8 Charts for Chilled Water Pipe Sizing | Augmintech

Facebook
LinkedIn
WhatsApp

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.

📏
Two criteria
Friction and velocity
🔁
Crossover
Around DN200
Hazen-Williams
No viscosity term
🔧
Fittings
Often the larger share

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.

Table 1: Pressure drop criteria in both unit systems
ft water / 100 ftPa / mkPa / 100 mWhen used
1.0989.8Long runs, district schemes, energy led design
2.019619.6Conservative commercial design
3.029429.4Common default, Carrier Systems Design basis
4.039239.2Upper 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.

Master Chilled Water Pipe Design

Learn pipe sizing, pressure drop calculation, fittings allowances, insulation specification, and full piping design for HVAC systems — structured for India and GCC MEP careers.

GET COURSE

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.

Chilled Water Pipe Friction Chart, Steel Schedule 40 at 7°C
DESIGN BAND 200 to 400 Pa/m 1 m/s 2 m/s 3 m/s DN15DN20DN25 DN32DN40DN50 DN65DN80DN100 DN125DN150DN200 DN250DN300 FLOW RATE (L/s) PRESSURE GRADIENT (Pa/m) 0.1110 100500 10,0001,00010010
Scroll horizontally, or tap EXPAND for fullscreen
Pipe size curves, DN15 to DN300 Constant velocity lines Normal design band Your operating point

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

  1. 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.

  2. 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.

  3. 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.

Chilled Water Pipe Sizing
Flow rate
Flow unit
Material
Friction target (Pa/m)
Fluid
Run length (m)

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.

Explore the live course

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.

Table 2: Steel Schedule 40 chilled water capacity, 4 ft/100 ft and 3.05 m/s limits
NominalBore (mm)Max flow, frictionMax flow, velocityGoverning capacitym³/hUS GPM
1/2 in, DN1515.80.1 L/s0.6 L/s0.1 L/s (friction)0.42
3/4 in, DN2020.90.2 L/s1.0 L/s0.2 L/s (friction)0.94
1 in, DN2526.60.5 L/s1.7 L/s0.5 L/s (friction)1.77
1-1/4 in, DN3235.11.0 L/s3.0 L/s1.0 L/s (friction)3.415
1-1/2 in, DN4040.91.5 L/s4.0 L/s1.5 L/s (friction)5.223
2 in, DN5052.52.9 L/s6.6 L/s2.9 L/s (friction)1045
2-1/2 in, DN6562.74.6 L/s9.4 L/s4.6 L/s (friction)1673
3 in, DN8077.98.2 L/s14.5 L/s8.2 L/s (friction)29129
4 in, DN100102.316.8 L/s25.1 L/s16.8 L/s (friction)61267
5 in, DN125128.230.6 L/s39.4 L/s30.6 L/s (friction)110485
6 in, DN150154.149.7 L/s56.9 L/s49.7 L/s (friction)179788
8 in, DN200202.7102.4 L/s98.4 L/s98.4 L/s (VELOCITY)3541,560
10 in, DN250254.5186.3 L/s155.2 L/s155.2 L/s (VELOCITY)5592,459
12 in, DN300303.2295.1 L/s220.2 L/s220.2 L/s (VELOCITY)7933,490

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.

Table 3: Copper Type L chilled water capacity, 4 ft/100 ft and 2.4 m/s limits
NominalBore (mm)Max flow, frictionMax flow, velocityGoverning capacitym³/hUS GPM
1/2 in13.80.1 L/s0.4 L/s0.1 L/s (friction)0.31
3/4 in19.90.2 L/s0.7 L/s0.2 L/s (friction)0.83
1 in26.00.5 L/s1.3 L/s0.5 L/s (friction)1.77
1-1/4 in32.10.8 L/s1.9 L/s0.8 L/s (friction)3.013
1-1/2 in38.21.3 L/s2.8 L/s1.3 L/s (friction)4.620
2 in50.42.7 L/s4.8 L/s2.7 L/s (friction)1043
2-1/2 in62.64.9 L/s7.4 L/s4.9 L/s (friction)1877
3 in74.87.9 L/s10.5 L/s7.9 L/s (friction)28125
4 in99.216.7 L/s18.5 L/s16.7 L/s (friction)60265
6 in148.548.9 L/s41.6 L/s41.6 L/s (VELOCITY)150659
8 in196.2102.3 L/s72.6 L/s72.6 L/s (VELOCITY)2611,150

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.

