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Thermal oscillations

As discussed in Sect. 6.2, the electronic states of a paramagnetic ion are determined by the spin Hamiltonian, (6.1). At finite temperamres, the crystal field is modulated because of thermal oscillations of the ligands. This results in spin-lattice relaxation, i.e. transitions between the electronic eigenstates induced by interactions between the ionic spin and the phonons [10, 11, 31, 32]. The spin-lattice relaxation frequency increases with increasing temperature because of the temperature dependence of the population of the phonon states. For high-spin Fe ", the coupling between the spin and the lattice is weak because of the spherical symmetry of the ground state. This... [Pg.211]

From Eq, (1) it is clear that a model of crystal polarization that is adequate for the description of the piezoelectric and pyroelectric properties of the P-phase of PVDF must include an accurate description of both the dipole moment of the repeat unit and the unit cell volume as functions of temperature and applied mechanical stress or strain. The dipole moment of the repeat unit includes contributions from the intrinsic polarity of chemical bonds (primarily carbon-fluorine) owing to differences in electron affinity, induced dipole moments owing to atomic and electronic polarizability, and attenuation owing to the thermal oscillations of the dipole. Previous modeling efforts have emphasized the importance of one more of these effects electronic polarizability based on continuum dielectric theory" or Lorentz field sums of dipole lattices" static, atomic level modeling of the intrinsic bond polarity" atomic level modeling of bond polarity and electronic and atomic polarizability in the absence of thermal motion. " The unit cell volume is responsive to the effects of temperature and stress and therefore requires a model based on an expression of the free energy of the crystal. [Pg.196]

The attenuation of die dipole of the repeat unit owing to thermal oscillations was modeled by treating the dipole moment as a simple harmonic oscillator tied to the motion of the repeat unit and characterized by the excitation of a single lattice mode, the mode, which describes the in-phase rotation of the repeat unit as a whole about the chain axis. This mode was shown to capture accurately the oscillatory dynamics of the net dipole moment itself, by comparison with short molecular dynamics simulations. The average amplitude is determined from the frequency of this single mode, which comes directly out of the CLD calculation ... [Pg.197]

The radii are so ohosen that their sums represent average internuclear distances for bonded atoms in molecules and crystals at room temperature. The atoms carry out thermal oscillations, which cause the internuclear distances to vary about their average values. At room temperature these are only slightly different from the values corresponding to the minima in the potential energy functions. [Pg.224]

Elements sensitive to piezoelectric thermal oscillation Pyroelectric sensors Black-body radiation sensors... [Pg.390]

It is important to know that this generally applied formula is connected with the vibration of two particles one creating the energy hyperplane, the other swinging in this plane or in an abstract sense two thermal oscillations superposed on one another. [Pg.10]

In Fig. 5 this probability is plotted for a free vibration (Gauss distribution) (a) for 2 coupled vibrations (Arrhenius formula) (b), for 4 vibrations (c) and for 6 vibrations (d). The picture will be completely changed, if we assume that only a share value 1/4 of the total energy of the thermal oscillations influences a special barrier process (b) in Fig. 6. Calculating the same for 6 oscillations superimposed on one another, we obtain curve (c) in Fig. 6. [Pg.12]

Because this kind of reaction takes place at low temperatures, thermal oscillations do not essentially contribute to backbone stretching. In fact, Ea is zero in this case. When Ea of bond scission is less than that required to form the active particles, cracking exhibits the character of a mechanically activated chemical reaction—chain scission in active particles takes place. There is a cause-and-effect relationship between the strain processes (which are cumulative in the deformed fragment to activate the backbone) and the destruction processes. [Pg.81]

The designers of SOFCs have to face the new developments posed by the circulators of Figures A.l and A.2. The letters SOFC denote a vigorous, diverse and expanding family of fuel cells based on the idea that at high temperature the thermal oscillations of the ions at the electrolyte/reactant/product interfaces lead to vigorous exchange... [Pg.34]

Lin Liu, H.T., (1993), Pressure Drop Type and Thermal Oscillations in Convective Boiling Systems, Ph.D. Thesis, University of Miami, Coral Gables, FL. [Pg.272]

