23-Chem-A2 Unit Operations and Separation Processes · December 2018
Question 2 of 6: Frictional Pressure Drop in Series Pipes with a Reducer
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. 16-CHEM-A2, Unit Operations and Separation Processes — December 2018, 3-hour open-book exam. Six 25-point problems: Part A (Unit Operations) — A1 continuous-thickener sizing, A2 series-pipe friction pressure drop, A3 packed/fluidized-bed pressure drop & power; Part B (Separation Processes) — B1 flash vs. differential distillation, B2 batch-drying time, B3 adsorption isotherm fitting & surface area. The rubric asks for two problems per part; all six are worked in full below.
Reference texts (subject). McCabe, Smith & Harriott, Unit Operations of Chemical Engineering (7th ed.); Coulson & Richardson, Chemical Engineering Vol. 2 (5th ed.); Geankoplis, Transport Processes and Separation Process Principles (4th ed.); Treybal, Mass-Transfer Operations (3rd ed.); Perry's Chemical Engineers' Handbook (§6 fluid & particle mechanics, §12 drying, §16 adsorption, §18 solid–liquid separation).
Question A2: Frictional Pressure Drop in Series Pipes with a Reducer (25 points)
Find. The total frictional pressure drop $\Delta P$ across the horizontal series system (both straight runs plus the reducer).
Figure A2 — Same mass flow in both runs; the velocity rises in the narrower pipe. Total loss = friction in pipe 1 + reducer minor loss + friction in pipe 2. Horizontal, so no elevation term.
Approach. Get the constant volumetric flow, then in each pipe compute velocity, Reynolds number, and a smooth-pipe (Blasius) Fanning factor; sum the two straight-pipe losses and the reducer velocity-head loss.
Volumetric flow (constant through the series). $Q=\dot m/\rho=3.333/850=\boxed{3.92\times10^{-3}\ \text{m}^3/\text{s}}$.
Pipe 1 — velocity and Reynolds number. $A_1=\tfrac{\pi}{4}(0.050)^2=1.963\times10^{-3}\ \text{m}^2$, so $u_1=Q/A_1=2.00\ \text{m/s}$ and $$Re_1=\frac{\rho u_1 D_1}{\mu}=\frac{850(2.00)(0.050)}{3\times10^{-3}}=2.83\times10^{4}\ (\text{turbulent}).$$ Smooth-pipe Blasius Fanning factor: $f_1=0.079\,Re_1^{-1/4}=6.09\times10^{-3}$.
Pipe 2 — velocity, Reynolds, factor. $A_2=\tfrac{\pi}{4}(0.038)^2=1.134\times10^{-3}\ \text{m}^2$, so $u_2=3.46\ \text{m/s}$, $$Re_2=\frac{850(3.46)(0.038)}{3\times10^{-3}}=3.72\times10^{4},\qquad f_2=0.079\,Re_2^{-1/4}=5.69\times10^{-3}.$$ Then $\Delta P_2=4f_2\frac{L_2}{D_2}\frac{\rho u_2^2}{2}=4(0.00569)\frac{60}{0.038}\cdot\frac{850(3.46)^2}{2}=\boxed{182.5\ \text{kPa}}.$
Reducer minor loss. Charged on the higher downstream velocity head: $$\Delta P_r=0.2\cdot\frac{\rho u_2^2}{2}=0.2\cdot\frac{850(3.46)^2}{2}=\boxed{1.0\ \text{kPa}}.$$
Total frictional pressure drop. $$\Delta P=\Delta P_1+\Delta P_2+\Delta P_r=82.6+182.5+1.0=\boxed{266\ \text{kPa}}.$$ The 38-mm run dominates: reducing the bore from 50 to 38 mm roughly triples the velocity head, since $(50/38)^4\approx3.0$, and raises $L/D$, so the shorter narrow pipe carries about two-thirds of the total loss.