The
Chemical Educator, Vol. 12, No. 1,
Published on Web 2/1/2007, 10.1333/ s00897071097a, © 2007 The Chemical
Educator
Determination of the Critical Micellar Concentration (CMC) of a Cationic Micelle from Stokes Shift Data
Mintu Halder*
Department of Chemistry, Iowa State University, Ames, IA-50011, mintu@chem.iitkgp.ernet.in
Received June 26, 2006. Accepted November 4, 2006.
Abstract: This is a new method for the determination of critical micellar concentration (CMC) based on the measurement of Stokes shift of a solvent-sensitive fluorescent probe located at the micellar aggregate. The variation of the Stokes shift with respect to bulk water is a result of the formation of micelles from the surfactant monomer, here, cetyl trimethyl ammonium bromide (CTAB) and is measured from the difference in the maxima of emission and excitation spectra of the probe. Earlier methods reported in literature were based on surface tension measurement and micellar catalysis. Stokes shifts can be further correlated to solvent reorganization energy (as Stokes shift is proportional to reorganization energy). The reorganization energy results from the creation of a transient solute dipole (by an exciting photon) in a solvent atmosphere. This induces a reorganization of the solvent molecules (dipoles; for nonpolar solvents there is no reorganization) about the dipole in a manner that stabilizes the energy of the system, and the energy term so involved is referred to as the reorganization energy.
Surfactants are molecules containing a hydrophobic long-chain (tail) with a polar head group and the head group may be ionic or neutral. If these molecules are dissolved in water, they have a tendency to form aggregates spontaneously, that is, surfactant molecules will arrange themselves into organized molecular assemblies, also called normal micelles (see Figure 1) [1, 2]. There is a particular concentration (the critical concentration) characteristic of the surfactant (in a given solvent) at or above which these will form micelles and this is called the critical micellar concentration (CMC). Before the critical concentration is reached aggregates may still be formed, which are premicellar aggregates [3]. The micellar aggregates have a certain number of monomer units on the average, which is known as aggregation number.
The formation of micelle from monomer with aggregation number n could be represented by the following scheme:
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Micelles are highly dynamic aggregates and rates of uptake of monomers into micellar aggregates are nearly at the diffusion-controlled limit [4, 5]. Initially, when the concentration is very low these monomers behave like independent molecular entities in water. As the concentration is increased they tend to come close to each other and form aggregates of various sizes as the process is favored thermodynamically. The formation of micelles can be followed by several methods based on the fact that in the vicinity of the CMC there is a sharp change in the experimental observables. There are many methods available in literature for the determination of the CMC [6, 7]: surface tension, spectrophotometric, kinetics, conductivity, osmotic pressure, etc.
Fluorescence spectroscopy [8] is a sensitive technique where we can utilize the environment sensitivity of a molecular probe situated in the micelle and this could also be an accurate method for CMC determination. The environment sensitivity can be quantified by the Stokes shift, measured by from the difference in emission and excitation maxima expressed in energy (wavenumber) scale, that is,
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the larger the Stokes shift the higher sensitive the probe is. We choose a polar probe where the Stokes shift is very sensitive to solvent environment (polarity) and which can preferentially bind to micelle. It may be noted that not all fluorescent probes are sensitive to solvent. With increase in monomer concentration more and more aggregates (micelle) are formed and so more of the probe molecules leave water and bind to the aggregates.Thus, the Stokes shift of the probe molecule will vary considerably as a function of the monomer concentration in the vicinity of the CMC. This is because the solvent environment (polarity) in bulk water is different than in aggregates (organized surfactant assembly), which brings about a change in emission/excitation frequency maximum and hence different Stokes shifts. When the monomer concentration is well below and above the CMC the Stokes shift does not change significantly with concentration of monomers.
The success of this experiment depends on two important factors: (i) the Stokes shift of the chosen probe molecule must be sensitive to environment (polarity) (not all probes can show sensitivity in Stokes shift) and (ii) it should preferentially attach to the aggregate. The surfactant molecules may be or may not be charged, but in the present case, we used

