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05 / Fluid systems & engineering economics

Piping & Pumping System Design

Move the fluid. Balance the cost.

A coolant-transfer design that connects hydraulic demand, pump selection and the cost of pipe diameter—and examines where the calculation needs more evidence.

My role
Member of a 3-student project team
Period
First semester 2025–2026
Tools & methods
Bernoulli · Darcy–Weisbach · Cost analysis
Project stage
Academic design study · Not built
The decision

Size the hydraulic duty first, then compare the energy and material costs of alternative diameters.

The evidence

A three-person academic calculation study; system-curve data and source limitations made explicit.

Coolant transfer / explanatory schematic 50% glycol–water
Lower open reservoir, suction-lift pump, gate valve and four-elbow pipeline to an upper open reservoir. Ten metres of elevation gain. Diagram is not to scale. 10 m elevation 01 02 / PUMP 03 LOWER RESERVOIR SUCTION LIFT UPPER RESERVOIR
5 L/s Design flow 100 m Total pipe length 10 m Static lift
Conceptual arrangement redrawn from report pp. 3–4 and 13–15. Both reservoirs are open to atmosphere. Four 90° elbows, one fully open gate valve, entrance and exit. Not to scale; fitting positions illustrate the specified inventory, not a documented installation layout.
16.37 m

Calculated head · initial pipe size

1.52 kW

Estimated pump shaft / motor-output requirement

3 inch

Report’s final nominal pipe recommendation*

Design of Thermal Fluids · King Saud University · report pp. 8, 13 and 20. *The economic recommendation is qualified below; the selected pump was assessed for the initial 2½-inch design.

01 / Set the duty

One flow requirement.
Several connected decisions.

Transfer 5 litres of coolant every second through 100 metres of carbon-steel pipe, with a 10-metre rise between two atmospheric reservoirs.

Our three-person team worked from the fluid properties and fitting inventory to select an initial pipe, calculate losses, choose a pump and examine the economics of other diameters. This was a calculation-based course project, not a commissioned system.

Fluid
50% ethylene glycol–water
Density / viscosity
1,080 kg/m³ / 0.005 Pa·s
Pipe roughness
0.045 mm
Initial pipe
2½-inch nominal, Schedule 40
62.71 mm internal diameter

Source: pp. 3–6. Fluid-property values are the report’s inputs; their temperature basis is not specified.

02 / Build the hydraulic requirement

The lift is only
part of the load.

Static elevation, pipe friction and fitting losses all contribute to the required head. An independent arithmetic check reproduces the headline result.

10.00 m Static elevation 5.75 m Pipe friction
Fittings add 0.62 m 10 + 5.75 + 0.62 ≈ 16.37 m
01 / Flow 1.62 m/s

Velocity from the initial pipe area.

02 / Regime ≈21,928

Reynolds number; turbulent flow.

03 / Losses 0.027

Darcy factor from the Moody chart; ΣK = 4.65.

04 / Power 867 W

Hydraulic power, before efficiency losses.

Report pp. 7–9. Budget values independently recomputed from the stated inputs and rounded. The report’s rounded area produces a slightly different Reynolds number in Table 3.

Hydraulic demand

The system sets the head.

Head / m
Required head
0 10 20 30 0 2 4 6 8 Flow rate / L/s 1.0 L/s: 10.37 m 2.0 L/s: 11.22 m 3.0 L/s: 12.56 m 3.5 L/s: 13.28 m 4.0 L/s: 14.21 m 5.0 L/s: 16.37 m 5.5 L/s: 17.50 m 6.0 L/s: 18.71 m 7.0 L/s: 21.65 m 7.5 L/s: 23.28 m 8.0 L/s: 24.95 m 8.5 L/s: 26.56 m
5 L/s → 16.37 m head · f = 0.027

Source: report p. 9, Table 3. All 12 calculated points preserved; straight segments connect samples. Friction factors were read individually from a Moody chart. Dashed horizontal line: 10 m static lift.

