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Molecules liquid

Spectroscopy, or the study of the interaction of light with matter, has become one of the major tools of the natural and physical sciences during this century. As the wavelength of the radiation is varied across the electromagnetic spectrum, characteristic properties of atoms, molecules, liquids and solids are probed. In the... [Pg.1232]

Condensed phase vibrational or vibronic lineshapes (vibronic transitions create vibrational excitations of electronic excited states) rarely provide infonnation about VER (see example C3.5.6.4). Experimental measurements of VER need much more than just the vibrational spectmm. The earliest VER measurements in condensed phases were ultrasonic attenuation studies of liquids [15], which provided an overall relaxation time for slowly (>10 ns) relaxing small molecule liquids. [Pg.3034]

The solidity of gel electrolytes results from chain entanglements. At high temperatures they flow like liquids, but on cooling they show a small increase in the shear modulus at temperatures well above T. This is the liquid-to-rubber transition. The values of shear modulus and viscosity for rubbery solids are considerably lower than those for glass forming liquids at an equivalent structural relaxation time. The local or microscopic viscosity relaxation time of the rubbery material, which is reflected in the 7], obeys a VTF equation with a pre-exponential factor equivalent to that for small-molecule liquids. Above the liquid-to-rubber transition, the VTF equation is also obeyed but the pre-exponential term for viscosity is much larger than is typical for small-molecule liquids and is dependent on the polymer molecular weight. [Pg.513]

Strictly speaking, the term racemic mixture applies only when the mixture of molecules is present as separate solid phases, but in this book we shall use this expression to refer to any equimolar mixture of enantiomeric molecules, liquid, solid, gaseous, or in solution. [Pg.192]

Generally, the values of the scaling exponent are smaller for polymers than for molecular liquids, for which 3.2 < y < 8.5. A larger y, or steeper repulsive potential, implies greater influence of jamming on the dynamics. The smaller exponent found for polymers in comparison with small-molecule liquids means that volume effects are weaker for polymers, which is ironic given their central role in the historical development of free-volume models. The reason why y is smaller... [Pg.661]

Russell, D. J., Calibration of high performance size exclusion chromatography for small epoxy molecules, /. Liquid Chromatogr., 11, 383, 1988. [Pg.365]

Phosphorus vapor consists of tetrahedral P4 molecules, and at higher temperatures also of P2 molecules (P=Pbond length 190 pm). White phosphorus forms by condensation of the vapor it also consists of P4 molecules. Liquid phosphorus normally consists of P4 molecules, but at a pressure of 1 GPa and 100 °C polymeric liquid phosphorus is formed which is not miscible with liquid P4. [Pg.108]

Figure 1 a) The effect of high pressure in gas—liquid two-phase systems, b) The effect of high pressure in a liquid one-phase system, (o) gas molecules ( ) liquid molecules... [Pg.145]

Flory, P.J. Orwoll, R.A. Vrij, A. "Statistical Thermodynamics of Chain Molecule Liquids," JACS, 86, 3515(1964). [Pg.378]

Specifically, the general approximation / 0.079 m has been suggested [142] for a wide range of both polymer and small molecule liquids. This relation implies that high molar mass F-S polymers should have steepness index m of about m 100, which is consistent in order of magnitude with estimates [142] for the representative F-S polymer, polystyrene (PS). [Pg.175]

A crucial feature of PNC experiments in atoms, molecules, liquids or solids is that for interpretation of measured data in terms of fundamental constants of the P,T-odd interactions, one must calculate those properties of the systems, which establish a connection between the measured data and studied fundamental constants (see section 4). These properties are described by operators heavily concentrated near or on heavy nuclei they cannot be measured and their theoretical study is not a trivial task. During the last several years the significance of (and requirement for) ab initio calculation of electronic structure providing a high level of reliability and accuracy in accounting for both relativistic and correlation effects has only increased (see sections 3 and 10). [Pg.254]

Flory has recently summarized the experimental evidence pertaining to local correlation and their effects on chain dimensions (49). There is experimental support for local alignment from optical properties such as stress-optical coefficients in networks (both unswelled and swelled in solvents of varying asymmetry), and from the depolarization of scattered light in the undiluted state and at infinite dilution. The results for polymers however, turn out to be not greatly different from those for asymmetric small molecule liquids. The effect of... [Pg.16]

The friction factor depends upon the same features that govern the viscosity of small-molecule liquids. At low temperatures f0 depends on T — T% (Tg < T< Tg+ 4-100° C), and at higher temperatures it depends on an activation energy for flow. The value of 3 for a solution depends on the properties of both components and their concentrations, but it is independent of the large scale structure of the polymer as long as its molecular weight is large (Mn > 104 for most linear polymers). [Pg.49]

Chikahisa (216) and Williams (217-219) have examined flow behavior in concentrated polymer systems without detailed consideration of the mechanism of intermolecular interaction. Williams explicitly limits his discussion to unentangled systems Chikahisa uses an entanglement terminology, although not in a specific way. Both approaches grow out of the formalism which was developed to deal with transport properties in small-molecule liquids. [Pg.74]

The derivation of this equation makes it seem more appropriate for small molecule liquids or suspensions of hard spheres than for interpenetrating random coil molecules however. Indeed, a somewhat modified version of the equation has approximately the form observed for rj(j) in concentrated suspensions of mono-disperse spheres. In this case I/r0 turns out to be of the order of the rotational... [Pg.144]