Hazen-Williams, SI form
hf= 10.67×L×Q1.852 C1.852×D4.87
  • 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.

Table 4: Hazen-Williams C values by material and condition
MaterialC, newC, designNote
PVC, HDPE, plastics150150Does not degrade with age
Copper, brass140 to 150140Very smooth
Cement lined ductile iron140130 to 140Lining protects the bore
New steel130120The usual chilled water assumption
Welded or galvanised steel120120Standard design value
Old, tuberculated cast iron100 or below100 or belowSurvey rather than assume

Worked Example

  1. 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.

  2. Convert to SI base units
    Q=0.042m³/sD=0.1023m
  3. Substitute
    hf=10.67×100×0.0421.8521201.852×0.10234.87
    hf = 28.2 m over 100 m, or 2,763 Pa/m
  4. 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.

Table 5: Hazen-Williams against Darcy-Weisbach, chilled water at 7°C in steel
DutyDarcy-WeisbachHW at C=100HW at C=120HW at C=130
DN50, 10 L/s4,206 Pa/m6,993 (+66%)4,989 (+19%)4,302 (+2%)
DN100, 42 L/s2,247 Pa/m3,873 (+72%)2,763 (+23%)2,382 (+6%)
DN150, 90 L/s1,222 Pa/m2,160 (+77%)1,541 (+26%)1,329 (+9%)
DN200, 160 L/s924 Pa/m1,650 (+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.

Dynamic loss at a fitting
Δp=K× ρV22
Or as an equivalent length of straight pipe
Leq=K×Df

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 Loss Calculator
Velocity (m/s)
Straight pipe (m)
Pipe gradient (Pa/m)
Long radius bends
Tees, branch flow
Gate valves, open
Globe valves, open
Check valves
Strainers
Butterfly valves, open
Table 6: Indicative K values for chilled water fittings
FittingKNote
Long radius 90° bend0.2 to 0.4The preferred elbow
Standard 90° elbow0.5 to 0.9Roughly double the long radius loss
Tee, flow through run0.2 to 0.4Straight through path
Tee, flow through branch1.0 to 1.8The branch path costs far more
Gate valve, fully open0.15 to 0.2Isolation duty, very low loss
Butterfly valve, fully open0.3 to 0.9Varies strongly with disc size
Globe valve, fully open6 to 10Regulating duty, very high loss
Swing check valve2 to 2.5Routinely forgotten in head build-ups
Y strainer, clean2 to 3Rises sharply as it fouls
Sudden exit to tank1.0All velocity head is lost

Fluid Properties That Change the Answer

Every table above assumes water. Three properties decide how far reality departs from that.

Table 7: Properties of chilled water and glycol solutions
FluidDensity (kg/m³)Kinematic viscosity (m²/s)Specific heat (kJ/kg·K)Effect on sizing
Water at 7°C10001.43 × 10−64.20Baseline for chilled water
Water at 20°C9981.00 × 10−64.18Reference condition in most tables
Water at 32°C9950.77 × 10−64.18Condenser water, lower friction
30% ethylene glycol at 7°C~1045~4.0 × 10−6~3.6Higher friction and higher flow needed
30% propylene glycol at 7°C~1035~6.0 × 10−6~3.8More 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.

