Calculate flow rate through orifices, nozzles, and weirs using discharge coefficients. Covers sharp-edge, rounded, and Venturi flow elements with Cd lookup tables.
The Discharge Coefficient Calculator determines volumetric flow rate through orifices, nozzles, Venturi tubes, and weirs by applying the appropriate discharge coefficient (Cd). The discharge coefficient corrects the theoretical (ideal) flow rate to account for real-world effects like viscous friction, flow contraction, and turbulence. That makes the result much more useful than an ideal-flow estimate when sizing or checking real hardware.
For orifice plates: Q = Cd × A × √(2ΔP/ρ), where Cd accounts for the vena contracta effect (flow contraction downstream of the orifice). Sharp-edge orifices have Cd ≈ 0.61. Rounded nozzles: Cd ≈ 0.95-0.99. Venturi tubes: Cd ≈ 0.98. The calculator also handles weir flow: Q = Cd × (2/3) × L × √(2g) × H^(3/2) for rectangular weirs.
Enter the flow element type, geometry, fluid properties, and differential pressure to calculate actual flow rate with the appropriate discharge coefficient. It gives you a realistic flow number instead of an idealized one.
Use this calculator when you need a realistic flow estimate from a measured pressure drop instead of an ideal Bernoulli result. It is helpful for orifice sizing, quick checks against ISO-style coefficients, and comparing how different primary elements trade accuracy against permanent pressure loss. That helps when selecting a flow element for measurement or piping work.
Orifice/Nozzle: Q = Cd × A₂ × √(2ΔP/ρ) / √(1 - β⁴). Where β = d/D (diameter ratio), A₂ = π d²/4 (orifice area). Rectangular Weir: Q = Cd × (2/3) × L × √(2g) × H^(3/2). V-Notch Weir: Q = Cd × (8/15) × tan(θ/2) × √(2g) × H^(5/2). Reynolds-dependent Cd: Reader-Harris/Gallagher equation (ISO 5167).
Result: Cd = 0.607, Q = 7.3 L/s
β = 50/100 = 0.5. A₂ = π×0.05²/4 = 0.00196 m². Q = 0.607 × 0.00196 × √(2×10000/1000) / √(1-0.5⁴) = 0.00729 m³/s = 7.3 L/s. Velocity through orifice: 3.7 m/s.
The sharp-edge orifice plate is the most common flow measurement device in process industries. ISO 5167-2 specifies detailed requirements: sharp upstream edge (radius < 0.0004d), plate thickness, pipe straightening requirements (minimum straight pipe lengths upstream/downstream), and pressure tap locations (corner, D and D/2, or flange taps).
The standard provides the Reader-Harris/Gallagher equation for Cd as a function of Re_D and β, which is accurate to ±0.5% for 0.2 ≤ β ≤ 0.75 and Re_D > 5000.
Weirs are used for open-channel flow measurement. The rectangular weir (with end contractions) uses Cd ≈ 0.62 (Francis formula). The V-notch (triangular) weir gives better accuracy at low flows; Cd ≈ 0.58 for a 90° notch. The Cipolletti (trapezoidal) weir has 1:4 side slopes that compensate for end contractions, simplifying the formula.
Flow measurement elements create permanent pressure loss. For orifice plates, the permanent loss is 40-90% of the measured differential pressure, depending on β. For Venturi tubes, it's only 5-20%. For nozzles, 30-60%. This pressure loss requires pumping energy, so element selection affects operating cost in large installations.
Cd is the ratio of actual flow to theoretical (ideal) flow. It accounts for energy losses not captured by Bernoulli's equation: friction, flow separation, turbulence, and the vena contracta effect. Cd < 1 always (actual flow is always less than ideal). Typical values: sharp-edge orifice 0.60-0.65, ISA nozzle 0.95-0.99, Venturi 0.98-0.99.
At a sharp-edge orifice, the flow separates at the edge and forms a vena contracta (minimum area) approximately 0.5 pipe diameters downstream. The actual flow area is only about 61% of the orifice area (contraction coefficient ≈ 0.61). Combined with friction losses, total Cd ≈ 0.60-0.65.
Beta (β = d/D) is the diameter ratio. For very small β (<0.2), Cd approaches 0.598. As β increases toward 0.7, Cd increases toward 0.62-0.65 for sharp-edge orifices. β should be between 0.2 and 0.75 for accurate measurement. Very large β (>0.75) gives unreliable results.
At low Reynolds numbers (Re_D < 10,000), Cd decreases because viscous effects become significant. The Reader-Harris/Gallagher equation (ISO 5167) accounts for Re effects. For most industrial applications (Re_D > 100,000), Cd is nearly constant at the fully turbulent value.
A Venturi tube has a gradual convergence, a short throat, and a gradual diffuser. The smooth geometry minimizes flow separation and turbulence losses, giving Cd ≈ 0.98-0.995. The trade-off: Venturis are larger, heavier, and more expensive than orifice plates. They also produce less permanent pressure loss.
Orifice plate: cheapest, easy to replace, but highest permanent pressure loss (40-90% of ΔP). Nozzle: moderate cost and loss. Venturi: most expensive, but lowest pressure loss (5-20% of ΔP) — best for large pipes or when pumping power matters. For measurement, orifice plates cover 90%+ of applications.