In this paper, the influences of Magnus force on the behaviour of small particles inside a microfluidics- based device are
theoretically investigated. The Magnus force is a lift force, which is caused by the rotation of particles within fluid flow. Explicit
relations are presented for calculating the Magnus force exerted on small particles inside fluid flow with small Reynolds numbers.
Moreover, the effects of the radius of a particle on the Magnus force are discussed. The obtained results and formulation would be
helpful in the design of inertial microfluidics-based devices.
Keywords:Inertial Microfluidics; Particle Separation; Magnus Force; Microsystems
Microtechnology and nanotechnology [1-8]. have many
promising applications in various areas of science and medicine.
Particularly, in medicine, novel diagnosis and treatment techniques
have been introduced using microscale and nanoscale devices [9].
These techniques are ultra-fast, portable, less costly and easy to use
compared to traditional techniques [10]. In addition, in engineering,
microscale structures [11-23]. and nanoscale structures [24-31].
have been utilized to fabricate microscale and nanoscale devices
such as ultra small actuators, sensors and energy harvesters.
Among different microscale systems, inertial microfluidics-based
devices have attracted much interest from scientific communities
due to their potential for the separation of particles and fluids at
ultra-small levels. When a particle travels inside the channel of a
microfluidics-based device, it is subject to several forces such as
drag, diffusion, Saffman and Magnus forces. In this paper, Magnus
force, as one of important forces in a group of microfluidics-based
devices, is investigated. A mathematical explicit relation is given for
the Magnus force. Furthermore, the effect of particle radius on the
Magnus force is studied in detail.
In this section, the Magnus force is formulated, and the influence
of particle radius on this force is studied. Let us consider a spherical
particle within the fluid of constant Velocity
and density (Figure 1). The fluid is assumed to be incompressible and viscous.
Furthermore, at the beginning, the particle is symmetrically
surrounded by the fluid. The angular velocity and radius of the
particle are denoted by and R, respectively. It is assumed that
there is no relative motion between the particle and fluid on the
interface. When the particle starts to spin as shown in Figure 1, the
fluid velocity below the particle is lower than the one above the
particle. As a result, the pressure is higher below the particle, and
this leads to a lift force. This lift force, which is technically
called Magnus force, is calculated by the following relation for
small Reynolds numbers [32].
Figure 1: Magnus Force Exerted on An Arbitrary Particle
In A Microfluidics-Based Device For The Separation Of
Circulating Tumor Cell.
where o(Re) is a function of Reynolds number (i.e. ). The dynamic viscosity of the
fluid is denoted by . For particles with a very small radius,
which is the case in microfluidic devices,
is independent of . In microfluidic devices, in addition to
rotation, particles usually travel along
the channel. Let us consider a small particle, which spins with
angular velocity and travels
with velocity inside the fluid. In this case, the Magnus force
is given by
in which and are , respectively, the fluid velocity
and relative velocity. Figure 2 shows the variation of the Magnus
force with particle radius. The results are calculated for the blood
flow with density 1060 kg/m3
and velocity 0.33 mm/s. It is observed
that the Magnus force rapidly increases with increasing the radius
of the particle. The formula and results of this paper would be
useful in the analysis of fluid-conveying ultra small systems such as
ultra small tubes conveying fluid [33-39] as well as microfluidicsbased devices [40-42].
Figure 2: Magnus Force Versus the Radius of The Particle
in A Microchannel.
The effect of Magnus force on the motion of particles with
relatively small sizes inside an inertial microfluidic device has
been examined. Explicit relations were given for determining the
Magnus force acting on particles within fluid flow of small Reynolds
numbers. It was observed that the Magnus force acts as a lift force
and is caused by the rotation of particles. In addition, it was
concluded that the radius of the particle has a significant role to play
in the Magnus force. The Magnus force substantially increases with
increasing particle radius.