Micellar
Drug Delivery System
Bhaskar
Kurangi1*, Sandesh Somnache1, Nilesh Jangade2
1Dept. of
Pharmaceutics, Rani Chennamma
College of Pharmacy, Belgaum, Karnataka, India
2Dept. of
Pharmaceutical Chemistry, Rani Chennamma
College of Pharmacy, Belgaum Karnataka, India
*Corresponding Author E-mail: bhaskarkurangi19@gmail.com
ABSTRACT:
Micelles are organized molecular assemblies of surfactants. In aqueous
solution, the hydrophilic head of the surfactant is in contact with solvent,
and the hydrophobic tail is sequestered within the center of the micelle. This
review article focusing on the structure, shape, types of the micelles. Critical micelle concentration (CMC) which is defined as the
concentration of surfactants above which micelles are spontaneously formed.
The various factors affecting the CMC to form the micelle and thermodynamics of
micelles also discussed in this review. The reverse micelle and polymeric
micelle which have wide application as the nanostructure vehicle for the
targeted drug delivery. The application of micelles in drug delivery, in order
to minimize drug degradation and loss, to prevent harmful side effects and to
increase drug bioavailability, is also presented. Special emphasis is given to
the more recent use of polymeric micelles. Importantly the various advantages,
applications and recent advances in micellar drug
delivery system are also discussed.
KEYWORDS: Micelle, Critical micelle concentration (CMC), Reverse micelle,
polymeric micelle, nanostructure.
INTRODUCTION:
Micelle:
1-5
Micelle is a
“particle of colloidal dimensions that exists in equilibrium with the molecules
or ions in solution from which it is formed.” A micelle is an aggregate of surfactant molecules dispersed in a liquid colloid. A typical micelle in aqueous
solution forms an aggregate
with the hydrophilic
"head" regions in contact with surrounding solvent, sequestering the hydrophobic single tail regions in the micelle centre.
This phase is caused by the insufficient packing issues of single tailed lipids in a bilayer. The difficulty filling all the volume of
the interior of a bilayer, while accommodating the
area per head group forced on the molecule by the hydration of the lipid head
group leads to the formation of the micelle. This type of micelle is known as a
normal phase micelle (oil-in-water micelle). Inverse micelles have the head
groups at the centre with the tails extending out (water-in-oil micelle).
Micelles are approximately spherical in shape. Other phases, including shapes such as ellipsoids,
cylinders, and bilayer are also possible.
The shape and size of a micelle is a
function of the molecular geometry of its surfactant molecules and solution
conditions such as surfactant concentration, temperature, pH and ionic strength. The process of forming micelle is
known as Micellization and forms part of the phase behavior of many lipids
according to their polymorphism.
Fig.
1: Cross section of micelle; liposome
Micelles are well oriented surfactant
molecules having hydrophilic head and hydrophobic tail. Micelle may contain 50
or more monomeric units of surface active agent.
There is equilibrium between monomers and micelle. Micelles have half life of centisecond or even less. Micellization
minimizes the contact between hydrophobic portion and surrounding water.
Forces
involved in micelle formation: 6- 8
Forces based on hydrophobicity:
1. Head-head attraction.-:
There are always attractive forces between
the head group of one micelle and head group of another micelle in the system.
2. Tail-tail attraction-:
Tail portion of all the
monomers in single micelle exhibit attractive forces so as to construct inner
hydrophobic core.
3. Tail-head repulsion-:
This is nothing but a force exhibited due
to opposite charges present on the head and tail portion of the micelle or
monomer.
4. Head-tail repulsion-:
This is again nothing but a force exhibited
due to opposite charges present on the head and tail portion of the micelle or
monomer.
Micellar structure:
In case of ionic micelles, there are three
main parts-
1.
Micellar liquid core: 6-11
Liquid core is formed by hydrocarbon chain
with the head group projecting out in water. Techniques which are used to
detect nature of micellar core are as follows:
i. Fluorescent probes: It shows fluorescence
in non polar region only and they are non fluorescent in water.
Eg. 8-anilino-1-napthalene-sulphonate
With respect to fluorescence phenomenon,
there are two techniques of micellar core determination-
A. Fluorescent depolarization B. Excitement
fluorescence
Drawbacks- i. Uncertainty of location of probe.
Possible
perturbation of micro environment.
ii. Hydrocarbon probes: used are pyrene and methyl anthracene. It
was concluded that interior of the micelle of several long chain cationic
surfactants were of liquid in nature.
iii. ESR spectra: is used to measure
electron spin resonance from free radicals which are incorporated in probes
within micelle. Restricted motion of probe results in hyperfine splitting in
ESR spectrum and broadening of the spectral lines indicates high local
viscosity.
iv. Raman spectra and NMR spectra: is used
to detect conformational state of hydrocarbon chain in micellar
core. Raman spectra indicated that in crystalline state, hydrocarbon chain
exists in all-trans conformation while in micellar
state it is in gauche conformation.
2.
Stern layer: 12, 13
The layer which
immediately next to the core is called as stern layer which contains ionic head
groups and (1-alpha) n counter ions. Stern layer contains inner part of the electric double layer
surrounding the micelle. The electric potential, at the interface between micellar core and surrounding water is estimated by Gouy-chapman theory. Measurement of electric potential is done
by probes of molecular sizes which are known to get solubilized
at the core water interface and which does not disturb the system.
Eg. Hydrogen ion concentration at the micellar surface was determined by pH indicators like bromophenol blue and bromocresol
green. The apparent pKa of the indicators when solubilized in ionic micelle differed from that in bulk and
this shift was related to electric potential assuming a Boltzmann distribution
of hydrogen ion concentration at the surface.
Drawback-
Equilibrium of indicators at the micellar surface is affected by dielectric constant which
is lower at the surface compared to the bulk solution. Dielectric constant for
stern layer is intermediate between 79 for water and it is 2 for hydrocarbons.
3.
Gouy-chapman layer: 12, 13
It is the outer layer which more diffused
in nature and it contains remaining counter ions which are not present in the
stern layer .It may get extended up to the aqueous environment.
Micelle
shape: 7, 8
Micelles are dynamic structures with a
liquid core. It is not a rigid structure with a precised
shape hence an average micelle shape is considered. For experimental
interpretation, micellar sphericity
is assumed. As no hole is present at the centre of the micelle, the micellar radius is always limited by maximum possible
extension of hydrocarbon chain.
The shape of the micelle = VH/lc.ao
Where, VH = volume of the hydrophobic group
in the micellar core.
lc= length of the hydrophobic group in the
core.
ao= cross sectional area occupied by hydrophilic
group at the micelle –solution interface.
Table:
1 Correlation between the parameter VH/ lc.ao and shape of micelle
|
Micellar shape |
VH/ lc.ao |
|
Spherical in aqueous medium |
0 to1/3 |
|
Cylindrical in aqueous medium |
1/3 to ½ |
|
Lamillar in aqueous
medium |
1/2 to 1 |
|
Reversed in non-aqueous medium |
>1 |
A spherical shape micelle is possible only
when many oxyethylene chains are embeded
in the hydrophobic core. Eg. Triton x-100 micelle was considered to be spherical.
Oblate shape is favoured when head group repulsion is
strong. Non ionic and ionic surfactants in presence of electrolyte favour oblate shape. Eg. n-alkylpolyoxyethylene
glycol monoethers, Lubrol
WX. For the ionic surfactants, oblate shape get transited to prolate ellipsoid shape with the increase in the solution
concentration provided that added salts are absent. Israela
chvilli et. al. rejected the oblate shape due to excessive curvature of
peripheral region and excessive thickness of the central region. He proposed
the distorted oblate spheroidal shape resembling RBC
in shape. Micellar shape get affected by factors such
as temperature, concentration, presence of added electrolyte etc. increase in
one of these parameters results in shape transition of the micelle from near spheroidal shape to asymmetric form. In case of cetyltrimethylammonium bromide (CTAB), flexible rod like
aggregates is formed at higher concentration. X-ray scattering measurements of
CTAB shown that at concentration 0.15M (approx), CTAB micelles undergoes
transition from spherical to rod shape.
Spherical Micelle
Cylindrical micelle
Lamellar Micelle
Fig.
2: Micelles of various shapes
Types
of micelles:
1. Monomeric
micelle:6-8
Individual surfactant molecules that are in
the system but are not part of a micelle are called "monomers." In
micelle, the hydrophobic tails of several surfactant molecules assemble into an
oil-like core the most stable form of which has no contact with water. By
contrast, surfactant monomers are surrounded by water molecules that create a
"cage" of molecules connected by hydrogen bonds. This water cage is
similar to ice-like crystal structure.
Micelles are dynamic species; there is a
constant rapid interchange of surfactant molecules between the micelle and the
bulk solution. Micelles cannot, therefore, be regarded as rigid structures with
a defined shape, although an average micellar shape
may be considered and Micelles are labile entities formed by the non-covalent
aggregation of individual surfactant monomers. Therefore, they can be
spherical, cylindrical, or planar (disc or bilayer).
