G= Plot both G1 vs = B, flfs + 1+√√f/2(g Pr0.57-B) 2/3 1+B, G (1+B)1.07+12.7 √,/2 (Pr2³-1)] E and G2 vs F on the same graph. The solution is where the two lines intersect. The solution should occur at G = 1.23 and 長 √F (1) 8.82 3. With √ √2/f known, calculate St from equation 9.25 of the book using n = 0.57. 4. Solve for A/A, from Eq. 5b (from the appendix of the Chapter 8 problem) evaluated at Q/Qs = 1. Note that ß= ß, for the rib roughness because the heat transfer coefficient is based on the smooth tube area, i.e., A/L = A/L. 5. The associated e/D is calculated from e* = (e/D)Re√√f/2 6. The remaining parameters (N/Ns, L/Ls) are easily calculated.

Elements Of Electromagnetics
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ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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Section: Chapter Questions
Problem 1.1MA
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Coding assistance. 
fs= .00743

 

G" =
Plot both G1 vs
B flfs +.
1+ B. G*
√B
0.57
1+√√f/2(g Prº. B)
(1+B) 1.07 +12.7√√/2 (P-1)
and G2 vs
√√₁
on the same graph. The solution is where the
1√ √=8
two lines intersect. The solution should occur at G* = 1.23 and
(1)
= 8.82
3. With √√2/f known, calculate St from equation 9.25 of the book using n = 0.57.
4.
Solve for A/A, from Eq. 5b (from the appendix of the Chapter 8 problem)
evaluated at Q/Qs = 1. Note that ß= B. for the rib roughness because the heat
transfer coefficient is based on the smooth tube area, i.e., A/L = As/L.
5. The associated e/D is calculated from e+ = (e/D)Re√√f/2
6. The remaining parameters (N/Ns, L/Ls) are easily calculated.
Transcribed Image Text:G" = Plot both G1 vs B flfs +. 1+ B. G* √B 0.57 1+√√f/2(g Prº. B) (1+B) 1.07 +12.7√√/2 (P-1) and G2 vs √√₁ on the same graph. The solution is where the 1√ √=8 two lines intersect. The solution should occur at G* = 1.23 and (1) = 8.82 3. With √√2/f known, calculate St from equation 9.25 of the book using n = 0.57. 4. Solve for A/A, from Eq. 5b (from the appendix of the Chapter 8 problem) evaluated at Q/Qs = 1. Note that ß= B. for the rib roughness because the heat transfer coefficient is based on the smooth tube area, i.e., A/L = As/L. 5. The associated e/D is calculated from e+ = (e/D)Re√√f/2 6. The remaining parameters (N/Ns, L/Ls) are easily calculated.
Calculate the
material savings for the VG-1 case offered by two-dimensional rib roughness. For this
roughness, the geometrical parameters are e/D, ple, tle, a. Calculate the material
savings for a = 90° with p/e = 10, t/e = 0.5, while using the smooth tube operating
parameters as used in the Chapter 8 problem: Res = 12320, Pr = 62, oil, etc.
Because fand St are functions of e/D and et (or Re), the PEC equation for A/As
implicitly contains two independent variables: e/D and et. Therefore, a range of
solutions exist. Corresponding to each arbitrary value of et is a particular value of Re
(or Gs/G) required to satisfy the constraints (P/Ps = Q/Qs = 1). And, with et and Re
defined, e/D is known and calculated from eq. (9.9) of the book: (e/D=
et/ (Re√√f/2)). Therefore, one should calculate A/As for a range of e* (or Re) to
define the minimum A/As. Webb and Eckert (1972) have calculated A/As vs. Gs/G for
ple = 10, a = 90° roughness over a range of Re (or Gs/G) and Pr and suggest that e* =
20 is a reasonably good design specification for the VG-1 criterion. However, if the
A/As vs. Gs/G curve shows a fairly flat minimum, the required flow frontal area will
increase with increasing e* (or e/D).
For this problem, we will select et = 20 for our design specification, which fixes the
g (et) and B(e) contained in the correlations for fand St. These values are: a = 90°:
at e = 20, B = 4.2, g = 11.
Use the following iterative solution outlined below and given in the notes:
1. Assume G* = G/G. So Re = Res/ G*
2. Solve for G* from eq. (22) of Webb and Eckert (1972):
G
=
Re
2e+
V.₁
exp
Devise a computer code to generate an array for
in increments of 0.01. Use the
√F
-√21f- -3.75
2.5
array Gl. Use the G1 array and the
√
with values from 7 to 11
array to evaluate eq. (22) for G*. This will
give you an array of G* for values associated with the
F
1₁
array. Call this G*
array to evaluate a new G using
eq. (1) of your roughness class notes given below (i.e., eq. (17) of Webb and
Eckert, 1972) with r = Bs, (call this array G2):
¹Please use the Filonenko and Petuknov equations to calculate fs and Sts, respectively, for this problem.
Transcribed Image Text:Calculate the material savings for the VG-1 case offered by two-dimensional rib roughness. For this roughness, the geometrical parameters are e/D, ple, tle, a. Calculate the material savings for a = 90° with p/e = 10, t/e = 0.5, while using the smooth tube operating parameters as used in the Chapter 8 problem: Res = 12320, Pr = 62, oil, etc. Because fand St are functions of e/D and et (or Re), the PEC equation for A/As implicitly contains two independent variables: e/D and et. Therefore, a range of solutions exist. Corresponding to each arbitrary value of et is a particular value of Re (or Gs/G) required to satisfy the constraints (P/Ps = Q/Qs = 1). And, with et and Re defined, e/D is known and calculated from eq. (9.9) of the book: (e/D= et/ (Re√√f/2)). Therefore, one should calculate A/As for a range of e* (or Re) to define the minimum A/As. Webb and Eckert (1972) have calculated A/As vs. Gs/G for ple = 10, a = 90° roughness over a range of Re (or Gs/G) and Pr and suggest that e* = 20 is a reasonably good design specification for the VG-1 criterion. However, if the A/As vs. Gs/G curve shows a fairly flat minimum, the required flow frontal area will increase with increasing e* (or e/D). For this problem, we will select et = 20 for our design specification, which fixes the g (et) and B(e) contained in the correlations for fand St. These values are: a = 90°: at e = 20, B = 4.2, g = 11. Use the following iterative solution outlined below and given in the notes: 1. Assume G* = G/G. So Re = Res/ G* 2. Solve for G* from eq. (22) of Webb and Eckert (1972): G = Re 2e+ V.₁ exp Devise a computer code to generate an array for in increments of 0.01. Use the √F -√21f- -3.75 2.5 array Gl. Use the G1 array and the √ with values from 7 to 11 array to evaluate eq. (22) for G*. This will give you an array of G* for values associated with the F 1₁ array. Call this G* array to evaluate a new G using eq. (1) of your roughness class notes given below (i.e., eq. (17) of Webb and Eckert, 1972) with r = Bs, (call this array G2): ¹Please use the Filonenko and Petuknov equations to calculate fs and Sts, respectively, for this problem.
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