There is one line in a tall-building chilled-water schematic that behaves completely differently from all the others, and it catches out engineers who have spent their careers on closed systems. The condenser water circuit is open — it ends in a cooling tower basin that is exposed to atmosphere — so the return column does not push back. The pump lifts the full height, every second, forever. Put the chillers in the basement and the towers on the roof of a 300 m tower and you have just specified 817 kW of condenser pumping to move heat you could have moved for a tenth of that. This single distinction, more than any efficiency curve, is what dictates where heat rejection plant goes in a tall building — and in the Gulf it competes with a second constraint that is becoming the harder one: the towers will drink about 2,400 m³ of water a day.

1 · The open circuit: what cancels and what does not

In a closed chilled-water loop the water that goes up comes back down and the static head cancels, which is why a 600 m tower needs only tens of metres of pump head — the argument set out in chilled-water pumps. The condenser circuit is the one loop in the building with an open surface in it, and the near-universal assumption is that this breaks the cancellation. It does not — provided the return leg runs full and sealed back to the pump suction:

\[ H_{CW} \;=\; \underbrace{z_{header} - z_{basin}}_{\text{a few metres, at the tower}} \;+\; h_{f} \;+\; h_{nozzle} \]

The break in the circuit sits at the top, where the water is at atmospheric pressure anyway. The rising column still has a falling column behind it, so the pump's differential head is friction, nozzle pressure and the short lift from the basin water level to the distribution header — not the height of the building. This is standard tower-pump sizing [1][2], and it is worth stating plainly because the opposite is asserted constantly.

What does not cancel is pressure. Static head that is recovered energetically is still present mechanically. Every metre between the plant and the tower basin puts 0.0981 bar on the condenser barrels, pumps, valves, strainers and gaskets at the bottom of the riser. At 150 m that is 14.7 bar — already past a standard 150 psi waterbox. At 600 m it is 59 bar, past anything in a catalogue.

And the cancellation is conditional, which is where the real risk lives. It is lost — completely — if:

Those four bullets, not the ρgh, are what drive the architecture:

2 · Interactive: what the open circuit really costs

Set how far the tower basin sits above the condenser pumps. The blue line is the pump power when the return column is kept full and sealed — flat, because the static cancels. The red curve is the same duty once that column is broken. The dotted line, on the right axis, is the static pressure the plant sits at regardless of which case you are in.

Condenser pump power vs tower height above the pumps
P = Q·H/(102·η). Sealed full return column: H = friction + nozzle only, independent of height. Broken column (open sump at plant level, or a part-full riser): H = static lift + friction + nozzle. Via a plate heat exchanger: friction + nozzle + 8 m for the exchanger. The dotted line is the static pressure at the plant, 0.0981 bar per metre, against standard 150 psi and 300 psi waterbox ratings.
Open Pump hydraulic power as a calculator
Vertical separation between the condenser pumps and the tower basin.
Roughly 0.05 L/s per kW of heat rejected at a 5 K range.
Condenser, pipework, strainer and tower distribution nozzles.
Wire-to-water for a large condenser pump.
Static at the plant
14.7 bar
Pump · sealed column
63 kW
Pump · via plate HX
83 kW
If the column breaks
440 kW
Pressure class
300 psi rating needed

Lift the basin 150 m above the pumps and the plant sits at 14.7 bar — past a standard 150 psi waterbox before anything else has happened — while the pump, if the return column is kept full and sealed, needs only 25 m of head and 63 kW. Break that column and the same duty costs 440 kW: a 377 kW continuous penalty, about 1,980 MWh a year, bought entirely with a hydraulic detail. So the open circuit's real cost is pressure class, and its real risk is whether the return leg stays full — at start-up, at part load, and after every trip. Closing the loop through a plate heat exchanger costs about 8 m of extra pumping (83 kW) and roughly 1 K of condenser approach, which is about 2.5 % on the chiller; what it buys is a building-side circuit that never sees the tower's static at all. That, not pump energy, is why the exchanger is usually the right answer above about 100 m.

3 · Approach, range and where the efficiency actually is

A cooling tower is defined by two temperature differences and one ambient condition[1][2]:

The design lever is that condenser water temperature and tower fan energy pull in opposite directions: a colder tower means a bigger, harder-working fan but a much more efficient chiller. The chiller is far larger than the fan, but fan power climbs steeply as the approach tightens, so the optimum is a real balance rather than a one-sided push — and its position is set by the fan-to-chiller power ratio, not by either machine alone. What is unambiguous is the operating case: a condenser-water reset that tracks the actual wet bulb is one of the highest-value control sequences in the plant, because for most of the year the wet bulb is far below design and the chiller will take every degree you give it.

4 · Interactive: approach, wet bulb & total plant power

Set the design wet bulb and the approach you are buying. The chart is total plant power — chiller plus tower fan — against approach, showing the optimum and how far it moves when the climate changes.

