1540470959-Boundary_Value_Problems_and_Partial_Differential_Equations__Powers

(jair2018) #1

208 Chapter 2 The Heat Equation


u( 0 ,t)=T 0 ,0<t,
u(x, 0 )=

{ 0 , 0 <x<a,
T 0 , a<x.

13.

∂^2 u
∂x^2 =

1

k

∂u
∂t,0<x<∞,0<t,
∂u
∂x(^0 ,t)=0,^0 <t,
u(x, 0 )=

{

T 0 , 0 <x<a,
0 , a<x.




(^2) u
∂x^2 =


1

k

∂u
∂t, −∞<x<∞,0<t,
u(x, 0 )=exp

(

−α|x|

)

, −∞<x<∞.

15.

∂^2 u
∂x^2 =

1

k

∂u
∂t, −∞<x<∞,0<t,

u(x, 0 )=

{ 0 , −∞<x<0,
T 0 , 0 <x<a,
0 , a<x<∞.

16.

∂^2 u
∂x^2 =

1

k

∂u
∂t,0<x<a,0<t,
∂u
∂x(^0 ,t)=0, u(a,t)=T^0 ,0<t,
u(x, 0 )=T 0 +S(a−x),0<x<a.
17.Give a physical interpretation for this problem and thus explain why
u(x,t)should increase steadily astincreases. (Assume thatSis a pos-
itive constant.)
∂^2 u
∂x^2

=^1

k

∂u
∂t

, 0 <x<a, 0 <t,
∂u
∂x

( 0 ,t)= 0 , ∂u
∂x

(a,t)=S, 0 <t,
u(x, 0 )= 0 , 0 <x<a.

18.Show thatv(x,t)=(S/ 2 a)(x^2 + 2 kt)satisfies the heat equation and the
boundary conditions of the problem in Exercise 17. Also findw(x,t),
defined byu(x,t)=v(x,t)+w(x,t).
19.Show that the four functions

u 0 = 1 , u 1 =x, u 2 =x^2 + 2 kt, u 3 =x^3 + 6 kxt
Free download pdf