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Product relative velocity

Hence the products relative velocity (i.e., Qi) has a component along the direction of the old bond. For a light atom attack (sin 1), that component can dominate so the products angular distribution reflects the distribution of the orientation of the old bond (with respect to the initial velocity) at the instant of... [Pg.406]

The 110(4 = ,/ = ) product, which is predominantly forward scattered, could be studied in Ml detail because the rotational angular momentum has such a small value. Its rotational angular momentum was found to lie preferentially perpendicular to the products relative velocity v, as is consistent with a late barrier meaning that the rotation of the products is determined as they separate, Figure 10.15. [Pg.418]

The product relative velocity is the difference between the velocities of the centers of mass of C and D. For example, the X component of the center-of-mass position and velocity of product D is given by... [Pg.400]

In the free-draining case sy/2 is also the relative velocity of the medium in the vicinity of a bead at a distance s from the center. Hence the frictional force acting on the bead is sy/2, and the rate of energy dissipation by the action of the bead is the product of the force and the velocity, or sy/2y. The total energy dissipated per unit time by the molecule will be given by the sum of such terms for each bead, or... [Pg.604]

To implement the Doppler-selected TOF measurement, the initial relative velocity is arranged to be parallel to the propagation vector of the probe laser. This critical configuration can readily be achieved in this rotating sources machine.36 Under this configuration, each Doppler-sliced 2D distribution exhibits a cylindrical symmetry The slit in front of the TOF spectrometer allows only those products with a rather small vx to be detected. Hence, only the -distribution, obtained by the TOF measurement, is needed to completely characterize the Doppler-sliced 2D (vx — vy) distribution. [Pg.6]

Fig. 24. YC3H4 and YCH2 product flux distributions from collisions of Y + propene at Boon = 12.3kcal/mol and 25.2 kcal/mol, respectively. Arrows represent the CM relative velocity vectors for the colliding reactants. Fig. 24. YC3H4 and YCH2 product flux distributions from collisions of Y + propene at Boon = 12.3kcal/mol and 25.2 kcal/mol, respectively. Arrows represent the CM relative velocity vectors for the colliding reactants.
It is to be expected that the equations relating electromagnetic fields and potentials to the charge current, should bear some resemblance to the Lorentz transformation. Stating that the equations for A and (j> are Lorentz invariant, means that they should have the same form for any observer, irrespective of relative velocity, as long as it s constant. This will be the case if the quantity (Ax, Ay, Az, i/c) = V is a Minkowski four-vector. Easiest would be to show that the dot product of V with another four-vector, e.g. the four-gradient, is Lorentz invariant, i.e. to show that... [Pg.151]

On the most basic level, since nuclear reactions result from collisions, the probability of formation of a given nuclear species depends on the target, the projectile and their relative velocity. Amongst all possible combinations involving as projectile either protons, neutrons or photons and as target any nucleus from hydrogen to uranium, what are the most productive reactions In fact they are simply the most probable ones. ... [Pg.69]

Boron particles are incorporated into GAP pyrolants in order to increase their specific impulse.[8-i2] xhe adiabatic flame temperature and specific impulse of GAP pyrolants are shown as a function of air-to-fuel ratio in Fig. 15.10 and Fig. 15.11, respectively. In the performance calculation, a mixture of the combustion products of the pyrolant with air is assumed as the reactant. The enthalpy of the air varies according to the velocity of the vehicle (or the relative velocity of the air) and the flight altitude. The flight conditions are assumed to be a velocity of Mach 2.0 at sea level. An air enthalpy of 218.2 kj kg is then assumed. [Pg.456]

In a typical modeling approach, the material removal rate is modeled as a function of easily controlled process parameters. The most basic model is one that predicts the bulk rate of material removal in a macroscopic fashion. An empirical observation by Preston is widely used, in which the rate of material thickness reduction is proportial to the product of (a) the relative velocity between the wafer and the polish pad and (b) the pressure on the surface of the wafer ... [Pg.91]

