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Potential temperature dependence

RadSigma=5.6686e-6 %watt/m2-K4 Stefan-Boltzmann for radiation calculation %Define Thermodynamic Nernst Potential Temperature Dependent Parameters (this is for a specific fuel)... [Pg.315]

With regard to differences in polymer behavior in solution versus the bulk state, several points must be made. Clearly, it is now well-established that the choice of theta solvent can affect chain dimensions to some extent [42-44, 46, 47]. Hence, only the chain in an amorphous melt of identical neighbors can be considered to be in the unperturbed state. Particularly striking are some of the differences noted in temperature coefficients measured by different techniques. Is it possible that the thermal expansion of a polymer molecule is fundamentally different in the bulk and in solution Can specific solvent effects exist and vary in a systematic way within a series of chemically similar theta solvents Does the different range of temperatures usually employed in bulk versus solution studies affect K Are chains in the bulk (during SANS and thermoelastic experiments) allowed adequate time to completely relax to equilibrium All of these issues need further attention. Other topics perhaps worthy of consideration include the study of the impact of deuterium labelling on chain conformation (H has lower vibrational energy than does H ) and the potential temperature dependence of the Flory hydrodynamic parameter . [Pg.45]

LEED angles must be corrected for refraction by the surface potential barrier [73]. Also, the intensity of a diffraction spot is temperature dependent because of the vibration of the surface atoms. As an approximation. [Pg.303]

Using the temperature dependence of 7 from Eq. III-l 1 with n - and the chemical potential difference Afi from Eq. K-2, sketch how you expect a curve like that in Fig. IX-1 to vary with temperature (assume ideal-gas behavior). [Pg.342]

Fluctuations of observables from their average values, unless the observables are constants of motion, are especially important, since they are related to the response fiinctions of the system. For example, the constant volume specific heat of a fluid is a response function related to the fluctuations in the energy of a system at constant N, V and T, where A is the number of particles in a volume V at temperature T. Similarly, fluctuations in the number density (p = N/V) of an open system at constant p, V and T, where p is the chemical potential, are related to the isothemial compressibility iCp which is another response fiinction. Temperature-dependent fluctuations characterize the dynamic equilibrium of themiodynamic systems, in contrast to the equilibrium of purely mechanical bodies in which fluctuations are absent. [Pg.437]

Figure B3.6.3. Sketch of the coarse-grained description of a binary blend in contact with a wall, (a) Composition profile at the wall, (b) Effective interaction g(l) between the interface and the wall. The different potentials correspond to complete wettmg, a first-order wetting transition and the non-wet state (from above to below). In case of a second-order transition there is no double-well structure close to the transition, but g(l) exhibits a single minimum which moves to larger distances as the wetting transition temperature is approached from below, (c) Temperature dependence of the thickness / of the enriclnnent layer at the wall. The jump of the layer thickness indicates a first-order wetting transition. In the case of a conthuious transition the layer thickness would diverge continuously upon approaching from below. Figure B3.6.3. Sketch of the coarse-grained description of a binary blend in contact with a wall, (a) Composition profile at the wall, (b) Effective interaction g(l) between the interface and the wall. The different potentials correspond to complete wettmg, a first-order wetting transition and the non-wet state (from above to below). In case of a second-order transition there is no double-well structure close to the transition, but g(l) exhibits a single minimum which moves to larger distances as the wetting transition temperature is approached from below, (c) Temperature dependence of the thickness / of the enriclnnent layer at the wall. The jump of the layer thickness indicates a first-order wetting transition. In the case of a conthuious transition the layer thickness would diverge continuously upon approaching from below.
Despite the apparent ease of determining an analyte s concentration using the Nernst equation, several problems make this approach impractical. One problem is that standard-state potentials are temperature-dependent, and most values listed in reference tables are for a temperature of 25 °C. This difficulty can be overcome by maintaining the electrochemical cell at a temperature of 25 °C or by measuring the standard-state potential at the desired temperature. [Pg.470]

The temperature dependence of K is weU known experimentally. At a given temperature, if the composition of the gas is fixed, then equiUbrium carbon content is fixed. This composition is sometimes referred to as the carbon potential. [Pg.213]

