Advances in Condensed Matter PhysicsVolume 2011 (2011), Article ID 174786, 8 pagesdoi:10.1155/2011/174786

Research Article

Effects of on the Lyotropic Liquid Crystalline Behavior in Nonaqueous and Aqueous Medium

Ravi K. Shukla and K. K. Raina

Materials Research Laboratory, School of Physics and Materials Science, Thapar University, Patiala 147004, India

Received 6 March 2011; Revised 29 May 2011; Accepted 9 June 2011

Academic Editor: Nigel Wilding

Copyright © 2011 Ravi K. Shukla and K. K. Raina. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

Effects of varying doping concentrations () of on the aggregation behaviour of cationic surfactant in nonaqueous and aqueous medium have been investigated. Mixed and pure lyotropic liquid crystalline LLC phases appeared in nonaqueous and aqueous ternary mixtures due to the fast quenching process and then characterized through polarizing optical microscopy and X-ray diffraction technique. The material parameters corresponding to these ternary nonaqueous and aqueous mixtures were evaluated to understand the mechanisms of deriving forces responsible for the modification of mesophases in the presence of metal salt.

1. Introduction

Lyotropic liquid crystals (LLCs) are the subset of the organic soft materials, self-assembled by the aggregation of amphiphilic molecules in the aqueous and nonaqueous domains. Their synthesis depends upon the micellization, reaction medium, thermodynamic equilibria, counter ion effect, optimal surface area of head group, and alkyl chain length [1]. These physicochemical conditions can be tuned to engineer new self-assembled structures, which exhibit unusual physical properties to enable them as prominent materials for variety of applications. The aggregation behaviour of micelles in aqueous medium is well documented in the literature and exploited in the key area of biology, cosmetics, and pharmaceuticals and as soft template to engineer functional nanomaterials [2–4]. New kinds of ternary systems like water, salt, and surfactant (WSS) have been synthesized and characterized to facilitate the development of modified mesostructured, mesoporous materials via self-assembly of ionic and nonionic amphiphilic molecules [3–9]. They could offer confinement of the metal ions in definite ordered geometry even at lower concentration, better control on shape, and size with higher yield [10–13]. However, due to the lack of stability at higher metal density and evaporation of water content from the media, these systems could not be exploited for the industrial applications [14].

Nonaqueous solvents were found to overcome such problem, as they do posses cohesive energy, dielectric constant and hydrogen bonding ability to initialize the micellization, and thus produce water-free or water-poor stable mesophases (soft templates). Ray [15] first studied the micellar aggregation of dodecyl pyridinium bromide (C₁₂PBr) and tetradecyl trimethyl ammonium bromide (C₁₄TAB) in ethylene glycol. Later, Evans and coworkers reported the lamellar liquid crystals phase formation by lipids in ethylammonium nitrate (EAN) [16, 17]. With the consistent developments of this field, the cubic phase in N-alkylpyridinium surfactants in nonaqueous medium of EAN was reported by Bleasdale et al. [18]. Self-assembly of nonionic polyoxyethylene alkyl ether surfactants into lyotropic liquid crystals in EAN and other systems was reported [19–22]. Recently, we reported the aggregation behaviour of the cetyl pyridinium chloride in the nonaqueous solvent (ethylene glycol) producing mixed (hexagonal + lamellar) and pure lamellar LLC mesophases at lower and higher concentrations, respectively [23].

In this communication, we report on the effects of transition metal salt CuCl₂ on the mesogenic lamellar phase of binary [CpCl-EG (40 : 60 wt%)] system in nonaqueous and aqueous medium. We characterized them to understand the packing behaviour of the micelles and the driving forces responsible for the self-assembly of surfactant molecules. In addition, the conductivity of nonaqueous ternary mixtures containing metal salt content  wt% has been investigated.

2. Experimental

Cetyl pyridinium chloride [(C₂₁H₃₈NCl) Merck, 99% purity], protic solvent ethylene glycol (EG) (SD Fine chemicals, 99% purity) and transition metal salt cupric chloride (CuCl₂) (Loba Chemie 99% purity) were used as received. The binary mixture (CpCl : EG) was prepared by dissolving appropriate amount of CpCl in the ethylene glycol (40 : 60 wt%) through several heating and cooling cycles between melting and room temperature followed by the sonication (37 KHz) for 1 hour near melting point of the surfactant material to ensure the homogeneity.