Micelle shape and size can be controlled by changing the surfactant chemical
structure as well as by varying solution conditions such as temperature,
overall surfactant concentration, surfactant composition (in the case of mixed
surfactant systems), ionic strength and pH. In particular, depending on the surfactant
type and on the solution conditions, spherical micelles can grow
one-dimensionally into cylindrical micelles or two-dimensionally into bilayer or discoidal micelles.
Spherical micelles exist at conc. relatively close to the CMC. At higher
concentration lamellar micelles have an increasing tendency to form and exist
in equilibrium with spherical micelle.
Micelle growth is controlled primarily by
the surfactant heads, since both one dimensional and two dimensional growth
require bringing the surfactant heads closer to each other in order to reduce
the available area per surfactant molecule at the micelle surface and hence the
curvature of the micelle surface.
Solution at CMC Solution above CMC
Fig.3:
formation of micelle from monomer
In polar solvent, the hydrophilic "heads" of
surfactant molecules are always in contact with the sequestering solvent and
the hydrophobic single tail regions in the micelle centre called normal micelle
(oil-in-water micelle). This phase is caused by the insufficient packing issues
of single tailed lipids in a bilayer. The difficulty
filling all the volume of the interior of a bilayer,
while accommodating the area per head group forced on the molecule by the
hydration of the lipid head group leads to the formation of the micelle.14
One of the most important applications of Micellization
in the context of pharmaceuticals is their ability to solubilize
drugs of poor aqueous solubility.
Fig. 4 Schematic
illustration of the reversible monomer-micelle thermodynamic equilibrium.
2.
Reverse micelle:15-17
In a non-polar solvent, the lipophilic
"tails" of surfactant molecules have less contact with water or the
exposure of the hydrophilic head groups to the surrounding solvent that is
energetically unfavorable. Therefore, the head groups are pulls at the centre
with the tails extending out called as Inverse/Reverse micelle (water-in-oil
micelle). Dipole–dipole interactions hold the hydrophilic heads of the
surfactant molecules together in the core, and in certain cases hydrogen
bonding between head groups can also occur.
Reverse micelle formed by the aggregation of the 3 to 20 monomer by oil
soluble surfactant. e.g. Scheme of an inverse micelle
formed by phospholipids in an organic solvent.
Fig.5(a):Reverse Micelle (in Non polar solvent)
Fig.5(a): Normal Phase Micelle
In the same way that normal micellar systems can be used for solubilizing
hydrophobic substances in an aqueous solution, reversed micellar
systems may be used for solubilizing water-soluble
drugs in an oil-continuous system.
Advantages of reverse micelle:
·
To solubilize water soluble drugs in an oil continuous system.
·
The
release rate of water soluble drug may be controlled.
·
Masking
of bitter taste for extensively water soluble drugs.
·
Passive
drug targeting.
3. Polymeric micelle: 18-21
In drug delivery, special attention has
been given to the polymeric micelles. Polymeric micelles are composed of block
or graft copolymers. Polymeric micelles are formed from copolymers consisting
of both hydrophilic and hydrophobic monomer units, such as PEO and PPO
(polyethylene oxide and polypropylene oxide), respectively. These amphiphilic block co-polymers with the length of the
hydrophilic block exceeding the length of the hydrophobic block can form
spherical micelles in aqueous solution. The micellar
core consists of the hydrophobic blocks and the shell region consists of the
hydrophilic blocks. The PEO coating has been shown to prevent subsequent
recognition by the macrophages of the reticuloendothelial
system (RES), allowing the micelles to circulate longer and deliver drugs more
effectively to the desired sites. Block copolymers are generally linear
polymers that are composed of a sequence of at least two polymer segments that
differ in physico-chemical properties, e.g. charge
and/or polarity.
Fig.6: A schematic representation
of the mechanism of block polymeric micelles formation
Formations of polymeric micelles from
different types of amphiphilic block co-polymers. In
graft copolymers, side chain segments are grafted to a main polymer chain.
Fully hydrophilic block or graft copolymers in which one of the segments carry
a charge may form stable complexes in water together with oppositely charged
(macro) molecules, resulting in, for instance, so-called poly ion complex
micelles or polyelectrolyte micelles. On the other hand, so-called amphiphilic block copolymers are capable to self-assemble,
when placed in a solvent that is selective for one of the polymeric segments,
to form micelles, vesicles or gels. In an aqueous environment, such
self-assembled structures are interesting for encapsulation and (controlled)
release of a variety of drugs.
Drug loading of amphiphilic
block copolymer micelles is generally accomplished by -
(a) Dissolving the polymer and the
hydrophobic drug in an organic solvent and subsequent dialyzing against water
or diluting in water and evaporating the solvent.
(b) Another method that is reported
occasionally is the ‘spontaneous’ hydration of a polymer/drug mixed film.
An interesting class of block copolymers is
amphiphilic or double hydrophilic block copolymers
that respond to an external stimulus, such as temperature, pH, electrolyte, redox potential or even light. These are especially
interesting for drug delivery systems, because the micelles can associate or
dissociate (encapsulate or release their contents) upon an external trigger.
Micelles formed by self-assembly of amphiphilic block
copolymers (5-50 nm) in aqueous solutions are of great interest for drug
delivery applications. The drugs can be physically entrapped in the core of
block copolymer micelles and transported at concentrations that can exceed
their intrinsic water- solubility. Moreover, the hydrophilic blocks can form
hydrogen bonds with the aqueous surroundings and form a tight shell around the micellar core. As a result, the contents of the hydrophobic
core are effectively protected against hydrolysis and enzymatic degradation. In
addition, the corona may prevent recognition by the reticuloendothelial
system and therefore preliminary elimination of the micelles from the
bloodstream. A final feature that makes amphiphilic
block copolymers attractive for drug delivery applications is the fact that
their chemical composition, total molecular weight and block length ratios can
be easily changed, which allows control of the size and morphology of the
micelles. Functionalization of block copolymers with
cross linkable groups can increase the stability of the corresponding micelles
and improve their temporal control. Substitution of block copolymer micelles
with specific ligands is a very promising strategy to a broader range of sites
of activity with a much higher selectivity.
Advantages of
polymeric micelle over monomeric micelle:
Polymeric micelles, which
are either formed from block copolymers by ionic or by hydrophobic interactions
have several advantageous features that make them interesting as drug delivery
systems. Some of them
mention below:
1)
Polymeric carriers might lead to precipitation in water, since the drug-polymer
interaction can result in conversion of functional water-soluble groups of the
drug into more hydrophobic groups.
2)
Polymeric micelles refer to the easy for sterilization via filtration and
safety for administration.
3) Some
polymeric micelles seem to present better solubilization
capacity when compared to surfactant micelles due to the higher number of
micelles and/or larger cores of the formers.
4) The slow
dissociation of kinetically stable polymeric micelles allows them to retain
their integrity and perhaps drug content in blood circulation above or even
below the CMC for some time, creating an opportunity to reach the target site
before decaying into monomers.
5) Well
defined core shell architecture. For example, the core of amphiphilic
block copolymer micelles is capable to accommodate (solubilize)
poorly water soluble drugs that are otherwise
difficult to administer to the body. The hydrophilic shell provides colloidal
stability to the whole assembly.
6) Small
size (< 150 nm). Since the smallest blood vessels in the body (the
capillaries) have a diameter of approx. 200 nm, polymeric micelles are able to
freely circulate in the blood stream after injection of the drug solubilisate.
7) High
physical stability. Because the critical micelle concentration (CMC) of a block copolymer can be several orders of
magnitude lower than that of a classical surfactant, the micelles are highly
resistant against dilution that unavoidable when administered to the patient
(e.g. by injection).
Critical
micelle concentration: 22-25
Critical micelle
concentration (CMC) is defined as the concentration
of surfactants
above which micelles
are spontaneously formed.22 Upon
introduction of surfactants (or any surface active materials) into the system
they will initially partition into the interface, reducing the system free energy by
(a) By lowering the energy of the interface (b) By removing the hydrophobic
parts of the surfactant from contacts with water.
Subsequently, when the surface coverage by
the surfactants increases and the surface free energy (surface tension)
decreases and the surfactants start aggregating into micelles, thus again
decreasing the system´s free energy by decreasing the contact area of
hydrophobic parts of the surfactant with water. Upon reaching CMC, any further
addition of surfactants will just increase the number of micelles (in the ideal
case).
There are several theoretical definitions
of CMC. One well-known definition is that CMC is the total concentration of
surfactants under the conditions:
If C = CMC, (d3F/dCt3)
= 0
F = a [micelle]
+ b [monomer]: function
of surfactant solution
Ct: total concentration
a, b:
proportional constants
Therefore, CMC depends on the method of
measuring the samples, since a and b
depend on the properties of the solution such as conductance
and photochemical
characteristics.
When the degree of aggregation is monodisperse,
the CMC is not related to the method of measurement. On the other hand, when
the degree of aggregation is polydisperse, CMC is related to
both the method of measurement and the dispersion. CMC is an important
characteristic of a surfactant. Before reaching the CMC, the surface tension
changes strongly with the concentration of the surfactant. After reaching the
CMC, the surface tension stays more constant. CMC is the concentration of
surfactants in the bulk at which
micelles start forming. The word BULK
is important because surfactants partition between the bulk and interface and
CMC is independent of interface and is therefore a characteristic of the
surfactant molecule.
