8 Charts for Chilled Water Pipe Sizing | Augmintech
- August 13, 2026
- 2:15 pm
- Augmintech
An undersized chilled water pipe does not fail. It just quietly costs money. Velocity climbs, friction loss rises with roughly the square of it, the pump works harder every hour of every year, and somewhere on the top floor a branch never gets its design flow. All of it is decided by a number chosen in an afternoon at design stage.
This guide puts the sizing criteria for steel, copper and cast iron in one place, explains where the numbers come from, and gives you a live chart and calculator so you can size a line rather than hunt for a row in a PDF.
- TL;DR
- The Two Sizing Criteria
- The Chilled Water Pipe Sizing Chart
- Live Pipe Sizing Calculator
- Steel Pipe, Schedule 40
- Copper Pipe, Type L
- Cast Iron Pipe Data
- The Hazen-Williams Formula
- Dynamic Losses Through Fittings and Valves
- Fluid Properties That Change the Answer
- Worked Example: Primary Secondary Network
- A Note on Insulation
- FAQs
- Sources and Further Reading
TL;DR
Key takeaways
- Every pipe is sized against two criteria at once: a pressure drop limit and a velocity limit. Whichever gives the smaller flow governs.
- Typical design values are 1 to 4 ft water per 100 ft (roughly 100 to 400 Pa/m) and 1.5 to 3 m/s for steel, with copper held lower to limit erosion corrosion.
- There is a crossover: below about DN150 the friction criterion governs; above about DN200 the velocity limit takes over. Knowing which one is binding tells you what to change.
- Steel Schedule 40 is the default for mains and risers. Copper Type L suits smaller sizes and final connections. Cast iron is not used for pressurised chilled water, only gravity drainage.
- Hazen-Williams has no viscosity term. It is calibrated for water at 40 to 75°F near 1.1 cSt, while chilled water at 7°C is nearer 1.43 cSt, so it cannot correct for the difference and cannot handle glycol at all.
- Against Darcy-Weisbach on chilled water, Hazen-Williams at C = 100 overestimates friction by 66 to 79%, while C = 130 lands within about 10%. The C value you pick matters more than the formula.
- Fittings are frequently the larger share of the loss in a plant room. One fully open globe valve is worth roughly twenty long radius bends.
- Glycol is denser, more viscous and lower in specific heat than water, and all three push toward a larger pipe.
The Two Sizing Criteria
Pipe sizing looks like a lookup and is actually a comparison. You apply two independent limits to the same pipe and take the more restrictive answer. For context on the wider system these pipes serve, see our guide to HVAC chilled water systems.
Criterion 1: Pressure Drop
Friction loss per unit length, because that is what the pump pays for continuously. Design practice is normally expressed as feet of water per 100 feet of pipe, and common values sit between 1 and 4.
| ft water / 100 ft | Pa / m | kPa / 100 m | When used |
|---|---|---|---|
| 1.0 | 98 | 9.8 | Long runs, district schemes, energy led design |
| 2.0 | 196 | 19.6 | Conservative commercial design |
| 3.0 | 294 | 29.4 | Common default, Carrier Systems Design basis |
| 4.0 | 392 | 39.2 | Upper end, space constrained risers |
Criterion 2: Velocity
Velocity limits exist at both ends, for different reasons.
- Minimum, around 0.6 to 1 m/s. Below this, entrained air is not swept along to the vent points and can collect at high points, forming an air lock that blocks flow entirely.
- Maximum, around 3 m/s for steel. Above this, noise becomes noticeable in occupied areas and erosion accelerates. The Carrier Systems Design criterion of 10 ft/s, which is 3.05 m/s, is the widely used ceiling.
- Copper is held lower, commonly 1.2 to 2.4 m/s, because copper suffers erosion corrosion at elevated velocity. The damage concentrates on the inside of elbows and at fitting entries where flow is turbulent.
Which criterion is binding, and why it matters
Run the numbers across the size range and a pattern emerges. On steel at 4 ft/100 ft, friction governs everything up to about DN150, and the velocity limit takes over from about DN200 upward. That crossover is worth knowing because it tells you what to change when a size does not work. If friction is binding, dropping the friction rate or going one size up fixes it. If velocity is binding, going up a size is the only option, because relaxing the friction target will not help. The tables below flag which criterion governs each row.