Nonaqueous ternary mixtures of CpCl : CuCl₂ : EG were prepared by dissolving the appropriate amount of CpCl in ethylene glycol along with the varying concentration of TMS (wt%). The resulting mixtures were homogenized by heating the sample to its melting point in a sealed glass vial followed by the sonication for 1 hour at elevated temperature. Similar procedure was employed to prepare CpCl : CuCl₂ : H₂O systems. Nonaqueous ternary mixtures of 2 and 4 wt% concentrations (in which cubic rods) were washed with distilled water and ethanol to separate out the cubic rods from the mesogenic template.

The prepared samples were filled between cleaned glass slides and then placed in a temperature controlled hot stage (Linkam TP 94 and THMS 600) with in ±0.1°C temperature precision fitted on the polarizing microscope (Olympus BX-51P) stage. X-ray diffraction (XRD) patterns of the soft matter samples were scanned by diffractogram (Philips XPERT-PRO MPD) using Cu kα radiation source and patterns were recorded at = 1–10° range. Scanning electron microscopic (SEM) textures were recorded through SEM Quanta, 200 (FEG and FEI Netherland). Thermodynamical behaviour was investigated using differential scanning calorimeter (DSC model LINSEIS L-63) with heating @ 5 degree/minute for each case. The conductivity of these systems has been evaluated by RCL meter (Fluke model PM 6306).

3. Results and Discussion

3.1. Morphological and Structural Analysis

3.1.1. Nonaqueous Medium

Optical textures of the as prepared, quenched, and aged, metal salt-doped nonaqueous ternary mixtures ( wt%) recorded at room temperature are shown in Figure 1(a). We noticed the absence of ordering in the as prepared mixtures. It reflects the lack of liquid crystallinity in them at different concentrations as evident from Figure 1(a) (col. 1). However, ternary mixtures spontaneously attained some degree of ordering upon quenching from isotropic to room temperature. We noticed that systems with  wt% doping concentrations displayed fanlike textures though disrupted focal cones and dendritic geometry did appear at and 10 wt%. To further explore the structural information of these systems, XRD measurements were carried out. The diffractogram of these ternary nonaqueous mixtures are presented in Figure 2(a), whereas their consequent spacing and (hkl) reflection are listed in Table 1. Four diffraction lines were noticed at  wt%, last three lines can be indexed as (001), (002), and (003) reflection of lamellar mesophases although first peak was matched with hexagonal phase. Peaks observed at  wt% is in 1 :  :  :  :  ratio, characterized as reflection of hexagonal mesophase. At and 5 wt%, diffraction peaks were found absent reflecting the lack of liquid crystallinity at these concentration. Diffraction peak observed at % indexed as reflection of lamellar mesophase. However, at  wt% system, diffract well-defined highly intense peaks indexed as (001), (002), and (003) planes of the layered lamellar phase Figure 2(a). Interestingly, some cubic rods, harvested at the nodal point of fan-like texture, were also found at 2 and 4 wt% concentrations. We presume that the growth of such well-ordered cubic rods at  wt% in the liquid crystalline moiety attributed to the confinement of released metal ions in the mesophase. In the pyridinium salts the following equilibrium exists In the presence of CuCl₂ salt a solid complex separates The resulting system is a complex mixture of liquid lyotropic and a solid system. The same should be observed for higher concentration of CuCl₂, but probably solid is separated in very small aggregates not confine into bigger crystals.

Table 1: spacing value and (hkl) planes obtained from XRD patterns of (a) non-aqueous ternary mixtures (b) aqueous ternary mixtures.

(a)

2 wt%
4 wt%
6 wt%
10 wt%

-spacing [Å]
[hkl]
-spacing [Å]
[hkl]
-spacing [Å]
[hkl]
-spacing [Å]
[hkl]

30.65952
*
26.92937
10
10.42664
003
30.56
001

27.05235
001
15.51670
11
—
—
15.5491
002

13.85762
002
13.81812
20
—
—
10.41412
003

9.32170
003
10.41088
21
—
—
—
—

—
—
9.28521
30
—
—
—
—

(b)

1 wt%
2 wt%
4 wt%

-spacing [Å]
[hkl]
-spacing [Å]
[hkl]
-spacing [Å]
[hkl]

