process and impart stability to nanoemulsion. The process of homogenization is
performed in cycles and optimized. During homogenization, sometimes heat is
generated which may have a detrimental effect on heat-sensitive bioactives. How-
ever, this situation can be countered through ice or cold water jacketing and reducing
the homogenization time of each cycle.
19.5.1.2 Microfluidization
The microfluidization process utilizes a static and mechanical mixer which involves
driving a fluid through microchannels under high pressure which results in ultrafine
droplets of dispersed phase. The positive pressure applied has a direct impact on size
reduction, which means an increase in pressure may result in a decrease in droplet
size. The principle of microfluidization is almost similar to high-pressure homoge-
nization except the passage through microchannels whose pore size ranges from
50 to 300 μm. Generally, a pressure of around 270 mPa is applied in
microfluidization, and the fluid is allowed to move downstream through
microchannels at a velocity of approximately 400 m/s. Through the inlet, the fluid
passes through the Y junction where it splits into two branches and then reconnects
at the interaction chamber at high velocity and high shear rate. After size reduction,
the surface area of dispersed phase increased significantly, and the surfactant has to
adsorb on the interface rapidly to avoid coalescence. Therefore, fast-adsorbing
surfactants
are
often
selected
for
fabricating
nanoemulsions
through
microfluidization. Also, increasing the viscosity of continuous phase also retards
the coalescence of ultrafine droplets. These forces result in mechanical energy with
high magnitude sufficient to counter the interfacial energy and significantly reduce
the droplet size (Che Marzuki et al. 2019; Villalobos-Castillejos et al. 2018).
19.5.1.3 Ultrasonication
Among other high-energy methods, ultrasonication is the simplest, is easy to use,
and requires low-end mechanical instruments. It is the ultrasound waves that are
responsible to produce shock waves, resulting in disruption of mainly oil droplets
into smaller size in water. These intensive ultrasonic waves generate vibrations and
acoustic cavitation which creates high pressure in dispersed phase and turbulence
that collapse the droplets. The frequency of sonic waves and time of sonication play
an important role for appropriate size reduction. An optimum frequency is necessary
to produce shock waves with sufficient high energy input that can disrupt the droplet.
Generally, frequency with more than 20 KHz is suitable for droplet size reduction.
Also, the more the time of ultrasonication, the more efficiently size reduction takes
place. This is because an increase in the time of ultrasonication produces higher
energy input capable to reduce the interfacial tension (Behrend et al. 2000).
19.5.2 Low-Energy Processes
Low-energy processes are of great interest for those bioactives which are heat
sensitive as in the case of high-energy processes, some of the heat energy is
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