1540470959-Boundary_Value_Problems_and_Partial_Differential_Equations__Powers

(jair2018) #1

5.3 Two-Dimensional Heat Equation: Solution 307


Thecoefficientsareeasilyfoundtobe


amn=

4 ab
π^2

cos(mπ)cos(nπ)
mn =

4 ab
π^2

(− 1 )m+n
mn ,

so the solution to this problem is


u(x,y,t)=

4 ab
π^2

∑∞

m= 1

∑∞

n= 1

(− 1 )m+n
mn sin

(mπx
a

)

sin

(nπy
b

)

exp

(

−λ^2 mnkt

)

.

(18)

This solution is shown animated on the CD. 


Thedoubleseriesthatappearherearebesthandledbyconvertingtheminto
single series. To do this, arrange the terms in order of increasing values ofλ^2 mn.
Then the first terms in the single series are the most significant, those that
decay least rapidly. For example, ifa= 2 b,sothat


λ^2 mn=

(m^2 + 4 n^2 )π^2
a^2 ,

then the following list gives the double index(m,n)in order of increasing
values ofλ^2 mn:


( 1 , 1 ), ( 2 , 1 ), ( 3 , 1 ), ( 1 , 2 ), ( 2 , 2 ), ( 4 , 1 ), ( 3 , 2 ),....

EXERCISES



  1. Write out the “first few” terms of the series of Eq. (18). By “first few,”
    we mean those for whichλ^2 mnis smallest. (Assumea=bin determining
    relative magnitudes of theλ^2 .)

  2. Provide the details of the separation of variables by which Eqs. (9)–(13)
    are derived.

  3. Find the frequencies of vibration of a rectangular membrane. See Sec-
    tion 5.1, Exercise 1.

  4. Ve r i f y t h a tumn(x,y,t)satisfies Eqs. (1)–(3).

  5. Show thatXm(x)=cos(mπx/a)(m= 0 , 1 , 2 ,...) if the boundary condi-
    tions Eq. (3) are replaced by
    ∂u
    ∂x(^0 ,y,t)=^0 ,


∂u
∂x(a,y,t)=^0 ,^0 <y<b,^0 <t.
What values will theλ^2 mnhave, and of what form will the solutionu(x,y,t)
be?
Free download pdf