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The Chilled Water Pipe Sizing Chart
This is the friction chart in its usual form: flow rate along the bottom, pressure gradient up the side, one curve per pipe size, both axes logarithmic. Constant velocity lines run diagonally across it, and the shaded band marks the normal design zone.
Figure 1: Chilled water pipe friction chart for Schedule 40 steel at 7°C. Use the calculator below to plot your own duty on it.
How to Read the Chart in Three Steps
- Find your flow rate on the bottom axis
Read across the logarithmic scale in litres per second. Convert from m³/h by dividing by 3.6, or from US GPM by dividing by 15.85.
- Go up to the design band
Travel vertically until you reach the shaded 200 to 400 Pa/m zone. That is the normal target for commercial chilled water.
- Read the pipe size curve you land on, then check velocity
The curve passing through that region gives your size. Now check where the point sits relative to the diagonal velocity lines. If it is above the 3 m/s line, the velocity limit is binding and you must go up a size regardless of what the friction reading says.
A note on the format of this chart
You will often see this chart circulated as a scanned image or a base64 embedded picture. This version is drawn as live vector graphics generated from the Darcy-Weisbach equation with a Colebrook-White friction factor, the same basis as the published ASHRAE friction chart. That means it scales without blurring on any screen, it can be read by search engines and screen readers rather than being an opaque image, and the calculator below can plot your operating point directly onto it. The underlying assumptions are stated in full at the end of this article.
Live Pipe Sizing Calculator
Enter a flow rate and the calculator applies both criteria, tells you which one governs, and marks your point on the chart above.
Learn to Apply Sizing Charts Like This in Real Projects
Load to flow, index circuit head build-up, pipe and pump schedules on real project drawings.
Steel Pipe, Schedule 40
Black steel to ASTM A53 or A106 in Schedule 40 is the default for chilled water mains and risers. It is economical at larger sizes, mechanically strong, available in every diameter, and welds or grooves readily.
The table below gives maximum flow for each size under both criteria at 4 ft per 100 ft and 3.05 m/s, with the governing one highlighted.
| Nominal | Bore (mm) | Max flow, friction | Max flow, velocity | Governing capacity | m³/h | US GPM |
|---|---|---|---|---|---|---|
| 1/2 in, DN15 | 15.8 | 0.1 L/s | 0.6 L/s | 0.1 L/s (friction) | 0.4 | 2 |
| 3/4 in, DN20 | 20.9 | 0.2 L/s | 1.0 L/s | 0.2 L/s (friction) | 0.9 | 4 |
| 1 in, DN25 | 26.6 | 0.5 L/s | 1.7 L/s | 0.5 L/s (friction) | 1.7 | 7 |
| 1-1/4 in, DN32 | 35.1 | 1.0 L/s | 3.0 L/s | 1.0 L/s (friction) | 3.4 | 15 |
| 1-1/2 in, DN40 | 40.9 | 1.5 L/s | 4.0 L/s | 1.5 L/s (friction) | 5.2 | 23 |
| 2 in, DN50 | 52.5 | 2.9 L/s | 6.6 L/s | 2.9 L/s (friction) | 10 | 45 |
| 2-1/2 in, DN65 | 62.7 | 4.6 L/s | 9.4 L/s | 4.6 L/s (friction) | 16 | 73 |
| 3 in, DN80 | 77.9 | 8.2 L/s | 14.5 L/s | 8.2 L/s (friction) | 29 | 129 |
| 4 in, DN100 | 102.3 | 16.8 L/s | 25.1 L/s | 16.8 L/s (friction) | 61 | 267 |
| 5 in, DN125 | 128.2 | 30.6 L/s | 39.4 L/s | 30.6 L/s (friction) | 110 | 485 |
| 6 in, DN150 | 154.1 | 49.7 L/s | 56.9 L/s | 49.7 L/s (friction) | 179 | 788 |
| 8 in, DN200 | 202.7 | 102.4 L/s | 98.4 L/s | 98.4 L/s (VELOCITY) | 354 | 1,560 |
| 10 in, DN250 | 254.5 | 186.3 L/s | 155.2 L/s | 155.2 L/s (VELOCITY) | 559 | 2,459 |
| 12 in, DN300 | 303.2 | 295.1 L/s | 220.2 L/s | 220.2 L/s (VELOCITY) | 793 | 3,490 |
Amber rows are where the velocity limit governs rather than friction. Note the crossover at DN200: below it, friction is the binding constraint; above it, velocity is. Bores are nominal Schedule 40 internal diameters; confirm against the actual specification, since a heavier schedule reduces bore and pressure drop varies with roughly the fifth power of diameter.
