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23-Chem-A3 Heat and Mass Transfer · December 2017

Question 1 of 6: Part A: Free-Convection Heat Loss from a Pipe, Horizontal vs. Vertical

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

National Exams — December 2017 — 16-Chem-A3 Heat and Mass Transfer. Three-hour, open-book exam (one textbook of the candidate’s choice; any non-communicating calculator). Format: two parts — Part A — Heat Transfer (Q1–Q3) and Part B — Mass Transfer (Q4–Q6). All problems are worth 25 points; the rubric requires at least two problems attempted from each part and marks only the first two per part, so a complete paper is four questions (100 points). All six problems are solved below for completeness. Property data are quoted as stated in each problem; where a value applies to a film condition it is used at the stated film temperature.

Reference texts: F. P. Incropera & D. P. DeWitt, Fundamentals of Heat and Mass Transfer (Wiley) — free/forced convection correlations, conduction shape factors, the heat–mass-transfer analogy; J. P. Holman, Heat Transfer (McGraw-Hill) — natural-convection constants $C,m$ and cylinder conduction; R. E. Treybal, Mass-Transfer Operations (McGraw-Hill) — wetted-wall $k_G$, gas absorption and the Chilton–Colburn analogy; R. B. Bird, W. E. Stewart & E. N. Lightfoot, Transport Phenomena (Wiley); supporting property data from Perry’s Chemical Engineers’ Handbook (9th ed.).

Question 1 — Part A: Free-Convection Heat Loss from a Pipe, Horizontal vs. Vertical (25 points)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. A pipe of diameter $D=0.040$ m and length $L=0.60$ m at surface temperature $T_s=85$ °C loses heat by free convection to still water at $T_\infty=15$ °C, so $\Delta T = 70$ K. Water properties (at the film temperature $T_f=50$ °C) are tabulated below.

PropertyValue
Density $\rho$988 kg/m³
Thermal conductivity $k$0.647 W/m·K
Dynamic viscosity $\mu$$5.493\times10^{-4}$ kg/m·s
Specific heat $c_p$4178 J/kg·K
Volume-expansion coeff. $\beta$$5.1\times10^{-4}$ K$^{-1}$

Find. The convective heat-loss rate $Q$ (a) with the pipe horizontal and (b) with the pipe vertical.

Horizontal pipesteam pipe, Ts = 85 °Cwater 15 °CL = 0.6 m, D = 40 mmVertical pipeTs = 85 °Cwater15 °Ccharacteristic length = L
Figure 1 — The same pipe loses heat to the surrounding water in two orientations. The characteristic length in $Gr$ is the diameter $D$ when horizontal and the height $L$ when vertical, which is what makes the two answers differ.

Approach. Form the Prandtl number, then the Grashof number on the correct characteristic length for each orientation, select the matching $(C,m)$ from the $Gr\,Pr$ band, evaluate $Nu$ and hence the film coefficient $h=Nu\,k/L_c$, and finally $Q=hA\,\Delta T$ over the same lateral area $A=\pi D L$.

  1. Prandtl number. This is a fluid property, common to both orientations: $$Pr = \frac{c_p\,\mu}{k} = \frac{(4178)(5.493\times10^{-4})}{0.647} = \boxed{3.55}.$$
  2. Horizontal pipe — Grashof number on $L_c=D$. The free-convection driving group uses the diameter for a horizontal cylinder: $$Gr_D = \frac{g\,\beta\,\Delta T\,D^{3}\rho^{2}}{\mu^{2}} = \frac{(9.81)(5.1\times10^{-4})(70)(0.040)^3(988)^2}{(5.493\times10^{-4})^2} = 7.25\times10^{7}.$$ Then $Gr_D\,Pr = (7.25\times10^{7})(3.55) = 2.57\times10^{8}$, which lies in the band $10^4$–$10^9$, so $C=0.53,\ m=0.25$.
  3. Horizontal film coefficient and heat loss. With $Nu = 0.53\,(Gr_D Pr)^{0.25}$, $$Nu = 0.53\,(2.57\times10^{8})^{0.25} = 67.1,\qquad h = \frac{Nu\,k}{D} = \frac{(67.1)(0.647)}{0.040} = 1086\ \text{W/m}^2\text{K}.$$ The lateral area is $A=\pi D L = \pi(0.040)(0.60)=0.0754\ \text{m}^2$, so $$Q_\text{horiz} = hA\,\Delta T = (1086)(0.0754)(70) = \boxed{5.73\times10^{3}\ \text{W} \approx 5.73\ \text{kW}}.$$ That is part (a).
  4. Vertical pipe — Grashof number on $L_c=L$. For a vertical cylinder the height replaces the diameter, and because $Gr\propto L_c^{3}$ the group jumps by $(L/D)^3=3375$: $$Gr_L = \frac{g\,\beta\,\Delta T\,L^{3}\rho^{2}}{\mu^{2}} = 2.45\times10^{11},\qquad Gr_L\,Pr = 8.68\times10^{11} > 10^{9},$$ so now $C=0.13,\ m=0.33$.
  5. Vertical film coefficient and heat loss. With $Nu = 0.13\,(Gr_L Pr)^{0.33}$, $$Nu = 0.13\,(8.68\times10^{11})^{0.33} = 1132,\qquad h = \frac{Nu\,k}{L} = \frac{(1132)(0.647)}{0.60} = 1220\ \text{W/m}^2\text{K}.$$ Over the same area $A=0.0754\ \text{m}^2$, $$Q_\text{vert} = (1220)(0.0754)(70) = \boxed{6.44\times10^{3}\ \text{W} \approx 6.44\ \text{kW}}.$$ That is part (b).
QuantityResult
Prandtl number3.55
(a) Horizontal: $Gr\,Pr$ / $Nu$ / $h$$2.57\times10^{8}$ / 67.1 / 1086 W/m²K
(a) Heat loss, horizontal≈ 5.73 kW
(b) Vertical: $Gr\,Pr$ / $Nu$ / $h$$8.68\times10^{11}$ / 1132 / 1220 W/m²K
(b) Heat loss, vertical≈ 6.44 kW
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