This preview shows page 1. Sign up to view the full content.
Unformatted text preview: 40 Chapter 3 Partial Diﬀerential Equations in Rectangular Coordinates
To simplify the notation, replace x0 and t0 by x and y in the coordinates of
the points Q1 and P2 and let φ(x, t) = −4t2 + x − x2 + 8tx. We have
u(x, t) = u(Q1) − u(P2 )
x + 1 − 2t 1 − x + 2t
=φ
,
2
4
= 5 − 12t − 5x + 12tx, −φ 3 − x − 2t −1 + x + 2t
,
2
4 where the last expression was derived after a few simpliﬁcations that we
omit. It is interesting to note that the formula satisﬁes the wave equation
and the boundary condition u(1, t) = 0 for all t > 0. Its restriction to the
line x + 2t = 1 (part of the boundary of region I ) reduces to the formula for
u(x, t) for (x, t) in region I . This is to be expected since u is continuous in
(x, t). ...
View
Full
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.
 Fall '11
 StuartChalk

Click to edit the document details