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Velocity normal

In order to relate the parameters of (4.5), the shock-wave equation of state, to the isentropie and isothermal finite strain equations of state (discussed in Section 4.3), it is useful to expand the shock velocity normalized by Cq into a series expansion (e.g., Ruoff, 1967 Jeanloz and Grover, 1988 Jeanloz, 1989). [Pg.80]

Figure 8.31. Fragment debris from high-velocity normal impact oflead projectile on lead plate at approximately 1.5 km/s. The high-speed photograph was taken approximately 200 /is after impact. A 1 cm interval grid indicates scale. Figure 8.31. Fragment debris from high-velocity normal impact oflead projectile on lead plate at approximately 1.5 km/s. The high-speed photograph was taken approximately 200 /is after impact. A 1 cm interval grid indicates scale.
The basically correct equation appears to be that of Giddings but, over the range of mobile phase velocities normally employed i.e., velocities in the neighborhood of the optimum velocity), the Van Deem ter equation is the simplest and most appropriate to use. [Pg.332]

Vapor space velocities normally should not exceed 100% of critical experience demonstrates that this keeps liquid entrainment into the flare line within acceptable limits. However, a velocity of 175% of critical is permitted when one is applyingthe 1.5 times Design Pressure Rule to remote contingencies,... [Pg.231]

Average fluid temperature Average velocity Normalized local velocity Streamwise velocity... [Pg.192]

Fig. 3.19 Schematic illustration of the measurement geometry for Mossbauer spectrometers. In transmission geometry, the absorber (sample) is between the nuclear source of 14.4 keV y-rays (normally Co/Rh) and the detector. The peaks are negative features and the absorber should be thin with respect to absorption of the y-rays to minimize nonlinear effects. In emission (backscatter) Mossbauer spectroscopy, the radiation source and detector are on the same side of the sample. The peaks are positive features, corresponding to recoilless emission of 14.4 keV y-rays and conversion X-rays and electrons. For both measurement geometries Mossbauer spectra are counts per channel as a function of the Doppler velocity (normally in units of mm s relative to the mid-point of the spectrum of a-Fe in the case of Fe Mossbauer spectroscopy). MIMOS II operates in backscattering geometry circle), but the internal reference channel works in transmission mode... Fig. 3.19 Schematic illustration of the measurement geometry for Mossbauer spectrometers. In transmission geometry, the absorber (sample) is between the nuclear source of 14.4 keV y-rays (normally Co/Rh) and the detector. The peaks are negative features and the absorber should be thin with respect to absorption of the y-rays to minimize nonlinear effects. In emission (backscatter) Mossbauer spectroscopy, the radiation source and detector are on the same side of the sample. The peaks are positive features, corresponding to recoilless emission of 14.4 keV y-rays and conversion X-rays and electrons. For both measurement geometries Mossbauer spectra are counts per channel as a function of the Doppler velocity (normally in units of mm s relative to the mid-point of the spectrum of a-Fe in the case of Fe Mossbauer spectroscopy). MIMOS II operates in backscattering geometry circle), but the internal reference channel works in transmission mode...
If the length scales associated with changes in velocity are normalized by Vv (characteristic length scale for Stokes flow), length scales associated with changes in curvature are normalized by Ss (typical striation thickness) and velocities normalized by V (a characteristic velocity), then the normal stress condition becomes,... [Pg.128]

Here V = (N Vj + N2S2) / N + N2) is the mean velocity of the pair of cells. By summing over the particles in cell 1 it is easy to verify that collision rule treats the particles in the two cells as groups that undergo elasticlike collisions. [Pg.137]

At an inflow boundary, the mean velocity vector will point into the flow domain. If we denote the component of the mean velocity normal to the inflow surface (Sin) by U n, then the total mass entering the system in time step At is34... [Pg.366]

The flame velocity—also called the burning velocity, normal combustion velocity, or laminar flame speed—is more precisely defined as the velocity at which unbumed gases move through the combustion wave in the direction normal to the wave surface. [Pg.153]

Vn mean velocity normal to the inter- rection of drop movement... [Pg.50]

Two alternative assumptions have been made for the manner in which the area variation occurs. The more realistic postulates that all elements of the surface remain in the surface throughout an oscillation cycle. Increasing surface area stretches the surface (A3, B5) and causes a velocity normal to the surface which increases the diffusion rate. For a surface of area Aq suddenly exposed at t = 0, the mass transfer product averaged over time is given by... [Pg.196]

In nonreacting, continuum fluid mechanics the fluid velocity normal to a solid wall is zero, which is a no-slip boundary condition. However, if there are chemical reactions at the wall, then the velocity can be nonzero. The so-called Stefan flow velocity occurs... [Pg.472]

Although the phenomena are not clearcut, partial settling out of solids from the gas stream and other instabilities may develop below certain linear velocities of the gas called choking velocities. Normal pneumatic transport of solids accordingly is conducted above such a calculated rate by a factor of 2 or more because the best correlations are not more accurate. Above choking velocities the process is called dilute phase transport and, below, dense phase transport. [Pg.119]

The time of return can itself be made the criterion of success, by forgetting about the B region and counting two consecutive crossings of S as independent transitions if and only if they are separated by a time interval greater than some characteristic time To, e.g. the autocorrelation time of the velocity normal to... [Pg.81]

Levich (L8, L9) has given an interesting treatment of fully turbulent film flow. In the absence of a flowing gas stream at the interface, Levich deduced that the scale of turbulence and the turbulent velocity normal to the interface must be proportional to the distance from the interface, so that all turbulent pulsations must disappear at the interface itself, leaving there a nonturbulent layer of thickness... [Pg.170]

This concentration is considerably lower than 330 pg C/L, the sum of all monomers in Figure 2. However, there are several caveats to consider. First, not all monomers can be expected to have the same lability as glucose, and, in fact, Figure 4 shows that at the velocities normal for White Clay... [Pg.111]

Prandtl velocity ratio t>+ V velocity normalized by friction velocity Turbulent flow near a wall, friction... [Pg.51]

The geometric factor in Eq. (5.44) is seen to be equal to one with this choice of dividing surface, and the velocity normal to the surface is... [Pg.120]


See other pages where Velocity normal is mentioned: [Pg.577]    [Pg.109]    [Pg.117]    [Pg.676]    [Pg.251]    [Pg.172]    [Pg.274]    [Pg.172]    [Pg.351]    [Pg.356]    [Pg.58]    [Pg.31]    [Pg.52]    [Pg.66]    [Pg.106]    [Pg.205]    [Pg.83]    [Pg.246]    [Pg.24]    [Pg.142]    [Pg.279]    [Pg.107]    [Pg.313]    [Pg.112]    [Pg.134]    [Pg.109]    [Pg.117]    [Pg.179]    [Pg.177]    [Pg.232]   
See also in sourсe #XX -- [ Pg.200 ]




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