Question 2 Based on question (1), sketch the dimensionless temperature profile 8(x) versus aL = 2, € [0, 1] aL = 3, Є [0, 1] L Ꮎ 1.2 1.0 0.8 0.6 0.4 0.2 Ꮎ 1.2- 1.0 0.8 0.6 0.4 0.2 for the two following cases. Ꮎ 1.2ㅏ 1.2 a L=3 1.0 1.0 0.8 0.8 a L=2 0.6 0.6 0.4 a L=2 0.4 a L=3 0.2 a L = 3 0.2 α L=2 Χ x Χ 0.2 0.4 0.6 0.8 1.0 1.2 L 0.2 0.4 0.6 0.8 1.0 1.2 L 0.2 0.4 0.6 0.8 1.0 1.2 L a L=2 a L-3 x 0.2 0.4 0.6 0.8 1.0 1.2 L Question 1 From the following equation, assume that the cross-sectional area A is a constant. d dx dT ка dx KAT) = hC(T - T fluid) Also assume that all other physical parameters k, h, A, C, L, Tw wall' and Tfluid are well known and assumed to be positive constants. (a) Based on these assumptions, the above ODE can be simplified to which of the follow? hc(T-Tfluid) T ка dx2 dA dk dT + A. dx dx dx hc(T-T fluid) dT Ока = (hC(T Tfluid)) dx dx 이은 dA dk d²T + A. = dx dx dx² hc(T-T fluid) dx -(KA) = (hC(T-Tfluid)) dT (b) Solve the ODE based on the following two boundary conditions. For simplicity, let a² Ch for when formulating your solution. (Use T, to represent T fluid and Tw to represent T ка wall in your response.) At x = 0, T = T¸ wall' dT At x = L, = 0. dx T T T(x) @ αχ 2aL 1+e e + (1-T)eal -αx e + 1+e 2aL - If - (c) Define a "dimensionless" variable (x) T(x) T₂ T wall-fluid fluid Based on the T(x) solution, rewrite the solution in terms of (x) and the hyperbolic cosine function, where cosh(y) 8(x) = cosh(x) + 1-e2aL ox 1+e 2aL 1+cosh(x) ey + e˜y = Again, let a² Ch α = 2 for when formulating your solution. ка

Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
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I need help with Question 2 described below and an explanation for the solution. (Differential Equations)

Question 2
Based on question (1), sketch the dimensionless temperature profile 8(x) versus
aL = 2, € [0, 1]
aL = 3,
Є [0, 1]
L
Ꮎ
1.2
1.0
0.8
0.6
0.4
0.2
Ꮎ
1.2-
1.0
0.8
0.6
0.4
0.2
for the two following cases.
Ꮎ
1.2ㅏ
1.2
a L=3
1.0
1.0
0.8
0.8
a L=2
0.6
0.6
0.4
a L=2
0.4
a L=3
0.2
a L = 3
0.2
α L=2
Χ
x
Χ
0.2
0.4
0.6
0.8
1.0
1.2 L
0.2
0.4
0.6
0.8
1.0
1.2 L
0.2
0.4
0.6
0.8
1.0
1.2 L
a L=2
a L-3
x
0.2
0.4
0.6
0.8
1.0
1.2 L
Transcribed Image Text:Question 2 Based on question (1), sketch the dimensionless temperature profile 8(x) versus aL = 2, € [0, 1] aL = 3, Є [0, 1] L Ꮎ 1.2 1.0 0.8 0.6 0.4 0.2 Ꮎ 1.2- 1.0 0.8 0.6 0.4 0.2 for the two following cases. Ꮎ 1.2ㅏ 1.2 a L=3 1.0 1.0 0.8 0.8 a L=2 0.6 0.6 0.4 a L=2 0.4 a L=3 0.2 a L = 3 0.2 α L=2 Χ x Χ 0.2 0.4 0.6 0.8 1.0 1.2 L 0.2 0.4 0.6 0.8 1.0 1.2 L 0.2 0.4 0.6 0.8 1.0 1.2 L a L=2 a L-3 x 0.2 0.4 0.6 0.8 1.0 1.2 L
Question 1
From the following equation, assume that the cross-sectional area A is a constant.
d
dx
dT
ка
dx
KAT) = hC(T - T fluid)
Also assume that all other physical parameters k, h, A, C, L, Tw
wall'
and Tfluid are well known and assumed to be positive constants.
(a) Based on these assumptions, the above ODE can be simplified to which of the follow?
hc(T-Tfluid)
T
ка
dx2
dA
dk dT
+ A.
dx
dx dx
hc(T-T fluid)
dT
Ока =
(hC(T Tfluid)) dx
dx
이은
dA
dk d²T
+ A.
=
dx
dx dx²
hc(T-T fluid)
dx
-(KA)
= (hC(T-Tfluid)) dT
(b) Solve the ODE based on the following two boundary conditions. For simplicity, let a²
Ch
for when formulating your solution. (Use T, to represent T fluid and Tw to represent T
ка
wall
in your response.)
At x = 0, T = T¸
wall'
dT
At x = L,
= 0.
dx
T T
T(x)
@
αχ
2aL
1+e
e +
(1-T)eal
-αx
e
+
1+e
2aL
- If
-
(c) Define a "dimensionless" variable (x)
T(x) T₂
T wall-fluid
fluid
Based on the T(x) solution, rewrite the solution in terms of (x) and the hyperbolic cosine function, where cosh(y)
8(x) =
cosh(x) +
1-e2aL
ox
1+e
2aL
1+cosh(x)
ey + e˜y
=
Again, let a²
Ch
α =
2
for when formulating your solution.
ка
Transcribed Image Text:Question 1 From the following equation, assume that the cross-sectional area A is a constant. d dx dT ка dx KAT) = hC(T - T fluid) Also assume that all other physical parameters k, h, A, C, L, Tw wall' and Tfluid are well known and assumed to be positive constants. (a) Based on these assumptions, the above ODE can be simplified to which of the follow? hc(T-Tfluid) T ка dx2 dA dk dT + A. dx dx dx hc(T-T fluid) dT Ока = (hC(T Tfluid)) dx dx 이은 dA dk d²T + A. = dx dx dx² hc(T-T fluid) dx -(KA) = (hC(T-Tfluid)) dT (b) Solve the ODE based on the following two boundary conditions. For simplicity, let a² Ch for when formulating your solution. (Use T, to represent T fluid and Tw to represent T ка wall in your response.) At x = 0, T = T¸ wall' dT At x = L, = 0. dx T T T(x) @ αχ 2aL 1+e e + (1-T)eal -αx e + 1+e 2aL - If - (c) Define a "dimensionless" variable (x) T(x) T₂ T wall-fluid fluid Based on the T(x) solution, rewrite the solution in terms of (x) and the hyperbolic cosine function, where cosh(y) 8(x) = cosh(x) + 1-e2aL ox 1+e 2aL 1+cosh(x) ey + e˜y = Again, let a² Ch α = 2 for when formulating your solution. ка
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