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Crystallization

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Crystallization
Introduction
• Crystal is a solid body with plane faces in which the atoms are
arranged in an ordinary repetitive array. Most crystals are
anisotropic; their mechanical, electrical, magnetic and optical
properties are often different in different directions.
• The atomic arrangements and interatomic distances remain constant
for the crystals of a particular solid irrespective of its size. Crystals
can be classified according to seven general systems. The relative
sizes of the faces of the crystals of a substance can vary
considerably. Such a variation is called a modification of habit.
• The relative growths of the faces of a crystal can be altered and
often controlled by adjusting a number of factors such as the rate of
cooling, presence of impurities, the type of solvent, etc. (Mullin,
2001). The study of geometry, properties and structure of crystals is
known as crystallography.
Types of crystal geometry
Conti.
Crystallization
• Crystallization is a process where solid particles are
formed from a homogeneous phase. When crystals are
produced by cooling a saturated solution, process is
called solution crystallization.
• When crystals are produced by cooling a molten solid
in absence of any solvent, it is called melt
crystallization.
• Some liquids (e.g., ammonium oleate) that exhibit
anisotropy at temperatures just above their melting
points are called liquid crystals because of their
similarity with crystalline solids.
Conti.
• When the concentration of a liquid solution is increased (for example, by
evaporation of the solvent, by cooling or by a combination of these), the
solution gradually reaches the saturation level. On further evaporation or
cooling, it attains a degree of 'supersaturation. If the concentration of a
solution is more than the solubility of the solid at a particular temperature, it
is called 'supersaturated.
• Supersaturation can be created and maintained for almost all systems.
However, the level of supersaturation attainable not only depends upon the
particular system but also on how calm and free from disturbances the
system is.
• For example, a sugar solution can have a very high degree or level of
supersaturation (the concentration may even be about 80% more than the
saturation value), but in a solution of sodium chloride, the maximum
attainable supersaturation is often too small to be measured.
• Spontaneous formation and growth of tiny crystals, called nuclei, take place
in a supersaturated solution. Also, if a nucleus or a seed crystal is added to a
supersaturated solution, it gradually grows to a larger size.
Conti.
• The supersaturation in a solution provides the driving force for transport of the
solute from bulk of solution to the crystal surface.
• On reaching the surface, the solute molecules get oriented and integrated into
the crystal lattice. The suspension or slurry containing the crystals and the
solution is called the magma, and the solution remaining after removal of the
crystals is called the mother liquor.
• The process of production of crystals from a solution and 'downstream
processing' consists of four major steps: (i) crystallization: (ii) separation of
crystals from the mother liquor by filtration or centrifugation; (iii) washing the
crystals with fresh solvent to remove the adhering mother liquor (the washings
are recycled back to the crystallizer); and (iv) drying of the moist crystals.
• Sometimes the crude crystals are washed, redissolved in the solvent and
recrystallized to make a purer product. The sequence (Wibowo et al., 2001) is
shown in Figure .
Solid – Liquid phase equilibrium
• Crystallization is opposite to dissolution of a solid in a
liquid or solvent. Particles of a solid undergo dissolution so
long as the solution concentration is less than the solubility
of the solid at the given temperature.
• Conversely, if we have a supersaturated solution, and a few
seed crystals are dropped into it, a driving force for
transportation of the solute from the bulk of the solution to
the crystal surface will come into play.
• Thus, the extent of supersaturation in a solution is the
driving force for crystallization. It may be mentioned that
the solubility of very small particles may be significantly
larger than the normal solubility of a substance as given by
Gibbs- Thompson equation (Mullin, 2001).
Conti.
Conti.
• Since the smaller particles have more than normal
solubility, they dissolve even in a saturated solution and
raise the concentration creating supersaturation. The larger
particles present in the suspension start growing. The
overall process consists of dissolution of smaller particles
making the larger particles grow. This phenomenon is called
Ostwald ripening.
• The solubility of a solid in a liquid at different temperatures
is conveniently represented on a solid-liquid phase diagram.
• To explain the characteristics of a phase diagram, we take
the simple example of the naphthalene-benzene binary
system shown in Figure.
Conti.
• A point on the line AEB represents the saturation
concentration (solubility) of naphthalene in benzene at
different temperatures. AEB is Solubility curve. Any point
above the curve is unsaturated solution.
• This type curve is called “liquidus”.
P1→P2 (saturated): naphthalene starts crystallizing out
(P2-E): State of solution change.
P3 → P4 (saturated): The point E is called Eutectic point.
• This is the lowest equilibrium solidification point possible
for any solution. Complete solidification of solution occurs
when the solution represented by point E is cooled.
Mechanism of Crystallization
Theory of Crystallization
• When crystallization starts in a homogeneous mixture,
a new solid phase is created. Basic steps of nucleus
formation or nucleation and crystal growth are overall
crystallization process.