26.98537
110
38.87693
10
15.71157
10

19.53447
210
27.29848
11
13.77588
11

13.81599
20
13.75712
20
10.35145
20

10.44494
21
11.32786
21
9.62659
21

9.30052
30
10.37896
30
—
—

(a)

(b)

Figure 1: The optical texture of fresh (Col. 1), quenched (Col. 2), and aged (Col. 3) nonaqueous ternary mixtures having metal salt ratio 1, 2, 4, 5, 6, and 10 wt%, respectively. The optical texture of fresh (Col. 1), quenched (Col. 2), and aged (Col. 3) aqueous ternary mixtures having metal salt ratio 1, 2, 4, 5, 6, and 10 wt%, respectively.

(a)

(b)

Figure 2: The XRD profiles of quenched ternary mixtures having metal salt ratio 1, 2, 4, 5, 6, and 10 wt% (a) nonaqueous (b) aqueous medium, respectively.

Origin of mesophase in nonaqueous mixtures attributed to the self-organization of amphiphilic and counter ions in the vicinity of solvophobic interactions and electrostatic forces. Structural studies infer that at low metal salt concentrations, disordering in the system owe to the strong attractive electrostatic interactions between ion and the positively charged head group. Growth of ordered mesophases at  wt% could corresponds to the increase in the aggregation of number of salt ions near the positively charged hydrophilic crown head group, which certainly enhance the repulsive force between hydrophobic chains (because of the increase in the curvature of hydrophilic crown), thus resulting into hexagonal phase than that of layered lamellar mesophase. Aging effects studied for these ternary systems depicts hexagonal to lamellar transition up to 4 wt% concentrations; however, lamellar phase remains conserved at higher concentrations Figure 1(a) [Col. 3]. The cubic rods thus harvested at nodal point of the focal conic become eventually free from liquid crystalline moieties with the passage of time as system undergoes phase transition. The scanning electron micrograph of obtained rods is presented in the Figure 1(1.1).

A proposed model of the lamellar-hexagonal-lamellar transition observed from the textural and structural studies is illustrated in Figure 3. It is worth emphasizing to say that such transition in these systems owes to the undulation at the interface.

Figure 3: Illustration of lamellar-hexagonal-lamellar transition in nonaqueous ternary mixtures.

3.1.2. Aqueous Medium

Micrographs of the freshly prepared, quenched, and aged aqueous ternary mixtures are presented in Figure 1(b). We noticed that the as-prepared systems did not show any ordered texture inferring the lack of liquid crystallinity in them Figure 1(b) (Col. 1). While, quenching (isotropic to room temperature) facilitates the development of well ordered fan like textures at  wt% though no ordered texture has been seen at 2, 5, 6, and 10 wt% as shown in (Col. 2) Figure 1(b). In order to ascertain the validity of our morphological observations, XRD measurements were performed. The observed XRD profiles of aqueous ternary mixtures are shown in the Figure 2(b) and their corresponding values are tabulated in Table 1. Five diffraction peaks noticed at  wt%, indexed as reflection of cubic phase {(110) and (210)} and hexagonal LLC phase. Diffraction peaks at and 4 wt% correspond to the 10, 11, 20, 21, and 30 plane of 2D hexagonal LLC phase. Liquid crystal order was found missing at  wt%, as no diffraction was observed. The lack of liquid crystallinity at higher may owe to the poor solubility of the metal salt. Mesophases observed in aqueous media were stable as a function of time, and no significant changes have been noticed in the optical texture at any concentration as evident from Figure 1(b) [Col. 3].

3.2. Thermodynamic Considerations

Thermodynamic response of both non-aqueous and aqueous ternary mixtures were investigated over wide temperature range 30°C–120°C to ascertain their thermal parameters and stability. The observed exo and endothermic peaks for nonaqueous and aqueous ternary mixtures are presented in Figures 4(a) and 4(b) respectively. Exotherms observed at lower (1, 2, and 4 wt%) indicates the nucleation of the ordered structures as shown in Figure 4(a) in the temperature range of 35°C–50°C. The transition temperature of these mixture increased gradually up to  wt% which decreased at higher values. The deviation in the transition temperature with the increment in the metal salt content in these systems may depend upon the ordering of the LLC phase (the fact that highly ordered geometries required higher thermal energy than that of less ordered during transitions). Endotherm noticed in high temperature range 65°C–80°C corresponds to the melting of the parent amphiphilic molecules. We observed around 27°C (±3°C) decrease in the transition with respect to pure system.

