2. A very narrow pipe of length L and cross-sectional area A is filled with water. At time t = 0, a certain amount of salt, of total mass M, is placed at one end the pipe, reaching a length d. The pipe is then sealed at both ends. We wish to know the concentration of salt, C, at any time. Since the pipe is narrow, of concentration of salt over the cross section of the pipe can be neglected, and the concentration is given by C = C(x,t). The concentration satisfies the 1-D diffusion equation: the variations = D- The initial concentration profile is C(x, 0) = { M Ad 0 < x < d 0, d

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1.0
0.5
8 0.0
-0.5
-1.0
-3
-2
-1
1
2
X
2. A very narrow pipe of length L and cross-sectional area A is filled with water.
At time t = 0, a certain amount of salt, of total mass M, is placed at one end the
pipe, reaching a length d. The pipe is then sealed at both ends. We wish to know
the concentration of salt, C, at any time. Since the pipe is narrow, the variations
of concentration of salt over the cross section of the pipe can be neglected, and the
concentration is given by C = C (x, t). The concentration satisfies the 1-D diffusion
equation:
D-
Ət
The initial concentration profile is
M
Ad
C(x, 0) = {
0 < x < d
0, d<x < L
and since the pipe is closed at both ends:
ƏC(0, t)
ƏC(L,t)
= 0
2
Transcribed Image Text:1.0 0.5 8 0.0 -0.5 -1.0 -3 -2 -1 1 2 X 2. A very narrow pipe of length L and cross-sectional area A is filled with water. At time t = 0, a certain amount of salt, of total mass M, is placed at one end the pipe, reaching a length d. The pipe is then sealed at both ends. We wish to know the concentration of salt, C, at any time. Since the pipe is narrow, the variations of concentration of salt over the cross section of the pipe can be neglected, and the concentration is given by C = C (x, t). The concentration satisfies the 1-D diffusion equation: D- Ət The initial concentration profile is M Ad C(x, 0) = { 0 < x < d 0, d<x < L and since the pipe is closed at both ends: ƏC(0, t) ƏC(L,t) = 0 2
a) Start with a solution of the form C(x, t)
equation and show that the problem reduces to two ordinary differential equations:
X (x)T(t), replace in the diffusion
X"(x) = AX(x); T'(t) = ADT(t)
where A is an arbitrary constant.
b) We seek time-decaying solutions, show that implies A = -k², where k is an arbi-
trary constant.
c) Solve the two ODES and show that after applying the two boundary conditions:
C(x, t) = an cos(-
Σ
n=0
d) Find C(x, t) so that it satisfies the initial concentration profile.
e) Show that your expression for C(x, t) satisfies the equilibrium profile C(x, t –)
expected from conservation of mass.
3
Transcribed Image Text:a) Start with a solution of the form C(x, t) equation and show that the problem reduces to two ordinary differential equations: X (x)T(t), replace in the diffusion X"(x) = AX(x); T'(t) = ADT(t) where A is an arbitrary constant. b) We seek time-decaying solutions, show that implies A = -k², where k is an arbi- trary constant. c) Solve the two ODES and show that after applying the two boundary conditions: C(x, t) = an cos(- Σ n=0 d) Find C(x, t) so that it satisfies the initial concentration profile. e) Show that your expression for C(x, t) satisfies the equilibrium profile C(x, t –) expected from conservation of mass. 3
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