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Crest surface

To follow to actually carry out a TSA simulation a three-dimensional grid, with grid interval of about 0.2 A (5 -106 equispaced points in (132)) is built and the Helmholtz energies at all grid points are computed. Before this can be done in practice, a value for (A2) must be found. Then, local minima and the crest surfaces must be found, using the procedures given in (130,132,165). To study the dynamics of the penetrant molecules on the network of sites a Monte-Carlo procedure is employed, which is presented is some detail in (97). [Pg.149]

Suppose that the solute distribution function p(r) is known. The real trajectorks of solute molecules that yield this distribution function arc very complex, but an important feature of this movement can be eluddated exf citly the solute molecules should spend a large fraction of tiuK in oscillations in the vicinity of the local maxima of the distribution function p(r). Any two adjacent local maxima, i and J, of this distribution function are separated by a common crest surface Qjj on which the foUowing condition holds ... [Pg.218]

Equation (28) gives the (absolute) rate constants for site-to-site transitions in the quasi-classical approximation. Evaluation of the Ry requires integration of the distribution function p(r) over the volume of site i and crest surface fiy separating sites i and j. [Pg.221]

The surface integrals Zy, see Eq. (28), can now also be detamiimd the crest surface Ojj must be located between adjacent grid points with allocation to sites i and j and one woidd expect (from the definition of the crest surface [%e Eq. [Pg.223]

There are four related electrokinetic phenomena which are generally defined as follows electrophoresis—the movement of a charged surface (i.e., suspended particle) relative to astationaiy hquid induced by an applied ectrical field, sedimentation potential— the electric field which is crested when charged particles move relative to a stationary hquid, electroosmosis—the movement of a liquid relative to a stationaiy charged surface (i.e., capiUaty wall), and streaming potential—the electric field which is created when liquid is made to flow relative to a stationary charged surface. The effects summarized by Eq. (22-26) form the basis of these electrokinetic phenomena. [Pg.2006]

A stone dropped in a pond pushes the water downward, which is countered by elastic forces in the water that tend to restore the water to its initial condition. The movement of the water is up and down, but the crest of the wai c produced moves along the surface of the water. This type of wave is said to be transverse because the displacement of the water is perpendicular to the direction the wave moves. When the oscillations of the wave die out, there has been no net movement of water the pond is just as it was before the stone was dropped. Yet the wave has energy associated with it. A person has only to get in the path of a water wave crashing onto a beach to know that energy is involved. The stadium wave is a transverse wave, as is a wave in a guitar string. [Pg.1221]

Cell adhesion molecules (CAMs) play critical roles in all facets of nervous system development and maintenance. Important phenomena in which CAMs are involved include initial formation of the neural tube and the neural crest, migration of all neurons and glial cells, axonal outgrowth and guidance, target selection, synaptic stabilization and plasticity, myelination and nerve regeneration after injury (see Chs 4,24,28-30 and 53). Adhesion molecules interact with each other and with nonadhesive cell-surface and/or cytoplasmic molecules, and, in the two... [Pg.111]

The physical situation is very similar to that of a boat moving on the sea surface, the gravity playing the role of the ponderomotive force in the previous case. The water moves from the immersed volume of the boat towards the stern, where it accumulates in the first crest of a wave produced in the boat... [Pg.165]

In the high-velocity atomization processes, the effect of the compressibility of atomization gas could be quite appreciable. Extending Taylor s analysis 245 for a gas flow over a liquid to a compressible gas flow, Bradley t329 330 developed an expression for the fastest growing wavelength that dominates the disruption at the interface. Supposing that surface tension nips off the crest of the wave into a filament whose diameter is some fraction of the... [Pg.188]

As mentioned, a laminar boundary layer separates a greater distance from the surface of a curved body than a turbulent one. The laminar boundary layer in the upper photograph of Figure 5 is shown separating from the crest... [Pg.137]

An easily visualised example of a transverse wave is that obtained when a stone is dropped into a pool of water. The disturbance, or water wave, can be seen spreading across the surface in the form of circular crests of increasing radius. Any objects in the pool (e. g. [Pg.25]


See other pages where Crest surface is mentioned: [Pg.10]    [Pg.149]    [Pg.221]    [Pg.223]    [Pg.10]    [Pg.149]    [Pg.221]    [Pg.223]    [Pg.665]    [Pg.666]    [Pg.698]    [Pg.92]    [Pg.149]    [Pg.897]    [Pg.511]    [Pg.261]    [Pg.145]    [Pg.114]    [Pg.454]    [Pg.151]    [Pg.429]    [Pg.127]    [Pg.232]    [Pg.65]    [Pg.216]    [Pg.221]    [Pg.53]    [Pg.135]    [Pg.149]    [Pg.154]    [Pg.168]    [Pg.36]    [Pg.349]    [Pg.100]    [Pg.592]    [Pg.32]    [Pg.391]    [Pg.57]    [Pg.158]    [Pg.254]    [Pg.23]    [Pg.393]   
See also in sourсe #XX -- [ Pg.218 , Pg.223 ]




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Crest

Cresting

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