Chem Differential Eq HW Solutions Fall 2011 97

Chem Differential Eq HW Solutions Fall 2011 97 - Section...

This preview shows page 1. Sign up to view the full content.

Section 6.2 Sturm-Liouville Theory 97 Since α ± = 0, it follows that sinh α ± = 0 and this implies that 1 - α 2 =0or α = ² 1. We take α = 1, because the value - 1 does not yield any new eigenfunctions. For α = 1, the corresponding solution is X = c 1 cosh x + c 2 sinh x = - c 2 cosh x + c 2 sinh x, because c 1 = - αc 2 = - c 2 . So in this case we have one negative eigenvalue λ = - α 2 = - 1 with corresponding eigenfunction X = cosh x - sinh x . Case III If λ = α 2 > 0, then the general solution of the diﬀerential equation is X = c 1 cos αx + c 2 sin αx. We have X ± = - c 1 α sin αx + c 2 α cos αx . In order to have nonzero solutions, one of the coeﬃcients c 1 or c 2 must be ± = 0. Using the boundary conditions, we obtain c 1 + αc 2 =0 c 1 (cos α - α sin α )+ c 2 (sin α + α cos α )=0 The ±rst equation implies that c 1 = - αc 2 and so both c 1 and c 2 are neq 0. From the second equation, we obtain - αc 2 (cos α - α sin α c 2 (sin α + α cos α - α (cos α - α sin α ) + (sin α + α cos α sin α ( α 2 +1) = 0 Since α 2 +1 ± = 0, then sin α = 0, and so α = , where n =1 , 2 ,...
This is the end of the preview. Sign up to access the rest of the document.

This note was uploaded on 12/22/2011 for the course MAP 3305 taught by Professor Stuartchalk during the Fall '11 term at UNF.

Ask a homework question - tutors are online