(a)

(b)

Figure 4: DSC profiles of ternary mixtures having metal salt ratio 1, 2, 4, 5, 6, and 10 wt% (a) Nonaqueous (b) aqueous medium, respectively.

Figure 4(b) shows the DSC spectra profiles of the aqueous ternary mixtures. We noticed that the transition temperature of dispersed matrix shifted to the lower value (ranging between 33°C–37°C) than that of pure LC matrix (42°C) in the lower temperature region. Similarly, endothermic peaks were observed for these ternary mixtures in the high temperature region (65°C–80°C) representing the melting of surfactant molecules. A small shift (≈5°C) to the higher side in the anisotropic to isotropic transition has been noticed for the dispersed samples.

Entropy (ΔS) calculated for these disordered and melting transitions of nonaqueous and aqueous ternary mixtures are listed in Table 2. The variation of entropy for nonaqueous and aqueous medium corresponding to disorder transitions (in lower temperature region) is illustrated in Figure 5(a). The entropy for the nonaqueous mixture in this temperature region was found less at lower , which increased gradually with the variation in and attained maxima at  wt%, whereas the system at  wt% shows decrease in the magnitude of ΔS. Such behaviour of the entropy corresponds to the order-disorder-order transition in these systems on the basis of structural considerations. The entropy of aqueous ternary mixture was found higher than that of nonaqueous mixture and did not display any regular trend as shown in Figure 5(a). We noticed that the entropy was low at lower .

Table 2: Thermodynamic parameters calculated on the base of DSC profiles (a) non-aqueous ternary mixtures (b) aqueous ternary mixtures.

(a)

Concentration (wt%)
Phase
Disordering temperatures (°C)
Enthalpy (ΔH)
Entropy (ΔS)
Melting temperature (°C)
Enthalpy (ΔH)
Entropy (ΔS)

Pure
L
—
—
—
104
−37.5
0.3

1%
No phase
42.6
5.05
−0.118
77
−173.9
2.26

2%
H + L
42.8
8.8
−0.2
73
−44.02
0.6

4%
H
45.4
14.2
−0.3
74
−38.49
0.5

5%
Disrupt
47.2
−32.43
0.6
79
−30.42
0.3

6%
One L peak
48.4
−123.19
2.5
76
−100.9
1.3

10%
L
46.7
−33.35
0.7
78
−45.39
0.5

(b)

Concentration (wt%)
Phase
Disordering temperatures (°C)
Enthalpy (ΔH)
Entropy (ΔS)
Melting temperature (°C)
Enthalpy (ΔH)
Entropy (ΔS)

Pure
No phase
42.1
−74
1.75
65
30.04
0.4

1%
Cubic + H
33.6
−22.2
0.6
76
−777.5
10

2%
2D H
35.1
−82.17
2.3
76
−527.80
6.9

4%
2D H
34.4
−63.03
1.8
74
−600.46
8.1

5%
No
35.6
−117.08
3.2
74
−533.81
7.5

6%
No
—
—
—
75
−454.7
6.0

10%
No
37.5
−97.59
2.6
70
−384.4
5.4

(a)

(b)

Figure 5: Variation of entropy versus metal salt concentrations ( wt%) (a) lower temperature region (35°C–50°C) (b) higher temperature region(65°C–80°C), respectively.

Figure 5(b) shows the variation of ΔS as function of metal salt concentration for aqueous and nonaqueous medium in higher temperature range (65°C–80°C). We observed that the degree of ordering is a function of metal salt content and the temperature as the magnitude of the ΔS shifts to higher value. For nonaqueous ternary mixture the magnitude of the entropy at  wt% was maximum, inferring that addition of the small amount of CuCl₂ disturbed the system vigorously. Further increase in , decreases the entropy of the system which remains almost constant up to 5 wt%. Similarly, the entropy of the aqueous ternary medium was found minimum for undoped matrix, while dispersion of the metal salt gives rise to ΔS. No specific pattern of the ΔS has been observed for these systems (entropy display minimum magnitude at higher ). It is quite reasonable to say on the basis of ΔS analysis that the nonaqueous ternary mixtures were more ordered than that of aqueous medium at lower and higher . Our thermodynamical measurements suggest that the formation of LLC phases in these media depends on the quenching, physicochemical interaction and metal salt concentration.

