1540470959-Boundary_Value_Problems_and_Partial_Differential_Equations__Powers

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2.10 Semi-Infinite Rod 191


Figure 8 Graphs of the solution of the example,u(x,t)as a function ofxover
the interval 0<x< 3 b,whereb=1andT 0 =100 for convenience. The times
have been chosen so that the dimensionless timekt/b^2 takes the values 0.001, 0.01,
0.1, and 1. Whenkt/b^2 = 0 .01, the temperature nearx=b/2 has not changed
noticeably from its initial value.


Therefore, the complete solution is


u(x,t)=

2

πT^0

∫∞

0

1 −cos(λb)
λ sin(λx)exp

(

−λ^2 kt

)

dλ.

In Fig. 8 are graphs ofu(x,t)as a function ofxforvariousvaluesoft;an
animation can be seen on the CD. 


EXERCISES



  1. Find the solution of Eqs. (1)–(3) if the initial temperature distribution is
    given by


f(x)=

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


  1. Ve r i f y t h a tu(x,t)as given by Eq. (9) is a solution of Eqs. (1)–(3). What is
    thesteady-statetemperaturedistribution?

  2. Find the solution of Eqs. (1)–(4) iff(x)=T 0 e−αx,x>0.

  3. Find a formula for the solution of the problem

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