Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Inelastic collisions temperature dependence

Figure 19. Temperature dependence of inelastic collision integral for attractive limb of Lennard-... Figure 19. Temperature dependence of inelastic collision integral for attractive limb of Lennard-...
The temperature instability of a two-dimensional reactive fluid of N hard disks bounded by heat conducting walls has been studied by molecular dynamics simulation. The collision of two hard disks is either elastic or inelastic (exothermic reaction), depending on whether the relative kinetic energy at impact exceeds a prescribed activation barrier. Heat removal is accomplished by using a wall boundary condition involving diffuse and specular reflection of the incident particles. Critical conditions for ignition have been obtained and the observations compared with continuum theory results. Other quantities which can be studied include temperature profiles, ignition times, and the effects of local fluctuations. [Pg.159]

At equilibrium, where the yelocity distribution is Maxwellian, it is straightforward to show that < > = 4 J p/7T, where 0p is the granular temperature. We should note that Eq. (6.109) corresponds to an inelastic Maxwell particle (Maxwell, 1879), and, most importantly, it still contains the exact dependence on tu = (1 + e)/2. We will therefore refer to this kinetic model as the inelastic Maxwell collision model. [Pg.247]

Specified electron energy distribution function The EEDF is specified, normally assumed Maxwellian (Eq. 9). The electron energy balance (Eq. 31) is solved assuming an adiabatic condition for electron temperature at the wall. The Maxwellian assumption is very common in the literature [100, 125, 126, 130, 133, 135-137]. Measured EEDFs in ICPs, however, have a Maxwellian bulk (due to electron-electron collisions), and a depleted tail due to inelastic losses and escape of fast electrons to the walls. Thus a bi-Maxwellian distribution may be more appropriate [154]. A Maxwellian distribution is not expected to have a great effect on ion densities since the ionization rate is self-adjusted to balance the loss rate of ions to the walls and the latter depends only very weakly on the EEDF. The good agreement with experimental data [101, 130, 148, 152] is an indirect evidence that the Maxwellian EEDF is reasonable for obtaining species densities and their distributions. Other forms of... [Pg.290]

Just as for gas-phase molecular collisions, gas-surface encounters can be elastic, inelastic, or reactive in nature. A wide range of scattering behavior is observed depending upon the gas molecules, the composition, structure, and temperature... [Pg.477]


See other pages where Inelastic collisions temperature dependence is mentioned: [Pg.194]    [Pg.204]    [Pg.194]    [Pg.15]    [Pg.147]    [Pg.47]    [Pg.69]    [Pg.505]    [Pg.66]    [Pg.43]    [Pg.45]    [Pg.261]    [Pg.115]    [Pg.258]    [Pg.72]    [Pg.76]    [Pg.137]    [Pg.163]    [Pg.133]    [Pg.516]    [Pg.529]    [Pg.539]    [Pg.660]    [Pg.578]    [Pg.26]    [Pg.241]    [Pg.506]    [Pg.5]    [Pg.438]    [Pg.487]    [Pg.747]    [Pg.323]    [Pg.540]   
See also in sourсe #XX -- [ Pg.375 ]




SEARCH



Collision inelastic

Collision temperature

Inelastic

Inelasticity

© 2024 chempedia.info