Orifice Flow Calculator

Calculate flow rate through an orifice using Q = CdA√(2gh). Supports sharp-edged, beveled, and rounded orifice types with multiple fluids.

mm
m/s²
Theoretical Velocity
6.264 m/s
V = √(2gh)
Actual Velocity
3.821 m/s
V_act = Cd × V_th, Cd = 0.61
Volume Flow (L/min)
112.54
1.8757 L/s · 29.73 gpm
Volume Flow (m³/h)
6.7525
Q = Cd × A × √(2gh)
Mass Flow
1.8720 kg/s
ṁ = ρQ
Orifice Area
490.87 mm²
d = 25.0 mm
Head
2.000 m
ΔP = 19.58 kPa

Flow Rate by Orifice Diameter

5
10
15
20
25
30
40
50
75
100
Orifice Diameter (mm)
d (mm)Area (mm²)Q (L/min)V (m/s)
519.64.503.821
1078.518.013.821
15176.740.523.821
20314.272.033.821
25490.9112.543.821
30706.9162.063.821
401,256.6288.113.821
501,963.5450.173.821
754,417.91,012.883.821
1007,854.01,800.683.821
Planning notes, formulas, and examples

About the Orifice Flow Calculator

When fluid flows through an orifice under a head of liquid, the theoretical jet velocity follows Torricelli's theorem: V = √(2gh). The actual discharge is lower because the jet contracts and loses energy, which is why the formula uses a discharge coefficient Cd.

This calculator applies Q = Cd × A × √(2gh) for a chosen orifice size, head, and fluid. It includes common entrance geometries such as sharp-edged, beveled, and rounded openings, and it lets you compare how changes in diameter or coefficient affect both velocity and flow rate.

That makes it useful for tank drain estimates, outlet sizing, simple irrigation checks, and other first-pass hydraulic problems where the geometry is known but a full pipe-network model would be excessive. It also keeps the theoretical velocity and the corrected discharge side by side so you can see how much the coefficient changes the final flow estimate before using it for design or troubleshooting.

When This Page Helps

Use this calculator when you need a first-pass flow estimate for a tank outlet, free discharge opening, or simple metering orifice.

It is useful for drain sizing, irrigation hardware, nozzle comparison, and quick hydraulic checks where head and opening diameter are known but a full CFD or piping model is unnecessary. It also helps you compare how much a change in diameter or entrance shape matters before you spend time on a more detailed analysis.

How to Use the Inputs

  1. Select the orifice type to set the discharge coefficient (or enter a custom Cd).
  2. Choose the fluid or enter a custom density.
  3. Enter the orifice diameter in mm, or click a preset size.
  4. Enter the upstream head or pressure driving flow through the orifice.
  5. Select the head unit (m, ft, kPa, or psi).
  6. Read the theoretical and actual velocity, volume flow, and mass flow from the outputs.
  7. Compare flow rates for different orifice diameters in the table.
Formula used
Torricelli's Theorem: V = √(2gh) Actual discharge: Q = Cd × A × √(2gh) Where: • Cd = discharge coefficient (0 to 1) • A = orifice area = πd²/4 (m²) • g = gravitational acceleration (m/s²) • h = head of fluid above orifice (m)

Example Calculation

Result: Q ≈ 1.88 L/s (112 L/min)

V_th = √(2 × 9.81 × 2) = 6.26 m/s. A = π/4 × 0.025² = 4.91×10⁻⁴ m². Q = 0.61 × 4.91×10⁻⁴ × 6.26 = 1.88×10⁻³ m³/s, which is about 1.88 L/s or 112 L/min.

Tips & Best Practices

  • For submerged orifices, use the net head (upstream head minus downstream head).
  • In time-to-drain calculations, combine this formula with the continuity equation dh/dt = −Q/A_tank.
  • Beveled and rounded orifices have much higher Cd — a small machining change can nearly double the flow.
  • For pulsating flow (e.g., engine intake), use time-averaged head or integrate over the cycle.
  • Temperature affects density and viscosity — correct for high-temperature applications.

Practical Guidance

Orifice flow is a good first-order model when the discharge is driven mainly by a liquid head and the opening geometry is known. It is especially helpful for comparing candidate diameters or checking whether a target drain time or emitter rate is realistic before moving to a more detailed design.

Common Pitfalls

The largest errors usually come from using the wrong head, ignoring downstream submergence, or assuming Cd stays fixed under every condition. Free-discharge tank outlets, submerged openings, and compressible gas flow are different cases, so make sure the physical setup matches the formula before you rely on the number.

Sources & Methodology

Last updated:

Frequently Asked Questions

  • After passing through a sharp-edged orifice, the jet contracts to a cross-section smaller than the orifice. This contracted section (vena contracta) occurs about half a diameter downstream and is the point of minimum pressure and area.