Published on 27 August 2019
The flow rate in every fluidic system can be computed with the following equation:
∆P=Q×Rh
Where: ∆P is the pressure difference between the inlet and the outlet of the system, Q is the flow rate throughout the system, Rh is the fluidic resistance of the system.
This equation is analog to the one that applies for electronic systems
∆U=i×RΩ
Calculations for the equivalent resistance with resistors in series or in parallel apply similarly for fluidics and electronics. Kirchhoff’s law for circuit calculations is also similar in both domains.
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Let’s take the example of a microfluidic chip with channels that are 500 µm wide, 70 µm high and 2 cm long. The fluidic resistance is quite small and implies an approximate pressure of 1 mbar for a flow rate of 5 µL/min. A user wanting to control the flow rate with an OB1 MK3+ 200 mbar and a flow-sensor MFS 2 will meet several difficulties:
– The resolution of 0.1 mbar of the OB1 200 mbar will only allow steps of 0.5 µL/min. The precision of the flow sensor becomes inadequate
– Flow rate instabilities may appear due to its sensitivity to small pressure variations
– The flow sensor will saturate at low pressure/high flow rate, leaving the major part of the pressure range unusable. The performance regarding the usable pressure range will be degraded.
Regarding the former example, it is easy to match the instrument performances to the setup by adding a flow restrictor in series with the microfluidic chip.
Increasing the resistance of the system enables decreasing its sensitivity; hence increasing its stability.
Nevertheless, the maximum reachable flow rate becomes smaller, which sometimes can be a limitation for flushing the system.
Flow restrictors consist of capillaries with different diameters. Their resistance depends on their inner diameter (ID), their length and the viscosity of the liquid that flows through them.
The flow restrictor should be connected directly on the reservoir. Due to the connector size, the flow restrictor must be longer than 10 cm. If it is long enough, the flow restrictor can be directly connected to the flow sensor or other instrument. Otherwise, it can be connected to an intermediate capillary adapted junction (see picture).
The following table gives the resistance of different flow restrictors for different liquids. A selection of Flow resistance kits can be found here.
Note that these values are given for a 1 cm-long flow restrictor. Since the resistance is proportional to the capillary length, you can easily adjust the length to reach the desired fluidic resistance.
With water, flow restrictors with an ID of 64 µm and a length of 10 cm will give a resistance of 38 mbar/(µL/min). A pressure drop of 38 mbar across the restrictor will result in a flow rate of 1 µL/min.
To reach the best flow control, the maximum pressure of your OB1 must match the maximum flow rate of your flow sensor, e.g. an OB1 200 mbar for a 7 µL/min flow sensor gives an ideal resistance of 28 mbar/(µL/min).
In the former example, the user cannot flush the system with a flow rate higher than 7 µL/min, which can be limiting for transient phases. If the user wants to reach a max flow rate of 20 µL/min, a resistance of 10 mbar/(µL/min) is more adapted.
Important Note : This table is not intended to provide absolute values for a particular setup and should only be seen as a beginners’ guide. The microfluidic resistance should be refined based on each setup characteristics. The particular conditions of your use and application of our products are beyond our control. Only a test in the specific conditions of your application will determine the appropriateness of a flow resistance size, which remains a hypothesis among other parameters (e.g. biophysical model chosen, length of fluidic channel, pressure source, chip height, etc …). To go even further in understanding the hydraulic resistance in microchannels, we highly recommend the following article on flow restrictors: Reexamination of Hagen-Poiseuille flow: Shape dependence of the hydraulic resistance in microchannels – NA Mortensen, F Okkels, H Bruus – Physical Review E 71 (5), 057301.
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