View the underlying system-curve data
Report Table 3 · original calculation precision
Flow / L/s Velocity / m/s Re f Head / m
1 0.323729362 4385.030754 0.041 10.37406855
2 0.647458725 8770.061509 0.033 11.22370403
3 0.971188087 13155.09226 0.0305 12.56168315
3.5 1.133052768 15347.60764 0.0285 13.27804885
4 1.294917449 17540.12302 0.028 14.21339064
5 1.618646811 21925.15377 0.027 16.37047742
5.5 1.780511492 24117.66915 0.0262 17.50214647
6 1.942376174 26310.18453 0.0255 18.71352529
7 2.266105536 30695.21528 0.025 21.65138954
7.5 2.427970217 32887.73066 0.0248 23.27949417
8 2.589834898 35080.24603 0.0245 24.94557125
8.5 2.751699579 37272.76141 0.024 26.56444261

03 / Select against the duty

Read the intersection.
Then check the power.

The report overlays the system curve on a centrifugal-pump performance chart at 1,750 rpm. Near the design flow of 80 US gpm, it identifies an approximately 180 mm impeller.

1,750rpm ≈180mm impeller ≈57%efficiency

The 57% efficiency estimate comes from the selection chart on p. 12. Dividing 867 W by that efficiency gives about 1.52 kW at the pump shaft. Motor efficiency and sizing margin are not included.

Original annotated figure retained because complete manufacturer curve data are not tabulated. No invented performance curve or new operating point is added.

Report p. 13, Fig. 3: team’s system-curve overlay on a Fristam performance chart (report reference 3). Original figure; approximate chart readings.

04 / Check the suction side

Placement is a
design constraint.

The report obtains a maximum suction lift of approximately 0.67 m. It is a conditional calculation, not an installation clearance proven safe.

0.76 m required NPSH 1.00 m assumed margin 1.76 m target available NPSH

The calculation uses 101.325 kPa atmospheric pressure and 6.666 kPa vapor pressure at 100°C. However, it applies the full 100 m pipe length and all fitting losses to the suction side, and reads a glycol vapor-pressure chart without establishing the 50% mixture’s value.

Before specifying pump elevation, the suction-only layout, mixture properties and operating temperature must be established. The 0.67 m result should not be reused as a general cavitation limit.

Source: report pp. 13–15. NPSHr ≈ 2.5 ft (0.76 m), read from the original pump chart.

05 / Compare the trade-off

Spend more on pipe.
Less on pumping.

The useful finding is the competing trend. The cost period and model assumptions determine what “economic” actually means.

Economic comparison

A larger pipe changes the balance.

Cost / USD
Pipe + one year’s energy Pipe cost · one-off Energy · annual
0 800 1,600 2,400 50 55 60 65 Internal diameter / mm 49.26 mm: 2076.51 USD 52.52 mm: 1895.62 USD 53.97 mm: 1840.09 USD 58.42 mm: 1734.35 USD 59.01 mm: 1725.92 USD 62.71 mm: 1694.09 USD 66.64 mm: 1689.75 USD 49.26 mm: 797.89 USD 52.52 mm: 850.70 USD 53.97 mm: 874.18 USD 58.42 mm: 946.26 USD 59.01 mm: 955.82 USD 62.71 mm: 1015.75 USD 66.64 mm: 1079.41 USD 49.26 mm: 1278.62 USD 52.52 mm: 1044.92 USD 53.97 mm: 965.90 USD 58.42 mm: 788.09 USD 59.01 mm: 770.10 USD 62.71 mm: 678.34 USD 66.64 mm: 610.34 USD
62.71 mm · Pipe $1015.75 · Energy $678.34/year · Combined $1694.09

Source: report p. 19, Table 6. All seven samples preserved. Combined cost adds pipe capital to one year of energy; it is not a 15-year life-cycle cost. The table’s 62.71 mm energy value differs from p. 17.

