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Boundary conditions reflective

Let us discuss the four main types of boundary conditions reflecting, absorbing, periodic, and the so-called natural boundary conditions that are much more widely used than others, especially for computer simulations. [Pg.363]

The standard boundary conditions reflect weakening of the correlations at large relative distances (oo,t) = Y(oo, t) = 1. We impose also the Smoluchowski boundary condition,... [Pg.247]

This boundary condition reflects the fact that the Jones vector will by unchanged by passage through an element of zero thickness. In reference 7, Jones was able to show that the solution to (2.44) is ... [Pg.33]

Boundary conditions on the surface of the k -th sphere at rk = ak can be formulated in different ways. We consider the case when the densities of surface charges are adjusted. The boundary conditions reflect a continuity of potentials and electric inductions on the surfaces of spheres, so we have... [Pg.115]

For fully developed electro osmotic flow in parallel plate micro channel the streamwise momentum equation [19] and boundary conditions reflecting no slip at the wall and no shear stress at the center are ... [Pg.54]

The UME response during the SECM chronoamperometric experiment is calculated by solving Eq. (1) with respect to the boundary conditions defining the processes occurring at the electrode and substrate. The initial conditions and boundary conditions are as previously stated in Eqs. (6)-(10), except C now corresponds to the normalized concentration of Cu2+. The substrate boundary condition, reflecting the dissolution rate law is ... [Pg.539]

The final boundary condition reflects symmetry of the concentration gradient between adjacent fibers and both ends of the Krough cylinder (Ye et al., 2006). [Pg.417]

Solution of Eq. (144) yields only the dimensionless axial velocity pf/(< ) = w(i)IB, which is analogous to Eq. (133). The boundary conditions reflecting no-slip at the feed tube and rotor wall are... [Pg.151]

The boundary conditions reflecting the existence of only one neighbor segment at the chain ends are... [Pg.25]

At the end of the collision (t +co) one expects to see part of the wavepacket moving to the right for v oo (tlie transmitted part) and part of it moving to the left for v -oo (the reflected part). Both this and the t -qo boundary condition can be satisfied by requiring that... [Pg.961]

Periodic boundary conditions can also be used to simulate solid state con dition s although TlyperChem has few specific tools to assist in setting up specific crystal symmetry space groups. The group operation s In vert, Reflect, and Rotate can, however, be used to set up a unit cell manually, provided it is rectangular. [Pg.201]

For some simulations it is inappropriate to use standard periodic boundary conditions in all directions. For example, when studying the adsorption of molecules onto a surface, it is clearly inappropriate to use the usual periodic boundary conditions for motion perpendicular to the surface. Rather, the surface is modelled as a true boundary, for example by e, plicitly including the atoms in the surface. The opposite side of the box must still be treated when a molecule strays out of the top side of the box it is reflected back into the simulation cell, as indicated in Figure 6.6. Usual periodic boundary conditions apply to motion parallel to the surface. [Pg.333]

T is often referred to as the drawdown time to reflect that it is the time requited to empty the contents from the crystallizer if the feed is set to zero. Equation 43 can be integrated using the boundary condition n = at L = 0 ... [Pg.349]

This has also commonly heen termed direct interception and in conventional analysis would constitute a physical boundary condition path induced hy action of other forces. By itself it reflects deposition that might result with a hyj)othetical particle having finite size hut no fThis parameter is an alternative to N f, N i, or and is useful as a measure of the interactive effect of one of these on the other two. Schmidt numher. [Pg.1583]

T he total or global solar radiation has a direct part (beam radiation) and a diffuse part (Fig. 11.31). In the simulation, solar radiation input values must be converted to radiation values for each surface of the building. For nonhorizontal surfaces, the diffuse radiation is composed of (a) the contribution from the diffuse sky and (b) reflections from the ground. The diffuse sky radiation is not uniform. It is composed of three parts, referred to as isotropic, circumsolar, and horizontal brightening. Several diffuse sky models are available. Depending on the model used, discrepancies for the boundary conditions may occur with the same basic set of solar radiation data, thus leading to differences in the simulation results. [Pg.1065]

The analysis of the behavior of the fluid temperature and the Nusselt number performed for a circular tube at the thermal wall boundary condition 7(v = const, also reflects general features of heat transfer in micro-channels of other geometries. [Pg.168]

Reflective symmetry boundary conditions are specified at the sides of the sample as... [Pg.303]

Particles are moved along their current velocity vectors without undergoing interactions for a time At which is chosen smaller than the mean collision time. If a particle hits the domain boundary, its velocity vector is modified according to the corresponding boundary condition (for example specular or diffuse reflection if a particle hits a wall) ... [Pg.133]

The solution of this problem, as given by Eq. (66), must now be analyzed with consideration of the boundary conditions- at x = 0 and x = . At these two points the potential function, V(jc), becomes infinite. Therefore, for the product V(x) i (x) in Eq. (64) to remain finite at these two points, the wavefimction rfr(x) must vanish. Clearly, if rj, which is one of the arbitrary constants of integration, is chosen equal to zero in Eq. (66), the wavefunc-tion will vanish at X = 0. However, at jc = i the situation is somewhat more complicated. A little reflection will show that if the argument of the sine... [Pg.264]

Reflecting Boundary. The reflecting boundary may be represented as an infinitely high potential wall. Use of the reflecting boundary assumes that there is no probability current behind the boundary. Mathematically, the reflecting boundary condition is written as... [Pg.364]

Natural Boundary Conditions. If the Markov process is considered in infinite interval, then boundary conditions at oo are called natural. There are two possible situations. If the considered potential at +oo or —oo tends to —oo (infinitely deep potential well), then the absorbing boundary should be supposed at Too or —oo, respectively. If, however, the considered potential at Too or — oo tends to Too, then it is natural to suppose the reflecting boundary at Too or —oo, respectively. [Pg.365]

Integrating Eq. (3.16) and taking into account the reflecting boundary conditions (probability current is equal to zero at the points d), we get... [Pg.370]


See other pages where Boundary conditions reflective is mentioned: [Pg.131]    [Pg.234]    [Pg.256]    [Pg.280]    [Pg.206]    [Pg.131]    [Pg.234]    [Pg.256]    [Pg.280]    [Pg.206]    [Pg.128]    [Pg.400]    [Pg.844]    [Pg.1880]    [Pg.1881]    [Pg.2298]    [Pg.2866]    [Pg.338]    [Pg.364]    [Pg.32]    [Pg.33]    [Pg.351]    [Pg.726]    [Pg.232]    [Pg.111]    [Pg.8]    [Pg.563]    [Pg.719]    [Pg.26]    [Pg.263]    [Pg.369]    [Pg.370]   
See also in sourсe #XX -- [ Pg.75 ]




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