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For the uncertainty of the critical temperatures, the authors give a value of ˙10 mK and that of the order parameter, the mass fraction wc , is ˙0:004. From a detailed analysis of the scaling laws, the following conclusions are drawn. The critical exponent ˇ for the coexistence curves lies near the Ising value, but shows systematic deviations with varying ", from ˇ D 0:315 at " D 16:8 to ˇ D 0:36 at " D 3:6. For larger reduced temperatures > 0:01 and using the mole fraction scale as order parameter, the critical exponent is near the mean field value of ˇeff D 0:5.
Finally, it must be noted that experimental investigations of the microscopic structure of the liquid/vapour interface of molten salts such as alkali halides are still missing. Such experiments are complicated due to the fact that alkali halides have a relatively high vapour pressure near their melting point, which makes the use of ultrahigh vacuum techniques difficult. g. 139]. It seems that this is not the case in salts such as the alkali halides. 140]. 141]. Using classic Born–Mayer–Huggins–Fumi–Tosi two-body potentials, these authors have performed extensive simulations for NaCl and have calculated the solid/liquid, liquid/vapour and solid/vapour interfacial free energies.
Strong motivations result from potential applications in lab-on-a chip devices or new kinds of electronic displays. Electrowetting enables the manipulation of tiny amounts of liquids on surfaces. 41) which describes the variation of the contact angle ‚ of a liquid droplet of a conducting fluid on top of a thin dielectric film with capacitance C as a function of voltage U applied across the droplet and film. The liquid/vapour surface tension of the droplet is denoted by lv . 151]. 154]. Essentially, they exhibit the same electrowetting features of a parabolic dependence of cos ‚ vs.
Acceptance of stay cable systems using prestressing steels by prepared by Task Group 9.2.