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Shape of Waves

In confined chges the steady-state deton head should, in this model, be somewhat larger because confinement would lower at least the initial velocity of the release Waves from the side. The detonation-head development and its steady-state fotm in confined and unconfined chges are illustrated in Fig 5.1 of Ref 52, p 92 (which is also reproduced here) taking into account the spherical shape of wave front... [Pg.694]

Figure 5 illustrates an ultrasonic system. The waves are transmitted and impinge on the material under examination, returning to a receiver variations in the shape of waves received indicate the defects. [Pg.10]

A series of fundamental studies on sonochemistry by Feng Ruo and his collaborators has been undertaken over a number of years. Their studies have focused on how the parameters of an ultrasonic field, such as sound intensity, frequency, shape of wave, etc., affect the cavitation yield which was detected by different methods. [Pg.171]

The improvements in this method yield detection limits near 10 M, perhaps slightly lower than those of conventional polarography. Since tast measurements are only sampled-current presentations of conventional polarographic currents, all conclusions about the shapes of waves and all diagnostics developed for conventional measurements of maximum currents apply to the tast technique. [Pg.276]

KSUGRBAUER 1959). Said by AGRIPPA 1510 to be based on the shape of waves, though this is noc a water sign. The graphic form is also, rather roolishly, traced by certain modern astrologers to the idea of electric waves. ... [Pg.54]

Fig. 2.44 The classic shapes of waves, a Incident wave, b reflective wave, c wave of regular reflection d wave of Mach reflection... Fig. 2.44 The classic shapes of waves, a Incident wave, b reflective wave, c wave of regular reflection d wave of Mach reflection...
We saw in Section ILB that kinetic energy dominates bonding in. An analysis of kinetic energy allows us to make some general predictions about the shape of wave functions. [Pg.374]

Fig. 5. Saw-tooth shape of wave fronts due to mutual acceleration of crossing waves propagating in two weakly coupled sublayers (from [51]). Fig. 5. Saw-tooth shape of wave fronts due to mutual acceleration of crossing waves propagating in two weakly coupled sublayers (from [51]).
Spectral lines are fiirther broadened by collisions. To a first approximation, collisions can be drought of as just reducing the lifetime of the excited state. For example, collisions of molecules will connnonly change the rotational state. That will reduce the lifetime of a given state. Even if die state is not changed, the collision will cause a phase shift in the light wave being absorbed or emitted and that will have a similar effect. The line shapes of collisionally broadened lines are similar to the natural line shape of equation (B1.1.20) with a lifetime related to the mean time between collisions. The details will depend on the nature of the intemrolecular forces. We will not pursue the subject fiirther here. [Pg.1144]

Another class of instabilities that are driven by differences in the diffusion coefficients of the chemical species detennines the shapes of propagating chemical wave and flame fronts [65, 66]. [Pg.3069]

Singly, these functions provide a worse description of the wave function than the thawed ones described above. Not requiring the propagation of the width matrix is, however, a significant simplification, and it was hoped that collectively the frozen Gaussian functions provide a good description of the changing shape of the wave function by their relative motions. [Pg.275]

A basis set is a set of functions used to describe the shape of the orbitals in an atom. Molecular orbitals and entire wave functions are created by taking linear combinations of basis functions and angular functions. Most semiempirical methods use a predehned basis set. When ah initio or density functional theory calculations are done, a basis set must be specihed. Although it is possible to create a basis set from scratch, most calculations are done using existing basis sets. The type of calculation performed and basis set chosen are the two biggest factors in determining the accuracy of results. This chapter discusses these standard basis sets and how to choose an appropriate one. [Pg.78]

Section 1 1 A review of some fundamental knowledge about atoms and electrons leads to a discussion of wave functions, orbitals, and the electron con figurations of atoms Neutral atoms have as many electrons as the num ber of protons m the nucleus These electrons occupy orbitals m order of increasing energy with no more than two electrons m any one orbital The most frequently encountered atomic orbitals m this text are s orbitals (spherically symmetrical) and p orbitals ( dumbbell shaped)... [Pg.47]

For the charac terization of wave shape and breakthrough cui ves, three methods are popular. The MTZ method [Michaels, Jnd. E/ig. Chem., 44,1922 (1952)] measures the breadth of a wave between two chosen concentrations (e.g., cf = 0.05 and 0.95 or cf = 0.01 and 0.99). Outside of a laboratory, the measurement of full breakthrough cui ves is rare, so the breadth of the MTZ is often estimated from an independently determined stoichiometric capacity and a measured small... [Pg.1530]

For high feed loads, the shape of the diffuse traihng profile and the location of the leading front can be predicted from local equihbrium theory (see Fixed Bed Transitions ). This is illustrated in Fig. 16-35 for Tp = 0.4. For the diffuse profile (a simple wave ), Eq. (16-131) gives ... [Pg.1535]

Prediction of multicomponent uouhuear chromatography accounting for rate factors requires numerical solution (see Gniochou et al., gen. refs., and Numerical Methods and Characlerizatiou of Wave Shape in Fixed Bed Transitions ). [Pg.1536]

I7.I I). To analyse the shape of a current wave on a short-circuit, consider the following conditions that may occur at the instant of the fault ... [Pg.361]

Spark gap These have a pair of conducting rods with an adjustable gap, depending upon the spark over voltage of the arrester. Precise protection is not possible, as the spark-over voltage varies with polarity, steepness and the shape of the wave. These arresters are also now obsolete for the same reasons. [Pg.589]


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See also in sourсe #XX -- [ Pg.22 , Pg.24 , Pg.25 , Pg.42 , Pg.78 , Pg.232 ]




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