LIGHT-SCATTERING AND SMALL-ANGLE X-RAY-SCATTERING ON MICELLAR BENZETHONIUM CHLORIDE (BROMIDE) SOLUTIONS .3. MICELLAR STRUCTURE OF BZCL AT DIFFERENT SOLVENT ELECTRON-DENSITIES
M. Thies et al., LIGHT-SCATTERING AND SMALL-ANGLE X-RAY-SCATTERING ON MICELLAR BENZETHONIUM CHLORIDE (BROMIDE) SOLUTIONS .3. MICELLAR STRUCTURE OF BZCL AT DIFFERENT SOLVENT ELECTRON-DENSITIES, Colloids and surfaces. A, Physicochemical and engineering aspects, 101(2-3), 1995, pp. 261-277
The micellar structure of the cationic surfactants benzethonium chlori
de (BZCl) and bromide (BZBr) was analyzed by small-angle X-ray scatter
ing and light scattering techniques. The shape, size and characteristi
cs of the internal structure of BZCl was studied by the contrast-varia
tion method at 20 degrees C (CMC = 1.78 mM) by changing the electron d
ensity of the solvent by addition of sucrose or glycerol. The morpholo
gical parameters, i.e. average electron density rho(1), radius of gyra
tion of micellar shape, R(v), apparent molecular weight, aggregation n
umber (52) and degree of hydration (0.24 g H2O g(mic)(-1)) were determ
ined using scattering data in the range 0 < h < 0.08 Angstrom(-1). The
micellar shape of BzCl was computed from R(v); the maximum dimension
of the micelle in solution was obtained from the distance distribution
function (D-max = 56.0 Angstrom), and is consistent with an oblate el
lipsoid of revolution (a = 27.8 Angstrom, b = 25.1 Angstrom). A three-
shell structure ellipsoid of revolution model was found to be an appro
priate model, consisting of a polar group layer L(pol) = 9.65), a laye
r consisting partly of the ether residues (L' = 9.20) and the hydrocar
bon core (R(HC) = 17.4 Angstrom). BZBr revealed a much lower aggregati
on number and different hydrodynamic properties, i.e. R(g) = 13.5 Angs
trom, D-max = 28.4 Angstrom, apparent molecular weight (MW(app)) = 160
00, apparent aggregation number (N-agg) = 36, CMC = 0.17 mM. The BZBr
micelles show a very narrow size distribution and are almost spherical
in shape when analyzed in terms of a structural system (Z(str) = 30),
but by decreasing the charge of the structural system to the effectiv
e charge (Z(eff) = 19.5), the S-pp(h, rho(0)) factor revealed no diffe
rences between the two systems. The polydispersity in micellar size fo
r both BZCl and BZBr was found to be small (approximate to 8%) at cons
tant chemical potential. The CMC and N-app are independent of the dens
ity of the solvent when using glycerol or sucrose as additives in the
presence of 0.01 M NaCl for BZCl (20 degrees C).