The viscosity of solutions is quite temperature dependent increasing the temperature leads to a reduction in viscosity, which approaches zero at approximately 60°C (322). The viscosity is relatively stable from pH 3—10 and is compatible with a number of inorganic salts other than sodium. The production of succinoglycan and its potential use in foods and industrial processes as a thickening agent has been described (322). [Pg.301]

Hot surfaces and electric sparks are potential ignition sources for carbon disulfide. The ignition temperature depends on specific conditions, and values from 90 to 120°C in air have been reported (2,22). Data on carbon disulfide oxidation and combustion have been summarized (18). Oxidation products ate generally sulfur dioxide [7446-09-5] and carbon dioxide [124-58-9J ... [Pg.27]

Flammability. Since almost all ethers bum in air, an assessment of their potential ha2ards depends on flash points and ignition temperatures. The flash point of a Hquid is the lowest temperature at which vapors are given off in sufficient quantities for the vapor—air mixture above the surface of the... [Pg.426]

Reference electrode Me/Me" system Electrolyte Potential at 25°C (V) Temperature dependence (mV/°C) Application... [Pg.80]

In addition, the temperature dependence of the diffusion potentials and the temperature dependence of the reference electrode potential itself must be considered. Also, the temperature dependence of the solubility of metal salts is important in Eq. (2-29). For these reasons reference electrodes with constant salt concentration are sometimes preferred to those with saturated solutions. For practical reasons, reference electrodes are often situated outside the system under investigation at room temperature and connected with the medium via a salt bridge in which pressure and temperature differences can be neglected. This is the case for all data on potentials given in this handbook unless otherwise stated. [Pg.87]

In addition to the health hazards mentioned above, it is important be aware of the potential for explosions due to the Cannizzarro reaction ([77], pp. 36-37). When strong alkali is mixed with formaldehyde solutions, the Cannizzarro reaction will result in a rapid and spontaneous reaction even at relatively low temperatures. Depending on conditions, an induction period may be seen. The main organic products of this reaction are methanol and formic acid (salt form). In addition, significant amounts of hydrogen are evolved. The potential for explosions in closed containers is high, and even open containers will often erupt. [Pg.875]

Next come the dihedral angles (or torsions), and the contribution that each makes to the total intramolecular potential energy depends on the local symmetry. We distinguish between torsion where full internal rotation is chemically possible, and torsion where we would not normally expect full rotation. Full rotation about the C-C bond in ethane is normal behaviour at room temperature (although 1 have yet to tell you why), and the two CH3 groups would clearly need a threefold potential, such as... [Pg.40]

At each temperature one can determine the equilibrium lattice constant aQ for the minimum of F. This leads to the thermal expansion of the alloy lattice. At equilibrium the probability f(.p,6=0) of finding an atom away from the reference lattice point is of a Gaussian shape, as shown in Fig. 1. In Fig.2, we present the temperature dependence of lattice constants of pure 2D square and FCC crystals, calculated by the present continuous displacement treatment of CVM. One can see in Fig.2 that the lattice expansion coefficient of 2D lattice is much larger than that of FCC lattice, with the use of the identical Lennard-Lones (LJ) potential. It is understood that the close packing makes thermal expansion smaller. [Pg.54]


See other pages where Potential temperature dependence is mentioned: [Pg.443]    [Pg.511]    [Pg.1495]    [Pg.3214]    [Pg.741]    [Pg.1392]    [Pg.2714]    [Pg.443]    [Pg.511]    [Pg.1495]    [Pg.3214]    [Pg.741]    [Pg.1392]    [Pg.2714]    [Pg.148]    [Pg.639]    [Pg.423]    [Pg.508]    [Pg.509]    [Pg.566]    [Pg.1094]    [Pg.2419]    [Pg.207]    [Pg.299]    [Pg.473]    [Pg.467]    [Pg.467]    [Pg.455]    [Pg.411]    [Pg.405]    [Pg.323]    [Pg.200]    [Pg.396]    [Pg.372]    [Pg.133]    [Pg.734]    [Pg.192]    [Pg.129]    [Pg.477]    [Pg.752]    [Pg.211]   
See also in sourсe #XX -- [ Pg.98 , Pg.100 ]




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