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23-Chem-A5 Chemical Plant Design and Economics · May 2015

Question 5 of 6: Equipment Design — Decanter/Settler

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

Notes on this paper

National Exams — May 2015 — 04-Chem-A5 Chemical Plant Design and Economics. Three-hour, closed-book exam (one two-sided aid sheet and an approved calculator permitted). Six equally weighted 20-mark questions are posed; the candidate answers any five and only the first five are marked. All six are worked below for completeness. Questions 2, 3 and 5 carry the numerical work (equivalent-annual-cost equipment selection, a discounted-cash-flow rate-of-return analysis, and a gravity-decanter sizing); questions 1, 4 and 6 are design / materials-selection / safety questions answered as organised prose, with Question 1 supported by a process flow sheet and a light overall material balance.

Reference texts: M.S. Peters, K.D. Timmerhaus & R.E. West, Plant Design and Economics for Chemical Engineers (5th ed., McGraw-Hill) — the exam's named primary text (cost–capacity estimation Ch. 6, interest and investment Ch. 7, profitability and rate of return Ch. 10); R.K. Sinnott & G. Towler, Chemical Engineering Design (Coulson & Richardson Vol. 6, 5th ed., Butterworth-Heinemann) — separator/decanter sizing (§10.6), materials of construction (Ch. 7) and the process-design safety checklist (Ch. 9); R. Turton et al., Analysis, Synthesis, and Design of Chemical Processes (4th ed., Prentice Hall) — flowsheet synthesis; supporting Canadian practice from CSA B51 / ASME BPVC (pressure vessels), API 650 (atmospheric storage tanks) and NACE corrosion guidance.

Question 5: Equipment Design — Decanter/Settler (20 marks)

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 liquid–liquid gravity separation:

PropertyLight oil (dispersed)Water (continuous)
Mass flow1000 kg/hr5000 kg/hr
Density, $\rho$900 kg/m³1000 kg/m³
Viscosity, $\mu$1 mN·s/m² ($10^{-3}$ Pa·s)$10^{-3}$ Pa·s
Droplet diameter, $d$150 µm ($150\times10^{-6}$ m)

Design constraints: dispersion band = 10 % of decanter height; oil–water interface at 50 % of height; light-oil take-off at 90 % of height.

Find. A decanter (horizontal gravity settler) sized so the oil droplets separate, together with the piping arrangement (feed, oil take-off, and water draw-off leg heights).

Approach. Follow Sinnott's decanter method: compute the Stokes settling (rise) velocity of the dispersed oil droplet, confirm laminar (Stokes) validity, size the interfacial area so the continuous-phase velocity stays below that settling velocity, choose vessel dimensions from that area, then fix the water draw-off leg height by a manometric balance across the interface.

  1. Settling (rise) velocity of the oil droplet — Stokes' law. The light oil droplet rises through the continuous water phase; for a small droplet the terminal velocity is $$u_d = \frac{d^2(\rho_c-\rho_d)\,g}{18\,\mu_c}= \frac{(150\times10^{-6})^2(1000-900)(9.81)}{18(10^{-3})}= 1.23\times10^{-3}\ \text{m/s}$$ i.e. $u_d \approx 1.23$ mm/s.
  2. Check Stokes' law is valid. The droplet Reynolds number is $$Re = \frac{\rho_c\,u_d\,d}{\mu_c}= \frac{(1000)(1.23\times10^{-3})(150\times10^{-6})}{10^{-3}}= 0.18 \;(<1)$$ so creeping (Stokes) flow holds. The value is also well below Sinnott's recommended design cap of 4 mm/s, so $u_d$ is used directly.
  3. Volumetric flows of each phase. Dividing mass flow by density (and by 3600 s/hr): $$Q_{oil}=\frac{1000}{900\cdot3600}=3.09\times10^{-4}\ \text{m}^3/\text{s},\qquad Q_{water}=\frac{5000}{1000\cdot3600}=1.39\times10^{-3}\ \text{m}^3/\text{s}$$ total $Q_t = 1.70\times10^{-3}$ m³/s ($\approx 6.1$ m³/hr).
  4. Interfacial (settling) area. For clean separation the upward/through velocity of the continuous phase must not exceed the droplet settling velocity, $u_c = Q_{water}/A_i \le u_d$, giving the minimum interfacial area $$A_i = \frac{Q_{water}}{u_d}= \frac{1.39\times10^{-3}}{1.23\times10^{-3}}= \boxed{1.13\ \text{m}^2}$$
  5. Vessel dimensions. Use a horizontal cylindrical decanter with the interface at the mid-diameter, so the interfacial area is $A_i = L\times D$. Taking a length-to-diameter ratio $L/D = 4$ gives $4D^2 = 1.13 \Rightarrow D = 0.53$ m, $L = 2.13$ m. Rounding up to a standard vessel, select $$\boxed{D = 0.6\ \text{m}, \quad L = 2.4\ \text{m}\ \;(A_i = 1.44\ \text{m}^2)}$$ which gives an actual continuous-phase velocity $u_c = Q_{water}/A_i = 0.96$ mm/s $< u_d$ — a comfortable margin.
  6. Piping arrangement — water draw-off leg height. The interface position is fixed by balancing the two liquid legs about the interface, $\rho_d(z_{oil}-z_{if})=\rho_c(z_{w}-z_{if})$, so the heavy-liquid (water) take-off height is $$z_w = z_{if}+\frac{\rho_d}{\rho_c}\,(z_{oil}-z_{if}) = 0.50H + \frac{900}{1000}(0.90H-0.50H)= 0.86H$$ With $H=D=0.6$ m: interface at 0.30 m, dispersion band $0.10H=0.06$ m straddling it, light-oil take-off at $0.90H=0.54$ m (near the top), and the water draw-off leg set at $0.86H=0.52$ m so the interface sits at mid-height as specified.
Feed 6.11 m3/hroil (disp.) + water (cont.)Light oiloff @ 0.90 HWaterleg @ 0.86 HOil layer (light)Water layer (heavy, continuous)dispersion band = 0.10 Hinterface 0.50 HD = 0.6 mL = 2.4 m (A_interface = L x D = 1.44 m2)
Figure 5.1 — Horizontal gravity decanter. Feed enters at mid-height; oil droplets rise at $u_d=1.23$ mm/s through the water and coalesce in the dispersion band ($0.10H$) at the interface ($0.50H$). Light oil overflows at $0.90H$; the water draw-off leg, set at $0.86H$, holds the interface at mid-height by the density balance. The interfacial area $L\times D = 1.44$ m² keeps the continuous-phase velocity ($0.96$ mm/s) below $u_d$.
QuantityValue
Droplet settling velocity, $u_d$ (Stokes)$1.23\times10^{-3}$ m/s (1.23 mm/s)
Droplet Reynolds number0.18 (Stokes valid)
Water / oil / total volumetric flow$1.39\times10^{-3}$ / $3.09\times10^{-4}$ / $1.70\times10^{-3}$ m³/s
Minimum interfacial area, $A_i$1.13 m²
Selected vessel (horizontal)$D=0.6$ m, $L=2.4$ m ($A_i=1.44$ m²)
Water draw-off leg height$0.86H = 0.52$ m
Check: the design assumes the oil droplets are 150 µm and monodisperse and that Stokes' law applies ($Re=0.18<1$, confirmed). A hydrocyclone or coalescer would be needed if the true droplet size were much smaller; the 10 % dispersion-band and mid-height-interface assumptions are given design targets, met by keeping $u_c