Hh. Paradies et M. Thies, MICELLAR PROPERTIES AND STRUCTURE OF BENZETHONIUM CHLORIDE IN ISOTROPIC AQUEOUS-SOLUTIONS, Berichte der Bunsengesellschaft fur Physikalische Chemie, 98(5), 1994, pp. 715-725
Citations number
42
Categorie Soggetti
Chemistry Physical
Journal title
Berichte der Bunsengesellschaft fur Physikalische Chemie
The micellar structure of the cationic surfactant benzethonium chlorid
e (BZCl) was analysed by small-angle x-ray scattering techniques. The
shape, size and characteristics of the internal structure of BZCl was
studied by the contrast variation method at 20-degrees-C (CMC = 5.35 x
10(-4) Mol/l) by changing the electron density of the solvent through
addition of polyols, e.g. sucrose or glycerol. The obtained scatterin
g data were converted to absolute intensities, and analysed for interm
icellar interference effects, by applying the rescaled mean spherical
approximation method. The morphological parameters, micellar volume, a
verage electron density, rho1BAR, radius of gyration, R(v), second mom
ent of the electron density distribution, ''a'', and square average of
the electron distribution, (DELTArho1(2)), were determined from scatt
ering data in the range of 0.001 < h < 0.08 angstrom-1. The apparent a
ggregation number (65 +/- 10), degree of ionization (alpha = 0.15) wer
e also determined by static light scattering. The micellar shape of BZ
Cl was computed from R(v), and the maximum dimension of the micelle D(
max) = 54.0 angstrom were obtained from the distance distribution func
tion. The shape of the BZCl micelle is consistent with an oblate ellip
soid -of revolution with a = 26.8 angstrom. The condensation effects o
f the chloride ions on the BZCl was compared for the ''structural'' mo
del vs. the ''effective model'' from static light scattering and x-ray
scattering.The polydispersity in micellar size was found to be small,
1.55 in the weight-average molecular weight and 17% in [V1]. These va
lues. including ([M(w,app)]), the one of the radius of gyration of the
exclude volume (R(g) = 20.3 +/- 0.3 angstrom) are independent of the
density of the solvent through addition of polyols.