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Four-velocity

Pressure drop through the return ends of exchangers for any fluid is given as four velocity heads per tube pass ... [Pg.211]

The four-velocity u is defined as the rate of change of the position vector of a particle with respect to its proper time... [Pg.148]

In Fig. 2.8, the neutral curves for the above four velocity profiles of Fig. 2.7 are compared. The deciding trend is that as H increases, Rccr decreases. And for flows with > 0, the critical Reynolds numbers are significantly lower. [Pg.52]

There is no entirely satisfactory method for estimating these losses. Kern (1950) suggests adding four velocity heads per pass. Frank (1978) considers this to be too high, and recommends 2.5 velocity heads. Butterworth (1978) suggests 1.8. Lord et al. (1970) take the loss per pass as equivalent to a length of tube equal to 300 tube diameters for straight tubes, and 200 for U-tubes whereas Evans (1980) appears to add only 67 tube diameters per pass. [Pg.668]

Figure 3. The normalized electron four velocity distribution function downstream of the shock. The dot-dashed line is a power law fit to the non-thermal high energy tail, while the dashed curve is a Lorentz boosted thermal electron population. Figure 3. The normalized electron four velocity distribution function downstream of the shock. The dot-dashed line is a power law fit to the non-thermal high energy tail, while the dashed curve is a Lorentz boosted thermal electron population.
In principle, only four velocity measurements are required to obtain the four stiffness constants. However, to achieve higher accuracy we adopt the following procedure. First, the sample is set at ij/ = 0. Only the longitudinal wave is generated in the sample and its velocity Is related to by... [Pg.452]

For the discussion of the chaotic behavior statistical methods will be used. The relative cumulative frequency or the probability, respectively, is shown in Figure 7 for four velocity classes, see Table 3. From these data the relative frequency or probability density, respectively, is obtained, see Figure 8. It turns out that the frequency distribution is completely non-Gaussian, and the range characterizing the statistical dispersion is increasing with the relative velocity of the impact, while midrange point and mean value coincide fairly well, see Table 4. [Pg.145]

When projected onto a three-dimensional lattice, four velocities project onto each direction that is parallel to a cube edge, while there is a one-to-one relationship between the directions parallel to face diagonals in three dimensions and four dimensions. To account for the above degeneracy, let us introduce the weighting factor, which is equal to unity in four dimensions. In three dimensions, mi has the following values ... [Pg.254]


See other pages where Four-velocity is mentioned: [Pg.524]    [Pg.667]    [Pg.209]    [Pg.501]    [Pg.119]    [Pg.125]    [Pg.126]    [Pg.1179]    [Pg.247]    [Pg.501]    [Pg.517]    [Pg.829]    [Pg.375]    [Pg.376]    [Pg.22]    [Pg.1362]    [Pg.241]    [Pg.524]    [Pg.149]    [Pg.22]    [Pg.254]    [Pg.244]    [Pg.297]    [Pg.243]   
See also in sourсe #XX -- [ Pg.148 ]




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Velocity four-vector

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