3.) Use the Maximum/Minimum Principles to deduce that the solution u of the problem D.E. ut = kuzr 00 B.C. u(0, t) = 0 u(7, t) = 0 I.C. u(x, 0) = sin(x) + ; sin(2x) %3D satisfies 0 < u(x, t) 0.

Advanced Engineering Mathematics
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ISBN:9780470458365
Author:Erwin Kreyszig
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Chapter2: Second-order Linear Odes
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3.) Use the Maximum/Minimum Principles to deduce that the solution u of the problem
D.E. u = kuz 0 <r < T, t N 0
B.C. u(0, t) = 0
u (π, t) 0
I.C. u(x, 0) = sin(x) + sin(2x)
%3D
satisfies 0 < u(, t) <V3 for all 0 < ¤ < T, t > 0.
Transcribed Image Text:3.) Use the Maximum/Minimum Principles to deduce that the solution u of the problem D.E. u = kuz 0 <r < T, t N 0 B.C. u(0, t) = 0 u (π, t) 0 I.C. u(x, 0) = sin(x) + sin(2x) %3D satisfies 0 < u(, t) <V3 for all 0 < ¤ < T, t > 0.
Expert Solution
Step 1

given

differential equation

ut=kuxx    ...i

where 0xπ, t0

boundary condition

u0,t=0       uπ,t=0

initial condition 

ux,0=sinx+12sin2x

satisfies

0ux,t343 for all 0xπ,t0

Step 2

solution

let the solution be of the form

ux,t=XxTt

differentiate it with respect to x and t

ux=X'xTt

ut=XxT't

again differentiate ux=X'xTt with respect to x

ux=X''xTt

substitute the values in equation i

we get

kX''xTt=XxT'tX''xTt=1kXxT't

Step 3

divide both sides by XxTt

X''xXx=1kT'tTt

let 

X''xXx=1kT'tTt=-p2

p is any constant

we have 

X''xXx=-p2X''x+p2Xx=0   ...ii

and 

1kT'tTt=-p2T'tTt=-p2k   ...iii

Step 4

solving equation (ii)

X''x+p2Xx=0

auxillary equation

m2+p2=0m2=-p2m=±ip

we have 

Xx=c1cospx+c2sinpx

integrate equation (iii) 

we get

T'tTt=-p2kdtlnTt=-p2ktTt=e-p2kt

thus the solution becomes

ux,t=c1cospx+c2sinpxe-p2kt

steps

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