Coriolis Micro Flow Sensor
Introduction
Accurate mass flow sensing is of the utmost importance for a vast number of micro-fluidic applications, such as DNA or chemical analysis devices. Using a Coriolis force-based sensor, a number of problems can be overcome in comparison to other flow sensor devices. The main advantages of a Coriolis-based sensor are that it is independent of:
· |
temperature |
· |
flow profile |
· |
density |
· |
viscosity |
· |
homogeneity |
The main principle of a Coriolis sensor can be seen in figure 1:

If there is a mass flow in the given direction, the Coriolis force causes the U-shaped loop which is vibrated with a frequency ω to deform over the angle θc. The force (and hence the deformation) is directly proportional to the mass flow rate:
![]()
Demands on the sensor
· |
Liquid flows with a maximum of 1 g/hr (H2O) |
· |
Low stiffness to maximize sensitivity (thin tube walls) |
· |
Maximum pressure drop = 0.5 bar |
This results in the following estimate for an U-shaped tube:
total length of tube: 10 mm
diameter of tube: 40 µm
Mode of operation
The sensor can be operated in two modes: the “swing” and the “torsion” mode. When operated in Swing mode, the Coriolis force gives rise to a torsional mode (which is measured), and vice versa:
|
|
|||
Actuation: Detection: |
Swing Torsion |
Torsion Swing |
|
Fabrication process of SiRN tubes

First results