Steel or Copper?
- Cost crossover. Copper is competitive at small sizes where labour dominates and jointing is quick. Steel becomes markedly cheaper as diameter grows, which is why you rarely see copper above about DN100 on chilled water.
- Size range. Steel covers the full range up to and beyond DN600. Copper availability and cost effectively cap it well below that.
- Corrosion. A closed chilled water loop with proper water treatment protects steel well, because the oxygen is consumed early and not replenished. Where treatment is unreliable, copper's inherent corrosion resistance is worth paying for. In coastal and humid GCC and Indian locations, the more likely corrosion problem is external, under damaged insulation, which affects both materials.
- Velocity headroom. Steel tolerates higher velocity than copper, which matters on space constrained risers.
Copper Pipe, Type L
Type L is the usual grade for chilled water and building services, heavier walled than Type M and lighter than Type K. Its lower velocity ceiling is the key sizing difference against steel.
| Nominal | Bore (mm) | Max flow, friction | Max flow, velocity | Governing capacity | m³/h | US GPM |
|---|---|---|---|---|---|---|
| 1/2 in | 13.8 | 0.1 L/s | 0.4 L/s | 0.1 L/s (friction) | 0.3 | 1 |
| 3/4 in | 19.9 | 0.2 L/s | 0.7 L/s | 0.2 L/s (friction) | 0.8 | 3 |
| 1 in | 26.0 | 0.5 L/s | 1.3 L/s | 0.5 L/s (friction) | 1.7 | 7 |
| 1-1/4 in | 32.1 | 0.8 L/s | 1.9 L/s | 0.8 L/s (friction) | 3.0 | 13 |
| 1-1/2 in | 38.2 | 1.3 L/s | 2.8 L/s | 1.3 L/s (friction) | 4.6 | 20 |
| 2 in | 50.4 | 2.7 L/s | 4.8 L/s | 2.7 L/s (friction) | 10 | 43 |
| 2-1/2 in | 62.6 | 4.9 L/s | 7.4 L/s | 4.9 L/s (friction) | 18 | 77 |
| 3 in | 74.8 | 7.9 L/s | 10.5 L/s | 7.9 L/s (friction) | 28 | 125 |
| 4 in | 99.2 | 16.7 L/s | 18.5 L/s | 16.7 L/s (friction) | 60 | 265 |
| 6 in | 148.5 | 48.9 L/s | 41.6 L/s | 41.6 L/s (VELOCITY) | 150 | 659 |
| 8 in | 196.2 | 102.3 L/s | 72.6 L/s | 72.6 L/s (VELOCITY) | 261 | 1,150 |
Note that copper's velocity crossover arrives one size earlier than steel, at 6 in rather than 8 in, purely because of the lower velocity ceiling. Copper is hydraulically smoother than steel, so at the same bore it carries slightly more flow for the same friction, but the velocity limit takes that advantage back at larger sizes.
Why copper gets a lower velocity limit
It is not a friction issue, it is a metallurgical one. Copper is subject to erosion corrosion, where fast moving water strips the protective oxide film from the pipe wall faster than it can reform, and the bare metal then corrodes. The effect is velocity dependent and concentrates exactly where turbulence is highest: the inside of elbows, the entry to fittings, and anywhere a burr or protruding solder ring disturbs the flow. That is why the limit is lower on hot water than cold, why it is lower still on recirculating systems, and why good workmanship at joints matters more on copper than on steel.