View the underlying cost data
Report Table 6 · original values (USD)
ID / mm Pipe · once Energy · annual Combined
49.26 797.8933 1278.620457 2076.514
52.52 850.6974 1044.923531 1895.621
53.97 874.1839 965.9044944 1840.088
58.42 946.2632 788.0894612 1734.353
59.01 955.8198 770.1025962 1725.922
62.71 1015.751 678.3399548 1694.091
66.64 1079.407 610.3375013 1689.745
Table 6 / diameter comparison

One year, not fifteen.

The displayed sum combines pipe cost with a single year of pumping energy. At 62.71 mm it reports $678.34/year, versus $713.94/year in the earlier energy calculation. That difference remains unresolved.

Separate example / pp. 17–18

$11,724.85 over 15 years.

The report separately calculates $1,015.75 + 15 × $713.94. This is an undiscounted pipe-and-energy sum, excluding pump purchase, installation, maintenance and replacement costs.

Study assumptions: 8,000 operating hours/year; 0.22 SAR/kWh, converted in the report to 0.05866 USD/kWh; 57% efficiency. Historical assumptions, not a current quotation or tariff.

06 / The recommendation

A standard size.
A qualified choice.

The report moves from an initial 2½-inch Schedule 40 design to a final 3-inch Schedule 40 recommendation after reporting a theoretical economic diameter of 64.45 mm.

That is a conceptual recommendation. The displayed optimization uses one year of energy, fixed friction and simplified linear pipe pricing. Its final 3-inch Schedule 40 choice is not one of the tabulated comparison points.

2½″Initial design
3″Recommended

Nominal sizes · illustrative comparison, not a scale drawing

07 / Engineering review

Know what the model
does—and does not—prove.

The calculations tell a useful design story. Reviewing their assumptions is part of that story, rather than evidence of a built or validated pumping system.

Reproducible hydraulic duty

Using D = 0.06271 m, Q = 0.005 m³/s, f = 0.027 and ΣK = 4.65 independently gives 16.372 m head and 867.29 W hydraulic power. These agree with the report’s rounded 16.37 m and 867.18 W. The original Table 3 values remain unchanged in the chart.

Cost model and optimum need reconciliation

Table 6 is a first-year combined-cost comparison, despite the conclusion’s life-cycle wording. The table’s energy value does not reproduce the earlier design-point calculation. The 64.45 mm optimum is reported, not independently validated, and the tabulated IDs include schedules other than 40 despite later wording. A smaller economic diameter alone does not prove that the required flow cannot be delivered.

The pipe-price reference numbering also needs correction. The stated 1,177 USD/ton and 8.63 kg/m give 10.15751 USD/m and 1,015.751 USD for 100 m; the intermediate printed unit price differs slightly. A final selection needs a consistent cost period, schedule-specific prices and a revised pump/system intersection.

The vibration check has a dimensional error

On p. 10, fLV²/(2gD) is head in metres, but the report labels its ≈57.44 result as kPa. Multiplying by ρg gives approximately 609 kPa per 1,000 m using the stated inputs. This does not support the report’s claim that the pressure loss is far below its cited 557–679 kPa range. No verified low-noise or vibration result is claimed here.

Cavitation is conditional on the suction layout

The 0.67 m lift result uses full-system losses on the suction side and an unverified mixture vapor-pressure assumption. Suction pipe lengths, fittings, fluid properties and temperature need to be reconciled before an installation recommendation.

The takeaway

Connect the calculation
to the decision.

This project brought hydraulic sizing, pump selection and engineering economics into one design process. It strengthened my ability to work within a team, compare alternatives and recognize when a plausible result still depends on unresolved assumptions.

Source: the complete 23-page course report. Shared team work; no unverified individual attribution, physical construction or experimental performance is claimed. Original reports and student identifiers are not published.

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