Figure 1. Micellar aggregate (An aqueous CTAB micelle).
(a)
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(b)

Figure 2. Stick diagram for (a) CTAB, (b) C-343 Na Salt.
hexadecyltrimethyl ammonium bromide, (cetyl trimethyl ammonium bromide, CTAB) a charged one (See Figure 2a).
Here the micellar aggregates formed in water are positively charged. Naturally, a negatively charged probe could bind to this positively charged micelle and micellar interface will be the preferred location of the negatively charged probe because of the positive zeta-potential and it should not look for the nonpolar hydrocarbon interior. Thus, the electrostatic force of attraction will bind the probe together with the aggregate [9]. As we approach the CMC, aggregates start to form and the Stokes shift starts to change indicating that the probe has bound to the micellar aggregate. With further increases in monomer concentration the aggregate will grow larger and larger with a further change in Stokes shift until a full grown micelle is formed. There will then be no further change in the Stokes shift.
Here, the sodium salt of coumarin-343 (C-343) (see Figure 2b) has been used, which is a negatively charged polar molecule showing considerable change in Stokes shift when compared with water and aqueous micellar mediums like CTAB.
Surfactants are the powerhouse of detergents. They have wide application in many consumer products in our day-to-day life and in industry. The type of surfactant used depends on the applications, which include removal of dirt and grease from fibers and surfaces and the conditioning of fibers.
Fabric conditioners are primarily cationic surfactants dispersed in aqueous systems. In water, cationic surfactants tend to form a lamellar liquid-crystal structure in which the surfactants form layers. Curling up of these layers in water leads to formation of small particles called liposomes. These are attracted to charged surfaces of the fabric materials and softening occurs in two ways: (i) surfactants tend to reduce the surface tension which causes fibrils to get pulled out easily, (ii) the spreading of surfactants to form a surface layer on fabrics acts to lubricate the fibers resulting in a soft and smooth feel of the fabric.
Foaming agents, emulsifiers, and dispersants are also surfactants, which suspend gases, immiscible liquids, or solid particles in water or in some other liquid, respectively. Although there is a similarity in these systems, in real practice surfactants required to perform the functions of these systems differ widely. An emulsion can be either oil droplets suspended in water, an oil-in-water (o/w) emulsion, water suspended in a continuous oil phase, a water-in-oil (w/o) emulsion, or a mixed emulsion.
Each of these three functions is related to the adsorption of surfactant at a surface with hydrophilic ends of the molecules oriented to the water phase. The surfactants form a protective coating around the suspended material, and these hydrophilic ends associate with the neighboring water molecules. Solubilization is another phenomena closely related to emulsification. As the size of the emulsified droplet becomes smaller, a condition is reached when this droplet and the surfactant micelle are of the same size. At this stage, an oil droplet can be thought of as being in solution with the hydrophobic tails of the surfactant (hydrocarbon core of micelle) and in this case, the term solubilization is used. Emulsions are milky in appearance, whereas, solubilized oils are clear.
The phenomena of detergency or cleaning by a detergent is a complex combination of all the above functions. The surface to be cleaned and the soil to be removed must initially be wet and the soils should be suspended, solubilized, dissolved, or separated in some way so that the soil will not just redeposit on the surface in question. In the case of surfactants, oil first gets distributed in the hydrophobic core of the micelle and remains encapsulated there so that it cannot return. From the above discussion it should be clear that the aggregates of surfactant monomers are the key ingredients for the various functions. A knowledge of the CMC of a surfactant is very essential and its determination is of great importance. Nonionic surfactants are important soil removers; they combine good detergent action with the ability to penetrate and soften fatty and oil-containing soil from tightly woven fabrics and hard surfaces.
Experimental
Materials and Methods. C-343 was purchased from Exciton and CTAB from Aldrich and were used as received. The salt of the dye was made by neutralizing it with aqueous NaOH. The concentration of the dye was maintained at ~1 × 10–6 M in the final mixture. A set of solutions were made with varying concentrations of CTAB and a fixed concentration of the dye. The CTAB concentration in the solutions was varied up to 1.5 mM with an increment of 0.1 mM. For this, a varying amount of 10 mM CTAB solution was mixed with a varying amount of water to reach the required concentration of CTAB, keeping the total volume of mixture fixed, and to all prepared

