18 An Introduction to Partial Differential Equations with MATLAB©R
- The heat equation in two space variables,ut=α^2 (uxx+uyy)
- Laplace’s equation in three space variables,uxx+uyy+uzz=0
- The wave equation in three space variables,
utt+c^2 (uxx+uyy+uzz)=0
- Use (1.12) to show that the functionu(x, t)=
∑∞
n=1
cne−n
(^2) t
sinnxis a
solution of the heat equationut=uxx(whenever the series converges,
of course).
- Show directly that the principle of superposition doesnothold for the
PDEux+u^2 =0,u=u(x, y), by finding two different solutions, then
finding a linear combination of them that isnota solution. - We may also prove theorems for solutions ofnonhomogeneous PDEs
that are analogous to those for ODEs. Prove that the general solution
of the nonhomogeneous PDEL[u]=fisu=uh+up,whereupis any
one particular solution ofL[u]=f,anduhis the general solution of the
associated homogeneous PDEL[u] = 0, as follows:
a) First, prove thatuh+upalways is a solution ofL[u]=f.
b)Next,provethat,ifuis any particular solution ofL[u]=f,then
we can always write
u=uh′+up,
whereuh′is a particular case of the solutionuh.
Illustrate the theorem that we proved in Exercise 7 for the nonhomogeneous
PDEs in Exercises 8–12. You may refer to the corresponding exercises in
Section 1.2.
8.uy=2x
9.ux=sinx+cosy
10.uxxy=12x
11.uzz=x+y
12.uxx+ux− 2 u=6,u=u(x, y).
- a) Ifvis a solution of the PDEL[u]=f,andwis a solution of
L[u]=g, find a solution of the PDEL[u]=αf+βg,whereαand
βare any two constants.
b) Use what you did in part (a) to find a solution of the PDEuxx+
uyy=3x− 5 y.