dc.contributor.author | Kotlarchyk, Michael | en_US |
dc.contributor.author | Chen, Sow-Hsin | en_US |
dc.contributor.author | Huang, John | en_US |
dc.contributor.author | Kim, Mahn Won | en_US |
dc.date.accessioned | 2006-12-18T17:41:12Z | en_US |
dc.date.available | 2006-12-18T17:41:12Z | en_US |
dc.date.issued | 1984-04 | en_US |
dc.identifier.citation | Physical Review A 29N4 (1984) 2054-2069 | en_US |
dc.identifier.issn | 1050-2947 | en_US |
dc.identifier.uri | http://hdl.handle.net/1850/3117 | en_US |
dc.description | RIT community members may access full-text via RIT Libraries licensed databases: http://library.rit.edu/databases/ | |
dc.description.abstract | The intensity distribution of the critical scattering from sodium di-2-ethylhexylsulfosuccinate AOT-D2O-n-alkane water-in-oil (W/O) microemulsions has been measured over an extensive range of droplet volume fractions (3-30 vol%) and temperatures (22 to 43°C) in the critical region. The water/surfactant molar ratio of the microemulsion was kept at a constant value of 40.8, for which previous experiments on the temperature variation have been well documented. A structural model of W/O microemulsions based on well-defined surfactant-coated water droplets is firmly established up to a volume fraction of about 20 vol% for all temperatures studied. Data analysis assumes that the cloud points and subsequent phase separation are caused by concentration fluctuations of polydisperse droplets. The major conclusions drawn from the analysis are as follows. (1) The order parameter of the critical phenomenon can be taken to be the volume fraction of the dispersed droplets. (2) The size and polydispersity of the droplets remain essentially constant in the vicinity of the critical point (for a fixed water/surfactant ratio). (3) The critical phenomenon is driven by an increased attraction between the droplets as the critical point is approached. (4) The critical point can be approached by either raising the temperature at fixed volume fraction or by varying the carbon number of the oil solvent at fixed volume fraction and temperature. (5) The nature of the droplets does not change upon a phase separation into two coexisting microemulsions. The data also gives some evidence that the droplet picture of the microemulsion breaks down at sufficiently high concentrations of water and surfactant. | en_US |
dc.description.sponsorship | We acknowledge the staff of the National Center for Small-Angle Scattering Research (NCSASR) at the Oak Ridge National Laboratory for their generous allocatioins of spectrometer time, making this extensive set of measurements possible within a reasonable amount of time. We would also like to thank Oak Ridge Associated Universities for financing the trips to NCSASR. This research was supported by the National Science Foundation and the Exxon Research and Engineering Company. Financial support for the primary author during this work was provided by the Thompson Memorial Fellowship awarded by the Nuclear Engineering Department at the Massachusetts Institute of Technology. | en_US |
dc.format.extent | 3115566 bytes | en_US |
dc.format.mimetype | application/pdf | en_US |
dc.language.iso | en_US | en_US |
dc.publisher | American Physical Society | en_US |
dc.relation.ispartofseries | vol. 29 | en_US |
dc.relation.ispartofseries | no. 4 | en_US |
dc.subject | Microemulsion | en_US |
dc.subject | Quasielastic light scattering | en_US |
dc.subject | Small angle neutron scattering | en_US |
dc.title | Structure of three-component microemulsions in the critical region determined by small-angle neutron scattering | en_US |
dc.type | Article | en_US |
dc.identifier.url | http://dx.doi.org/10.1103/PhysRevA.29.2054 | |