In most of the situations like for e.g. in
surface tension measurements or conductivity measurements, the amount of
surfactant at the interface is negligible compared to that in the bulk and CMC
is approximated by the total concentration as is done in most of the textbooks.
There are important situations where
interfacial areas are large and the amount of surfactant at the interface
cannot be neglected. For example if we take a solution of a surfactant above
CMC and start introducing air bubbles at the bottom of the solution, these
bubbles, as they rise to the surface, pull out the surfactants from the bulk to
the top of the solution creating a foam column thus bringing down the
concentration in bulk to below CMC. This is one of the easiest methods to
remove surfactants from effluents (foam flotation). Thus in
foams with sufficient interfacial area there will not be any micelles. Similar
reasoning holds for emulsions.
Factors
affecting CMC and micellar size:
1)
Nature of hydrophobic group-
For ionic amphiphiles,
increase in the number of carbon atoms in an unbranched
hydrocarbon chain tends to decrease CMC. CMC is halved when length of the
hydrocarbon chain is increased by one methylene group
but this relationship no longer holds beyond 16 carbon atoms. Further increase
in carbon atoms shows no appreciable effect on CMC due to coiling of long chain
in solution. For non ionic surfactants, increase in hydrocarbon chain length
decreases CMC and addition of one methylene group
decrease the CMC one third of its original value. Replacement of methyl group
by trifluoromethyl group doubles CMC. Addition of
phenyl ring to straight chain hydrocarbon shows equivalent effect on CMC as
that of the effect shown by three and a half methylene
groups. Substituent’s such as –Cl, -Br, -F ,-I , on the phenyl ring increase the hydrophobicity
and thereby decreases CMC.
2)
Nature of hydrophilic group-
For the non ionic surfactant, in case of
polar group, the factor that controls the micellar
size is-
i)
The mean distance of the closest approach of the counter ion to the
charged centre of the surfactant.
Eg- decylammonium
bromide forms much larger micelle than decyltrimethylammonium
bromide because bromide counter ions approach more closely towards the charged
nitrogen atom of decylammonium thus shields the
repulsive electric forces and forms large micelle.
ii)
Solvent interactions -
Eg- Hydrogen bonding between oxygen atom of decylmorpholinium bromide and water is responsible for its
smaller size micelle as compared to decylpiperidinium
bromide which does not interact with solvent.
iii)
Effectiveness of dielectric constant -
Eg-When ethyl group associated with polar
head is replaced by ethanol group in compounds like decylethylammonium
bromide or decyldiethylammonium bromide its
aggregation number is increased due to change in effective dielectric constant
produced when polar head structure is changed. Replacement of nitrogen by phosphorus
or arsenic in decyltrimethylammonium bromide
increases aggregation number by at least 20% and decreases CMC by 35%. Increase
in the number of the ionized groups present in the surfactant higher CMC.
Position of the ionic group affects the micellar
properties. Eg-CMC of sodium alkyl sulphate increases when sulphate
group moves from terminal site to medial position. For polyoxyethylated
ether type non ionic surfactants, increase in polyoxyethylene
chain length increases CMC because increase in polyethylene chain length tends
to increase hydrophilicity.
3)
Nature of the counter ion -
Counter ions associated with
the ionic amphiphile have a pronounced effect on the micellar properties. With amphiphile
drugs like mepyramine and bromopheniramine
maleate containing pyridine ring; proton transfer
interaction occurs between maleate counter ion and
nitrogen of the pyridine ring as a result there is no clear CMC. Increase in
the size of the counter ion tends to increase CMC value.
4)
Effect of additives -
Addition of the electrolytes
decreases the ionic atmosphere around the polar group as well as decreases the
repulsion between them and thus decreases CMC. Most effective electrolytes
causing lowering of CMC are nitrates of sodium and potassium. Lower alcohols
when added to the ionic surfactants tend to decrease CMC but in case of non
ionic surfactants; reason for this is decreased free energy of micelles due to
diluted surface charge density on the micelles. Addition of water soluble
alcohols like methanol or ethanol tend to increase CMC and this is due to the
weakening of the hydrophobic bonds.
5) Effect of temperature -
Decrease in the CMC of the
ionic surfactants with increase in the temperature at lower range is due to
dehydration of the monomer further increase in temperature tend to disrupt
structured water molecules around the hydrophobic groups which oppose micellization. Increase in the temperature tends to
decrease the micellar size of the ionic surfactants
and increase in temperature increases size of the polyoxyethylene
non ionic surfactants. Increased temperature tends to extend polyoxyethylene chain thereby increase the amount of water
physically trapped by the micelle.
6)
Effect of pressure-
Effect of pressure on the CMC of alkyltrimethylammoniun bromide was studied by conductivity
technique and it was found that up to 150Mpa there is increase in CMC followed
by decrement at higher pressure. Such behavior is rationalized in the terms of
solidification of the micellar interior and pressure
induced increase in the dielectric constant of the water.
Thermodynamics of micelle formation: 26-32
Thermodynamics
of micelle formation can be explained by using two models
1. Phase
separation approach:-
Micelles are considered to form separate
phase at CMC.
a. Application to non ionic surfactant
∆Gmφ = 2.303RT [log cmc-log w].
∆Gmφ=std free energy
change for transfer of one mole of amphiphile from
solution to micellar phase.
b. Application to ionic surfactant
∆Gmφ = 4.606RT [log cmc-log w]
2. Mass action
approach:
Micelles and unassociated monomers are
considered to be in association-dissociation equilibrium.
∆Gmφ = RT log Xcmc
Xcmc=CMC expressed as mole fraction.
Mass action model can be considered as more
realistic process than phase separation model.
Advantages
of Micellization: 4, 6,
(1)Incorporation of large quantity of
hydrophobic drug - By using micelles
we can incorporate essentially hydrophobic drug into the micellar core
which is surrounded by hydrophilic groups thus it helps in increasing the
solubility of the drugs having limited aqueous solubility.
(2) Increased chemical stability of drug- As micelles protect the hydrophobic
drugs by their entrapment into the micellar core;
they are supposed to increase the chemical stability of the drug by preventing
their hydrolysis or enzymatic degradation.
(3) Increased efficacy of drug - Naturally as the drug is in the
protective core of the micelles; it offers site specific delivery of the drug
thereby increases efficacy of the drug.
(4) Taste masking-This is the important
case with respect to the aesthetic properties of the drug. Drugs having
essentially bitter taste can be effectively kept in the micellar
core to mask its taste and thus it can be made aesthetic.
(5) Passive targeting- By keeping a hydrophobic drug in the micellar
core we can locate the drug in the microorgans like
arteries because the smallest artery in the body is larger than the micellar size hence micelles can easily enter the arteries.
Applications of Micellization:
1.
Solubilization: 33-39
Solubilization can be defined as ‘‘the preparation of a
thermodynamically stable isotropic solution of a substance normally insoluble
or very slightly soluble in a given solvent by the introduction of an
additional amphiphilic component or components.’’ The
amphiphilic components (surfactants) must be
introduced at a concentration at or above their critical micelle
concentrations. Simple micellar systems (and reverse micellar) as well as liquid crystalline phases and vesicles
referred to above are all capable of solubilization.
In liquid crystalline phases and vesicles, a ternary system is formed on
incorporation of the solubilisate and thus these
anisotropic systems are not strictly in accordance with the definition given
above.
Solubilization by micelles Micelles resembles miniscule pools of liquid
hydrocarbon surrounded by shells of polar head. They solubilize
poorly water soluble drugs. Solubilization depends
upon the chemical structure of solublizate. It does
not occur below CMC. The location of a solubilized
molecule in a micelle is determined primarily by the chemical structure of the solubilisate. Solubilization can
occur at a number of different sites in a micelle:
1. On the surface,
at the micelle–solvent interface
2. At the surface
and between the hydrophilic head groups
3. In the
palisades layer
4.
More deeply in the palisades layer and in the micelle inner core.
Fig.
7: In aqueous systems - solubilization of drugs at
diff. positions of micelle
Examples:
1. Polar
alcohols are soluble in aqueous solution, so it located in solution / on
surface of micelle.
2. Phenol
are having polar –OH group and non polar benzene ring. In which –OH gr. Located
in hydrophilic environment and benzene ring in hydrophobic environment, so it
located at the surface and between the hydrophilic head groups.
3. Semipolar materials, such as fatty acids are usually
located in the palisades layer, the depth of penetration depending on the ratio
of polar to non-polar structures in the solubilisate
molecule.
4. Non-polar
additives such as hydrocarbons tend to be intimately associated with the
hydrocarbon core of the micelle.
