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AT vibrations

Rao et al. (R5) and Raju et al. (R2) also investigated mass transfer at vibrating electrodes for low vibration frequencies (higher frequencies would cause cavitation). Mass transfer follows a laminar-type correlation both for a transverse vibration of a vertical cylinder and for a vertical plate vibrating parallel to the face. In the case of the plate, the Reynolds number is based on width, indicating the predominance of form drag. When vibrations take place perpendicular to the thickness, skin friction predominates and the Reynolds number is then preferably based on the equivalent diameter (total surface area divided by transverse perimeter). [Pg.273]

The potential energy curves of the species AB, AB+, and AB- are used in figure 4.1 to summarize the definitions of the adiabatic ionization energy and electron affinity of AB. Note that the arrows start and end at vibrational ground states (vibrational quantum number v = 0). [Pg.49]

As a consequence of the extremely high mass transport rates attainable at UMEs, HM effects at vibrating UMEs are normally small. However when the electrode is in close proximity to a surface these effects can be greatly enhanced. Although the modulation of the signal is not hydrodyn-... [Pg.404]

The use of a surface selection rule in infrared spectroscopy and in EELS has been widespread and has yielded much valuable information on surface orientation of adsorbed species. The rule is a very simple one for adsorbates at metal surfaces, only vibrational modes which modulate a component of the molecular dipole perpendicular to the surface are active in these spectroscopies. This rule arises from the fact that metals have high electrical conductivities at vibrational mode frequencies and this results in the parallel (but not the perpendicular) component of the radiation field going to zero at the surface. [Pg.99]

Much work, both experimental and theoretical, has been carried out on the radiationless transitions of collision-free Si benzene. At vibrational energies greater than about 3000cm"1, both the quantum yield [58] and lifetime [59] of fluorescence and the quantum yield of S, - TISC [60-62] decrease dramatically relative to those at lower excess energies. Concomitantly, the Al9(S0) absorption system exhibits a sudden... [Pg.202]

It is seen that the S vector is oriented in the direction in which a given displacement of the ith atom will produce the greatest increase in Aror Aa. Formulas for obtaining the S vectors of other internal coordinates such as those of out-of-plane (A0) and torsional (At) vibrations are also available [3]. [Pg.63]

It seems well established that the vibrational relaxation in small molecules is correctly described by the SSH model assuming the dominant role of repulsive interactions. The mechanisms of the vibrational relaxation in medium-size molecules is certainly more complex and not completely elucidated. Recent studies carried out in the low-pressure range (one collision per lifetime) indicate that collisions may lead to highly selective transitions to some specific vibronic states these propensity rules cannot be explained by simple consideration of (energy) and At> (vibrational quantum number) changes (as in the SSH model) but are related to some dynamical properties of vibrational modes ... [Pg.347]

Here Xe is the coefficient of anharmonicity and B is the normalizing factor. Comparison of the parabolic-exponential Treanor distribution with the linear-exponential Boltzmann distribution is illustrated in Fig. 3-3. A population of highly vibrationally excited levels at TV > To can be many orders of magnitude higher than that predicted by the Boltzmaim distribution even at vibrational temperature. The Treanor distribntion resnlts in very high rates and energy efficiencies of chemical reactions stimulated by vibrational excitation in plasma. [Pg.99]

Figure 3-8. Non-equilibrium vibrational distributions in nitrogen at vibrational temperature Ty = 3000 K and dilFerent translational temperatures = 1 indicates vibrational energy when VV- and VT-relaxation rates are equal. Figure 3-8. Non-equilibrium vibrational distributions in nitrogen at vibrational temperature Ty = 3000 K and dilFerent translational temperatures = 1 indicates vibrational energy when VV- and VT-relaxation rates are equal.
Ad 5.1 eV/mol is the H2O dissociation energy. The total chain reaction rate obviously depends on the chain length, which can be numerically estimated as v >= 100 at vibrational temperature 7(, = 0.5 eV and water vapor density [H2O] = 3 10 cm . The total chain reaction rate can be calculated by taking into account both the chain initiation rate (5-115) and the chain length as follows ... [Pg.320]