Figure 3. Normalized emission spectra of C-343 Na salt with varying concentrations of CTAB in water.

Figure 4. Normalized excitation spectra of C-343 Na salt with varying concentration of CTAB in water.
solutions a fixed small amount (1 mL, this volume does not bring about any change of CTAB concentration practically) of the stock dye solution was added to reach the target dye concentration in the final mixture. All solutions were prepared with deionized or distilled water and then allowed to equilibrate for 15 to 20 minutes. Emission spectra were recorded at 440 nm and excitation spectra were monitored at 620 nm using a 1-cm-path-length cuvette and a Perkin Elmer MPF 44B spectrofluorimeter.
Safety. Coumarin 343 is an irritant to the respiratory system and skin, an eye irritant, and harmful if absorbed through skin (use safety goggles and gloves). CTAB is an irritant to the respiratory system and skin with a risk of damage from eye contact. Care must be taken to avoid inhalation and use of safety goggles is recommended. Sodium hydroxide can cause serious damage upon eye contact, use of safety goggles is recommended. An eye-wash station should be available in the laboratory.
Results and Discussion:
Emission spectra for the C-343-Na salt in a CTAB/water system are shown in Figure 3. The emission maxima were shifted to the higher frequency near the CMC with increasing surfactant concentration. There was no significant shift in emission maxima when the surfactant concentrations were much below or above the CMC. Similar effects were observed in the excitation spectra (Figure 4): the maxima shifted to the higher-energy side. This means that possibly the ground state of the probe was also destabilized energetically as a result of its incorporation into less polar aggregates. Water, being a highly polar hydrogen-bonding solvent, could bring about significant stabilization of the electronic state of the polar probe as opposed to the less polar environment inside the aggregate.
It was observed that the shift in excitation maximum was more than that of emission, which resulted in a net increase (positive) in the Stokes shift. This increase in Stokes shift continued with surfactant concentration until the CMC and remained almost constant with further increase of monomer concentration signifying that micelle formation was complete. Analysis of Figures 5 and 6 showed the Stokes shift gradually move to a higher value with surfactant concentration until a certain concentration was reached, and it remained practically constant with further addition of monomer. The point of inflection corresponds to the CMC value.
To determine the point of inflection and hence the CMC from Figure 6, the rising part and the plateau were fitted with linear functions. These two fitted lines cut each other at a point corresponding to the inflection [10], which was found to be at ~0.75 mM and this value is in good agreement with the literature reported value from other methods [11]. Determination of the maxima of emission or excitation spectra was crucial for getting a good result and could be accurately assigned manually by careful examination, otherwise, one might fit the individual spectrum with a lognormal function, especially when the spectrum looked broad it was difficult to find the exact position of the maximum manually. By examining the laboratory reports from a group of students it was found that the typical error for locating the maxima of emission and excitation ranged from 40 to 90 cm–1 .The analytical form for the lognormal function [12] is

The fitting function can be used in
scientific graphing software, like Origin or similar software. It should also
be noted that the Stokes shift can be equated to the reorganization energy
using the formula D
(Stokes) = 2 × reorganization energy [13]. So, one
can calculate the reorganization energy from the Stokes shift using this
relationship. This gradual change in Stokes shift until the CMC is reached may
be attributed to the fact that as surfactant is added gradually the size of the
aggregate increases and the probe bound to the aggregate experiences a changing
environment until the CMC is reached. After reaching the CMC there is no
further change

Figure 5. Emission and excitation maxima of C-343 Na salt with varying concentration of CTAB in water. Vertical lines with cap indicate error bars.

