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Liquids weakly bonded pure

Weakly bonded pure liquids. The average number of molecules with their centers of mass at distances within a distance R from the origin (the center of mass of the reference molecule) can be calculated from the pair correlation function 0(J ), which is defined by the relation... [Pg.520]

Arsenic and antimony are metalloids. They have been known in the pure state since ancient times because they are easily obtained from their ores (Fig. 15.3). In the elemental state, they are used primarily in the semiconductor industry and in the lead alloys used as electrodes in storage batteries. Gallium arsenide is used in lasers, including the lasers used in CD players. Metallic bismuth, with its large, weakly bonded atoms, has a low melting point and is used in alloys that serve as fire detectors in sprinkler systems the alloy melts when a fire breaks out nearby, and the sprinkler system is activated. Like ice, solid bismuth is less dense than the liquid. As a result, molten bismuth does not shrink when it solidifies in molds, and so it is used to make low-temperature castings. [Pg.745]

Adsorbed species that desorb when the pressure of the bulk species is greatly reduced by pumping, in gas phase studies, are designated weakly bonded. The analogous procedure in electrochemical studies consists in replacing the mixture of fuel and electrolyte by pure electrolyte in the case of liquid fuels or by reducing the pressure of gaseous fuels... [Pg.113]

The molecular orbital description of the bonding in NO is similar to that in N2 or CO (p. 927) but with an extra electron in one of the tt antibonding orbitals. This effectively reduces the bond order from 3 to 2.5 and accounts for the fact that the interatomic N 0 distance (115 pm) is intermediate between that in the triple-bonded NO+ (106 pm) and values typical of double-bonded NO species ( 120 pm). It also interprets the very low ionization energy of the molecule (9.25 eV, compared with 15.6 eV for N2, 14.0 eV for CO, and 12.1 eV for O2). Similarly, the notable reluctance of NO to dimerize can be related both to the geometrical distribution of the unpaired electron over the entire molecule and to the fact that dimerization to 0=N—N=0 leaves the total bond order unchanged (2 x 2.5 = 5). When NO condenses to a liquid, partial dimerization occurs, the cis-form being more stable than the trans-. The pure liquid is colourless, not blue as sometimes stated blue samples owe their colour to traces of the intensely coloured N2O3.6O ) Crystalline nitric oxide is also colourless (not blue) when pure, ° and X-ray diffraction data are best interpreted in terms of weak association into... [Pg.446]

Unfortunately the Raman active vOH(OD) frequency could not be identified in the gas phase, for reasons well known to spectroseopists. (The OH bond is too polar and not sufficiently polarisable.) Haurie and Novak measured the Raman spectrum in the pure liquid state and saw a weak band at 3032 cm-1 which they assigned to vOH while the IR value is 3027 in the gas phase and 3028 in the liquid. For CD3COOH the Raman frequency they found is 2985 cm-1 and the IR frequency is 3040 in the gas phase and 3028 in the liquid. The IR and Raman values differ astonishingly little. [Pg.70]

Scientists realized early on that the forces between symmetrical, nonpolar molecules existed but were weak. Because they are weak, very low temperatures are required to liquify gases in which the molecules have pure covalent bonds. Flydrogen (H2), for instance, must be cooled to -252°C, only 21° above absolute zero, before it condenses into a liquid. The question was, Why does it condense at all What forces are acting on the nonpolar molecules... [Pg.97]

Surprisingly, the low solubility of small-sized particles does not stem from a weak interaction of particles with their surrounding water environment (77). For example, the heat of solvation of methane in water at ambient temperature is of similar magnitude as the heat of vaporization of pure liquid methane (80). The positive solvation free energy of small apolar particles at low temperatures is the consequence of negative solvation entropy, which overcompensates for the negative solvation enthalpy. It is widely believed that this entropy penalty is caused by the orientation order introduced to the hydration-shell water molecules as they try to maintain an intact hydrogen bond network (77). Parallel to the entropy decrease observed for low... [Pg.1918]

Consider a hydrated metal ion (for instance Co(H20)6 ) which is dissolved in a weakly coordinating medium such as 1,2-dichloroethane on the one hand, and in pure water on the other hand. In the latter case, water molecules of the first hydration shell will interact via hydrogen bonds with surrounding water molecules and this will tend to increase the EPD properties of the water molecules immediately bonded to the cation ("enthalpic effect ). This meams that water in the pure liquid state will probably behave as a considerably stronger EPD as compared with its EPD properties exhibited in weakly coordinating media such as 1,2-dichloroethane 2). If it is tentativdy assumed that the negative shifts... [Pg.124]


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See also in sourсe #XX -- [ Pg.505 , Pg.506 , Pg.509 , Pg.510 , Pg.511 , Pg.512 , Pg.513 ]




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