The C2 radical is produced by multiple-photon dissociation of CF3CCCF3 at 193 nm. Approximately 20 torr of helium is used to translationally and rotationally equilibrate the C2 with the bath gas. The dissociation produces both C2 and C2 and a significant amount of the C2 is vibrationally excited. Our experiments indicate that at these pressures helium is not effective at vibrationally quenching the C2, although the rapid rotational thermalization is clearly evident. For measurements of the reaction rates of C2, 1 2 mtorr of CF3CCCF3 is used with 20 torr of 99.99% helium and 0-0.8 torr of 99.99% O2. [Pg.259]

The radiation from the infrared region is able to promote transitions at vibrational level. The infrared spectroscopy is used to acquire information about the nature of the functional groups present in a molecule. The infrared region is conventionally divided into three sub-regions near (750-2500 nm), medium (2500-50000 nm) and far infrared (50-1000 pm). [Pg.219]

If pad materials and shims were used to help reduce vibration and level the machine, the pads and shims should be replaced each time the machine is releveled. Some pads absorb cutting and lubricating fluids, reducing their effectiveness at vibration control, and compress over time when under load. The elevation and level of the machine may change even if the floor or foundation does not settle, requiring that the pads be replaced and the leveling process be repeated. [Pg.613]

Gomaa, H., Al Taweel, A.M. and Landau, J. (2004). Mass transfer enhancement at vibrating electrodes. Chemical Engineering Journal, Vol. 97, pp. 141-149. [Pg.75]

Small-grained specimens (0.019 mm mean diam) were tested at vibration frequencies of 0.5 Hz an 1 Hz, while the large-grained specimen was tested at 0.5 Hz. [Pg.88]

Applying vibration, the handling and storage of fine powders can be promoted. That is illustrated below by means of the critical uniaxial compressive strength Oc.crit, compare Fig., and consequently the minimum outlet diameter to avoid bridging in a mass-flow hopper b,nin, Fig.. The critical outlet diameter bmin decreases v/ith increasing vibration velocity, for example, the conical outlet width is still reduced from 0.85 m to about 0.3 m. Nevertheless, at vibration velocities with more than 10 mm/s bmin remains more or less constant. [Pg.54]

Figure 2. Loci combined by two vectors at vibrated on x plane and on y plane, (a) In the ease that the phase shift between the two vectors is zero, and (b) the phase shift is (jt/2)... Figure 2. Loci combined by two vectors at vibrated on x plane and on y plane, (a) In the ease that the phase shift between the two vectors is zero, and (b) the phase shift is (jt/2)...
Nevertheless, things are even more complicated. It has been shown [50,51] that the analytic critical point (ACP - maximum, minimum or saddle point of dispersion, in case of MgB2 it is maximum) of the o band at F point crosses Fermi level (FL) at vibration displacement 0.016A°/B-atom, i.e. with amplitude 0.032A°, which is smaller than root-mean square (rms) displacement ( 0.036A°) for zero-point vibration energy in Egg mode. Thus, in vibrations when ACP approaches FL for... [Pg.485]


See other pages where AT vibrations is mentioned: [Pg.357]    [Pg.364]    [Pg.83]    [Pg.197]    [Pg.398]    [Pg.109]    [Pg.23]    [Pg.129]    [Pg.75]    [Pg.76]    [Pg.14]    [Pg.289]    [Pg.85]    [Pg.167]    [Pg.169]    [Pg.217]    [Pg.118]    [Pg.312]    [Pg.368]    [Pg.782]    [Pg.784]    [Pg.110]    [Pg.254]    [Pg.451]    [Pg.456]    [Pg.271]    [Pg.259]    [Pg.809]    [Pg.398]    [Pg.241]    [Pg.33]   
See also in sourсe #XX -- [ Pg.257 ]




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