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Displacement normal

Clearance is the volume remaining in a cylinder end when the piston is at the end of its stroke. This is die sum of the volume between the head of the cylinder and the piston, and the volume under tlie valve seats. The total clearance is expressed in percent of the total piston displacement, normally between 4 and 30%. [Pg.305]

In most transition metal and organometallic compounds, many modes are displaced. In the case of many displaced normal modes, the total overlap is... [Pg.177]

This expression for the complete overlap is Fourier transformed to give the electronic emission spectrum. In order to carry out the calculation it is necessary to know the frequencies and the displacements for all of the displaced normal modes. In addition, the energy difference between the minima of the two potential surfaces E0 and the damping r must be known. As will be discussed below, the frequencies and displacements can be experimentally determined from pre-resonance Raman spectroscopy, and the energy difference between the ground and excited states and the damping can be obtained from the electronic absorption spectrum and/or emission spectrum. [Pg.43]

The vector R in Eq. (5.21) describes the displacements normal to the slip plane of the dislocation. These displacements cause a buckling of the reflecting plane, which is the origin of the contrast. A plane that is parallel to the slip plane is the most severely buckled, and thus the contrast is greatest if this plane is the reflecting plane. For these conditions, g is... [Pg.151]

W(CO)s(pyridine) [3]. Which displaced normal modes contribute to the... [Pg.202]

We conclude with a final example of a spectroscopic feature which is caused by distortions in more than one mode and which is readily explained from the time-dependent point of view. This feature is a repetitive pattern of vibronic bands in emission or absorption spectra consisting of clusters of bands. The energy separations between the components of the clusters are the energy differences between displaced normal modes. A good example is provided by the emission spectrum of ruthenocene (Figure 19). The explanation of these features lies in the modulation or beat in the time-dependent overlap. [Pg.208]

We begin with a case considered by Griffiths Campbell (1991) where the blob is inviscid and all the resistance to flow is within the displaced normal mantle. We modify their derivation to aid comparison with lubrication theory results. [Pg.148]

UFAD systems have the potential to produce better indoor air quality in buildings during normal operation (Bauman, 2003), but they could be more vulnerable to indoor biological and chemical attacks than conventional ducted air distribution systems. One of the claimed advantages of UFAD is that it supplies clean air to displace normal indoor contaminants (such as bioeffluent and emissions of... [Pg.40]

One striking feature of the conformation of isolated tails is that the spatial extension of the chain is expanded in a direction normal to the interface whilst being unaffected parallel to the interface. This is illustrated by Figs 4.8 and 4.9. These show that for poly(methylene) the mean square displacement normal to the interface for high molecular weight polymers asymptotes in value to twice that for chains in free solution. This result was first derived by DiMarzio and McCrackin (1965) for a 1-D random walk normal to an impenetrable interface. The doubling of the mean square displacement can be understood in terms of the halving of the available space normal to the interface by the presence of the impenetrable barrier. The components of the mean square displacement parallel to the interface are unaffected by its presence. [Pg.77]

Based on this analysis, the energy release rates can be partitioned into the energy release rates associated with crack opening displacement (Gj) and shear displacement normal to the crack surface (Gn) ... [Pg.248]

A model that invokes the concept of cooperative behavior and simultaneously incorporates to some extent membrane structure has been formulated by Grodsky. This model is based upon a type of lattice statistics formulation in which the polar head groups of membrane lipid moieties occupy one set of lattice sites, and displaced normal to the plane... [Pg.295]

Is there really some displacement The term displacement, normally meaning a change of position in space, is strangely borrowed from translational mechanics by analogy between the work of a force equal to its strength multiplied by the displacement (distance) F.d and the work of electric volume forces equal to E.dD. [Pg.220]

The highly elastic material region of the displacement amplifier in Fig. 6.19a is locally concentrated, while the designs in Fig. 6.19b and c make use of the global elastic behaviour of metallic materials. The so-called moonie transducer in Fig. 6.19b consists of a piezoelectric disk sandwiched between two metal end caps. The ceramic is poled in the thickness direction and uses the dai mode. In this way the small radial displacement of the disk is transformed into a much longer axial displacement normal to the surface of the... [Pg.114]

Figure 17.2.2 Dependence of tip current (normalized to on relative tip displacement (normalized to tip radius) over a conductive n-TiOj substrate (Eg = -0.7 V vs. SCE), curve 1, and an insulating n-TiOj substrate (Eg = 0.0 V vs. SCE), curve 2, in a solution containing 2 mM Cp2FeTMA+ and 1.0 M NaN03. The tip was biased at 0.60 V vs. SCE. The tip moved to the substrate surface at a rate of 38 A/sec. Solid curves are experimental data and symbols are theory. Squares Simulated data for conducting substrate pluses calculated data based on equation 17.2.4 triangles simulated data for insulating substrate. Fitting parameters = 45 nm, (, = 67 nm, I = 28 nm, and D = 5.0 X 10 cmVsec. Experimental i.j. is equal to 9.0 pA. Adapted with permission from reference (8). Figure 17.2.2 Dependence of tip current (normalized to on relative tip displacement (normalized to tip radius) over a conductive n-TiOj substrate (Eg = -0.7 V vs. SCE), curve 1, and an insulating n-TiOj substrate (Eg = 0.0 V vs. SCE), curve 2, in a solution containing 2 mM Cp2FeTMA+ and 1.0 M NaN03. The tip was biased at 0.60 V vs. SCE. The tip moved to the substrate surface at a rate of 38 A/sec. Solid curves are experimental data and symbols are theory. Squares Simulated data for conducting substrate pluses calculated data based on equation 17.2.4 triangles simulated data for insulating substrate. Fitting parameters = 45 nm, (, = 67 nm, I = 28 nm, and D = 5.0 X 10 cmVsec. Experimental i.j. is equal to 9.0 pA. Adapted with permission from reference (8).
Its value is crucial, because the magnitude and characteristics of mean-squared displacement (normal vs. anomalous diffusion) are sensitive functions of (A ). Regrettably, several practitioners of this method omit (A ) values from their publications. Arizzi [93] noted that an analytic form is available from the X-ray scattering literature [148],... [Pg.449]


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See also in sourсe #XX -- [ Pg.59 , Pg.79 , Pg.82 , Pg.85 , Pg.99 , Pg.174 ]




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Internal displacement coordinate normal coordinates

Normal internal displacement coordinates

Normal phase displacement model

Normal-mode displacements

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