In
non aqueous system-
Reverse micelles formed in non-polar
solvent systems containing surfactant, polar additives may be solubilized in the core where a polar interaction of head
groups occurs. A preferred location of the solubilisate
molecule within the micelle is largely dictated by chemical structure. However,
solubilized systems are dynamic and the location of
molecules within the micelle changes rapidly with time. Solubilization
in surfactant aqueous systems above the critical micelle concentration offers
one pathway for the formulation of poorly soluble drugs. From a quantitative
point of view, the solubilization process above the
CMC may be considered to involve a simple partition phenomenon between an
aqueous and a micellar phase. Thus the relationship
between surfactant concentration Csr and drug
solubility Cdss is given by following equation.
Cdss = Cdsa + P Cdsa. Csr
Where Cdsa is the
drug solubility in the absence of surface active agent and P is the
distribution coefficient of drug between the micelle and bulk phases. A plot of
Cdss versus Cs is linear with a slope of P Cdsa, which is the solubilizing
capacity of the micelle. The effect of altering the pH of the vehicle, in the
case of a partly ionized drug will be to alter the apparent partition
coefficient. Thus the effect of increasing the pH of a vehicle containing an
acidic drug is to reduce the proportion of drug in the micellar
phase. If the surfactant is a weak electrolyte, it may induce a
concentration-dependent change in pH thus altering drug partitioning and
solubility. In general the solubilizing capacity for
surfactants with the same hydrocarbon chain length increases in the order
anionic < cationic < non-ionic, the effect being attributed to a
corresponding increase in the area per head group, leading to looser micelles
with less dense hydrocarbon cores which can accommodate more solute.
The solubilizing
capacity for a given surfactant system is a complex function of the
physicochemical properties of the two components which, in turn, influence the
location or sites where the drug is bound to the micelle. The molar volume of
the solubilisate together with its lipophilicity is important factors, the former reducing and
the latter increasing solubilization.
Many pharmaceutical products contain a
number of solutes potentially capable of being solubilized
within the micellar phase. Thus competition can occur
between solutes resulting in an altered solubilizing
capacity. Furthermore, the addition of a second highly solubilized
component to form a mixed micellar system may greatly
alter the structure, size and solubilizing capacity
of the system, thereby greatly enhancing drug solubility.
Pharmaceutical Examples of solubilization:
·
The solubilization of phenolic
compounds such as cresol, chlorocresol, chloroxylenol and thymol with
soap to form clear solutions for use in disinfection.
·
Solubilized
solutions of iodine in non-ionic surfactant micelles (iodophors)
for use in instrument sterilization.
·
Solubilization of drugs (for example, steroids and water insoluble vitamins),
and essential oils by non-ionic surfactants (usually polysorbates
or polyoxyethylene sorbitan
esters of fatty acids).
2. Stabilization of the biphasic system-
Micelles
formed by the surfactants tend to stabilize biphasic systems like emulsions by
decreasing the surface free energy of the system.
3. Site specific drug delivery-
Micelles are able to give site specific drug delivery which
is of prime importance in the areas like cancer treatment thus it also supposed
to increase the bioavailability of the drugs. It is briefly discussed in
following points.
Recent advances in micellar
drug delivery system:
1. Multifunctional polymeric Micellar
Nanomedicine for Cancer Therapy:
Polymeric
micelles are supramolecular, core-shell nanoparticles that offer considerable advantages for cancer
diagnosis and therapy. Their relatively small size (10-100 nm), ability to solubilize hydrophobic drugs as well as imaging agents, and
improved pharmacokinetics provide a useful bioengineering platform for cancer
applications. Several polymeric micelle formulations are currently undergoing
phase I/II clinical trials, which have shown improved antitumor efficacy and
reduced systemic toxicity.40-42
This minireview will
focus on recent advancements in the multifunctional design of micellar Nanomedicine with tumor
targeting, stimulated drug release and cancer imaging capabilities. Such Functionalization strategies result in enhanced micellar accumulation at tumor sites, higher drug
bioavailability as well as improved tumor diagnosis and visualization of
therapy. Ultimately, integrated nanotherapeutic
systems (e.g., theranostic Nanomedicine)
may prove essential to address the challenges of tumor heterogeneity and
adaptive resistance to achieve efficacious treatment of cancer. 43, 44.
Cancer
remains as one of the leading causes of mortality worldwide, and is responsible
for approximately 13% of all deaths, according to world health organization.45
Currently, the treatment options include surgical
resection, radiation, and chemotherapy. However, although over 90
chemotherapeutic drugs have been approved by the FDA for clinical use, their efficacy
has been severely hindered by dose-limiting toxicity and patient morbidity.
Recently, nanoscale (10-200 nm) therapeutic systems
have emerged as novel therapeutic modalities for cancer treatment. These
systems include polymeric micelles, polymer-drug conjugates, dendrimers, liposomes and
inorganic particulates. Compared to conventional small molecule-based therapy, nanotherapeutic systems have several potential advantages
for cancer therapy, including higher payload capacity, prolonged blood circulation
times, reduced toxicity to healthy tissues and improved anti-tumor efficacy. In
this article, we will review key advances of one of these emerging nanotherapeutic systems, polymeric micelles and discuss
their potential for cancer therapy.46-48.
Polymeric Micelles: Properties and
Advantages for Cancer Treatment-
The use of polymeric micelles for cancer
treatment was first reported in the early 1980s by Ringsdorf
and coworkers. These spherical particles are nanosized
(typically in the range of 10-100 nm) supramolecular
constructs formed from the self-assembly of biocompatible amphiphilic
block copolymers in aqueous environments. In water, the hydrophobic portion of
the block copolymer self-associates into a semi-solid core, with the
hydrophilic segment of the copolymer forming a coronal layer. The resulting
core-shell architecture is important for drug delivery purposes, because the
hydrophobic core can act as a reservoir for water insoluble drugs, while the
outer shell protects the micelle from rapid clearance. Although several
functional aspects of the constituent blocks have been explored (e.g.
temperature or pH sensitive blocks), the most important criteria are
biocompatibility and/or biodegradability. Currently, the most commonly used
corona-forming polymer is polyethylene glycol (PEG), with a molecular weight
range from 2 to 15 kD.
Core-forming blocks typically consist of poly(propylene
oxide) (PPO), poly(D,L-lactic acid) (PDLLA), poly(ε-caprolactone)
(PCL), and poly(L-aspartic acid) to name a few. Given their lipophilic
nature, most anticancer drugs are inherently water insoluble. As an example, paclitaxel, a highly effective anticancer agent that
inhibits microtubule growth by binding to the β subunit of tubulin, has a water solubility of 0.0015 mg/mL. While this degree of hydrophobicity
is favorable for drug permeation through cell membranes, intravenous (i.v.) administration would result in rapid drug aggregation
and formation of capillary embolisms. By encapsulation of the drug within the
hydrophobic core of the micelle, the apparent solubility of the drug can be
significantly increased. For example, micelle encapsulation of paclitaxel increased the solubility over three orders of
magnitude from 0.0015 to 2 mg/mL. Hence, polymer
micelles allow for the in vivo use
of previously existing drugs otherwise deemed too hydrophobic or toxic, without
having to manipulate the chemical structure of the agent. Additionally,
encapsulating the drug within the polymer core affords drug stability by
hindering enzymatic degradation and inactivation.
The hydrophilic micellar
corona also plays an important role in in
vivo applications by reducing particle recognition by opsonin
proteins. In the absence of this brush-like coating, the micelle would undergo
rapid phagocytic clearance by the reticuloendothelial
system (RES). Additionally, the critical micelle concentration (CMC, the
concentration threshold of polymers at which micelles are formed) is very low
for polymeric micelles, typically on the order of 10−6-10−7
M, resulting in stable constructs that are not easily dissociable in vivo. These characteristics together
contribute to longer blood circulation times, and this longevity results in an
increase in the bioavailability of the drug. The long circulation times and
small size of polymer micelles also aid in the preferential accumulation of
micelles in tumor tissue through the enhanced permeability and retention (EPR)
effect, which allows for passive targeting due to fenestrations between
endothelial cells in angiogenic tumor vessels.46-52.
These
polymeric micelles act by following path-
1.
Enhancement in solubility-
Polymeric micelles provide a unique and complementary
nanoplatform to the above nanosystems
for drug delivery applications. The hydrophobic cores of micelles provide a
natural carrier environment that allows easy encapsulation of poorly soluble
anticancer drugs. The non-covalent encapsulation strategy makes it feasible to
entrap drugs without the requirement of reactive chemical groups. Meanwhile,
the unique chemistry of the polymer constituents does allow for the chemical
conjugation of anticancer drugs, such as doxorubicin, to these chains, effectively
enhancing drug loading and hindering premature drug release upon
administration. Additionally, the size of polymeric micelles, 10-100 nm, can be
easily controlled by varying the hydrophobic block of the amphiphilic
copolymer. This size range also permits for evasion of renal filtration while
allowing for increased tumor penetration compared to liposomes.
41, 53, 54.
2.
Site specificity-
Active targeting strategies, which involve
the functionalization of the micelle surface with a
ligand that recognizes tumor-specific receptors, are an intense area of study
with several potential advantages. These include increased accumulation at
tumor sites as well as increased uptake into cancer cells via receptor-mediated
endocytosis. Commonly used ligands are grouped into
the following classes: small organic molecules, peptides, carbohydrates,
monoclonal antibodies, and DNA/RNA aptamers.