Cast Iron Pipe Data
Cast iron appears in this article's outline, and the most useful thing to say about it is a clarification: cast iron is not used for pressurised chilled water distribution. It belongs to a different part of the building.
Where you will meet it:
- Gravity drainage. Soil and waste stacks, particularly where acoustic performance matters, because cast iron is significantly quieter than plastic for falling water in a stack adjacent to occupied space.
- AHU condensate drainage in some specifications, for the same durability and acoustic reasons.
- Older retrofit systems, where existing buried or riser pipework may be cast iron and has to be surveyed, assessed and either retained or replaced.
- Buried municipal and fire mains, usually ductile iron rather than grey cast iron in modern work.
If you are surveying an old cast iron system
The critical figure is not the nominal dimension but the effective bore after tuberculation. Unlined cast iron corrodes internally over decades, building up nodular deposits that both reduce the bore and dramatically increase roughness. A Hazen-Williams C value that started around 130 when new can fall to 100 or well below in an aged unlined pipe, and since friction scales with C to the power 1.852, dropping C from 150 to 100 roughly doubles the friction loss for the same flow. Never size a retrofit from new-pipe data. Measure, or assume conservatively.
The Hazen-Williams Formula
For the Darcy-Weisbach approach used in detailed hydraulic design, see our companion guide on pressure drop piping calculations — it covers friction factor, Reynolds number, and equivalent length methods for fittings.
Hazen-Williams is an empirical formula from 1902 that estimates friction loss for water without needing viscosity, Reynolds number or a friction factor. That simplicity is why it survives in fire protection, municipal water and irrigation work.
- hf head loss, metres of water
- L pipe length, metres
- Q flow rate, cubic metres per second
- C Hazen-Williams roughness coefficient, dimensionless
- D internal diameter, metres
Note what is absent: there is no viscosity term, no density term and no Reynolds number. The coefficient C bundles all roughness and flow effects into one empirical number, which is exactly what makes the formula quick and exactly what limits it.
| Material | C, new | C, design | Note |
|---|---|---|---|
| PVC, HDPE, plastics | 150 | 150 | Does not degrade with age |
| Copper, brass | 140 to 150 | 140 | Very smooth |
| Cement lined ductile iron | 140 | 130 to 140 | Lining protects the bore |
| New steel | 130 | 120 | The usual chilled water assumption |
| Welded or galvanised steel | 120 | 120 | Standard design value |
| Old, tuberculated cast iron | 100 or below | 100 or below | Survey rather than assume |
Worked Example
-
State the duty
42 L/s of chilled water through 100 m of DN100 Schedule 40 steel, bore 102.3 mm, taking C = 120 for design.
-
Convert to SI base unitsQ=0.042m³/sD=0.1023m
-
Substitutehf=10.67×100×0.0421.8521201.852×0.10234.87hf = 28.2 m over 100 m, or 2,763 Pa/m
-
Cross-check against Darcy-Weisbach
The same duty solved properly, with a Colebrook-White friction factor at 7°C, gives 2,247 Pa/m. Hazen-Williams at C = 120 is 23% high here. That is conservative, so it will not undersize the pipe, but it will oversize the pump if carried through to a head calculation unchecked.
The limitation that matters for chilled water specifically
Hazen-Williams is calibrated for water in turbulent flow at roughly 40 to 75°F (5 to 25°C), assuming a kinematic viscosity near 1.1 cSt. Chilled water at 7°C sits at the cold edge of that window with a viscosity closer to 1.43 cSt, about 30% higher, and the formula has no viscosity term with which to account for it. For glycol solutions it is simply invalid, since they differ from water in density, viscosity and specific heat all at once. Use Darcy-Weisbach with a Colebrook-White friction factor for chilled water design, and treat Hazen-Williams as a quick check rather than the basis of an issued calculation.
| Duty | Darcy-Weisbach | HW at C=100 | HW at C=120 | HW at C=130 |
|---|---|---|---|---|
| DN50, 10 L/s | 4,206 Pa/m | 6,993 (+66%) | 4,989 (+19%) | 4,302 (+2%) |
| DN100, 42 L/s | 2,247 Pa/m | 3,873 (+72%) | 2,763 (+23%) | 2,382 (+6%) |
| DN150, 90 L/s | 1,222 Pa/m | 2,160 (+77%) | 1,541 (+26%) | 1,329 (+9%) |
| DN200, 160 L/s | 924 Pa/m | 1,650 (+79%) | 1,177 (+27%) | 1,015 (+10%) |
The practical conclusion: the C value you choose matters more than the choice of formula. At C = 130 the two methods agree within about 10%. At C = 100 they diverge by three quarters. If you use Hazen-Williams, be deliberate about C and know which direction the error runs.
