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Darcy-Weisbach Pressure Drop

This formula calculates how much pressure is lost due to friction when fluid flows through a straight pipe. It equals a friction factor f times (length divided by diameter) times (density times velocity squared divided by 2). The friction factor depends on the pipe roughness and the Reynolds number. For example, a long, narrow, rough pipe causes a much bigger pressure drop than a short, wide, smooth one. Engineers use it to size pumps and choose pipe diameters.

Chemical Engineering Fluid Mechanics Process Design
VORZEP · FLUID MECHANICS & PIPE FLOW TOOLS

Darcy–Weisbach Pressure Drop Calculator

Solve the classic pipe-loss relation ΔP = f · (L/D) · (ρv²)/2 for any of its six unknowns — pressure drop, friction factor, pipe length, diameter, fluid density, or velocity — with step-by-step math, a live pipe schematic, and companion head-loss metrics.

ΔP = f · ( L / D ) · ( ρ · v² ) / 2 · friction · geometry · dynamic pressure
Solve for
Pressure Drop (ΔP) Pressure lost to friction as the fluid travels along the pipe. Expressed here in Pa; 1 bar = 100,000 Pa, 1 psi = 6,894.76 Pa. Typical: a few hundred Pa in a short HVAC duct, 10–50 kPa in a water main, and 1–10 MPa in a long oil pipeline. The Darcy–Weisbach form is valid for both laminar and turbulent flow once f is chosen correctly.
Pa
Pressure drop must be greater than zero.
Friction Factor (f) The Darcy–Weisbach friction factor — a dimensionless measure of how much the pipe wall resists the flow. In fully developed laminar flow f = 64/Re exactly. In turbulent flow it depends on Reynolds number and relative roughness, and is read from the Moody chart or the Colebrook equation. Typical: 0.005–0.01 for smooth polished pipe, 0.02–0.03 for commercial steel, 0.04–0.08 for aged cast iron or heavy corrosion. Note: the Darcy factor is 4× the older Fanning factor.
–
Friction factor must be greater than zero.
Pipe Length (L) Straight-run length of pipe carrying the flow, in metres. For a network, use the total equivalent length including fittings: each elbow, valve, or tee is replaced by an equivalent length of straight pipe (Le/D from a handbook). Typical: 5–30 m for a domestic branch, 100–1,000 m for a plant run, 10–1,000 km for a transmission pipeline.
m
Length must be greater than zero.
Pipe Diameter (D) Internal diameter of the pipe, in metres. Use the true inside diameter — wall thickness and scale build-up matter. Because ΔP ∝ 1/D, diameter is the single most powerful variable: a 10% reduction in D raises the pressure drop by about 11% at constant flow. Typical: 0.015 m for a domestic branch, 0.05–0.3 m for plant piping, 0.5–1.2 m for transmission mains.
m
Diameter must be greater than zero.
Fluid Density (ρ) Mass per unit volume of the fluid being pumped. Air at 20 °C and 1 atm is 1.204 kg/m³; water at 20 °C is 998 kg/m³; seawater 1025 kg/m³; SAE 30 oil about 890 kg/m³; mercury 13,546 kg/m³. Pressure drop is directly proportional to ρ, so heavy fluids cost proportionally more to move.
kg/m³
Density must be greater than zero.
Flow Velocity (v) Average bulk velocity of the fluid through the pipe cross-section, in m/s. Because ΔP ∝ v², doubling the velocity quadruples the pressure drop — velocity is the second most powerful variable after diameter. Typical design limits: 1–3 m/s for suction lines, 2–4 m/s for water mains, 6–10 m/s for HVAC ducts, 15–30 m/s for compressed air. High velocities cause noise, erosion, and water hammer.
m/s
Velocity must be greater than zero.
PRESSURE DROP (ΔP)
79,840.0 Pa
79.84 kPa · 0.798 bar · 11.58 psi · 8.15 m H₂O
TYPICAL PIPE FLOW — WATER MAIN REGIME
ΔP = f · (L/D) · (ρv²/2)
Step-by-step solution
Pressure drop vs. velocity
Current f f × 0.7 f × 1.4
Pressure drop vs. pipe length
Current D D × 0.7 D × 1.5
Sensitivity (+1% input)
Companion head-loss metrics
Pressure drop along the pipe — live schematic
Static pressure falls along the pipe (P₁ → P₂) Flow velocity vectors (length ∝ speed) Wall shear stress opposing the flow
What the Darcy–Weisbach equation really measures
ffriction factor
×
L/Dgeometry ratio
×
½ρv²dynamic pressure
=
ΔPpressure drop

