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54
Nano Physical Pharmaceutics of Micelle-Based Systems
polymerization of PEG is high at room temperature, because water only exists in the thin layer among micelles, while the high-concentration aqueous solution is extremely viscous. As the temperature increases, the hydrogen bond between PEG and water molecules is destroyed, causing water loss and spherical micelle formation. Becher et al. studied the shape of micelles by measuring the light scattering data and viscosity of polyethylene glycol lauryl ether aqueous solution and found that when the number of
          
the surfactant molecules are longitudinally arranged into round rod-shaped micelles.

2.1.3 Mixed Micelle

Mixed micelles are mixtures of amphiphile systems (including surfactants, polymers, and copolymers) that aggregate into the
      
the individual amphiphile. Alcohol with six or more carbon atoms can be added to the micelle solution, and embedded between the surfactant molecules to form a mixed micelle. Since the total surface charge of the micelle remains unchanged, while the surface area expands due to the embedding of alcohol molecules, the surface charge density of the micelle decreases, and hence the decrease of ionic repulsion and CMC value. The mixed micelle

mentioned above.

2.2 Preparation of Micelles

Polymeric micelles (PMs) are formed from amphiphilic block copolymers, which have hydrophobic polymer chains linked to hydrophilic polymeric chains. Their good biocompatibility, stability and drug-loading capability have led to the development of nanomedicines, and some are already industrialized or currently being tested in clinical trials. The preparation of PMs, which are the focus of this chapter, can be summarized into two methods.

Effects on Micelle Assembly

55
     
the segments to dissolve the bulk sample. Notably, this method only works under the premise that the total MW of the copolymer is small enough with a short-length insoluble block. Other ways including prolongated stirring, thermal, or ultrasound treatments are used to “anneal” the solution for better solubility. However, research shows that these techniques have the disadvantage that they easily lead to non-equilibrium micelles, especially when the core-forming chains are below phase transition temperature (Tg). The annealing treatment can only lead to the dispersion of samples into the selective solvent, rather than forming micelles based on a unimer–aggregate equilibrium. In other words, the
    
morphology of the starting bulk sample [8].
         
a non-selective solvent to achieve complete dissolution at the molecular level. Then, a selective solvent for one segment is added in order to trigger aggregation of the dissolved chains and hence micelle formation. To remove the initial non-selective solvent, the method of evaporation or dialysis against selective solvent was
   
common way to prepare micelle solution [9]. Other ways, such as changing pH value or temperature to reach the unimer–micelle equilibrium, can be used to prepare stimulus-responsive micelles that undergo morphology change with applied stimulus, as will be discussed in Section 2.5.
2.3 Effects on Micelle Assembly

2.3.1 Critical Micelle Concentration

The minimum concentration of surfactant molecules that associate to form micelles in the solvent is the CMC. When the concentration of the surfactant is below CMC, it has a strong adsorption tendency
  
such that the hydrophilic group is dissolved in water and the hydrophobic group is exposed to the air to reduce the surface tension of the air/water interface. As the concentration increases,
56
Nano Physical Pharmaceutics of Micelle-Based Systems
the adsorbed molecules at the interface increase until saturation. Then the surfactant enters the solution, and when reaching CMC, micelles are formed through intermolecular association. If so, the properties of the solution, such as osmotic pressure, density, interfacial tension, and molar conductivity, all show sudden changes.
Therefore, when the concentration of many aqueous solutions
of amphiphilic substances increases, the properties of the
        
is usually much larger than that caused by the increase of strong electrolytes in the aqueous solution. For example, by plotting the surface tension, conductivity or light scattering intensity against concentration, it is easy to see the non-ideal deviation through the change of the slope of the curve, and the root cause is the formation of micelles. As the concentration of surfactant molecules increases, their structures can change from single molecules to spherical, rod-shaped and layered micelles. It is generally believed that the concentration when spherical micelles are formed is the
        
transformed into rod-shaped micelles is the second CMC.

2.3.2 Mechanism of Micellization

The micellization of surfactants can reduce the total free energy of the solution. The aggregation of the hydrophobic moiety makes it lose a certain degree of freedom, which means that the entropy will decrease [4]. Compared with single molecules, the translational entropy and rotational entropy of micelles are both reduced. On the other hand, the interaction between the hydrophilic group in the surfactant molecule and water reduces the free energy of the system, while the free energy of the system increases by reducing the contact between the hydrophobic moiety and water molecules through micellization. In addition, the hydrophilic groups may be ionized and charged, and the resulting electrostatic repulsion will not be conducive to the generation of micelles. It can be seen
         
micelle assembly from block copolymer.
Effects on Micelle Assembly
57
Micellization is mainly driven by the entropy change