Table 8: Sizing each leg of a 250 TR primary secondary network
LegFlowSizeVelocityGoverningNote
Each primary loop (per chiller)21 L/sDN1251.63 m/sFrictionShort circuit, low head, size generously
Common header and decoupler42 L/sDN1502.25 m/sFrictionDecoupler sized to carry full imbalance at low loss
Secondary main42 L/sDN1502.25 m/sFrictionThe index run starts here
Riser after 1st floor takeoff31.5 L/sDN1252.44 m/sFrictionReduce as load drops off
Riser after 2nd floor takeoff21 L/sDN1251.63 m/sFrictionOne size may serve two segments
Floor branch10.5 L/sDN1001.28 m/sFrictionIncludes balancing valve allowance
AHU connection2.6 L/sDN501.20 m/sFrictionPlus 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.

Not Sure Which Course Fits Your Background?

Talk to an advisor about where you are now and the fastest route into an HVAC or MEP design role.

Book a counselling call

Frequently Asked Questions

Which pipe is used for chilled water?
Black steel to ASTM A53 or A106, normally Schedule 40, is the default for mains and risers because it is economical at larger sizes, strong and available in every diameter. Copper, usually Type L, is common at smaller sizes and final connections for its ease of jointing and corrosion resistance. Cast iron is not used for pressurised chilled water, only gravity drainage. Galvanised steel is generally avoided, since the zinc coating can be attacked by treated closed loop water chemistry.
What velocity should chilled water pipes be designed for?
1.5 to 3 m/s is the normal band for distribution, mains toward the upper end and branches lower. Below about 1 m/s entrained air may not be swept to vent points. Above about 3 m/s noise and erosion become concerns. Copper is held lower, commonly 1.2 to 2.4 m/s, because erosion corrosion of copper is velocity dependent and concentrates at elbows and fitting entries.
What pressure drop should chilled water pipes be sized for?
1 to 4 feet of water per 100 feet, approximately 100 to 400 Pa/m, with many offices standardising on 3 to 4 ft/100 ft for mains. A lower friction rate gives larger pipes with lower pumping energy but higher material cost, so it is an economic trade off between first cost and operating cost over the system life rather than a fixed rule.
Is the Hazen-Williams formula suitable for chilled water?
Only with caution. It is calibrated for water in turbulent flow at roughly 40 to 75°F assuming about 1.1 cSt viscosity. Chilled water at 7°C sits at the cold edge of that window at nearer 1.43 cSt, and the formula has no viscosity term to correct for it. It cannot be used for glycol at all. Use Darcy-Weisbach with a Colebrook-White friction factor for chilled water design and treat Hazen-Williams as a quick check. Note also that the C value matters more than the formula: at C = 130 the two agree within about 10%, at C = 100 they diverge by three quarters.
What size is a standard cold water pipe?
There is no single standard size, because size follows flow. In domestic plumbing, 15 mm and 22 mm copper are common for branches with 28 mm for small mains. In commercial chilled water systems sizes run from DN25 on individual fan coil connections to DN300 and beyond on plant room headers. The correct size is always set by the flow the pipe carries, checked against both a pressure drop criterion and a velocity limit, with the more restrictive governing.
How do fittings affect chilled water pipe sizing?
Fittings add dynamic loss, calculated as a loss coefficient K multiplied by velocity head, or approximated as an equivalent length of straight pipe. Their contribution is routinely underestimated. In a compact plant room where a few metres of pipe carry isolation valves, a check valve, a strainer, a balancing valve and several bends, the fittings can exceed the straight pipe friction several times over. One fully open globe valve at K around 8 is worth roughly twenty long radius bends.
Does glycol change chilled water pipe sizing?
Yes, in three compounding ways. Glycol is denser than water, so it carries more mass at the same volumetric flow. It is significantly more viscous, especially at low temperature, which raises friction loss for the same flow and pipe size. And it has lower specific heat, so a higher volumetric flow is needed to move the same cooling duty at the same delta T. All three push toward a larger pipe than a water calculation suggests, and Hazen-Williams cannot model any of them.

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.

Ready to start your engineering career journey?

Investing in structured training is one of the best ways to set yourself apart in MEP engineering. Our Courses cover HVAC, electrical and plumbing design in depth, plus tools like HAP software — the exact skillset that sets you apart in a competitive field.