Static contact angle and dynamic (advancing and
receding) contact angles of water on polymeric surfaces
were investigated using microscope cover glasses coated with various
plasma polymers of trimethylsilane
and oxygen. By variation of the mole fraction of the TMS/oxygen
mixture, glass surfaces having varying
degrees of wettability were prepared. The advancing contact angle
of a sessile droplet, which is independent
of the droplet volume, is considered as the static contact angle of
water on a polymeric surface, θS, which
is a parameter characteristic to a polymeric surface. The dynamic
contact angle of water refers to the
contact angle of which three-phase contact line is in motion with
respect to the surface. The dynamic
advancing (immersing) contact angle, θD,a, and receding
(emerging) contact angle, θD,r, were measured
by
the Wilhelmy balance. The difference between θD,a
and θD,r is mainly due to the direction of dynamic
force
acting on the three-phase contact line. The discrepancy between
the immersion and the emersion buoyancy
lines and the corresponding values of contact angles can be used to
indicate the hysteresis due to the
dynamic factor (the dynamic hysteresis). The dynamic hysteresis is
largely determined by the critical
immersion depth in which the three-phase contact line remains at the
same place on the surface while
the shape of meniscus changes when the motion of the sample is
reversed. The dynamic hysteresis may
contain the contribution of the change of static contact angle due to
the surface-configuration change
caused by the wetting of the surface (the intrinsic hysteresis).
The dynamic hysteresis varies according
to the value of cos θS, with the maximum at the threshold
value around 0.6 and linearly decreases above
this value, as the emersion line approaches the limiting buoyancy line
determined by the surface tension
of the liquid. The intrinsic hysteresis follows the same trend
with the maximum at around 0.8. The three
contact angles are related by cos θS = (cos
θD,a + cos θD,r)/2.
Magnetic sensors based on tunneling magnetoresistance (TMR) effect exhibit high sensitivity, small size, and low power consumption. They have gained a lot of attention and have potential applications in various domains.This study first introduces the development history and basic principles of TMR sensors. Then, a comprehensive description of TMR sensors linearization and Wheatstone bridge configuration is presented. Two key performance parameters, the field sensitivity and noise mechanisms, are considered. Finally, the emerging applications of TMR sensors are discussed.
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