between the hydrophobic moiety and water, water molecules have a tendency to be driven from the hydrophobic region to the bulk aqueous solution, for which the disorder increases, so the entropy of the system increases. The micellization process can be expressed by free energy and CMC through the following equation:
DG0 = RT ln(CMC) (2.1)
where DG0 is the standard free energy change of micellization, R is the gas constant, T is the absolute temperature of the system, and CMC can also be expressed by enthalpy:
ln(CMC) =
DH
0
+Constant
(2.2)
RT
It is assumed that the standard enthalpy change of micellization is DH0, and is independent of the aggregation number and temperature.
From the perspective of thermodynamics, there is a dynamic equilibrium in the process of forming micelles with an aggregation number of “m” from a single surfactant molecule (Z), where the equilibrium constant K is:
mZ Zm (2.3)
Zm
[]
=
(2.4)
K
m
m
Z
[]
DGm0 refers to the free energy for transferring a single surfactant molecule from water medium to a micelle.
mDGm0 = –RT ln K (2.5)
In the basic equation of micellization, RT lnK can be replaced equivalently by mDGm0, where the concentration is expressed in mole fraction.
58
Nano Physical Pharmaceutics of Micelle-Based Systems
0
mDGm
lnXm =− + mln X1 + lnm
(2.6)
RT
Xm refers to the number of moles of surfactant molecules in a
micelle with aggregation number of m, X1 is the mole fraction of the monomer, and Xm is a function of m X1.
This equation can be regarded as a distribution function of the micelle volume, and the collaboration of micelle formation is
X1 in the equation. Xm obtained by X1 in a narrow
range close to the CMC is more reasonable.
DGm0 = DUm0 + Wm 
DUm0 represents the change of the free energy of hydrophobic
hydrocarbyl groups in the surfactant molecule in the transfer from water to the micelle core. Wm represents the free energy resulting from repulsion between polar head groups. For a given surfactant system, the micellization and CMC depend on the relative balance of forces that favor and delay molecular aggregation, and also


2.3.3 Influence of the Surfactant Structure on CMC

The micellization of surfactants in aqueous solution is controlled by two opposite forces. The hydrophobic force, which drives hydrophobic moiety out of the aqueous environment and aggregate to form the nucleus, is the main driving force for micellization. The polar head group extends into the water to form a shell after being dissolved, and the electrostatic repulsion or steric hindrance is not conducive to the formation of micelles. There is a delicate balance between the driving force and the counterforce. In addition, factors such as the volume of hydrophobic groups, the structure of polar groups, co-solutes, pH and temperature

2.3.3.1 Volume of hydrophobic groups
The volume of the hydrophobic group in surfactant has the greatest
      
hydrophobic moiety, it is possible to enhance the hydrophobic
Effects on Micelle Assembly
59
         
Table 2.2 lists corresponding values to some surfactants.
Table 2.2 Value A & B of various surfactants
Surfactant Temperature/°C A B
C
m
 25 1.92 0.290
C
mSO2
Na 40 1.59 0.294
C
mSO4
Na 45 1.42 0.265
C
mNH3
HCl 25 – 
Note: Cm represents the carbon chain with m carbon atoms.
        
phobicity of surfactants can be estimated by Table 2.3 and can
the micelles increases.
Table 2.3 Properties of substituent groups
Substituent Group Classification
–CH
3
Hydrophobic
–CH
2
– Hydrophobic
–Cl, –Br, –F Hydrophobic
–N(CH
3)2
Hydrophobic
CMC
of surfactant
the molecule
decreases
increases.
as
For
compounds
the length of
with
the
carbon
the
same
chain
polar
in
group, the relationship is described as Equation 2.8:
where
m is the number
B are constants,
which are
of carbon
related
atoms
to the
in
the carbon
structure
chain,
of
surfactants,
A and
be used to speculate and compare structures. drugs that as the the CMC value
Table
and the
hydrophobicity
2.4 lists a
properties
variety
of
their micelles. of the
of the drug drops
the micellization
of amphiphilic
The comparison shows
substituents
and
the aggregation
of similar
diphenylmethane
gradually
elevate,
number
of
Table 2.4 Eect of substuent on diphenylmethane drugs and properes of
micelles
Drug R R¢ R
CMC (mol·kg–1)
Aggregation Number
Diphenylamine H H H 0.132
3
O-methyl-diphenhydramine CH3 H H 0.096

Brominated diphenylamine Br H H 0.053
11
H H H 0.132
3
O-methyl-diphenhydramine CH3 H H 0.096