S. Jensen, J.L. Olsen, H. Hansen, U.J. Quaade, Reaction rate enhancement of catalytic CO oxidation under forced thermal oscillations in microreactors with real time gas detection, in AIChE (Ed.), International Conference on Microreaction Technology (IMRET 8), Atlanta, 2005, p. 134h. [Pg.122]

Fig. 5.10.5 Three-omega technique the calculated normalized slope (d(AT)/d (log /)) of the thermal oscillation amplitude AT as a function of frequency/for a 100 nm thick aluminum heater element on a 500 nm thick Si02 layer and a 1 mm thick silicon substrate is shown as a function of thermal oscillation frequency/ With increasing frequency, the thermal wave penetrates deeper, allowing different sections of a (multilayered) sample to be scanned... Fig. 5.10.5 Three-omega technique the calculated normalized slope (d(AT)/d (log /)) of the thermal oscillation amplitude AT as a function of frequency/for a 100 nm thick aluminum heater element on a 500 nm thick Si02 layer and a 1 mm thick silicon substrate is shown as a function of thermal oscillation frequency/ With increasing frequency, the thermal wave penetrates deeper, allowing different sections of a (multilayered) sample to be scanned...
It has to be clearly understood, however, that the electronic excitation and the formation of the metal and halogen atoms are different processes. Thus temperature, which has little effect on the ultra-violet absorption spectrum of potassium bromide in a wider range (100-400°C) has a marked influence on the quantum efficiency of the reaction forming colour centres31 32. Thus at — 100°C no metal atoms are formed whereas at 400°C almost every quantum absorbed gives rise to a metal atom. The quantum efficiency at 0°C is J. This implies that the production of metal atoms is a secondary process, dependent on the thermal oscillations of the crystal lattice, which, however, has little or no effect on the primary process of electron excitation on absorption of light quanta. The reaction may therefore be represented as follows for the alkali halide, MX. [Pg.112]

If phase transitions occur in condensed phases, a nucleus is in contact with a large number of molecules in the initial metastable phase. In this case the lifetime of the critical nucleus is determined by the number of molecules present on its surface, Scr / b2 (b is the intermolecular distance), their oscillation frequency, vM, and the height of the potential energy barrier, U, that a molecule has to overcome in order to become attached to the nucleus surface. The frequency of thermal oscillations of molecules can be obtained from the expression vM = kT / h, where h is Planck s constant. The latter allows one to write the pre-exponential factor, J0, as... [Pg.293]

At high electrolyte concentrations the films become so thin that they loose ability to reflect light there are the so-called common black films. In addition to that, an increase in electrolyte concentration results in a decrease of the height of potential barrier which preserves the film in the state of this metastable equilibrium, i.e., film stability decreases. Thermal oscillations of interface, i.e., the Mandel shtam waves (See Chapter VI, 1), help the system to overcome a potential barrier. If other stabilizing factors are absent, such (local) overcoming of potential barrier results in film rupture. [Pg.550]

THERMAL OSCILLATION IN SIMPLE WALLS IN A STATE OF RESONANCE. [Pg.172]

Kanig " related ATg to the intermolecular interaction in polymer that was treated as a liquid saturated with holes. As the volume of holes, the free volume was estimated without considering a volume occupied by molecules at thermal oscillations. At temperatures... [Pg.222]

Dynamic Thermal oscillations Occur in film boiling -... [Pg.1133]

Dynamic instabilities are driven by the inertia of the system the stationary state is not sufficient to predict the destabilization threshold of theses instabilities such as acoustic waves, pressure drop oscillations, or thermal oscillations. [Pg.1133]

The thermal oscillation of a lattice is considered as the movement of an elastic body with the energy hv. This is known as a phonon. [Pg.520]


See other pages where Thermal oscillations is mentioned: [Pg.315]    [Pg.17]    [Pg.487]    [Pg.493]    [Pg.246]    [Pg.66]    [Pg.94]    [Pg.536]    [Pg.262]    [Pg.94]    [Pg.76]    [Pg.277]    [Pg.310]    [Pg.262]    [Pg.45]    [Pg.221]    [Pg.297]    [Pg.118]    [Pg.166]    [Pg.46]    [Pg.215]    [Pg.74]    [Pg.78]    [Pg.138]    [Pg.123]    [Pg.129]    [Pg.174]    [Pg.335]   
See also in sourсe #XX -- [ Pg.15 ]




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