Chiller + tower fan power vs design approach
Condenser water leaving = wet bulb + approach. Chiller power scaled 2.5 % per K from a 30 °C reference; fan power scaled as (reference approach / approach)^1.6 to represent the airflow needed to close the approach.
Riyadh ≈ 20 °C, Jeddah and Doha ≈ 29 °C, London ≈ 20 °C.
Leaving water minus wet bulb. Tighter = larger tower and bigger fan.
Compressor power at 30 °C entering condenser water.
Total tower fan power for the design airflow at a 5 K approach.
Condenser water
33.0 °C
Chiller power
1,290 kW
Fan power
129 kW
Total
1,419 kW
Optimum approach
4.9 K

At a Jeddah wet bulb of 29 °C, a 4 K approach gives 33 °C condenser water and about 1,419 kW of combined plant power, with the optimum sitting at 4.9 K. The balance is genuine rather than one-sided: the chiller is fourteen times the size of the fan, but the fan power rises steeply as the approach tightens, so the two meet near 5 K. What moves the answer is the ratio — halve the fan power and the optimum falls to 3.8 K; double it and it climbs to 6.4 K. Drop the wet bulb to Riyadh's 20 °C and the whole curve falls by roughly a fifth for the same building: the same tower and the same chiller are a fundamentally different plant on the coast than they are inland. Design the tower for the site's wet bulb, not for a regional average, and reset the condenser set-point against measured wet bulb in operation.

5 · Water — the constraint that is overtaking energy

A cooling tower rejects heat mainly by evaporating water, and that water is consumed. The arithmetic is simple and the totals are startling[3]:

\[ E \approx \frac{\dot{Q}}{h_{fg}} \approx 1.5\ \text{m}^3/\text{h per MW rejected}, \qquad B = \frac{E}{\text{CoC}-1}, \qquad M = E + B \]

where \(E\) is evaporation, \(B\) blowdown and \(M\) makeup, and cycles of concentration (CoC) is how many times the dissolved solids are allowed to concentrate before water is dumped. A 50 MW tower evaporates 75 m³/h no matter what you do — that is physics — but the blowdown is entirely a water-treatment decision: at two cycles it is another 75 m³/h, at six cycles just 15. Raising the cycles from 2 to 6 saves 1,440 m³ a day on a single plant, which in a water-scarce region is a far more valuable saving than most energy measures.

Cooling tower makeup water vs cycles of concentration
E = 1.5 m³/h per MW rejected; B = E/(CoC−1); makeup M = E + B. Evaporation is fixed by physics; blowdown is a treatment decision.
Total tower duty ≈ chiller cooling × 1.25.
Limited by the makeup water chemistry and the treatment programme.
Annual operation at full rejection.
Local potable or treated-water rate, in your currency.
Evaporation
75 m³/h
Blowdown
25 m³/h
Makeup
100 m³/h
Per day
2,400
Annual cost
2.4 M

A 50 MW plant at four cycles consumes 100 m³/h — 2,400 m³ a day, comparable to the domestic demand of several thousand people. Push the cycles from 2 to 6 and the makeup falls from 150 to 90 m³/h with no change to the towers at all, purely through a better treatment programme and tighter conductivity control. In the Gulf this is where the real design conversation is heading: side-stream filtration, higher cycles, treated sewage effluent or condensate as makeup, and in some projects the decision to accept air-cooled chillers and their energy penalty rather than consume the water at all.

6 · Placement, wind and plume

7 · Water treatment and Legionella

A cooling tower is a warm, aerated, nutrient-rich aerosol generator located near fresh-air intakes and public space. Control is a designed system, not a maintenance activity[4]:

8 · Installation & execution tricks

9 · The design & installation checklist

The one-line summary Condenser water is the one open circuit in the building, but the static still cancels as long as the return column stays full and sealed — what does not cancel is the pressure, so a 150 m separation is 14.7 bar on the waterbox, and a broken return column is a 377 kW permanent penalty you will never see on a schematic. Design the tower on the site's wet bulb, optimise the approach on chiller-plus-fan power rather than tower cost (the balance lands near 5 K and moves with the fan-to-chiller power ratio), and treat the water balance as a first-order design output: 2,400 m³ a day is what a 50 MW plant drinks, and the cycles of concentration — not the towers — decide how much of that you can give back.

References & standards

  1. ASHRAE Handbook — HVAC Systems and Equipment, Cooling Towers chapter — range, approach, wet-bulb performance and tower types.
  2. Cooling Technology Institute (CTI) ATC-105 Acceptance Test Code for Water Cooling Towers and CTI certification standards — performance testing and correction to design conditions.
  3. ASHRAE Handbook — HVAC Applications, Water Treatment chapter — cycles of concentration, blowdown, scale and corrosion control, side-stream filtration.
  4. ASHRAE Standard 188 Legionellosis: Risk Management for Building Water Systems and ASHRAE Guideline 12; HSE ACOP L8 and HSG274 Part 1 for evaporative cooling systems.
  5. ANSI/ASHRAE/IES Standard 90.1 — condenser water reset, tower fan control and minimum equipment efficiency.
  6. ASHRAE Design Guide for Tall, Supertall, and Megatall Building Systems, 2nd ed. — heat rejection plant location and condenser water strategy in tall buildings.
  7. ASHRAE Handbook — Fundamentals, Climatic Design Information — design wet-bulb data by location.
  8. Saudi Building Code SBC 501 and Saudi water regulations on cooling tower makeup, alternative water sources and discharge.
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