Direct visualization of the potential-controlled transformation of hemimicellar aggregates of dodecyl sulfate into a condensed monolayer at the Au(111) electrode surface
I. Burgess et al., Direct visualization of the potential-controlled transformation of hemimicellar aggregates of dodecyl sulfate into a condensed monolayer at the Au(111) electrode surface, LANGMUIR, 15(8), 1999, pp. 2607-2616
Electrochemical measurements, atomic force microscopy, and scanning tunneli
ng microscopy have been combined to present the first direct images of the
potential-controlled. phase transition between the hemimicellar and condens
ed states of a dodecyl sulfate (SDS) film at the Au(lll) electrode surface.
The adsorbed SDS forms stripe-shaped hemimicellar aggregates at small or m
oderate charge densities at the electrode. High-resolution STM images of th
ese aggregates revealed that adsorbed SDS molecules are ordered and form a
long-range two-dimensional lattice. A unit cell of this lattice consists of
two vectors that are 4.4 and 0.5 nm long and are oriented at an angle of 7
0 degrees. We propose that each unit cell contains two flat-laying SDS mole
cules stretched out along the longer axis of the cell with the hydrocarbon
tails directed toward the interior of the cell. The remaining SDS molecules
in the hemimicelle assume a tilted orientation. This long-range structure
is stabilized by the interactions of sulfate groups belonging to the adjace
nt cells. The sulfate groups of the flat-laying SDS molecules are arranged
into a characteristic (root 3 x root 7) structure in which the sulfate grou
ps along the root 7 direction are bridged by hydrogen-bonded water molecule
s. When the positive charge on the metal either becomes equal to or exceeds
the charge of adsorbed surfactant, the surface aggregates melt to form a c
ondensed film. The transition between the hemimicellar and condensed states
of the film is reversible. The hemimicellar aggregates may be re-formed by
decreasing the charge density at the electrode surface. The charging and d
ischarging of the gold electrode can be easily controlled by a proper varia
tion of the electrode potential.