An example of a small organic molecule for
cancer targeting applications is folic acid, whose receptor is over-expressed
(100-300 times) in a variety of tumors. Park and coworkers functionalized
DOX-containing PEG-PLGA micelles with folic acid and were able to show
significantly increased uptake and cytotoxicity in KB
cells In vivo studies showed that folate-labeled
micelles led to a 2-fold decrease in tumor growth rate compared to non-targeted
micelles. Peptides are also actively explored as ligands for tumor-targeted
drug delivery. Recent work by our laboratory has investigated the use of cyclic
(Arg-Gly-Asp-D-Phe-Lys) (cRGDfK) peptide, which
targets the αvβ3 integrin
over expressed on the surface of angiogenic tumor
vessels.
Carbohydrate molecules, such as galactose and lactose, have also been used to functionalize
micelles. These ligands have high affinity for the asialoglycoprotein
receptor (ASGPR) over expressed in hepatocellular
carcinoma. A galactose-labeled poly(ethylene
glycol)-co-poly(γ-benzyl L-glutamate) block copolymer was used by Cho and
coworkers to produce micelles encapsulating paclitaxel,
and exhibited a 30% increased uptake in ASGPR cells. Monoclonal antibodies
represent another wide class of active targeting ligands. Recently, Torchilin and coworkers reported diacyllipid-PEG
(PE-PEG) micelles conjugated with an anti-cancer monoclonal antibody (mAb 2C5) or an anti-myosin mAb
2G4 antibody to target lung cancer cells. Micelles encoded with 2C5 were able
to increase paclitaxel accumulation (four-fold after
2 h) and cytotoxicity in lung tumors over control
micelles. Finally, tumor-specific aptamers, DNA or
RNA oligonucleotides identified by library screening,
are also gaining potential as targeting ligands. Docetaxel-loaded
PEG-PLGA micelles were recently conjugated with an RNA aptamer
specific for the prostate specific membrane antigen (PSMA) to treat prostate
tumors. In vivo studies in LNCaP xenografts showed overall increased anti-tumor efficacy and
lesser systemic toxicity than non-targeted micelles and more importantly, total
tumor regression in five of seven mice was reported.55, 56.
3.
Stimulated release of therapeutics-
Upon entering the tumor site, it is
desirable that the therapeutic agent be released from the micelles in a
controlled fashion in order to reach cytotoxic
levels. To achieve this, several strategies have been explored that include
pH-, temperature-, and ultrasound-stimulated release.
It is now well known that tumor tissues
tend to have lower pH values (as low as 5.7) than normal tissue environments
(pH 7.4), due to the glycolysis metabolism of cancer
cells. Additionally, the process of endocytosis or
the sequestration of the nanocarriers into vesicles
(e.g. late endosomes, and heavily degradative
lysosomes) is one associated with low pH values of
~5.0-5.5. Hence, changes in pH values encountered by micelles upon intravenous
injection provide a possible venue through which to achieve stimulated release
of drugs. Two different strategies have been reported to induce pH-sensitive
release of drugs from micelles. These include the use of acid-labile bonds and
non-covalent strategies involving selective protonation
of pH-sensitive components inside the micelle. In the first strategy, Kataoka and coworkers were able to formulate micelles where
doxorubicin was conjugated to the PEG-pAsp copolymer
via a hydrazone linkage. The resulting micelles had
high loading of DOX (42.5%) and pH sensitive release; 3% of the drug was
released after 48 h in pH 7.4 and 25% release of drug was achieved at the same
time at pH 5.5. In vivo studies showed increased tumor accumulation,
greater tolerance for the drug and tumor regression in 50% of mice.
Non-covalent strategies for pH-sensitive release were explored by several
groups. For example, Tang et al. devised a triblock
polymer of PEG, poly (2-(dimethylamino) ethyl methacrylate) (DMA), and poly (2-diethylamino) ethyl acrylate (DEA) resulting in a system that dissolves
completely in acidic solution but forms micelles at high pH (pH 8.0). Acid
sensitive release of dipyridamole was observed with a
50% increase of drug release at pH 3.0 over that at pH 7.4. 57- 61
Technologies that permit for site-specific
elevation of temperature have led to the development of heat-sensitive polymer
micelles. The polymer of choice is poly (N-isopropylacrylamide)
or pNIPAM, which has a lower critical solution
temperature (LCST) of 32 °C. Okano and coworkers reported micelles where poly
(butyl methacrylate) (PBMA) was used to form the
hydrophobic core while pNIPAM was used as the thermosensitive corona. The resulting pNIPAM-b-PBMA
micelles were loaded with DOX and released 15% of the drug after 15 h at 30°C,
compared to 90% release in the same time period at 37°C. Cytotoxicity
experiments showed less than 5% cell death at 29°C, but 65% cell death at 37°C.
Presently, ultrasound is used to trigger
drug release from drug delivery systems through mechanisms that include local
temperature increase, cavitation which increases the
permeability of cell membranes, and the production of highly reactive free
radical species which can accelerate polymer degradation. Pitt and coworkers
designed ultrasound-sensitive pluronic micelles
containing doxorubicin. Following stabilization of these pluronic
micelles with PEG-phospholipid (PEG-DSPE), in
vivo experiments showed that ultrasound was able to improve the antitumor
efficacy of both free DOX and micelle incorporated DOX, with ultrasound
delaying tumor growth significantly longer over micelles without ultrasound.62-65.
Thus unique architecture of polymeric micelles allows for
the incorporation of multiple functional components within a single micelle. By
combining tumor targeting, stimulated release of therapeutics, and the delivery
of imaging agents, multiple interventions against a tumor can be integrated
into one platform. Such a ‘theranostic’ entity has
been defined as a Nanomedicine platform that can
diagnose, deliver targeted treatment in a controlled manner, and monitor
response to cancer therapy.
2. Ultrasonic-Activated Micellar
Drug Delivery for Cancer Treatment-
The high toxicity of potent
chemotherapeutic agents limits the therapeutic window in which they can be utilized. This window can
be expanded by controlling the drug delivery in both space (selective to the
tumor volume) and time (timing and duration of release) such that non-targeted
tissues are not adversely affected. Research in this area has focused on the
synthesis of different drug depots that are capable of delivering a high
concentration of chemotherapy drugs to cancerous tissues without affecting
cells and organs in the systemic circulation. These depots can be broadly classified
into three groups: liposomes, micelles and shelled
vesicles. In this review we focus on the use of micelles in conjunction with
ultrasound (US) to treat cancerous tissues. Low frequency ultrasound refers to
frequencies less than 1 MHz, while the ranges for medium and high acoustic
frequencies are 1-5 MHz and 5-10 MHz, respectively. We will present the
advantages and disadvantages of such a drug delivery system, the recent
advancements in this field, the future directions, and some unanswered questions
that remain in this research topic; but first we will discuss the advantages of
ultrasound.
The mechanisms of this acoustically
activated micellar drug delivery system are still
under investigation, and in vitro there is a strong correlation with insonation frequency and power density that suggests a
strong role of cavitation. Here we will discuss the
two main mechanisms that render this micellar drug
delivery system effective. Ultrasound appears to disrupt the core of polymeric
micelles, allowing the drug to be released in the volume of the ultrasonic
field. Additionally, ultrasonic waves have been shown to cause the formation of
micropores in cell membranes, which in turn allows
for the passive diffusion of drugs into cell.66, 67, 70
Disruption of micelles:
After proving that Dox
and Rb were released from micelles under the action
of ultrasound, Husseini et al. embarked on a study of
the mechanism underlying this release. They improved their previously designed
ultrasonic exposure chamber with fluorescence detection so as to record
acoustic emissions at 70 kHz while simultaneously recording the decrease in
fluorescence. This in vitro study showed that there is a threshold
value of about 0.38 W/cm2 below which no measurable release
occurred. Furthermore the onset of Dox release from
P105 micelles corresponded to the emergence of a subharmonic
peak in acoustic spectra at this same threshold. The existence of a threshold
at this intensity tends to point toward a strong role of cavitation,
particularly inertial or collapse cavitation, in this
release phenomenon. Several groups have reported the existence of a threshold
for the onset of inertial cavitation. 68, 69
Several publications have reported
ultrasonic intensity thresholds for an observed biological effect in cells and
tissues Mitrogotri et al. were the first to show the
existence of an ultrasonic threshold for enhancing skin permeability. This
threshold is a strong function of ultrasound frequency; as the frequency
increases so does the threshold. Tang el al. showed that low-frequency sonophoresis (LFS) was able to permeabilize
pig skin using 20 kHz ultrasound.71 They postulated that the key mechanism
involved in LFS is cavitation bubbles induced by US.
Copious research has been conducted on increased cell membrane permeability
under the action of ultrasound For example; there is a reported threshold for
DNA delivery to rabbit endothelial cells of about 2,000 W/cm2 at a
pulse average intensity 0.85 MHz (short pulse average intensity). Another example
is the threshold of 0.06 W/cm2 at 20 kHz reported by Rapoport et al. for HL-60 lysis.