4. Conductivity Measurement

Figure 6 illustrates the variation of conductivity as a function of temperature for the nonaqueous ternary mixtures  wt%. Undoped liquid crystalline matrix was found metallic in nature though systems with % exhibit semiconducting nature as evident from the Figure 6. It seems quite reasonable to say that such transitions attributed to the percolated defects in the LLC matrix, which consequently decreased the mean-free path of the conduction electrons and likely metal to semiconductor transition takes place. Note that the different subphases being observed in this semiconducting matrix are due to the changes in the morphological structures with the increase in the temperature as displayed in the Figure 6. At  wt%, system shows metallic nature, which may be due to increase in the metal salt density. It seems that the released metal ions in the LLC matrix are not percolated in the matrix but forming the cluster, which enhances such conductions in the system.

Figure 6: Variation of conductivity as a function of temperature for pure, 2 and 4 wt% metal salt concentrations in nonaqueous medium.

5. Conclusions

In summary, we have investigated the effects of transition metal salt on the aggregation of cationic surfactant in nonaqueous and aqueous medium. (1)Highly ordered mixed (lamellar + hexagonal), 2D hexagonal and lamellar layered mesophases were observed in the ternary nonaqueous medium at lower and higher value of ; however, the liquid crystalline order was found restricted to the lower value of metal salt content in the aqueous media.(2)Nonaqueous ternary mixtures with 2 and 4 wt% metal salt content was found stable template as it facilitates the in situ growth of cubic rods (4-5 μ diameter) in the mesophase. These phases can be exploited as soft templates for the fabrication of various metallic and semiconducting materials ranging from micro to nanometer length scale. (3)Calorimetric measurements indicate the formation of stable mesophase in nonaqueous and aqueous medium due to fast quenching process. (4)The conductivity measurement hints at the use of such soft conducting matrix in many technological applications.

Acknowledgments

The authors wish to thank the Department of Science and Technology (DST), India, for the financial support. The valuable comments and suggestions of reviewers are duly acknowledged.

References

M. L. Moyá, A. Rodríguez, M. del Mar Graciani, and G. Fernández, “Role of the solvophobic effect on micellization,” Journal of Colloid and Interface Science, vol. 316, no. 2, pp. 787–795, 2007.

P. S. Kumar, S. K. Pal, S. Kumar, and V. Lakshminarayanan, “Dispersion of thiol stabilized gold nanoparticles in lyotropic liquid crystalline systems,” Langmuir, vol. 23, no. 6, pp. 3445–3449, 2007.

T. Imura, Y. Hikosaka, W. Worakitkanchanakul et al., “Aqueous-phase behavior of natural glycolipid biosurfactant mannosylerythritol lipid A: sponge, cubic, and lamellar phases,” Langmuir, vol. 23, no. 4, pp. 1659–1663, 2007.

H. Kawasaki, A. Sasaki, T. Kawashima et al., “Protonation-induced structural change of lyotropic liquid crystals in oley- and alkyldimethylamine oxides/water systems,” Langmuir, vol. 21, no. 13, pp. 5731–5737, 2005.

V. Percec, D. Tomazos, J. Heck, H. Blackwell, and G. Ungar, “Self-assembly of taper-shaped monoesters of oligo(ethylene oxide) with 3,4,5-tris(n-dodecan-1-yloxy)benzoic acid and of their polymethacrylates into tubular supramolecular architectures displaying a columnar hexagonal mesophase,” Journal of the Chemical Society, Perkin Transactions 2, no. 1, pp. 31–44, 1994.

M. Lee and B.-K. Cho, “Induction of thermotropic liquid crystalline phases in coil-rod-coil triblock molecules containing poly(propylene oxide) through complexation with LiCF₃SO₃,” Chemistry of Materials, vol. 10, no. 7, pp. 1894–1903, 1998.

T. Ohtake, M. Ogasawara, K. Ito-Akita et al., “Liquid-crystalline complexes of mesogenic dimers containing oxyethylene moieties with LiCF₃SO₃: self-organized ion conductive materials,” Chemistry of Materials, vol. 12, no. 3, pp. 782–789, 2000.