Dynamic Losses Through Fittings and Valves
Straight pipe friction is only part of the total. Every bend, tee, valve and transition adds a dynamic loss, and in a compact plant room those losses commonly exceed the straight pipe entirely.
Because the velocity head term ρV²/2 scales with velocity squared, fitting losses grow rapidly with velocity. A fitting on a fast main costs far more than the identical fitting on a slow branch, which is another argument for the lower end of the velocity band wherever space allows.
| Fitting | K | Note |
|---|---|---|
| Long radius 90° bend | 0.2 to 0.4 | The preferred elbow |
| Standard 90° elbow | 0.5 to 0.9 | Roughly double the long radius loss |
| Tee, flow through run | 0.2 to 0.4 | Straight through path |
| Tee, flow through branch | 1.0 to 1.8 | The branch path costs far more |
| Gate valve, fully open | 0.15 to 0.2 | Isolation duty, very low loss |
| Butterfly valve, fully open | 0.3 to 0.9 | Varies strongly with disc size |
| Globe valve, fully open | 6 to 10 | Regulating duty, very high loss |
| Swing check valve | 2 to 2.5 | Routinely forgotten in head build-ups |
| Y strainer, clean | 2 to 3 | Rises sharply as it fouls |
| Sudden exit to tank | 1.0 | All velocity head is lost |
Fluid Properties That Change the Answer
Every table above assumes water. Three properties decide how far reality departs from that.
| Fluid | Density (kg/m³) | Kinematic viscosity (m²/s) | Specific heat (kJ/kg·K) | Effect on sizing |
|---|---|---|---|---|
| Water at 7°C | 1000 | 1.43 × 10−6 | 4.20 | Baseline for chilled water |
| Water at 20°C | 998 | 1.00 × 10−6 | 4.18 | Reference condition in most tables |
| Water at 32°C | 995 | 0.77 × 10−6 | 4.18 | Condenser water, lower friction |
| 30% ethylene glycol at 7°C | ~1045 | ~4.0 × 10−6 | ~3.6 | Higher friction and higher flow needed |
| 30% propylene glycol at 7°C | ~1035 | ~6.0 × 10−6 | ~3.8 | More viscous still than ethylene |
Glycol figures vary with concentration and supplier. Always use the manufacturer's published property data for the actual mixture rather than a generic value.
How Each Property Bites
- Viscosity raises friction loss directly, through a higher friction factor at the same velocity. Chilled water at 7°C is already about 40% more viscous than the 20°C reference most published tables assume, which is why this article's tables are computed at 7°C rather than 20°C.
- Density raises both the pressure loss for a given velocity and the mass the pump must move. Glycol at roughly 1045 kg/m³ is about 4.5% denser than water.
- Specific heat is the one people forget. Glycol carries less heat per kilogram, so you need more volumetric flow for the same cooling duty at the same delta T. That larger flow then has to pass through a pipe that is already more resistive because of the viscosity. The two effects compound.
Worked Example: Primary Secondary Network
A 250 TR plant, two chillers, serving four floors. Design delta T is 5°C, so total flow is 42 L/s. Here is where each sizing decision applies.
