation
  | 
(1) | 
 
where 
 and 
, the adjoint operator 
 is defined by
Write the two Linearly Independent solutions as 
 and 
.  Then the adjoint
operator can also be written
![\begin{displaymath}
{\tilde {\mathcal L}}^\dagger u = \int (y_2 {\tilde {\mathca...
...\,dx
= {\left[{{p_1\over p_0} ({y_1}'y_2-y_1{y_2}')}\right]}.
\end{displaymath}](a_389.gif)  | 
(3) | 
 
See also Self-Adjoint Operator, Sturm-Liouville Theory
 
© 1996-9 Eric W. Weisstein 
1999-05-25