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Energy distribution method

Other variations on these basic free energy methods have been published, although for various reasons they have not yet been widely adopted. These methods include MD/MC methods,38 the acceptance ratio method,39, 40 the weighted histogram method,41 the particle insertion method,42 43 and the energy distribution method.39 The reader is referred to the original publications for additional discussion of these approaches. [Pg.15]

Figure 1. Test of site energy distribution method... Figure 1. Test of site energy distribution method...
Other approaches, such as the particle insertion method and the energy distribution method, have been described, but their application has been as yet relatively limited. [Pg.1041]

Although modem laser teelmiques ean in prineiple aehieve mueh narrower energy distributions, optieal exeitation is frequently not a viable method for the preparation of exeited reaetive speeies. Therefore ehemieal aetivation—often eombined with (laser-) flash photolysis—still plays an important role in gas-phase kmeties, in partieular of unstable speeies sueh as radieals [ ]. Chemieal aetivation also plays an important role in energy-transfer studies (see chapter A3.13). [Pg.2138]

One of the drawbacks of the multicanonical method is that, during the simulations tc derive the weight factor, the energy distribution in H(E) can oscillate rather than steadilj approaching a limiting distribution. Another drawback is that it can fail to properlj... [Pg.453]

Control of sonochemical reactions is subject to the same limitation that any thermal process has the Boltzmann energy distribution means that the energy per individual molecule wiU vary widely. One does have easy control, however, over the energetics of cavitation through the parameters of acoustic intensity, temperature, ambient gas, and solvent choice. The thermal conductivity of the ambient gas (eg, a variable He/Ar atmosphere) and the overaU solvent vapor pressure provide easy methods for the experimental control of the peak temperatures generated during the cavitational coUapse. [Pg.262]

PP2- However, there is an alternative theoretical mechanism by which the two Ps could be emitted without any neutriao, denoted PPq- The experimental methods that are used to look for the double P decay mode are often more sensitive to one of these decay modes than the other. The difference ia the expected energy distribution of the electrons is clear from the fact that ia the first case the total decay energy is divided between four particles, including the two antineutfinos that caimot be observed ia the second, it is only divided between the two electrons. As more exotic modes of decay are measured and even larger limits are placed on some of the half-fives, the constraints on theory become even stronger. [Pg.453]

In rooms where energy is introduced primarily by supply air jets, air distribution methods are referred to as mixing type. With a perfect mixing-type air distribution, airflow pattern and air velocity at any point in the room are... [Pg.434]

C. Topp, and P. Heiselberg, Obstacles—an energy-efficient method to reduce downdraught from glazed surfaces, in Proceedings of the Fifth International Conference on Air Distribution in Spaces, Spacevent 96 Yokohama, japan 1996. [Pg.640]

A sound is generally not a pure tone, as the latter is only emitted from particular sources. It can be demonstrated that a sound can be divided into different pure tones (superposition method). The waves at different frequencies give the spectrum of the sound, which also describes its energy distribution. In frequency analysis, the spectrum is divided into octave bands. An octave band is defined as the frequency range with its upper boundary twice the frequency of its lower boundary. For every octave band, a central band frequency ( f. ) is defined as follows ... [Pg.793]

Several numerical procedures for EADF evaluation have also been proposed. Morrison and Ross [19] developed the so-called CAEDMON (Computed Adsorption Energy Distribution in the Monolayer) method. Adamson and Ling [20] proposed an iterative approximation that needs no a priori assumptions. Later, House and Jaycock [21] improved that method and proposed the so-called HILDA (Heterogeneity Investigation at Loughborough by a Distribution Analysis) algorithm. Stanley et al. [22,23] presented two regularization methods as well as the method of expectation maximalization. [Pg.247]

The major mechanism of a vapor cloud explosion, the feedback in the interaction of combustion, flow, and turbulence, can be readily found in this mathematical model. The combustion rate, which is primarily determined by the turbulence properties, is a source term in the conservation equation for the fuel-mass fraction. The attendant energy release results in a distribution of internal energy which is described by the equation for conservation of energy. This internal energy distribution is translated into a pressure field which drives the flow field through momentum equations. The flow field acts as source term in the turbulence model, which results in a turbulent-flow structure. Finally, the turbulence properties, together with the composition, determine the rate of combustion. This completes the circle, the feedback in the process of turbulent, premixed combustion in gas explosions. The set of equations has been solved with various numerical methods e.g., SIMPLE (Patankar 1980) SOLA-ICE (Cloutman et al. 1976). [Pg.111]

The combined experimental and theoretical investigation of Dixon et al. [75] applied the H-atom Rydberg time-of-flight method to measure the translational energy distribution of H atoms from the photodissociation... [Pg.257]

In silane discharges several ions are observed to be involved in a charge exchange process, and therefore maxima in their ion energy distribution at distinct energies are observed. The charge carrier density and the plasma potential that result from the fit of the lED allow for the quantification of the related parameters sheath thickness and ion flux. This method has been be used to relate the material quality of a-Si H to the ion bombardment [301. 332] see also Section 1.6.2.3. [Pg.97]

It has been shown that the potential energy distribution provides an approximate method to evaluate the relative contribution of each symmetry coordinate to a given normal mode of vibration. From the definition of the symmetry coordinates, the relation... [Pg.333]

Luntz and co-workers have recently carried out an impressive study that follows in the spirit of the Eley-Rideal work.44 Specifically, laser-assisted recombination of N-atoms desorbing to form gas-phase N2 on Ru(0001) was investigated. Experimental measurements of state-selectively detected N2 recoiling from the surface recombination event were obtained using resonance enhanced multiphoton ionization and ion time-of-flight methods. In this way translational energy distributions of individual rovibrational states could be obtained experimentally. In addition, N2-vibrational population distributions could be derived. [Pg.393]


See other pages where Energy distribution method is mentioned: [Pg.14]    [Pg.14]    [Pg.657]    [Pg.659]    [Pg.872]    [Pg.873]    [Pg.1331]    [Pg.2138]    [Pg.2382]    [Pg.345]    [Pg.45]    [Pg.397]    [Pg.111]    [Pg.246]    [Pg.251]    [Pg.253]    [Pg.260]    [Pg.182]    [Pg.331]    [Pg.246]    [Pg.74]    [Pg.124]    [Pg.15]    [Pg.358]    [Pg.2]    [Pg.104]    [Pg.114]    [Pg.150]    [Pg.164]    [Pg.210]    [Pg.475]    [Pg.480]    [Pg.495]    [Pg.505]   
See also in sourсe #XX -- [ Pg.14 ]

See also in sourсe #XX -- [ Pg.14 ]




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