The range reported for biological thresholds is obviously very large, and thus
provides little guidance for a priori prediction of threshold values
for biological events. One must remember that in biological systems, the
observed event is not the threshold of inertial cavitation;
there is usually an ultrasonic intensity beyond the simple inertial cavitation threshold that is required to provide sufficient
numbers and sufficient intensities of damaging cavitation
events. Biological systems are much more complicated. In addition to the
experimental factors mentioned above (e.g., level of gas saturation and
heterogeneous nucleation materials), one must also consider the cells involved.
For example, biological manifestations will be related to things such as the
proximity of the cells to the collapse events, the presence of microjets from collapse events, the cell membrane strength
and integrity, the requirements following cell membrane permeation (transport
only to the cytosol or all the way to the nucleus) to
produce a biological response, and much more. Obviously, much research remains
to be done in this area of predicting thresholds for cellular response.
In this review, we will devote some
discussion to the origin of the subharmonic acoustic
peak, inertial cavitation, and its relation to the
release phenomena. As bubbles oscillate with increasing amplitude in an
ultrasonic field (of frequency f), they start to generate higher
harmonic (2f, 3f, etc.), ultraharmonic
(3/2 f, 5/2f, etc.), and subharmonic
(f/2, f/3, etc.) emissions. There are reports that correlate
the subharmonic emission with certain indicators of
inertial cavitation, including sonoluminescence,
acoustic white noise, and iodine generation. Leighton used mathematical
modeling of cavitating bubbles to simulate a signal
at f/2 (the subharmonic) and came to the
conclusion that a subharmonic occurs due to a
prolonged expansion phase immediately preceding a delayed collapse phase of the
bubble implosion even. However, modeling by others show that the f/2
signal can be produced (mathematically at least) without collapse cavitation occurring, albeit the definition of “collapse”
is difficult to define in a mathematical model.
Also the membrane permeability of 3T3 mouse
cells correlates with an increase in background noise in acoustic spectra. The
group came to the conclusion that ultrasound-induced permeabilization
of cell membranes is caused by collapse cavitation events.
On the other hand, Liu et al. found a strong dependence of the degree of hemolysis (permeabilization of
red blood cells as measured by the degree of hemoglobin release) on the
intensities of the subharmonic and ultraharmonic frequencies, but not on the broadband noise
The group concluded that the best correlation between ultrasonic parameters and
hemolysis was the product of the total ultrasonic
exposure time and the subharmonic pressure.
Accordingly, there are varied opinions as to whether the subharmonic
emission always correlates with biological phenomena, or even with collapse cavitation.
As to the relationship between the
mechanism of release and inertial cavitation, Husseini et al. postulated that as the shock wave caused by
collapse cavitation propagates through the vicinity
of a micelle, the abrupt compression and expansion of fluid in the shock wave
is able to shear open the micelle so that the drug is released or at least
exposed to the aqueous environment. Oscillating bubbles, even in stable cavitation, create very strong shear forces near the
surface of the bubble. The shearing velocity of fluid near a 10 micron
(diameter) bubble, with a 1 micron oscillation amplitude and 70 kHz oscillation
frequency is approximately 1 m/s
Additionally, it important to keep in mind that the extremely high
viscous shear rates near the surface of 10-μm bubbles are on the order of
105 sec-1.
Furthermore, this rate is equivalent to shearing water in a 1 mm gap between
parallel plates in which plate is stationary and the other moving at 100 m/s.
Thus, the group speculated that these shear forces may be strong enough to open
up a P105 micelle, exposing the hydrophobic drug inside its core to the
surrounding aqueous environment.
The group also extended their study of the
release mechanism to stabilized and unstabilized
micelles. In this study they compared the release of Dox
from the core of unstabilized Pluronic®
105 micelles to the release from stabilized micelles such as NanoDeliv™ micelles and micelles of pENHL
described previously in section 3. They found that the release of Dox at 37 °C from Pluronic®
micelles appeared to be several times higher than the release from the more
stabilized micelles. Interestingly, the onset of release occurred at about the
same power density for all carriers investigated in their study, whether
stabilized or not. Similarly, the threshold of Dox
release from all three micelles correlated with the emergence of subharmonic peaks in the acoustic spectra. Apparently the
structures of the stabilized and non-stabilized micelles are perturbed by cavitation events that cause the release of Dox. The group hypothesized that stabilized micelles are
less susceptible to disruption by the shearing forces of shock waves produced
by cavitation events since the threshold of release
also correlates with the subharmonic peak in all micellar systems investigated, discovering the origin of
the subharmonic peak is vital in understanding drug
release from micelles under the action of ultrasound. 72-77
Disruption of cell membrane:
Although Pitt's group has focused on
studying the possible mechanisms by which the P105 micelles and ultrasound drug
delivery system induce drug uptake by the cancer cells, is has also studied the
biological mechanism involved here. The comet assay was used to quantify the
amount of DNA damage in HL-60 cells by measuring the fraction and length of
broken nuclear DNA strands. Large amounts of DNA damage as measured by the
comet assay are indicative of cell death, either by necrosis or by apoptosis 18. Results of the
comet assay show that Dox eventually binds to the DNA
and causes it to fragment. In a separate but related study, Husseini
et al. reported on the mode of cell death exhibited by cells exposed to a
combination of Pluronic® micelles,
ultrasound and Dox. Using the comet assay, the group
observed the electrophoretic pattern of the nuclear
DNA from HL-60 cells insonated at 70 kHz in a
solution of P105 micelles containing 10 μg/ml
Dox for 30 minutes, 1 hour and 2 hours. The
pattern of the DNA fragments as well as the gradual damage observed after two
hours of ultrasonic exposure were consistent with apoptosis as a mode of cell
death rather than necrosis. However, the question remains as to if and how
ultrasound enhances uptake of Dox by the cell. In
this section, we will discuss three postulated mechanisms that have been tested
in an attempt to answer the above question. These mechanisms are 1) ultrasonic
release of the drug from micelles is followed by normal transport into the
cell; 2) ultrasound upregulates endocytosis
of the micelles (with drug) into the cell; 3) ultrasound perturbs the cell
membrane which increases passive transport of the drug and Pluronic®
molecules into the cell.68, 69, 72-74
The first hypothesis proposes that the drug
is released from micelles outside the cancer cells, followed by normal
penetration of the polymer and drug into the cells by simple diffusion or
normal cellular uptake mechanisms. To test this postulated mechanism, the
hydroxyl groups at the ends of P105 chains were labeled with a fluorescein derivative. HL-60 cells were then incubated or sonicated with the fluorescein-labeled
P105 micelles containing Dox, which fluoresces at a
different wavelength. Results showed that Dox in 10
wt % P105 appeared inside the cells.
The next question was whether the
fluorescently-labeled P105 entered the cells along with or independent of the Dox. The experiments revealed the presence of P105 inside
the cells when incubated or insonated for 20 minutes.
Because the labeled P105 molecules themselves were found inside the HL-60
cells, they rejected the first hypothesis of external drug release followed by
passive drug diffusion without the polymeric diffusion into the cells. Although
their experiment showed that the P105 entered the cells, it was not possible to
determine whether the copolymer entered the cells through holes punched in the
cell membrane or through endo-/pino-cytotic
routes.
Next they turned their attention to the
second hypothesis whereby entire micelles (with drug) are endocytosed
into the cells. Since it is unlikely that HL-60 cells express a receptor for Pluronic® micelles, receptor-induced endocytosis was considered to be very unlikely. However, pinocytosis involves vesicles that nonspecifically engulf
small volumes of extracellular fluid and any material contained therein. To
test the postulate that the cells were taking up the drug and P105 in by endocytosis, a model drug that fluoresces more strongly in
acidic environments was used, namely Lysosensor
Green. This probe has a pKa of 5.2, which causes it
to fluoresce more strongly in an acidic compartment such as a lysosome. The great majority of endosomes fuse with a primary lysosome
to form a secondary lysosome, which has a pH of about
4.8 while the pH outside these compartments is about 7.1. Cells exposed
to US and P105 micelles with Lysosensor Green were
examined by flow cytometry, which showed no
difference in fluorescence between cells incubated and insonated
for 1 hour at 70 kHz. Thus, ultrasonic exposure did not cause the probe to
partition to a more acidic environment anymore than it did without ultrasound,
and the hypothesis was rejected that US induces upregulation
of endo-/pino-cytosis. The
observation that US enhanced the uptake of both drug and labeled Pluronic® supported the third hypothesis that
drug-laden micelles entered through holes in the membranes of insonated cells in these studies. It is relevant that Rapoport et al. reported that US-assisted micellar
drug delivery enhances the rate of endocytosis into
cells.70,71,78
3. Micellar Nanoparticles: Applications for Topical drug delivery
This is used to deliver API locally in an efficient manner. This concept
is explained by using acyclovir which is an antiherpes
agent. Commercially available acyclovir product - Zovirax
which is to be applied for 5to7 times a day for 4–7 days. Comparative
investigations were done with zovirax and MNP (for
topical drug delivery).It was found that the amount of drug retained within
skin was twofold higher for MNP than zovirax.
