Reduce following the heat conduction equation to the ordinary differential equations and separate the given homogeneous boundary conditions by using the method of separation of variables u(0.1)=0, t>0 (the end x-0 is held at zero temperature) u(2t)=0, t>0 (no heat loss from this end) A X"-4AX-0, X(0)=0, X(2)=0 T'-AT=0, A<0. B X-AX=0, X(0)=0, X'(2)=0 T-4AT=0. A<0. C. X"-AX=0, X(0)=0, X(2)-0 T-4AT=0. D. X"-AX-0, X(0)=0, x(2)=0 T-4AT-0. X-AX-0, X(0)-0, X'(2)-0 T-AAT 0.

Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
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Reduce following the heat conduction equation to the ordinary differential equations and separate the given homogeneous boundary conditions by using
the method of separation of variables
Ut=4ux
u(0,t)=0, t>0 (the end x-0 is held at zero temperature)
u,(2,t)=0, t>0 (no heat loss from this end)
A
X"-4AX=0, X(0)=0, X(2)=0
T'-AT=0,
A<0.
B
X"-AX=0, X(0)=0, X'(2)=0
T'-4AT=0.
A<0.
X"-AX-0, X(0)=0, X(2)=0
T'-4AT=0.
A>0.
X"-AX=0, X(0)-0, X(2)-0
T-4AT-0.
A<0.
X-AX-0, X(0)-0, X'(2)-0
T-4AT-0.
A0.
yazın
Transcribed Image Text:Reduce following the heat conduction equation to the ordinary differential equations and separate the given homogeneous boundary conditions by using the method of separation of variables Ut=4ux u(0,t)=0, t>0 (the end x-0 is held at zero temperature) u,(2,t)=0, t>0 (no heat loss from this end) A X"-4AX=0, X(0)=0, X(2)=0 T'-AT=0, A<0. B X"-AX=0, X(0)=0, X'(2)=0 T'-4AT=0. A<0. X"-AX-0, X(0)=0, X(2)=0 T'-4AT=0. A>0. X"-AX=0, X(0)-0, X(2)-0 T-4AT-0. A<0. X-AX-0, X(0)-0, X'(2)-0 T-4AT-0. A0. yazın
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