Results
| Channel (connection order) | Flow rate [µL/min] | Pressure drop [kPa] | Resistance [kPa/(µL/min)] | Re |
|---|
Each channel uses the resistance equation for its rectangular or circular cross-section. The model assumes steady, fully developed laminar flow of an incompressible Newtonian fluid and omits local losses at junctions. The signs of flow rate and pressure drop follow the connection order shown in the table.
Rectangular cross-section R = 12μL / {ab³ [1 − (192b/π⁵a) Σ tanh(nπa/2b)/n⁵]}. Here, a is the larger of the width and height, and b is the smaller. The series is evaluated for odd n = 1, 3, …, 99.
Circular cross-section R = 8μL/(πr⁴) (Hagen–Poiseuille equation). Here, r is the radius.
μ is the dynamic viscosity and L is the channel length. Resistance R is calculated in SI units [Pa·s/m³], and flow rate follows from Q = ΔP/R.