Figure 6. Stokes shift of C-343 Na salt with varying concentration of CTAB in water. Vertical lines with cap indicate error bars.
in the micellar aggregate and hence the Stokes shift stops changing.
Conclusion
The reorganization energy results from the creation of a transient solute dipole (by an exciting photon) in a solvent atmosphere. This induces a reorganization of the polar solvent molecules (for nonpolar solvents―no solvent reorganization) about the dipole in a manner that stabilizes the energy of the system. The energy term so involved may be called the reorganization energy. The Stokes shift is monitored as a function of monomer concentration. When micelle formation is complete there is no further change in Stokes shift, that is, no further reorganization of the solvent atmosphere is evident. Thus, the Stokes shift may be regarded as a marker for probing the micellization process. This experiment is not only a new technique for CMC measurement, but students learn the new concept of solvent reorganization during formation of an organized molecular assembly in a solvent, and this is reflected on the spectra of the probe dye.
Similar experiments can be carried out with other cationic surfactants, such as cetyl pyridinium chloride (CPCl) using the same C-343 Na salt as the probe. For anionic surfactants, we can, in principle, apply a similar method. This experiment has been regularly conducted in the Iowa State University physical chemistry laboratory for senior undergraduates since last year. The experiment is appropriate for undergraduate courses particularly for seniors who have acquired at least a basic knowledge of spectroscopy. Based on the results obtained from a group of undergraduate students at Iowa State University, it was found that the reported results (CMC value) are within ±10% of the literature reported value for CTAB from other methods.
Acknowledgment. The author is thankful to Professor J. W. Petrich, the Chemistry Department Chair, Iowa State University, for carefully going through the manuscript and for his valuable comments.
Supporting Materials. Instructions for the instructor and for students are available as supporting materials ((http://dx.doi.org/10.1333/s00897071097a)
References and Notes
1. Menger, F. M. Acc. Chem. Res. 1979, 12, 111–117
2. Morai, Y. Micelles, Plenum Press, NY, 1982.
3. Kunitake, T. Angew. Chem., Int. Ed. Engl. 1992, 31, 709–726.
4. Sams, P. J.; Wyn-Jones, E.; Rassing, J. Chem. Phys. Lett. 1972, 13, 233–236.
5. Aniansson, E. A. G.; Wall, S. N.; Almgren, M.; Hoffmann, H.; Kielmann, I.; Ulbricht, W.; Zana, R.; Lang, J.; Tondre, C. J. Phys. Chem. 1976, 80, 905–922.
6. Hunter, R. J. Fundamentals of Colloid Science, Vol. 1&2; Oxford University Press: New York, 1989.
7. Atkins, P. W. Physical Chemistry; W. H. Freeman and Co.: New York, 1998.
8. Kalyanasundaram, K. Photochemistry in Microheterogeneous Systems; Academic Press, New York, 1987.
9. Haldar, M.; Chowdhury, M., Chem. Phys. Letts. 1999, 312, 432–439.
10. Dominguez, A.; Fernández, A.; Gonzalez, N.; Iglesias, E.; Montenegro, L., J. Chem. Educ. 1997, 74, 1227–1231.
11. Huang, X.; Yang, J.; Zhang, W.; Zhang, Z.; An, Z. J. Chem. Educ. 1999, 76, 93–94.
12. Maroncelli, M.; Fleming, G. R. J. Chem. Phys. 1987, 86, 6221–6239
13. Jordanides, X. J.; Lang, M. J.; Song, X.; Fleming, G. R. J. Chem. Phys. 1999, 110, 5884–5892.
[*] Current address: Department of Chemistry, Indian Institute of Technology, Kharagpur-721 302, India