B. Donnio, “Lyotropic metallomesogens,” Current Opinion in Colloid and Interface Science, vol. 7, no. 5-6, pp. 371–394, 2002.

H. Kunieda, G. Umizu, and K. Aramaki, “Effect of mixing oils on the hexagonal liquid crystalline structures,” Journal of Physical Chemistry B, vol. 104, no. 9, pp. 2005–2011, 2000.

Ö. Dag, A. Verma, G. A. Ozin, and C. T. Kresge, “Salted mesostructures: salt-liquid crystal templating of lithium triflate-oligo(ethylene oxide) surfactant-mesoporous silica nanocomposite films and monoliths,” Journal of Materials Chemistry, vol. 9, no. 7, pp. 1475–1482, 1999.

P. V. Braun, P. Osenar, and S. I. Stupp, “Semiconducting superlattices templated by molecular assemblies,” Nature, vol. 380, no. 6572, pp. 325–328, 1996.

G. S. Attard, P. N. Bartlett, N. R. B. Coleman, J. M. Elliott, J. R. Owen, and J. H. Wang, “Mesoporous platinum films from lyotropic liquid crystalline phases,” Science, vol. 278, no. 5339, pp. 838–840, 1997.

Y. Yamauchi, T. Momma, T. Yokoshima, K. Kuroda, and T. Osaka, “Highly ordered mesostructured Ni particles prepared from lyotropic liquid crystals by electroless deposition: the effect of reducing agents on the ordering of mesostructure,” Journal of Materials Chemistry, vol. 15, no. 20, pp. 1987–1994, 2005.

C. Albayrak, A. M. Soylu, and Ö. Dag, “Lyotropic liquid-crystalline mesophases of [Zn(H₂O) ₆](NO₃)₂-C₁₂EO₁₀-CTAB- H₂O and [Zn(H₂O)₆](NO₃)₂-C₁₂EO₁₀-SDS-H₂O systems,” Langmuir, vol. 24, no. 19, pp. 10592–10595, 2008.

A. Ray, “Micelle formation in pure ethylene glycol,” Journal of the American Chemical Society, vol. 91, no. 23, pp. 6511–6512, 1969.

D. F. Evans, A. Yamauchi, G. J. Wel, and V. A. Bloomfield, “Micelle size in ethylammonium nitrate as determined by classical and quasi-elastic light scattering,” Journal of Physical Chemistry, vol. 87, no. 18, pp. 3537–3541, 1983.

D. F. Evans, E. W. Kaler, and W. J. Benton, “Liquid crystals in a fused salt: β,γ-distearoylphosphotidylcholine in N-ethylammonium nitrate,” Journal of Physical Chemistry, vol. 87, no. 4, pp. 533–535, 1983.

T. A. Bleasdale, G. J. T. Tiddy, and E. Wyn-Jones, “Cubic phase formation in polar nonaqueous solvents,” Journal of Physical Chemistry, vol. 95, no. 14, pp. 5385–5386, 1991.

M. U. Araos and G. G. Warr, “Self-assembly of nonionic surfactants into lyotropic liquid crystals in ethylammonium nitrate, a room-temperature ionic liquid,” Journal of Physical Chemistry B, vol. 109, no. 30, pp. 14275–14277, 2005.

T. L. Greaves, A. Weerawardena, C. Fong, and C. J. Drummond, “Many protic ionic liquids mediate hydrocarbon-solvent interactions and promote amphiphile self-assembly,” Langmuir, vol. 23, no. 2, pp. 402–404, 2007.

T. L. Greaves and C. J. Drummond, “Ionic liquids as amphiphile self-assembly media,” Chemical Society Reviews, vol. 37, no. 8, pp. 1709–1726, 2008.

T. L. Greaves, A. Weerawardena, I. Krodkiewska, and C. J. Drummond, “Protic ionic liquids: physicochemical properties and behavior as amphiphile self-assembly solvents,” Journal of Physical Chemistry B, vol. 112, no. 3, pp. 896–905, 2008.

R. K. Shukla and K. K. Raina, “Observations on lyotropic liquid crystalline behavior of a cationic surfactant and polar solvent in a nonaqueous medium,” International Journal of Modern Physics B, vol. 23, no. 25, pp. 5075–5083, 2009.