The friction factor is the engine of the loss

The Darcy friction factor f packs all the physics of the wall–fluid interaction into a single dimensionless number. In fully developed laminar flow it is purely a function of Reynolds number, f = 64/Re. In turbulent flow it depends on both Re and the relative roughness ε/D, and must be read from the Moody chart or solved implicitly with the Colebrook–White equation. Smooth pipe at high Re has f ≈ 0.008–0.012; commercial steel is typically 0.02–0.03; heavily corroded or scaled pipe can exceed 0.05. Every doubling of f doubles the pressure drop at the same flow.

Diameter dominates everything else

Because ΔP ∝ 1/D, diameter is the single most powerful variable in the equation. At the same volumetric flow, halving the diameter multiplies the pressure drop by 32 (2⁵) — a factor of 2 from the 1/D term itself and a further 16 from the velocity quadrupling as the same flow is forced through a quarter of the area. This is why modestly upsizing a pipe is the classic energy-saving move in pumping systems: a small increase in capital cost buys a large reduction in pumping power.

Velocity enters squared

ΔP scales with v², so the pressure drop is extremely sensitive to how fast the fluid is pushed. Doubling the flow rate through the same pipe quadruples the pressure drop and therefore quadruples the pumping power (since power = ΔP × Q, and Q itself doubled). This squared dependence is the reason designers aim for the lowest practical velocities — and why flow balancing in a large network is so difficult. The friction factor itself also drifts with Reynolds number, so the exponent is not exactly 2 in practice, but the v² term dominates.

Length enters linearly, roughness enters non-linearly

Pressure drop is directly proportional to pipe length — double the length and you double the loss. This linearity is what makes equivalent-length tables so useful: every fitting can be replaced by an equivalent straight length, and the whole system summed. Roughness is subtler: it only affects turbulent flow, and its influence saturates at high Re when the flow becomes fully rough and f depends only on ε/D. This is why a very rough pipe cannot be fixed by pumping slower — the friction factor stops falling once the roughness sublayer is fully exposed.

How to Use This Calculator

The Darcy–Weisbach equation links six quantities: the pressure drop ΔP, the friction factor f, the pipe length L, the internal diameter D, the fluid density ρ, and the average velocity v. Give the tool five of them and it will find the sixth.

1. Choose what to solve for

Pick any one of the six variables from the toggle. The calculator rearranges ΔP = f·(L/D)·(ρv²)/2 for whichever you choose and locks that field while you fill in the rest.

2. Enter the pipe geometry

Give the internal diameter D (not the nominal size) and the total straight-run length L. If you have fittings, convert them to equivalent lengths and add them to L for a first estimate.

3. Enter the fluid properties and flow rate

Set the density ρ from the presets (air, water, seawater, oil, mercury) or type your own. Then set the average velocity v — or derive it from volumetric flow using v = Q/(πD²/4).

4. Pick a realistic friction factor

The single most error-prone input. Use 0.005–0.01 for smooth pipe, 0.02–0.03 for commercial steel, 0.04–0.08 for rough or corroded pipe. In the Advanced panel, enter the fluid viscosity to check the Reynolds number and confirm whether the flow is laminar, transitional, or turbulent.

5. Read the result and the budget

The result card shows ΔP in Pa, kPa, bar, psi, and metres of fluid head. A colour-coded verdict classifies the flow regime, and the pressure budget bars put ΔP in context against the dynamic pressure and one atmosphere.

