The sonoluminescence generated in water with pulsed 515 kHz ultrasound
has been studied in the presence of different chain length (C-1-C-5)
aliphatic alcohols and the surfactants sodium dodecyl sulfate (SDS), d
odecyltrimethylammonium chloride (DTAC), and -dodecyl-N,N-dimethyl-3-a
mmonio-1-propanesulfonate (DAPS). The ultrasound pulse widths used ran
ged from 1 to 10 ms, with duty cycles (on/off ratios) of 1:3 to 1:9. I
t was found that the sonoluminescence from the initial pulses was very
low but increased in intensity and reached a maximum after 20-50 puls
es, for all systems studied, depending on the purse width and duty cyc
le. In the presence of alcohol the maximum signal decreased with incre
asing alcohol concentration, and the signal decline was more pronounce
d with increasing chain length of the alcohol. A good correlation was
found to exist between the decline in the sonoluminescence signal and
the Gibbs surface excess of the alcohol at the air/water interface. In
the presence of SDS (an anionic surfactant) and DTAC (a cationic surf
actant), quite different behavior was observed. At low concentrations
of these two surfactants the maximum signal was significantly enhanced
over that obtained in pure water, reaching a maximum at about 1 mM of
surfactant. At higher concentrations the signal decreased again reach
ing a limiting value similar to that obtained in pure water. The sonol
uminescence signal in DAPS (a zwitterionic surfactant) solutions remai
ned much the same as in pure water. On the addition of 0.1 M NaCl to t
he three different types of surfactin solutions, the intensities of th
e emission signals obtained were essentially the same as in pure water
. Possible mechanisms responsible for the different behavior in the so
noluminescence signal in the presence of the alcohols and surfactants
are discussed.