Poiseuille's Law Calculator

Enter your pipe's radius, length, dynamic viscosity, and pressure drop to calculate the volumetric flow rate (Q) using Poiseuille's Law (Hagen-Poiseuille equation). Switch the calculation mode to solve for pressure drop, pipe radius, pipe length, or viscosity instead. You'll also get the average velocity and Reynolds number to confirm laminar flow conditions.

Pa

Pressure difference between inlet and outlet (Pascals)

m

Inner radius of the pipe in meters

m

Length of the pipe in meters

Pa·s

Dynamic viscosity of the fluid (water ≈ 0.001 Pa·s at 20°C)

m³/s

Required only when solving for pressure drop, radius, length, or viscosity

Results

Primary Result

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Flow Rate (Q)

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Pressure Drop (ΔP)

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Average Velocity (v)

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Reynolds Number (Re)

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Flow Regime

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Flow Resistance (R)

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Flow Parameters Breakdown

Frequently Asked Questions

What is Poiseuille's Law (Hagen-Poiseuille equation)?

Poiseuille's Law (also called the Hagen-Poiseuille equation) describes the volumetric flow rate of a viscous, incompressible fluid through a long, straight, cylindrical pipe under laminar flow conditions. The formula is Q = (π·ΔP·r⁴) / (8·η·L), where Q is flow rate, ΔP is pressure drop, r is pipe radius, η is dynamic viscosity, and L is pipe length.

Why does pipe radius have such a large effect on flow rate?

Because flow rate (Q) is proportional to the fourth power of the radius (r⁴). This means doubling the pipe radius increases flow rate by a factor of 16 (2⁴). Even small changes in radius dramatically affect how much fluid can pass through a pipe, which is why this relationship is critical in medical applications like blood vessel constriction.

What are the conditions for Poiseuille's Law to apply?

Poiseuille's Law applies only under specific conditions: the flow must be laminar (Reynolds number < 2100), the fluid must be Newtonian and incompressible, the pipe must be straight, rigid, and cylindrical with a constant circular cross-section, and the flow must be fully developed (steady-state). It does not apply to turbulent flow or non-Newtonian fluids like blood at high shear rates.

How do I calculate flow resistance using Poiseuille's Law?

Flow resistance (R) is calculated as R = 8·η·L / (π·r⁴). It is the ratio of pressure drop to flow rate (R = ΔP / Q), analogous to electrical resistance in Ohm's Law. Higher viscosity, longer pipes, and smaller radii all increase flow resistance, reducing the flow rate for a given pressure difference.

What is the Reynolds number, and why does it matter here?

The Reynolds number (Re) is a dimensionless quantity that predicts whether flow is laminar or turbulent. It is calculated as Re = (2·ρ·v·r) / η, where ρ is fluid density and v is average velocity. For Poiseuille's Law to be valid, Re must be less than approximately 2100 (laminar regime). Values above 4000 indicate turbulent flow, and Poiseuille's equation no longer applies.

What are typical real-world applications of Poiseuille's Law?

Poiseuille's Law is widely used in biomedical engineering to model blood flow in capillaries and arteries, in hydraulic system design, in microfluidics, in IV drip rate calculations, and in designing piping networks for water, oil, or chemical transport. It helps engineers select appropriate pipe diameters and predict pressure losses in fluid systems.

What is the dynamic viscosity of common fluids?

Common dynamic viscosity values include: water at 20°C ≈ 0.001 Pa·s (1 mPa·s), blood ≈ 0.003–0.004 Pa·s, air at 20°C ≈ 0.0000181 Pa·s, glycerin ≈ 1.5 Pa·s, and honey ≈ 2–10 Pa·s. Temperature significantly affects viscosity — most liquids become less viscous as temperature increases.

Can Poiseuille's Law be used for gases like air?

Yes, Poiseuille's Law can be applied to gases under certain conditions — specifically when the flow is laminar, the pressure changes are small relative to absolute pressure (so the gas behaves as incompressible), and the Mach number is very low. In pulmonary physiology, it is used to model airflow in small airways of the lungs where these conditions are approximately met.

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