Brominated diphenylamine Br H H 0.053
11
3
60
Nano Physical Pharmaceutics of Micelle-Based Systems
Table 2.3 (Continued)
Substituent Group Classification
–SCH
3
–OCH
2CH3
–OCH
3
–NO
2
–CHO
–COOH
–COO
–NH
2
–NH
3
Hydrophobic
Hydrophobic
Slightly hydrophilic
Slightly hydrophilic
Hydrophilic
Slightly hydrophilic
Slightly hydrophilic
Hydrophilic
Slightly hydrophilic
–OH Slightly hydrophilic
Oxy Mephenhydramine Cl H CH 0.045
13
Regardless of ionic or non-ionic surfactants, the CMC decreases with
longer carbon reduced ionic
surfactants
for of
the former is hydrophilic group is the same the
same
branched
carbon
atom
in the
to about
surfactant
value of
chains
chain.
carbon
1/2
is
reduced
with
generally
carbon
in
the carbon
Generally
chain,
of the
to
the same
much
atoms,
speaking, for each additional
the
CMC
of ionic
original
about 1/3
number
one,
of carbon
smaller
and
the CMC
of the original
than the latter. If the
and the hydrophobic
the CMC of surfactant
chain
is higher than the CMC
surfactant
of non­one.
atoms, the
CMC
group contains
s with
is
As
of
Table 2.5 CMC and micelle volume of hexadecyl PEG
CMC × 10
4
n (mol·kg–1) Micelle Volume × 10
–1
Aggregation Number
6  12.3 2430    590
9 2.1 1.4 220
12 2.3  150
21 3.9 0.82 150
Effects on Micelle Assembly
61
surfactants without branched chains. The benzene ring is slightly
          
despite being composed of six carbon atoms.
2.3.3.2 Chemical structure and volume of hydrophilic groups
          
hydrophobic groups are the same, non-ionic surfactant generally shows lower CMC value than ionic surfactant, and the micellar aggregation number is higher. As for non-ionic surfactants with
         
the length of PEG chain segments. As shown in Table 2.5, with the increase of the PEG chain length, the hydrophilicity and CMC values both rise.
2.3.3.3 Synergy of hydrophilic groups and hydrophobic
groups
During micellization, due to the simultaneous existence of driving force and counterforce in the system, the delicate balance between
           
Table 2.6 lists the corresponding micellar aggregation number of various surfactants in water.
The following Fig. 2.1 shows the general principal and the process of micelle assembly from the block copolymers. The detail mechanism and structural tailoring of such micelle. Here, for
       
Surfactant Temperature/°C Aggregation Number
C
8HSO4
Na Room temperature 20
C
10H21SO4
Na Room temperature 50
C
12H25SO4
Na 23 
C
12H25
N(CH3)3Br – 50
C
14H29
N(CH3)3Br – 
C
12H25
O(C2H4O)8H 25 123
C
12H25
O(C2H4O)12H 25 81
C
12H25
O(C2H4O)18H 25 51
C
9H19(C6H4
)O(C2H4O)10H 25 
C
9H19(C6H4
)O(C2H4O)15H 25 80
C
9H19(C6H4
)O(C2H4O)20H 25 62
62
Nano Physical Pharmaceutics of Micelle-Based Systems
Figure 2.1 The spherical micelle and its microstructure assembly from block
copolymer. The formula related to the table is shown in 1.10, 1.15.
Effects on Micelle Assembly
63
length of amphiphilic block copolymer should be tuned in the polymerization for getting the Flory parameter c
hydrophobic
> 0.5
while c
hydrophilic
< 0.5 by the function 2.18. This is the thermo­dynamic condition for the self-assembly of amphiphilic block copolymers in solutions. Then, the composition of the copolymer should be further regulated for tuning the packing parameter (b) in the range of 0~1/3 according to function 2.20, which results in a spherical morphology.
2.3.3.4 Eects of counterions

process. For example, the micelle volume of cationic surfactants changes with the order of the counterion I– > Br– > Cl–, while the micelle size corresponding to anionic surfactants varies with the order of counterion Cs+ + > Na+. In general, the weaker hydration ability of the counterion, the larger the micelles formed by the surfactant. This is due to the fact that ions with weak hydration are more easily adsorbed on the surface of the micelles, thereby reducing the electrostatic repulsion between polar groups. The CMC of surfactants under organic counterion (e.g., maleic
        

2.3.4 Influence of External Conditions on CMC

2.3.4.1 Temperature
The solubility of ionic surfactant in water is limited, it rises up slowly as the temperature increases, resulting in the slight increase of CMC. In the meantime, the molecular thermal movement is aggravated, which is not conducive to the formation of micelles, leading to higher CMC as well. However, for non-ionic surfactants, the CMC decreases with increasing temperature.
Krafft Point. For ionic surfactant, the solubility in water varies with temperature. As the temperature rises, the solubility increases sharply at a certain point, and the temperature

the corresponding solubility is called the ionic surfactant CMC [11].