6. Check the schematic and the charts

The schematic shows the pressure gradient falling along the pipe, velocity vectors scaled to speed, and wall shear stress opposing the flow. The main chart plots ΔP against velocity for three friction factors; the Advanced chart plots ΔP against length for three diameters.

What This Tool Offers

Built around the Darcy–Weisbach relation ΔP = f·(L/D)·(ρv²)/2, the fundamental link between pipe friction, geometry, and flow energy.

Six-way solving

Solve for pressure drop, friction factor, length, diameter, density, or velocity. The calculator rearranges the Darcy–Weisbach equation automatically for whichever variable you choose.

Live pipe schematic

A scale drawing of the pipe with the pressure gradient falling along it, velocity vectors scaled to speed, wall-shear arrows opposing the flow, and dimension lines for L and D.

Pressure budget bars

See at a glance how the pressure drop compares with the dynamic pressure ½ρv² and with one atmosphere, so you can judge whether the loss is significant.

Flow-regime verdict

Each result is classified from creeping / nearly static through typical process piping, water mains, HVAC, and up to erosion-risk velocity, with a note when the value sits outside normal design limits.

Multi-unit hints

Each field shows the value converted to related units — kPa, bar, psi, atm and metres of fluid head for ΔP; km/h, knots and ft/s for velocity; mm for diameter.

Reference tables

A pressure unit converter, a ΔP lookup grid across lengths and velocities, typical values by pipe system, and a full variable reference table.

Reference Tables & Conversions

A pressure unit converter, a ΔP lookup grid, typical Darcy–Weisbach values by system, and the full variable list.

Pressure unit converter

Pa
kPa
bar
psi
atm
m H₂O
m Hg
= 79,840 Pa = 79.84 kPa = 0.7984 bar = 11.5799 psi = 0.78797 atm = 8.1543 m H₂O

Pressure Drop ΔP Lookup

Computed from ΔP = f·(L/D)·(ρv²/2) with ρ = 1.225 kg/m³ (air), f = 0.02, D = 0.1 m. Values in Pa. Multiply by ρ/1.225 for other fluids, and by 1/f×0.02 for other friction factors.

Length L (m)v = 1 m/sv = 5 m/sv = 10 m/sv = 20 m/sv = 50 m/sv = 100 m/s

Typical Darcy–Weisbach Values by Pipe System

Representative order-of-magnitude values. ΔP is computed from the other columns using ΔP = f·(L/D)·(ρv²/2).

Systemρ (kg/m³)D (m)L (m)v (m/s)f (–)ΔP (Pa)

Typical Friction Factors by Pipe Material

Darcy–Weisbach friction factor f for fully turbulent flow in clean, new pipe. Real values rise with age and fouling.

MaterialRelative roughness ε/DTypical f (–)Notes
Drawn tubing (copper, brass)~0.00000150.008–0.012Hydraulically smooth
PVC / plastic pipe~0.00000150.008–0.012Smooth, low loss
Commercial steel (new)~0.000450.018–0.025Standard pipework
Galvanised iron~0.00150.022–0.032Common in HVAC and water
Cast iron (new)~0.00250.025–0.035Water mains
Cast iron (aged, tuberculated)~0.02–0.050.045–0.08Heavy internal fouling
Concrete pipe~0.0030.025–0.040Large water and sewer mains
Riveted steel~0.005–0.020.035–0.060Old industrial piping

Variable Reference

SymbolMeaningTypical rangeUnits
ΔPPressure drop across the pipe1 – 10⁷Pa
fDarcy–Weisbach friction factor0.005 – 0.10–
LPipe straight-run length0.1 – 10⁶m
DPipe internal diameter0.005 – 2m
ρFluid density0.09 – 13 546kg/m³
vAverage bulk velocity0.01 – 100m/s
ReReynolds number Re = ρvD/μ10² – 10⁷–
εAbsolute wall roughness0.0000015 – 0.005m
hfHead loss hf = ΔP/(ρg)0.01 – 1000m
KLoss coefficient K = f·L/D0.1 – 10⁴–
τwWall shear stress f·ρv²/80.1 – 10³Pa

What Does ΔP = f·(L/D)·(ρv²)/2 Measure?

