1.1.2. Dyeing:
The use of ultrasound in the dyeing of textile can be
explained as: when ultrasound waves are absorbed in the liquid system the phenomenon
of cavitation takes place. Cavitation can liberate entrapped gases from liquid
or porous materials like textiles, dyebath etc. The influence of ultrasound on
dyeing is explained to have three-way effects:
(I) Dispersion: Breaking up of micelles and high molecular weight aggregates
in to uniform dispersion in the dyebath.
(ll) Degassing: Expulsion ( dissolved or entrapped gases or air molecules
from fiber capillaries and interstices at the cross over points of fiber in to
liquid and removed cavitations.
(Ill) Diffusion: Accelerating the rate of diffusion of dye inside the fiber
by piercing the insulating layer covering the fiber and accelerating the
interaction between dye and fiber.
Effects 1 and II are promoted by the mechanical action of
cavitation, while effect III is due to both the mechanical action and the
heating of the fiber surface. In case of water soluble dyes, ultrasound
constitutes mostly an effective means of mechanical agitation, whereas in case
of pigments, which are not soluble in water, ultrasound provides means of
pigment dispersion and penetration, which is not provided by the conventional
method. The dyeing results are affected by the frequency of the ultrasound
used. Irradiation at very low frequencies of the order of 50 or 100 cps
produces no effects. Frequencies in the range between 22 and 175 KHz have been
found to be most effective, the latter frequency being preferable for silk,
wool and nylon.
1.1.3. Diffusion mechanism:
The diffusion of dye inside the fiber is speeded up in the
ultrasonic field. The speed of dye diffusion inside the fiber depends upon the
size of the dye molecular and the state of the fiber i.e. the smaller the dye
molecule and greater the fiber swelling the higher is the mobility of the dye
molecules and the quicker they penetrate inside the fiber.
Another factor, which influences the diffusion of dye inside
the fiber, is its activated state. The dye diffuses in the fiber pores, which
are full of water and at the same time it is adsorbed by the adjacent
macromolecules. Owing to adsorption only a small part of dye can freely move
inside.
The dye molecules spent much of their time in vibrating to
and fro before they are adsorbed on the surface. Because of the simultaneous
adsorption and diffusion, the diffusion slows down if the rate of adsorption is
slow. However, because of the intense cavitation force in the ultrasonic field
the dye molecules arrive at the fiber surfaces at a much faster rate as they
gain additional kinetic energy. The dye must be in the activated state to
diffuse. This activated state to be brought about by ultrasonic energy, which
furnishes the vibrating molecules with the critical energy they need to break
their static equilibrium and thus to diffuse.
Pressure of the ultrasonic radiation on the surface of the
fiber is another factor, which influences the diffusion process. There may be
some loosening in the crystalline structure although most transient but of
great significance in speeding up the rate of diffusion. Therefore, dyeing
carried out at low temperature in the ultrasonic field showed adsorption
equivalent to that in dyeing carried out without ultrasound at higher
temperature.
1.1.4. Equipment for ultrasound:
Generator and converter or cleaning bath are the two main
components of ultrasound equipment. Generator converts 50 to 60 Hz alternate
current to electrical energy of high frequency. This electrical energy is fed
to the transducer where it is transformed to mechanical vibration. The
transducer system vibrates longitudinally transmitting waves into liquid
medium. As these waves propagate cavitation occurs. Prototype dyeing machine
was designed for continuous dyeing of yam and fabric. The system mainly
consists of the tank, transport system and microprocessor, which is used to
monitor the process. Ultrasonic tank is of 92 x 60 cm dimensions and capacity
up to 200 liters. Temperature can be varied up to 100C by thermostatic
control.