By J.A. Callow, H.W. Woolhouse (Eds.)
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Figure 8 shows two measured heterodyne correlation functions. In one case only diffusive motion was present and the correlation function simply decays exponentially. The other case corresponded to diffusive motion plus overall /r) M. W . STEER ET AL. 10 TIME ( t ) (msec) Fig. 8. Experimentally observed correlation functions: (A) corresponding to diffusive motion alone; (B) corresponding to diffusion superposed on an overall flow. translation; the damped cosine wave lies upon a flat background as the optimum conditions just described were used.
The spectrum of the scattered light reflects the propagation and decay of the interfacial capillary waves. In general this depends upon four membrane parameters: the membrane tension and compressibility and two separate interfacial viscosities. Various other methods 46 M. W. STEER ET AL. for assessing some of these properties exist, but all involve perturbation of the membrane or the insertion of molecular probes. Laser light scattering is essentially a nonperturbative technique. The spectrum of the scattered light may be calculated in terms of the properties of the fluid interface.
For assessing some of these properties exist, but all involve perturbation of the membrane or the insertion of molecular probes. Laser light scattering is essentially a nonperturbative technique. The spectrum of the scattered light may be calculated in terms of the properties of the fluid interface. Early experiments on the surfaces of pure liquids (Langevin, 1974; Byrne and Earnshaw, 1979a) concentrated on verifying the correctness of these calculations. , scattering vector q) was analyzed. Theoretical predictions of the dependences of the frequency and linewidth of the scattered light upon q were verified.