The Darcy–Weisbach equation is the standard engineering formula for the pressure lost to friction as a fluid flows through a pipe. It says that the pressure drop is proportional to the dynamic pressure of the flow (½ρv²), to the friction factor of the pipe wall, and to the ratio of pipe length to diameter (L/D). The equation is dimensionally clean, valid across the full range from laminar to fully turbulent flow, and used in every branch of fluid engineering — from municipal water networks and HVAC systems to oil pipelines, chemical plants, and aircraft fuel lines.

Darcy–Weisbach Formula

The defining relationship is:

ΔP = f · (L / D) · (ρ · v²) / 2

Rearranged to solve for the other five unknowns:

f = 2 · ΔP · D / (L · ρ · v²)
L = 2 · ΔP · D / (f · ρ · v²)
D = f · L · ρ · v² / (2 · ΔP)
ρ = 2 · ΔP · D / (f · L · v²)
v = √( 2 · ΔP · D / (f · L · ρ) )

Dividing through by ρg converts the equation to the head-loss form used by hydraulic engineers:

hf = f · (L / D) · v² / (2g)   (head loss in metres of fluid)

The group f·L/D is often called the loss coefficient K. Using it, the equation collapses to ΔP = K·(½ρv²) — the pressure drop is simply K times the dynamic pressure.

Darcy–Weisbach Variables

SymbolMeaningNotes
ΔPPressure dropPa; the friction loss over the pipe run
fDarcy friction factorDimensionless; 4× the Fanning friction factor
LPipe lengthm; straight-run, or straight + equivalent lengths
DInternal diameterm; the true inside diameter, not nominal size
ρFluid densitykg/m³; assume constant along the pipe
vAverage bulk velocitym/s; equal to Q / (πD²/4)
μDynamic viscosityPa·s; needed only to compute the Reynolds number

How Each Variable Affects the Result

The equation is a product, so it is linear in f, L, and ρ: doubling any of these doubles the pressure drop. Velocity enters squared, so doubling the flow velocity quadruples the loss — and, at constant pipe size, doubles the volumetric flow, so the pumping power rises by a factor of eight. Diameter enters through 1/D directly and through v² indirectly when the flow rate is fixed, giving an effective 1/D⁵ dependence at constant Q. That is why the diameter is the single most powerful design lever in any piping system.

The friction factor f is the most nuanced term. In laminar flow it falls as 1/Re, so a slower, more viscous flow has a higher f — the opposite of the turbulent trend. In turbulent flow it rises with relative roughness ε/D and falls with Re, and at high Re it saturates at a value that depends only on roughness. The transition between laminar and turbulent (Re ≈ 2300–4000) is the region where simple correlations break down and the friction factor can jump abruptly.

Length is the dullest but most honest variable: pressure drop is directly proportional to L, so adding pipe is always costly. This is why designers work hard to shorten runs, use generous bend radii to reduce equivalent lengths, and place pumps and tanks as close to the load as the layout allows.

Darcy–Weisbach Calculation Examples

Water in a steel pipe: ρ = 998 kg/m³, v = 2 m/s, D = 0.05 m, L = 100 m, f = 0.02 — solve for ΔP
ΔP = 0.02 × (100/0.05) × (998 × 4)/2 = 0.02 × 2000 × 1996 = 79,840 Pa
Air in a duct: ρ = 1.2 kg/m³, v = 10 m/s, D = 0.3 m, L = 30 m, f = 0.018 — solve for ΔP
ΔP = 0.018 × (30/0.3) × (1.2 × 100)/2 = 0.018 × 100 × 60 = 108.0 Pa
Implied friction factor: ΔP = 79,840 Pa, L = 100 m, D = 0.05 m, ρ = 998 kg/m³, v = 2 m/s
f = 2 × 79,840 × 0.05 / (100 × 998 × 4) = 7,984 / 399,200 = 0.02000
Head loss: ΔP = 79,840 Pa in water at 998 kg/m³
hf = ΔP / (ρg) = 79,840 / (998 × 9.80665) = 8.154 m of water