| Leg | Flow | Size | Velocity | Governing | Note |
|---|---|---|---|---|---|
| Each primary loop (per chiller) | 21 L/s | DN125 | 1.63 m/s | Friction | Short circuit, low head, size generously |
| Common header and decoupler | 42 L/s | DN150 | 2.25 m/s | Friction | Decoupler sized to carry full imbalance at low loss |
| Secondary main | 42 L/s | DN150 | 2.25 m/s | Friction | The index run starts here |
| Riser after 1st floor takeoff | 31.5 L/s | DN125 | 2.44 m/s | Friction | Reduce as load drops off |
| Riser after 2nd floor takeoff | 21 L/s | DN125 | 1.63 m/s | Friction | One size may serve two segments |
| Floor branch | 10.5 L/s | DN100 | 1.28 m/s | Friction | Includes balancing valve allowance |
| AHU connection | 2.6 L/s | DN50 | 1.20 m/s | Friction | Plus control valve, strainer, isolation |
Three things this example demonstrates
Size each section for the flow it actually carries, not for the plant total. The riser reduces at every takeoff, and that stepping down is where most of the material saving on a project lives. The decoupler is a special case: it must carry the full flow imbalance between the loops at negligible resistance, so it is sized generously and never fitted with a valve. And only the index run sets the pump head, so identify the hydraulically worst path first, because sizing every branch beautifully and then totalling the wrong path gives you the wrong pump.
A Note on Insulation
Pipe sizing and insulation are specified together, because the insulated outside diameter is what actually has to fit through the building.
- Insulation thickness scales with pipe size, so a larger pipe costs void space twice over: once for the bore and again for the thicker jacket around it. Coordinate the insulated OD, not the nominal size.
- The vapour barrier matters more than the thickness on chilled water in humid climates. A cold surface below the ambient dew point will condense moisture, and if the barrier is broken that moisture reaches the pipe wall inside the insulation, where it corrodes steel from the outside in, invisibly, for years.
- Seal at every interruption. Supports, valves, flanges and hanger penetrations are where vapour barriers fail. A perfectly insulated straight run with an unsealed valve box is not insulated.
- External corrosion under insulation is the dominant failure mode for chilled water pipework in coastal Indian and GCC locations, more than internal corrosion in a properly treated closed loop.
Where This Skill Leads
Pipe sizing is one of the first genuinely engineering tasks a junior MEP engineer is handed, and it is a good test of whether someone understands a system or only a table. Our dedicated pipe sizing calculation guide covers the full step-by-step method beyond the chart lookup. Reading a chart is straightforward. Knowing which criterion is binding, what a C value assumption costs you, why the fittings on a short plant room run outweigh a long straight riser, and how glycol changes all of it, is the part that turns into a defensible design.
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Frequently Asked Questions
Sources and Further Reading
- ASHRAE Handbook: Fundamentals, Pipe Sizing and Fluid Flow chapters, ASHRAE. Source of the friction chart basis, fitting loss data and fluid property tables for water and glycol solutions.
- ASPE Data Book, American Society of Plumbing Engineers. Velocity and pressure drop criteria for copper and steel water piping.
- Carrier System Design Manual, Part 3, Piping Design. Source of the widely used 10 ft/s velocity ceiling and the ft per 100 ft pressure drop criteria.
- Crane Technical Paper No. 410, Flow of Fluids Through Valves, Fittings and Pipe. The standard industry reference for loss coefficients, valve data and worked hydraulic examples.
- ASME B36.10M, Welded and Seamless Wrought Steel Pipe, for Schedule 40 dimensional data, and ASTM B88 for copper water tube Types K, L and M.
- Copper Development Association guidance on velocity limits and erosion corrosion in copper tube systems.
Calculation basis for this article's charts, tables and tools
All pressure gradients, the friction chart and the sizing tables are computed from the Darcy-Weisbach equation with a Colebrook-White friction factor, the same basis as the published ASHRAE friction chart, solved iteratively. Assumptions: chilled water at 7°C, density 1000 kg/m³, kinematic viscosity 1.43 × 10−6 m²/s; absolute roughness 0.045 mm for commercial steel and 0.0015 mm for copper; nominal Schedule 40 and Type L internal diameters. Note this differs from many published tables computed at 20°C, which understate chilled water friction. The Hazen-Williams comparison uses the SI form with the 10.67 constant. Fitting K values are indicative order of magnitude figures for orientation. These are teaching and first pass design tools. Issued designs should use validated hydraulic software, manufacturer valve data and the standards adopted by your project.
Standards are revised on fixed cycles. Confirm the edition adopted by your project before issuing a specification. This article was last verified against the sources above on 1 August 2026.
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