The reaction rate coefficients in the above equations may be related to reaction rates per pair of particles 2/, in nuclear physics (e.g., Fowler et al., 1975 Harris et al., 1983) by k = Xj/(1 + 5/ ), where 8 = 0 except for i= , for which 5/ = 1. That is, for Reactions 2-145 and 2-147 in which two identical particles collide to react, the definition of k is half of defined by nuclear physicists and for reactions in which different particles collide, the definition of k is the same as Xij. The reaction rate coefficients depend on temperature in a complicated way (Table 2-3) and may be calculated as the average value of the product of relative velocity times cross section. The concentrations of the intermediate species can be derived as follows. From Equation 2-155, 145 [ H] = ki4e[ H]pH]. That is. [Pg.152]

The instant at which combination of the combustion and shock waves begins is not necessarily the point at which the steady-state detonation velocity has been reached. Because of the turbulence generated by the flame, the velocity of the products relative to the initially forming detonation front may be subsonic. This state cannot last very long because rarefaction waves thru the burnt gas can move right up to the detonation wave and weaken it until its speed drops to unit Mach number relative to the products... [Pg.550]

This explains illumination and extinction but what of the colours To understand the production of colours We must consider the relative velocities of the two components X and Zj in the crystal. We have already seen that in a crystal of monammonium phosphate the refractive index for component 7j is greater than for component X tins means... [Pg.70]

Traces of hydrocarbons have been added to slowly reacting H2 + 02 mixtures in aged boric-acid-coated vessels at 480°-500°C. Measurements of hydrocarbon loss and H20 formation have enabled relative velocity constants for the attack of the radicals H, O, OH, and H02 on the additive to be assessed for CH,t and C2H6. With CHhy the results also show that CHS radicals react at almost equal rates with H2 and 02 at 500 mm. Hg pressure, and that the reaction with 02 appears to have both second- and third-order components. Detailed analyses of the reaction products obtained with ethane and neopentane enable the reactions of the radical produced in the primary attack to be elucidated, and mechanisms to account for the various products are given. [Pg.128]

Velocity Constants. Providing the reaction path is clear, relative velocity constants may be obtained by measuring relative rates of formation of products. Three illustrations will be given. [Pg.143]

Relatively, increasing the interface area, i.e.. enhancing the dispersal of a liquid or a solid, is a measure that can be employed widely, and, in fact, has been applied successfully in a number processes, such as spray drying and cooling etc. However, it is also limited to an extent. For example, spray drying can only be applied in the production of powdery products, and excessive dispersion may give rise to difficulties in powder collection etc while spray cooling is only applicable to the cases where moisture increase is permitted. On the other hand, in common equipment systems, the maximum relative velocity between phases is mostly just equal to the terminal velocity, which... [Pg.1]

That is, the Maxwell-Boltzmann distribution for the two molecules can be written as a product of two terms, where the terms are related to the relative motion and the center-of-mass motion, respectively. After substitution into Eq. (2.18) we can perform the integration over the center-of-mass velocity Vx. This gives the factor y/2iVksTjM (IZo eXP( —ax2)dx = sjnja) and, from the equation above, we obtain the probability distribution for the relative velocity, irrespective of the center-of-mass motion. [Pg.28]

Due to the simple product form of the Maxwell-Boltzmann distribution, the derivations given above are easily generalized to the expression for the relative velocity in three dimensions. Since the integrand in Eq. (2.18) (besides the Maxwell-Boltzmann distribution) depends only on the relative speed, we can simplify the expression in Eq. (2.18) further by integrating over the orientation of the relative velocity. This is done by introducing polar coordinates for the relative velocity. The full three-dimensional probability distribution for the relative speed is... [Pg.28]


See other pages where Product relative velocity is mentioned: [Pg.302]    [Pg.231]    [Pg.400]    [Pg.302]    [Pg.231]    [Pg.400]    [Pg.874]    [Pg.2060]    [Pg.2062]    [Pg.1883]    [Pg.995]    [Pg.223]    [Pg.376]    [Pg.84]    [Pg.3]    [Pg.4]    [Pg.231]    [Pg.353]    [Pg.31]    [Pg.165]    [Pg.207]    [Pg.242]    [Pg.103]    [Pg.65]    [Pg.47]    [Pg.91]    [Pg.581]    [Pg.47]    [Pg.592]    [Pg.202]    [Pg.235]    [Pg.128]    [Pg.306]    [Pg.325]   
See also in sourсe #XX -- [ Pg.400 ]




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Relative velocity

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