FUTURE
PROSPECTUS:
Development
of micellar syrup-
Current
research is going on the development of the vitamin micellar
syrup with the aim of increasing the absorption of the vitamins as well as to
reduce the dose frequency. Use of biodegradable polymers in
formation of micelle for targeted drug delivery system. The agents that
have been encapsulated in nanoparticles for
ultrasonic delivery have been primarily hydrophobic drugs. Future work includes
other drug delivery vehicles having hydrophilic volumes and is able to
sequester and deliver hydrophilic drugs. Development of core-crosslinked micelles in order to enhance in vivo stability.
CONCLUSION:
Micelles
are dynamic structures having polar head and non-polar tail. They are formed from monomers. They can be
normal phase micelles or reverse phase micelle. Distribution and orientation of drug in micelle depends upon hydrophilicity or hydrophobicity
of the drug. Micellization has a prime role in solublization of the essentially insoluble drug as it tends
to encapsule those insoluble drugs into partially
aqueous environment. Block copolymers which are formed by the hydrophilic as
well as hydrophobic blocks are used to form micelles shows enhanced efficacy in
targeted drug delivery system. Currently polymeric micelles are enjoying
topmost position in micellar drug delivery system
mainly in the case of delivery of the chemotherapeutic agents. They increase
the solublization of the drug; actively target them
as well as release the drug in the stimulus response manner. In addition to
this they are also used as diagnostic agents in cancer treatment. Thus many of
the advantages related to drug delivery in cancer are integrated in a single
platform of polymeric micelle hence they are popularly termed as
multifunctional nanomedicinal systems.
REFERENCES:
1.
Alan D, Mac Naught, Andrew R. Wilkinson (Eds.).
Compendium of Chemical Terminology: IUPAC Recommendations (2nd Ed.)
(The "Gold Book”). Blackwell Scientific Publications, Oxford. 1997.
2.
J. W. McBain. Transactions
of the Faraday Society, 9; 1913:
93-107.
3.
G. S.
Hartley. Aqueous Solutions of Paraffin Chain Salts, a Study in Micelle Formation.
Hermann et Cie, Paris: 1936.
4.
Mittal K. Micellization, Solubilization and
Microemulsions (2), Plenum Press, New York. 1965.
5.
Tanford C.
The Hydrophobic Effect: formation of micelles and biological membranes. John
Wiley, New York. 1973.
6.
Chevalier
Y, Zemb T. The structure of micelles and microemulsions. Reports on Progress in Physics, 53; 1990: 279-371.
7.
Tanford C.
The hydrophobic effect: Formation of
micelles and biological membranes. Wiley, New York, 1980.
8.
Israelachvili JN. Intermolecular and
surface forces, 2nd Ed. Academic Press, London, 1991.
9.
Nakul C, Maiti
MM, G. Krishna, PJ Britto and N. Periasamy.
Fluorescence Dynamics of Dye Probes in Micelles, The Journal of Physical Chemistry B, 101; 1997:
11051-11060.
10. Ettireddy PR, Lev Davydov and Panagiotis G. Smirniotis, characterization of Titania
Loaded V-, Fe and Cr-Incorporated MCM-41 by XRD, TPR, UV−VIS, Raman, and
XPS Techniques The Journal
of Physical Chemistry B, 106 (13); 2002: 3394–3401.
11. Faheem NP, Mohammed Yaseen, Barbara Gore, Sarah Rogers,§Gordon
Bell and Jian RL. Influence of Molecular Structure on the Size,
Shape, and Nanostructure of Nonionic CnEm Surfactant
Micelles The Journal
of Physical Chemistry B, 118; 2014: 179−188.
12. Florence AT, Attwood D. Physicochemical Principles of Pharmacy,
3rd Ed. The MacMillan Press, London, 2003.
13. Keith BO,
A Gouy–Chapman–Stern model of the double layer at a
(metal)/(ionic liquid) interface, Journal
of Electroanalytical Chemistry, 613; 2008:
131–138.
14. Scheme CO, Rangel Y, A Pessoa-Jr,
LC Tavares. Micellar solubilization
of drugs. Journal of Pharmacy and Pharmaceutical Sciences, 2; 2005: 147-163.
15. Sherman P. Emulsion science. Academic
Press, New York. 1968.
16.
Shinoda K.
Solvent properties of surfactant solutions. Marcel Dekker, New York 1967.
17.
McBain E,
Hutchinson. Solubilization and related phenomenon,
Academic Press, New York. 1955.
18. Torchilin VP. Micellar nanocarriers: pharmaceutical perspectives. Pharmaceutical Research, 24(1); 2007:
1-16.
19. Lavasanifar A, Samuel J, Kwon GS. Poly(ethylene
oxide)-block-poly(L-amino acid)
micelles for drug delivery. Advanced Drug Delivery Reviews,
54; 2002: 169-190.
20. Adams ML, Lavasanifar
A, Kwon GS. Amphiphilic block copolymers for drug
delivery. Journal of Pharmaceutical Science, 92(7); 2003: 1343-1355.
21. Gadelle F, Koros WJ,
Schechter RS. Solubilization of aromatic solutes in
block copolymers. Macromolecules, 28; 1995:
4883–4892.
22. Shah DO, Micelles: microemulsion
and monomer science and technology. 1-3; 1998: 101-176.
23. Hobbs ME. The effect of salts on the critical
concentration, size, and stability of soap micelles. The Journal of physical
and colloid chemistry,
55(5); 1951: 675–683.
24. Flochart BD. The effect of temperature on the
critical micelle concentration of some paraffin-chain salts; Journal of colloidal science, 16, 1961:
484-92.
25. Mukerjee P and Mysels KJ.
Critical Micelle Concentration of Aqueous Surfactant Systems. Data Sevr. Natl. Bur. Stand. U.S 36, US Government Printing
Office, Washington D.C. 1971.
26. Molyneux P, Rhodes CT and Swarbrick
J. Thermodynamics of Micellization of N-alkyl betaines. Transactions
of the Faraday Society, 61;
1965: 1043–52.
27. Angelica RG, E. JV Carter and NA Demarse.
Thermodynamics of Micelle Formation TA
Instruments – Applications Note MCAPN,
05; 2010.
28. C. Carnero Ruiz.
Thermodynamics of micellization of tetradecyltrimethylammonium bromide in ethylene glycol
water binary mixtures: short communication. Colloid and Polymer Science, 277: O Springer Verlag;
1999: 701-707.
29. Okawauchi M, Shinoza M, Ikawa Y and Tanaka MJ. Kinetic studies of some esters and amides in presence of micelles, The journal Physical
Cemistry, 91; 1987: 109.
30. Hall DG and Tiddy
GJT. “Anionic surfactants, physical
chemistry of surfactant action. (E.H. Lucassen Reynders.) Marcel Dekker, New York. 55; 1981.
31. Krassimir D, Danov A,
Peter A, Kralchevsky A, Kavssery
P. Ananthapadmanabhan.Micelle–monomer equilibria in solutions of ionic surfactants and inionic–nonionic mixtures: A generalized phase separation
model, Advances in Colloid and Interface
Science, 206; 2014: 17–45.
32. PA Koya, Kabir-ud-Din,
K Ismail. Micellization and Thermodynamic Parameters
of Butanediyl-1,4-bis(tetradecyldimethylammonium
Bromide) Gemini Surfactant at Different Temperatures: Effect of the Addition of
2-Methoxyethanol, Journal of Solution Chemistry, 41; 2012: 1271–1281.
33. Mall S, Buckton
G, Rawlins DA. Dissolution
behaviour of sulphonamides into sodium dodecyl sulphate micelles: A
thermodynamic approach. Journal of Pharmaceutical Science,
85(1); 1996: 75-78.
34. Allen TM, Hansen CB, Menenez
DEL. Pharmacokinetics of long-circulating liposomes.
Advanced
Drug Delivery Reviews, 16; 1995: 267–284.
35. Canto GS, Dalmora
SL, Oliveira AG. Piroxicam encapsulated in liposomes: characterization and in vivo evaluation of
topical anti-inflammatory effect. Drug Development Industrial Pharmacy,
25; 1999: 1235-1239.
36. Gref R, Minamitake Y, Peracchia MT, Trubetskoy VS, Torchilin VP,
Langer R. Biodegradable long-circulating polymeric nanospheres.
Science,
263; 1994: 1600–1603.
37. Torchilin, V.P. Structure and design of polymeric
surfactant-base drug delivery systems. Journal of Control Release, 73;
2001: 137-172.
38. Rosen MJ. Surfactants and Interfacial phenomena, 2nd Ed, John
Wiley and Sons, New York, 1989.
39. Dutt GB. Rotational diffusion of hydrophobic
probes in Brij-35 micelles: Effect of temperature on micellar
internal environment. Journal of Physical Chemistry B,
107; 2003: 10546-10551.
40. S Danson, D
Ferry, V Alakhov, J Margison,
D Kerr, D Jowle, M Brampton, G Halbert,
and M Ranson. Phase I dose
escalation and pharmacokinetic study of pluronic polymerbound doxorubicin (SP1049C) in patients with
advanced cancer. British Journal of Cancer,
90; 2004: 2085-2091.