• Nucleation means formation of tiny new crystals in a
supersaturated solution. A new crystal thus formed is
called a nucleus.
• Nucleation is of two types: primary and secondary.
Primary nucleation is also divided into two categories;
homogeneous and heterogeneous. Contact, shear,
fracture and attrition are secondary nucleation
Primary Nucleation
• It is the phenomenon of formation of new crystals independent
of the presence of other crystals in the medium.
• It is of two types- Homogenous and Heterogeneous.
• In a homogenous solution. as a result of rapid random
fluctuation, molecules may come together and associate into a
cluster.
• A nucleus is formed if the cluster size exceeds a critical size. A
theoretical analysis of the energetics of cluster formation
shows that a high degree of supersaturation is necessary in
order that a cluster of size larger than the critical size is
formed.
• The theoretical rate of homogeneous nucleation can be derived
from energy considerations (see Randolph and Larson, 1988:
Myerson, 2002).
Conti.
• Here A’ a constant; vM = volume of a molecule; k =
Boltzmann constant; T= absolute temperature; s = degree
(or level) of supersaturation.
• At normal levels of supersaturation, homogeneous
nucleation proceeds very slowly. It increases rapidly if the
supersaturation level is high.
• The formation of clusters of small molecules is slowed
down if the solution viscosity is high.
• So, an increase in temp. has an additional +ve effect on the
nucleation rate because of the reduced viscosity.
Conti.
• The formation of crystals of a solute on tiny suspended
foreign solid particles or on the surfaces of the
crystallizer is called heterogeneous nucleation.
• The rate of heterogeneous nucleation depends not only
on supersaturation but also on the availability of the
'active sites' for nucleation (Mullin, 2001).
• It has been found that if a solution is very pure and
clean (i.e. foreign particles are absent), a very high
degree of supersaturation is required for heterogeneous
nucleation to occur.
Secondary nucleation
• Now whenever we will be talking about the secondary nucleation the
formation of the new crystals actually from the existing microscopic crystals
in the magma actually is called secondary nucleation.
• So for that we have 4 different types of nucleation. The first one is this contact
nucleation. It is the most common type of nucleation in the industrial
crystallizer.
• If a suspension of crystals is vigorously agitated, fracture of crystals occurs by
impact with the impeller (Bennett et al., 1973). Attrition between two crystals
in suspension or between a crystal and the crystallizer surface also leads to the
formation of small fragments.
• In either case, small crystals or nuclei are formed which grow to larger sizes in
the supersaturated solution. However, it has been found that more nuclei are
formed by contact nucleation than by fracture or attrition.
• In the process of crystallization, ion-pairs or molecules of a solute reach the
surface of a crystal by diffusive or convective transport from the bulk of the
solution. The solute molecules are continuously adsorbed on a crystal and are
simultaneously accommodated into the lattice, resulting in crystal growth.
Conti.
• But accommodation of the ion-pairs or molecules in the crystal lattice does not
occur instantaneously. Contact of a crystal with the agitator wall causes
displacement of the adsorbed layer of solute on the crystal surface.
• Some of the 'cluster of molecules or "loosely ordered phase in an adsorbed
layer get displaced by the action of the agitator or due to shear at the wall and
give rise to a new crystal nucleus. At a high level of supersaturation, the
adsorbed layer is thicker and more particles are formed by contact nucleation.
• When there is a high relative motion between a fluid and a crystal, the
"loosely ordered phase near the crystal surface is carried into the bulk of the
liquid (this is shear nucleation). Such a cluster of molecules acts as a
secondary, nucleus. Secondary nucleation is sometimes called breeding.
• The formation of a secondary nucleus by contact nucleation involves three
major steps (i)the generation of a cluster of molecules near or at the crystal
surface, (ii) the removal of the cluster, and (iii) the growth of the cluster to
form a nucleus.
Conti.
•
The degree or level of supersaturation is a very important factor. Numerous evidences
exist in this regard. For example. Garade et al. (1979) reported their experimental results
on size distribution of potassium alum nuclei generated by contact nucleation.They
conducted experiments at constant energy input but at varying levels of supersaturation.
Conti.
• The intensity of agitation, is an important factor in contact nucleation. An
intense agitation or a high agitator speed helps in quickly dislodging an
'adsorbed cluster of molecules from the crystal surface.
• The 'hardness' of the impeller is also important. Below figure shows the
effect of impeller material (its hardness) on the nucleation rate. A steel
impeller is more effective to cause nucleation than a plastic impeller.
Besides dislodging the cluster of molecules, a hard impeller causes
breakage of crystals, particularly at the corners, to form secondary nuclei.
Conti.
• In connection with the design and analysis of a crystallizer, a simple powerlaw nucleation correlation of the following type is generally used to
calculate the overall rate of nucleation by all of the above mechanisms
(Garside, 1985; Myerson, 2002).
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