Scattering from Short Stiff Cylindrical Micelles Formed by
Fully Ionized TDAO in NaCl/Water Solutions
Vasil M. Garamus,*
,†
Jan Skov Pedersen,
‡
Hiroshi Maeda,
§
and
Peter Schurtenberger
|
GKSS Research Centre, Max-Planck Strasse, 21502 Geesthacht, Germany, Department of
Chemistry, University of Aarhus, Langelandsgade 140, DK-8000 Aarhus C, Denmark,
Department of Chemistry, Faculty of Science, Kyushu University, Fukuoka 812-8581, Japan,
and Department of Physics, University of Fribourg, Perolles, 1700 Fribourg, Switzerland
Received December 2, 2002. In Final Form: February 18, 2003
Aqueous solutions of fully ionized tetradecyldimethylamine oxide (TDAO) with addition of 0.1 M NaCl
were investigated by small-angle neutron scattering (SANS) and static light scattering (SLS). The analysis
of the data showed that the surfactant under these conditions forms short stiff cylindrical micelles. The
surfactant concentration ranges from 2 times the critical micelle concentration to well above the overlap
concentration of the cylindrical micelles. A self-consistent approach was used for analyzing the SANS and
SLS data simultaneously. The forward scattering was determined from the scattering at low scattering
vectors, and from this, the apparent molar mass of the micelles was derived. It was fitted by a model with
a power-law growth law combined with a term which describes intermicellar interaction effects. The length
of the micelles was derived from the growth law using the mass per unit length as determined from the
scattering data at high scattering vectors. Finally, the data in the full range of measured scattering vectors
were fitted for all concentrations by a model based on the polymer reference interaction site model with
a simple ansatz for the direct correlation function. The variations of the parameters of the micelles as
obtained in the analysis were compared to the parameters for solutions of half-ionized TDAO for which
semiflexible micelles are formed.
1. Introduction
The formation of long micelles is observed in solutions
of ionic surfactant under certain conditions.
1-3
These
micelles are generally formed in the presence of a high
salt concentration. The physical properties of such systems
are of great interest, because a small change in the
surfactant molecular structure, the type of counterion, or
the amount of added salt may alter the size, flexibility,
and interactions of the micelles. This, in turn, gives marked
effects on the macroscopic rheological properties.
The relationship between the flexibility of micelles,
which can be characterized by the persistence l
p
or Kuhn
length b, and the rheological properties is yet not known,
and it is not possible to predict rheology a priori. There
are currently a lot of efforts to study the above-mentioned
relationship.
2-4
Some of the results of these studies are
that the linear rheological properties (“Maxwell-like”) can
be scaled with concentration
4-7
and the increase of fluidity
is due to the transformation from linear micelles to
branched systems.
4,8
There are still open questions such
as, what is the origin of the maximum of the zero shear
viscosity as a function of the surfactant concentration and
salt concentration?
There has been significant progress during the last years
in the study of the dependence of the flexibility of micelles
on the salinity of the solutions.
9-14
It has been clearly
shown that flexibility increases with salt addition. The
persistence length is conventionally described as being
the sum of two contributions: an intrinsic contribution,
as one has for neutral chains, and an electrostatic
contribution. Even at a high concentration of salt (2 M),
the electrostatic contribution to the persistence length is
detected in the case of the anionic surfactant sodium
dodecyl sulfate (SDS).
9
In the case of nonionic surfactants or ionic surfactants
in high-salt solutions, the growth of elongated micelles
versus surfactant concentration is predicted by mean-
field theory
1
to have a simple power-law form, that is, 〈L〉
w
∼ c
0.5
, where 〈L〉
w
is the weight-average length of the
micelles in dilute solutions and 〈L〉
w
∼ c
0.6
in the semidilute
regime. A lot of attempts to experimentally verify the
mean-field theory predictions have been made by means
of rheological techniques and scattering methods. The
results are quite different and strongly influenced by the
procedure used for analyzing the data. Rheological
* Corresponding author. Phone: +49 4152 871290. Fax: +49
4152 871356. E-mail: vasyl.haramus@gkss.de.
†
GKSS Research Centre.
‡
University of Aarhus.
§
Kyushu University.
|
University of Fribourg.
(1) Cates, M. E.; Candau, S. J. J. Phys.: Condens. Matter 1990, 2,
6869.
(2) Walker, L. M. Curr. Opin. Colloid Interface Sci. 2001, 6, 451-
456.
(3) Magid, L. J. Phys. Chem. B 1998, 102, 4064.
(4) Koehler, R. D.; Raghavan, S. R.; Kaler, E. W. J. Phys. Chem. B
2000, 104, 11035-11044.
(5) Maeda, H.; Yamamoto, A.; Souda, M.; Kawasaki, H.; Hossain,
Kh. S.; Nemoto, N.; Almgren, M. J. Phys. Chem. B 2001, 105, 5411-
5418.
(6) Kim, W. J.; Yang, S. M. Langmuir 2000, 16, 6084-6093.
(7) Raghavan, S. R.; Kaler, E. W. Langmuir 2001, 17, 300-306.
(8) Candau, S. J.; Oda, R. Colloids Surf., A 2001, 183,5-14.
(9) Magid, L. J.; Li, Z.; Butler, P. D. Langmuir 2000, 16, 10028-
10036.
(10) Arleth, L.; Bergstro ¨m, M.; Pedersen, J. S. Langmuir 2002, 18,
5343-5353.
(11) Jerke, G.; Pedersen, J. S.; Egelhaaf, S. U.; Schurtenberger, P.
Langmuir 1998, 14, 6013.
(12) Cannvacciulo, L.; Sommer, C.; Pedersen, J. S.; Schurtenberger,
P. Phys. Rev. E 2000, 62, 5409.
(13) Cannavacciuolo, L.; Pedersen, J. S.; Schurtenberger, P. J. Phys.:
Condens. Matter 2002, 14, 2283.
(14) Sommer, C.; Pedersen, J. S.; Egelhaaf, S. U.; Cannavacciuolo,
L.; Kohlbrecher, J.; Schurtenberger, P. Langmuir 2002, 18, 2495-2505.
3656 Langmuir 2003, 19, 3656-3665
10.1021/la026938i CCC: $25.00 © 2003 American Chemical Society
Published on Web 03/29/2003