41. Y Matsumura, T Hamaguchi,
T Ura, K Muro, Y Yamada, Y
Shimada, K Shirao, T Okusaka,
H Ueno, M Ikeda, and N Watanabe. Phase I clinical trial
and pharmacokinetic evaluation of NK911, a micelle-encapsulated doxorubicin. British Journal of Cancer, 91; 2004: 1775-1781.
42. TY Kim, DW Kim, JY Chung, SG Shin, SC Kim,
DS Heo, NK Kim and YJ Bang. Phase
I and pharmacokinetic study of Genexol-PM, a cremophor-free, polymeric micelleformulated
paclitaxel, in patients with advanced malignancies. Clinical Cancer Research, 10; 2004:
3708-3716.
43. Chris O, Wouter
B, Mariska B, Gert S, Frank
WJN, Wim EH. Polymeric micelles in Anticancer
Therapy: targeting, imaging and triggered release. Pharmaceutical Research, 27; 2010: 2569-2589.
44. Damon S, Norased
N, Elvin B, Jinming G. Functionalised
Micellar systems for cancer targeted drug delivery. Pharmaceutical Research, 24(6); 2007:
1029-1046.
45. World health organization: fact shhet cancer. http:// www.who.int/mediacentre/factsheets/fs297//en/index.html.
(accessed 10-12-09).
46. Torchilin VP. Micellar nanocarriers: pharmaceutical perspectives. Pharmaceutical Research. 24(1); 2007:
1-16.
47. Mishra B, PatelBB, Tiwari S. Colloidal nanocarriers:
a review on formulation technology, types and applications toward targeted drug
delivery. Nanomedicine, 6; 2010: 9-24.
48. Torchilin VP Targeted pharmaceutical nanocarriers for cancer therapy and Imaging. American Association of Pharmaceutical
Scientists, 9th Ed. 2007: 128-147.
49. M Jones and J Leroux.
Polymeric micelles : a new generation of colloidal
drug carriers. European Journal of Pharmaceutics and
Biopharmaceutics, 48; 1999: 101-111.
50. Adams ML, lavasanifar
A, Kwon GS. Amphiphilic block polymers for drug
delivery. Journal of Pharmaceutical
Science, 92; 2003: 1343-55.
51. Trubetskoy VS. Polymeric micelles as carriers of
diagnostic agents. Advanced drug
delivery reviews, 37; 1999: 81-88.
52. V. P. Torchilin.
Structure and design of polymeric surfactant-based drug delivery systems. Journal of Control Release, 73;
137-172: 2001.
53. O Soga, CF van Nostrum, M Fens, CJ Rijcken, RM Schiffelers, G Storm
and WE Hennink. Thermosensitive
and biodegradable polymeric micelles for paclitaxel
delivery. Journal of Control Release,
103; (2005): 341-353.
54. DM Lynn, MM Amiji
and R Langer. pH-responsive polymer microspheres:
rapid release of encapsulated material within the range of intracellular pH. Angewandte Chemie International Edition, in English,
40; (2001): 1707-1710.
55. HS Yoo and TG
Park. Folate receptor targeted biodegradable
polymeric doxorubicin micelles. Journal
of Control Release, 96; 2004: 273-283.
56. Nasongkla N, Shuai X, Ai H, Weinberg BD, Pink J, Boothman DA et al. cRGD- delivery. Angewandte Chemie
International Edition, in English, 43; 2004: 6323-27.
57. H Hayashi, M Iijima,
K Kataoka and Y Nagasaki. pHsensitive nanogel
possessing reactive PEG tethered chains on the surface. Macromolecules, 37; 2004: 5389-5396.
58. TK Bronich, PA Keifer, LS Shlyakhtenko and AV Kabanov. Polymer micelle with cross-linked ionic core. Journal of the American Chemical Society,
127; 2005: 8236-8237.
59. J van der Zee.
Heating the patient: a promising approach? Annals of
Oncology, 13; 2002: 1173-1184.
60. KS Soppimath, DCW
Tan and YY Yang. pH-triggered thermally responsive
polymer core-shell nanoparticles for drug delivery. Advanced Materials, 17; 2005: 318.
61. SQ Liu, YW Tong and YY Yang. Incorporation
and In vitro release of doxorubicin in thermally sensitive micelles made from poly(N-isopropylacrylamide-co-N,N-dimethylacrylamide)- b-poly(D,L-lactide-co-glycolide) with varying compositions. Biomaterials, 26; 2005: 5064-5074.
62. JE Chung, M Yamato, T Aoyagi, M Yokoyama, Y
Sakurai and T Okano. Temperature-responsive polymeric micelles as intelligent
drug carriers. Journal of the American
Chemical Society, U5; 1998: 216.
63.
XM
Liu, KP Pramoda, YY Yang, SY Chow and C B He. Cholesteryl grafted functional amphiphilic
poly (N isopropylacrylamide-co-N-hydroxylmethylacrylamide):
synthesis, temperature sensitivity, self assembly and encapsulation of a
hydrophobic agent. Biomaterials, 25;
2004: 2619-2628.
64. XM Liu, YY Yang and KW Leong. Thermally
responsive polymeric micellar nanoparticles
self-assembled from cholesteryl end-capped random poly(N-isopropylacrylamide-
co-N,N-dimethylacrylamide): synthesis, temperaturesensitivity, and morphologies. Journal of Colloid and Interface
Science, 266; 2003: 295-303.
65. E Ruel-Gariepy
and JC Leroux. In situ-forming hydrogels
preview of temperature-sensitive systems. European Journal of Pharmaceutics and
Biopharmaceutics, 58; 2004: 409-426.
66. S Mitragotri.
Innovation- Healing sound: the use of ultrasound in drug delivery and other
therapeutic applications. Nature Reviews
Drug Discovery, 4; 2005: 255-260.
67. N Rapoport, AI
Smirnov, A Timoshin, AM
Pratt and WG Pitt. Factors affecting the permeability of Pseudomonas aeruginosa cell walls toward lipophilic
compounds: Effects of ultrasound and cell age. Archives of Biochemistry
and Biophysics, 344; 1997: 114-124.
68. GA Husseini, CM Runyan and WG Pitt. Investigating the mechanism of
acoustically activated uptake of drugs from Pluronic
micelles. BMC Cancer. 2: 2002.
69. GA Husseini, NY Rapoport, DA Christensen, JD Pruitt and WG Pitt. Kinetics
of ultrasonic release of doxorubicin from pluronic
P105 micelles. Colloids Surface B: Biointerfaces, 24; 2002: 253-264.
70. N Rapoport, WG
Pitt, H Sun and JL Nelson. Drug delivery in polymeric micelles: from in vitro
to in vivo. Journal of Control Release,
91; 2003: 85-95.
71. Tang RP, Ji WH,
Wang C. Amphiphilic block copolymers bearing ortho ester side-chains: pH-dependent hydrolysis and
self-assembly in water. Macromol Bioscience, 10; 2010: 192–201.
72. Marin A, Sun H, Husseini GA, Pitt WG, Christensen DA, Rapoport
NY. Drug delivery in pluronic micelles: effect of
high frequency ultrasound on drug release from micelles and intracellular
uptake Journal of Control Release.
84; 2002: 39–47.
73. Husseini GA, Christensen DA, Rapoport
NY, Pitt WG. Ultrasonic release of doxorubicin from Pluronic
P105 micelles stabilized with an interpenetrating network of N,N-diethylacrylamide. Journal of Control Release, 83;
2002:303–315.
74. Husseini GA, O’Neill KL, Pitt WG. The comet assay
to determine the mode of cell death for the ultrasonic delivery of doxorubicin
to human leukemia (HL-60 Cells) from Pluronic P105
micelles. Technology
in cancer research and treatment,
4; 2005: 707–711.
75. Husseini GA, El-Fayoumi RI,
O’Neill KL, Rapoport NY, Pitt WG. DNA damage induced
by micellar-delivered doxorubicin and ultrasound:
comet assay study. Cancer Letters, 154;
2000: 211–216.
76. Rapoport N. Combined cancer therapy by micellar-encapsulated drug and ultrasound International Journal of Pharmaceutics, 277; 2004: 155–162.
77. Pruitt JD, Pitt WG. Sequestration and
ultrasound-induced release of doxorubicin from stabilized Pluronic
P105 micelles. Journal of Drug Delivery, 9; 2002:
253–261.
78. RW Jansen, G Molema,
TL Ching, R Oosting, G
Harms, F Moolenaar, MJ Hardonk
and DK Meijer. Hepatic endocytosis of various types
of mannose-terminated albumins. What is important, sugar recognition net charge
or the combination of these features. Journal
of Biological Chemistry, 266; 1991: 3343-3348.
Received on 10.07.2014 Modified on 22.07.2014
Accepted on 14.08.2014 ©A&V Publications All right reserved
Res. J. Pharm.
Dosage Form. and Tech. 6(4):Oct.- Dec.2014; Page 267-281