Frequently Asked Questions

They are the same physical idea scaled by a factor of 4. The Darcy–Weisbach factor (sometimes written fD) is what this calculator uses: ΔP = fD·(L/D)·(ρv²/2). The older Fanning factor fF is defined with a factor of 2 instead of 4 in the denominator, so fD = 4·fF. A Fanning factor of 0.005 corresponds to a Darcy factor of 0.020. Mixing the two conventions is one of the most common errors in pipe-loss calculations — if your answer is off by a factor of four, check which one your source is using. This calculator uses the Darcy convention throughout.

For laminar flow (Re < 2300) the exact answer is f = 64/Re — no chart needed. For turbulent flow, the Haaland equation is a good explicit approximation: 1/√f ≈ −1.8·log₁₀[ (ε/D / 3.7)¹·¹¹ + 6.9/Re ]. It is accurate to about 1% against the Colebrook–White equation, which is the standard but must be solved iteratively. For very rough pipe at high Re, f ≈ 0.25 / [log₁₀(ε/(3.7D))]², the fully-rough limit. In day-to-day work, a value of 0.02 for commercial steel and 0.01 for smooth plastic is often close enough for a first estimate.

Because the friction loss is the mechanical work done by the wall shear stress against the flow, and wall shear stress itself scales with the dynamic pressure ½ρv². The dynamic pressure is the kinetic energy per unit volume of the moving fluid, and it scales with v² for the same reason that kinetic energy does — it is the energy the fluid carries that must be dissipated into heat by friction. The L/D factor simply says the loss accumulates linearly along the pipe, and f is the efficiency of that dissipation. Put together: pressure drop = (friction efficiency) × (geometric accumulation) × (energy density), which is the whole equation in words.

Major losses are the friction losses in straight pipe — what the Darcy–Weisbach equation computes. Minor losses are the additional losses from fittings, bends, valves, entrances, exits, and other disturbances; despite the name, in short, compact systems they can easily dominate. Minor losses are usually written as ΔPminor = K·(½ρv²), where K is a fitting-specific loss coefficient (0.9 for a 90° elbow, 10 for a fully open gate valve, 0.5 for a sharp entrance, 1.0 for a sharp exit). To include them in this calculator, convert each fitting to an equivalent length Le = K·D/f and add it to L.

Several common reasons. First, the actual pipe is rarely the nominal size — internal diameter shrinks with wall thickness, scale, and deposits, and 1/D⁵ amplifies small errors. Second, fittings and valves are usually neglected — in a short, bendy run they can double the loss. Third, elevation change adds hydrostatic pressure that is not a friction loss at all. Fourth, the friction factor used may not match the actual Reynolds number. Fifth, the real flow may not be steady — surges, water hammer, and two-phase flow all behave differently. And finally, the pump curve gives the total head the pump delivers, which must cover friction plus elevation plus any residual pressure at the outlet — not just the friction loss computed here.

Roughness is folded into the friction factor f, not entered separately in the Darcy–Weisbach equation itself. To get f from roughness you need the relative roughness ε/D and the Reynolds number, then either read the Moody chart or use the Colebrook–White or Haaland equation. Absolute roughness ε for common materials runs from about 0.0015 mm for drawn tubing to 0.045 mm for commercial steel, 0.15 mm for galvanised iron, 0.26 mm for cast iron, and 1–5 mm for heavily tuberculated pipe. In the Advanced panel of this calculator you can enter the fluid viscosity to compute the Reynolds number and confirm which regime you are in.

