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Contact angles temperature dependence

Early transport measurements on individual multi-wall nanotubes [187] were carried out on nanotubes with too large an outer diameter to be sensitive to ID quantum effects. Furthermore, contributions from the inner constituent shells which may not make electrical contact with the current source complicate the interpretation of the transport results, and in some cases the measurements were not made at low enough temperatures to be sensitive to 1D effects. Early transport measurements on multiple ropes (arrays) of single-wall armchair carbon nanotubes [188], addressed general issues such as the temperature dependence of the resistivity of nanotube bundles, each containing many single-wall nanotubes with a distribution of diameters d/ and chiral angles 6. Their results confirmed the theoretical prediction that many of the individual nanotubes are metallic. [Pg.75]

Fig. 4 Dependence of the advancing water contact angle on annealing temperature for PS-based diblock copolymer brush layers (filled squares) Si/Si02//PS- -PHFA, (filled triangles) Si/Si02//PS- -PPFA, (filled diamonds) Si/Si02//PS- -PPFS. Lines added as guide for the eye... Fig. 4 Dependence of the advancing water contact angle on annealing temperature for PS-based diblock copolymer brush layers (filled squares) Si/Si02//PS- -PHFA, (filled triangles) Si/Si02//PS- -PPFA, (filled diamonds) Si/Si02//PS- -PPFS. Lines added as guide for the eye...
Finally, an important feature of gels made of adhesive emulsions arises from the deformation of the droplets. Indeed, as the temperature is lowered the contact angles between the droplets increase [27,28] (see Chapter 2, Section 2.3). Consequently, the structure of the final floes depends on the time evolution of the strength of the adhesion. Initially, the adhesion results in the formation of a random, solid gel network in the emulsion. Further increase of adhesion causes massive fracturing of the gel, disrupting the rigidity of the structure and leading to well separated, and more compact floes [27,28]. [Pg.123]

Fig. 8 Ambient temperature dependence of the change in water contact angle on a highly hydrophilic HO2 surface in the dark... Fig. 8 Ambient temperature dependence of the change in water contact angle on a highly hydrophilic HO2 surface in the dark...
Figure 1.7. Dependence of contact angle on the metal droplet radius for Pb on vitreous carbon at a temperature close to the melting point of Pb. The horizontal line identifies the macroscopic contact angle. Data from work reported in (Chizhik et al. 1985). Figure 1.7. Dependence of contact angle on the metal droplet radius for Pb on vitreous carbon at a temperature close to the melting point of Pb. The horizontal line identifies the macroscopic contact angle. Data from work reported in (Chizhik et al. 1985).

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