In recent years, the behaviour of liquid crystalline polymers including elastomers has been a subject of considerable interest 104,105). It is known that small molecule liquid crystals turn into a macroscopic ordered state by external electric or magnetic fields. A similar behaviour seems to occur for liquid-crystalline polymer networks under mechanical stress or strain. [Pg.67]

A characteristic of small-molecule liquid chromatography is the reversibility of their contacts with the stationary phase. The distribution equilibrium constant determines the duration of the stationary periods and, thus, the retention of the solute. With polymers, isocratic retention factors of normal degree (i.e., 1 gk 10) generally do not occur. A fractional alteration of elution conditions may cause transition from zero retention to infinity. As a rule of thumb, polymers either pass without retention or remain in the column. This off or on behavior produces the impression of irreversible fixation under the conditions of retention. [Pg.162]

Movable water molecules weak bonded to the hydrophilic membrane groups and less water molecules liquid-like. [Pg.172]

The picture of consequent SB in condensed matter by cooling is illustrated in Fig. 3. Each SB has its own independent coordinate Q, and only the temperature scale is in common. The temperatures of SB are indicated by orders of magnitude, while their sequence is self-explanatory atoms => molecules => liquid => crystal(I) => crystal(II) => and so on. [Pg.14]

SIMS. Secondary Ion Mass Spectrometry is particularly suited for ionization of nonvolatile, polar, and thermally labile molecules. Liquid SIMS, using liquid glycerol matrices, is best done in the differentially-pumped external ion source, because matrix effects and the high vapor pressure of glycerol make liquid SIMS unsuitable for single cell low-pressure FTMS. [Pg.85]

The coloring and bleaching phenomena are caused by changes in molecular configuration of colloidal phosphorus formed in the glasses. The P molecule (liquid or white phosphorus) is colorless. It polymerizes thermally or photochemically to the... [Pg.376]

Analyzer Monoxide Dioxide Molecules Molecules Liquids Comments... [Pg.350]

Although the microscopic motions in a liquid occur on a continuum of time scales, one can still partition this continuum into two relatively distinct portions. The short-time behavior in a liquid is characterized by frustrated inertial motions of the molecules. While an isolated molecule in the gas phase can translate and rotate freely, in a liquid these same motions are interrupted by collisions with other molecules. Liquids are dense enough media that collisions occur very frequently, so that molecules undergo pseudo-oscillatory motion in the local potentials defined by their... [Pg.483]

Loughnane BJ, Scodiunu A, Farrer RA, Fourkas JT, Mohanty U. Exponential intermolecular dynamics in optical Kerr effect spectroscopy of small-molecule liquids. J Chem Phys 1999 111 2686-2694. [Pg.520]


See other pages where Molecules liquid is mentioned: [Pg.247]    [Pg.181]    [Pg.660]    [Pg.237]    [Pg.142]    [Pg.609]    [Pg.2]    [Pg.34]    [Pg.132]    [Pg.170]    [Pg.180]    [Pg.103]    [Pg.130]    [Pg.1038]    [Pg.16]    [Pg.325]    [Pg.148]    [Pg.84]    [Pg.276]    [Pg.19]    [Pg.272]    [Pg.216]    [Pg.130]    [Pg.211]    [Pg.419]   
See also in sourсe #XX -- [ Pg.161 ]




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Aggregation of Molecules to Solids and Liquids

Bent-core molecules liquid crystals

Chiral liquid crystals, bent-core molecules

Coherent control of large molecules in liquids

Condensation The process by which vapor molecules re-form a liquid

Discotic liquid crystals disc-shaped molecules

Dynamics of Materials at the Nanoscale Small-Molecule Liquids and Polymer Films

Emulsions small molecule liquid

Ferroelectric liquid crystalline molecules

Ionic liquid-supported synthesis of small molecules

Ionic liquids hydrogen-bonding molecules

Light scattering in liquids with anisotropic molecules

Light scattering in liquids with isotropic molecules

Liquid chromatography-mass small molecules

Liquid crystal formation of small-molecule surfactants

Liquid crystal molecules

Liquid crystals achiral molecules

Liquid crystals chiral discotic molecules

Liquid crystals cone-shaped molecules

Liquid crystals of disc-like molecules

Liquid crystals of rod-like molecules

Liquid crystals self-assembled molecules, chirality

Liquid guest molecules

Liquid-crystalline molecules

Liquid-crystalline molecules Subject

Molecules in liquids

Molecules liquids and

Nematic liquid crystals formed from flexible molecules

Rigid rod molecules as liquid-crystalline

Rigid rod molecules as liquid-crystalline thermosets

Self-assembled molecules discotic liquid crystals

Small molecule and polymeric liquid

Small molecule and polymeric liquid crystals

Small molecule liquid crystals SMLCs)

Small-molecule liquid crystals

Structure of Liquids Containing Elongated Molecules

The H2O Molecule in Liquid Water

Thermotropic liquid-crystal-forming molecules, structure

Vitrification of liquids many-molecule dynamics

WATER MOLECULES MOVE FREELY BETWEEN THE LIQUID AND GASEOUS PHASES

X-Shaped Polyphiles Liquid Crystalline Honeycombs with Single Molecule Walls

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