The calculator works in SI internally — Pa, m, kg/m³, m/s, and a dimensionless f. The hints under each field show the value in common alternative units (kPa, bar, psi, atm for pressure; feet for length and diameter; km/h, knots, ft/s for velocity), and the pressure unit converter at the bottom of the page converts freely between all the common pressure units. If you have friction factor in the Fanning convention, multiply by 4 before entering it. If you have flow rate in m³/h, convert to velocity first with v = Q/(3600·πD²/4).

Calculating...

Variables

Symbol Quantity Unit
delta_P Pressure drop Pa
f Darcy friction factor
L Pipe length m
D Pipe diameter m
rho Fluid density kg/m3
v Average velocity m/s

What it means

The Darcy‑Weisbach equation is the standard method for calculating the pressure drop due to friction in a pipe with steady, incompressible flow. It is expressed as ΔP = f (L/D) (ρ v² / 2), where f is the Darcy friction factor (dimensionless), L is pipe length, D is internal diameter, ρ is fluid density, and v is average velocity. The friction factor depends on the Reynolds number and the relative roughness of the pipe, and it is obtained from the Moody chart or empirical correlations like the Colebrook equation. This equation is essential for designing piping systems, selecting pump sizes, and estimating energy losses. It accounts for head loss due to viscous shear. The equation is also used in conjunction with minor loss coefficients for fittings and valves. Understanding the Darcy‑Weisbach equation is crucial for civil, mechanical, and chemical engineers who work with fluid transport. It is also the basis for more complex network analysis using the Hardy Cross method.

Worked example

Darcy-Weisbach Pressure Drop – Two Examples

Real‑World
Scenario: Water flows in a 0.1 m diameter, 100 m long pipe at 2 m/s. f = 0.02, ρ = 1000 kg/m³. Find ΔP.
ParameterValue
f0.02
L100 m
D0.1 m
ρ1000 kg/m³
v2 m/s
1ΔP = f·(L/D)·(ρv²/2) = 0.02×(100/0.1)×(1000×4/2) = 40,000 Pa = 40 kPa
Result 40 kPa ✓ Moderate loss
Scenario: L = 50 m, D = 0.05 m, v = 1.5 m/s, f = 0.025, ρ = 1000 kg/m³. Find ΔP.
ParameterValue
f0.025
L50 m
D0.05 m
v1.5 m/s
1ΔP = 0.025×(50/0.05)×(1000×2.25/2) = 28,125 Pa ≈ 28.1 kPa
Result 28.1 kPa ✓ Significant loss
Key insight: ΔP increases with length, v², and friction factor – essential for pipe design.

Common mistakes

  • Friction factor f: For laminar flow, f = 64/Re; for turbulent, use the Colebrook equation or Moody chart. Do not assume a constant f.
  • Length L and diameter D: Use the same units (e.g., m).
  • Velocity v: Average velocity, not maximum.
  • Pressure drop units: The result is in Pa (N/m²) if all SI units are used.
  • Minor losses: This formula accounts only for pipe friction; add fittings, valves, and entrance/exit losses separately.

Applications

The Darcy‑Weisbach equation, ΔP = f·(L/D)·(ρv²/2), calculates the pressure drop due to friction in pipe flow. It is the most widely used formula for head loss in liquid and gas pipelines. The friction factor f depends on Reynolds number and pipe roughness, and can be determined from the Moody chart or explicit correlations. Engineers use this equation to size pumps, to design pipe networks, and to predict energy consumption in fluid transport systems. It is applied in water supply, oil and gas transportation, and chemical plant piping. By estimating the pressure drop, professionals can select appropriate pipe diameters, determine pump power requirements, and ensure that the system operates within acceptable pressure limits. Accurate prediction prevents over‑sizing of equipment and reduces operational costs.

  • Design of water distribution and sewage networks
  • Sizing of pipelines for oil, gas, and chemicals
  • Pump selection and power requirement calculations
  • Analysis of existing piping systems for capacity and energy efficiency
  • Hydraulic design of fire protection systems