Technical Notes
A High-Performance and Simplified Quasi-Elastic
Laser Scattering Method Using Homodyne
Detection in Beam Divergence
Isao Tsuyumoto* and Hiroshi Uchikawa
Department of Environmental Systems Engineering, Kanazawa Institute of Technology, 7-1 Ohgigaoka,
Nonoichi, Ishikawa 921-8501, Japan
We devise the new principle of the quasi-elastic laser
scattering (QELS) method using a homodyne detection
technique in a beam divergence and successfully facilitate
the equipment. The QELS method is a unique technique
for the noncontact and time-resolved study of surface
tension at liquid surfaces and liquid/ liquid interfaces. The
conventional QELS method requires a precise optical
alignment using a local oscillator such as a diffraction
grating, and the determination of the surface tension
accompanies much difficulty because of the low S/ N ratio
of the power spectra. Our new principle allows high-
performance QELS measurements by only a simple align-
ment of a downsized experimental setup. The power
spectra are obtained with 5 0 -1 0 0 times higher S/ N ratios
than the conventional ones. The power spectra are ana-
lyzed by a new theory, and the calculated surface tensions
agree with the literature values. The accuracy of the
surface tension measurements using the QELS method
is substantially improved.
Surface tension measurements provide much information on
surfactant dynamics at liquid surfaces and liquid/ liquid interfaces.
Common industrial processes such as washing, printing, and
coating are closely related to the adsorption of surfactants, and
surface tension measurements are widely used for quality control,
research, and development in various industries. The measure-
ments are also helpful for fundamental studies in view of the
interfacial thermodynamics, properties, and structures. A number
of methods for surface tension measurements such as the
Wilhelmy method, the Du Nou ¨ y method, the spinning drop
method have been reported so far,
1
but these methods bring about
mechanical perturbation and are not suitable for time-resolved
measurements. Katyl and Ingard reported a quasi-elastic laser
scattering from liquid surfaces by capillary waves (ripplons), which
are spontaneously generated at liquid surfaces.
2
Several research-
ers reported that the QELS method is an appropriate method for
surface tension measurements, indicating that the surface tensions
calculated from the capillary wave frequencies agreed with the
other methods.
3-5
Tsuyumoto and co-workers have fabricated the
conventional QELS measurement system based on a laser
heterodyne apparatus
6
using a diffraction grating as a local
oscillator and have reported on the dynamics of mass transfer of
surfactants at the water/ nitrobenzene interface.
7-11
However,
many experimental difficulties arose in the measurements, e.g.,
the detection of the signal from the capillary waves was very
difficult because of the extremely small amplitude of the waves
( ∼10 nm), and the determination of the surface tensions included
accidental errors due to the low S/ N ratio of the observed power
spectra. In this study, to improve the QELS method, we devise a
homodyne detection technique using a beam divergence instead
of heterodyne detection using the diffraction grating. We present
here the measurement results of standard samples and discuss
the advantages of the new homodyne QELS method.
PRINCIPLE
The principles of the conventional and the new homodyne
QELS methods are shown in Figure 1a and b, respectively. A
thermally generated spontaneous density fluctuation occurs at the
liquid surface. The surface tension acts as a restoring force on
the fluctuation, and it excites a surface tension wave, which is
called a capillary wave or ripplon. The capillary waves occurring
on liquid surfaces have various wavelengths, and each frequency
is dependent on each wavelength. This makes it essential to select
a capillary wave with a certain wavelength to determine the
dispersion relation of the waves. The QELS methods measure the
(1) Mingins, J.; Taylor, J. A. G.; Pethica, B. A.; Jackson, C. M.; Yue, B. Y. T. J.
Chem. Soc., Faraday Trans. 1 1982 , 78, 323.
(2) Katyl, R. H.; Ingard, U. Phys. Rev. Lett. 1968 , 20, 248.
(3) Sakai, K.; Tanaka, H.; Takagi, K. Jpn. J. Appl. Phys. 1990 , 29, L2247.
(4) Sauer, B. B.; Chen, Y. L.; Zografi, G.; Yu, H. Langmuir 1988 , 4, 111.
(5) Sano, M.; Kawaguchi, M.; Chen, Y.-L.; Skarlupka, R. J.; Cheng, T.; Zografi,
G.; Yu, H. Rev. Sci. Instrum. 1986 , 57, 1158.
(6) Ha ¨ rd, S.; Hamnerius, Y.; Nilsson, O. J. Appl. Phys. 1976 , 47, 2433.
(7) Uchiyama, Y.; Tsuyumoto, I.; Kitamori, T.; Sawada, T. J. Phys. Chem. B
1999 , 103, 4663.
(8) Uchiyama, Y.; Kitamori, T.; Sawada, T.; Tsuyumoto, I. Langmuir 2000 ,
16, 6597.
(9) Uchiyama, Y.; Fujinami, M.; Sawada, T.; Tsuyumoto, I. J. Phys. Chem. B
2000 , 104, 4699.
( 10) Zhang, Z. H.; Tsuyumoto, I.; Kitamori, T.; Sawada, T. J. Phys. Chem. B 1998 ,
102, 10284.
( 11) Zhang, Z. H.; Tsuyumoto, I.; Takahashi, S.; Kitamori, T.; Sawada, T. J. Phys.
Chem. A 1997 , 101, 4163.
Anal. Chem. 2001, 73, 2366-2368
2366 Analytical Chemistry, Vol. 73, No. 10, May 15, 2001 10.1021/ac001338e CCC: $20.00 © 2001 American Chemical Society
Published on Web 04/05/2001