Poiseuille's Law Calculator

Enter a tube's radius and length, the pressure difference driving the flow, and the fluid's viscosity to find the volumetric flow rate, mean and centerline velocity, and wall shear stress using the Hagen-Poiseuille equation, Q = πΔPr⁴ / (8μL).

Quick Facts

Hagen-Poiseuille equation
Q = πΔPr⁴ / (8μL)
Volumetric flow rate for steady, laminar flow of a Newtonian fluid through a rigid cylindrical tube.
Fourth-power sensitivity
Q ∝ r⁴
Doubling the tube radius increases flow rate 16-fold if pressure, length, and viscosity stay fixed.
Laminar flow limit
Reynolds number < ~2300
Poiseuille's law only holds for smooth, laminar flow; turbulence above this threshold breaks the formula.

Your Results

Calculated
Volumetric Flow Rate
-
Q = πΔPr⁴ / (8μL)
Average (Mean) Velocity
-
v = Q / (πr²)
Maximum (Centerline) Velocity
-
v_max = 2 × average velocity
Wall Shear Stress
-
τ_w = ΔP·r / (2L)

Ready

Enter the tube radius, length, pressure difference, and fluid viscosity, then press Calculate.

Formula and Method for Poiseuille's Law

The Hagen-Poiseuille equation describes how a fluid flows steadily through a narrow, rigid, cylindrical tube when it is driven by a pressure difference between the two ends. First derived independently by Gotthilf Hagen and Jean Léonard Marie Poiseuille in the 1840s, it applies to laminar (smooth, non-turbulent) flow of a Newtonian fluid — one whose viscosity does not change with shear rate, such as water, air, or light oil. The volumetric flow rate is Q = πΔPr⁴ / (8μL), where ΔP is the pressure difference across the tube, r is the tube's internal radius, μ is the fluid's dynamic viscosity, and L is the tube's length.

How the calculation works

Enter the tube radius, tube length, the pressure difference driving the flow, and the fluid's dynamic viscosity, choosing whichever units match your data — the calculator converts everything to SI base units (meters, pascals, and pascal-seconds) before computing. It plugs the converted values into Q = πΔPr⁴ / (8μL) to get the volumetric flow rate, then divides by the tube's cross-sectional area (πr²) to get the average velocity. Because laminar flow through a pipe has a parabolic velocity profile, the fastest-moving fluid is at the center of the tube, moving at exactly twice the average velocity (v_max = 2 × v_avg). The calculator also reports the wall shear stress, τ_w = ΔPr / (2L), the frictional force per unit area the fluid exerts on the tube wall.

Common mistakes

  • Using diameter instead of radius: the formula calls for radius, not diameter — if you only know the diameter, divide it by 2 before entering it, or the fourth-power term will overstate flow by a factor of 16.
  • Ignoring the fourth-power radius sensitivity: because flow rate scales with r⁴, small measurement errors in radius produce large errors in the result — a 10% error in radius changes flow rate by roughly 46%.
  • Applying the formula to turbulent flow: Poiseuille's law is only valid when the Reynolds number stays below about 2300 (laminar regime); above that, turbulence dominates and this formula understates the pressure needed to sustain a given flow.
  • Mixing viscosity units: water's viscosity is about 1 mPa·s (1 centipoise) at room temperature, not 1 Pa·s — entering the wrong order of magnitude changes every result by a factor of 1000.

Real-world applications

  • Medicine uses Poiseuille's law to size IV catheters and estimate infusion rates, and to model how vessel narrowing (stenosis) restricts blood flow.
  • Microfluidics and lab-on-a-chip devices rely on it to design channel dimensions that deliver a target flow rate of reagents or samples.
  • Hydraulic and pneumatic system designers use it to size tubing and estimate pressure losses in slow, viscous-dominated flows.
  • Petroleum and chemical engineers apply it, or its turbulent-flow analogs, to estimate pumping pressure for viscous fluids in pipelines.

Frequently Asked Questions

What is Poiseuille's law?
Poiseuille's law (the Hagen-Poiseuille equation) describes the volumetric flow rate of a viscous, incompressible fluid in steady laminar flow through a rigid cylindrical tube: Q = πΔPr⁴ / (8μL), where ΔP is the pressure difference across the tube, r is the tube's internal radius, μ is the fluid's dynamic viscosity, and L is the tube's length.
Why does flow rate depend so strongly on the tube radius?
Flow rate is proportional to the radius raised to the fourth power (Q ∝ r⁴), because a wider tube both increases the cross-sectional area and lets fluid move faster near the center for a given pressure gradient. Doubling a tube's radius increases flow rate 16-fold at the same pressure difference, which is why even small narrowing or clogs dramatically cut flow.
When does Poiseuille's law not apply?
The formula assumes steady, laminar flow (Reynolds number below roughly 2300), a Newtonian fluid with constant viscosity, a rigid straight cylindrical tube, and no entrance or exit effects. It breaks down for turbulent flow, non-Newtonian fluids such as blood at very low shear rates, flexible or non-circular tubes, and very short tubes where entrance effects dominate.
What is wall shear stress and why does it matter?
Wall shear stress (τ_w = ΔPr / (2L)) is the frictional force per unit area that the moving fluid exerts on the tube's inner wall. It matters in biomedical engineering, where abnormal shear stress on blood vessel walls is linked to plaque formation, and in process engineering, where it affects fouling and erosion near pipe walls.