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Space diffusion

The PC version runs comparatively slow on large problems. FIRAC can perform lumped parameter/control volume-type analysis but is limited in detailed multidimensional modeling of a room or gaa dome space. Diffusion and turbulence within a control volume is not modeled. Multi-gas species are not included in the equations of state. [Pg.354]

Fig. 3.7.1 Schematic of the DDIF effect in porous medium. The black areas are solid grains and the white areas are pore space. Diffusing spins in permeating fluid sample the locally variable magnetic field B(r) (solid contours sketched inside pore space) as it diffuses. Fig. 3.7.1 Schematic of the DDIF effect in porous medium. The black areas are solid grains and the white areas are pore space. Diffusing spins in permeating fluid sample the locally variable magnetic field B(r) (solid contours sketched inside pore space) as it diffuses.
The chemiluminescent emission spectrum of GeCl2 was obtained by burning GeCl4 in potassium vapor using a diffusion flame technique 11 The spectrum consisted of a series of closely spaced diffuse bands in the region 4900—4100 A with an underlying continuum. The bands resemble those of SnCl2. [Pg.30]

In the ultraviolet SnCl2 showed a continuous absorption with a maximum intensity at about 21,044 cm"1 (3220 A). The absence of discrete bands is probably due to overlapping of closely spaced diffuse bands. For PbCl2 three regions of continuous absorption were observed. These had maximum intensities at 3600, 3200 and below 2916 A. The SnCl2 and PbCl2 spectra were interpreted as being due to 1A2 - 1B2 transitions 119 ... [Pg.33]

If the total current can be assumed to be limited by diffusion to the STM tip, Case III is similar to diffusion to a microdisk electrode (one electrode) thin-layer cell (63). Murray and coworkers (66) have shown that for long electrolysis times, diffusion to a planar microdisk electrode TLC can be treated as purely cylindrical diffusion, provided that the layer thickness is much smaller than the disk diameter (66). In contrast to the reversible case discussed above (Case I), the currents in this scenario should decrease gradually with time at a rate that is dependent on the tip radius and the thickness of the interelectrode gap. Thus, for sufficiently narrow tip/sample spacings, diffusion may be constrained sufficiently (ip decayed) at long electrolysis times to permit the imaging of surfaces with STM. [Pg.185]

CSF compartment ventricles, basal cisternae, subarachnoid space (CSF flow), and the narrow zone of adjacent extracellular space (diffusion)... [Pg.7]

One example of half-space diffusion is the cooling of an oceanic plate. The oceanic plate when created at the mid-ocean ridge is hot, with a roughly uniform temperature of about 1600 K. It is cooled at the surface (quenched by ocean water) as it moves away from the ocean ridge. For simplicity, ignore complexities... [Pg.41]

Another example of half-space diffusion problem is as follows. A thin-crystal wafer initially contains some " Ar (e.g., due to decay of " K). When the crystal is heated up (metamorphism), " Ar will diffuse out and the surface concentration of " Ar is zero. If the temperature is constant and, hence, the diffusivity is constant, the problem is also a half-space diffusion problem. [Pg.42]

A third example is as follows. Initially a crystal has a uniform 8 0. Then the crystal is in contact with a fluid with a higher 8 0. Ignore the dissolution of the crystal in the fluid (e.g., the fluid is already saturated with the crystal). Then would diffuse into the crystal. Because fluid is a large reservoir and mass transport in the fluid is rapid, 8 0 at the crystal surface would be maintained constant. Hence, this is again a half-space diffusion problem with uniform initial concentration and constant surface concentration. The evolution of 8 0 with time is shown in Figure l-8b. [Pg.42]

For a diffusion couple, the definition of Amid requires some thinking because the mid-concentration of the whole diffusion couple is right at the interface, which does not move with time. This is because for a diffusion couple every side is diffusing to the other side. On the other hand, if a diffusion couple is viewed as two half-space diffusion problems with the interface concentration viewed as the fixed surface concentration, then. Amid equals 0.95387(Df), the same as the half-space diffusion problem. [Pg.45]

Example 1.4 Knowing D = 10 m /s, for half-space diffusion, estimate the... [Pg.45]

For one-dimensional half-space diffusion with constant D and an initial distribution of C t o = f(x) as well as other conditions, the solutions can be found in Appendix 3. [Pg.209]

Figure 3-29 A half-space diffusion profile of Ar. Ca, = 0.00147 wt% is obtained by averaging 45 points at 346 to 766 /an. Points are data, and the solid curve is a fit of (a) all data by the error function with D = 0.207 /im /s and Co = 0.272 wt%, and (b) data at v < 230 fim (solid dots) by the inverse error function. In (b), for larger x, evaluation of erfc [(C —Cot)/(Co —Coa)] becomes increasingly unreliable and even impossible as (C - Cot)/(Cq — Coo) becomes negative. Data are adapted from Behrens and Zhang (2001), sample AbDArl. Figure 3-29 A half-space diffusion profile of Ar. Ca, = 0.00147 wt% is obtained by averaging 45 points at 346 to 766 /an. Points are data, and the solid curve is a fit of (a) all data by the error function with D = 0.207 /im /s and Co = 0.272 wt%, and (b) data at v < 230 fim (solid dots) by the inverse error function. In (b), for larger x, evaluation of erfc [(C —Cot)/(Co —Coa)] becomes increasingly unreliable and even impossible as (C - Cot)/(Cq — Coo) becomes negative. Data are adapted from Behrens and Zhang (2001), sample AbDArl.
Figure 1-8 Half-space diffusion profiles (cooling of oceanic plate) 43... Figure 1-8 Half-space diffusion profiles (cooling of oceanic plate) 43...
H(+, H >) (another part of space, diffusion of protons down a... [Pg.103]

The principal role of diffusion in these processes could be established considering rather simple examples [2]. If the kinetic equations for a well-stirred system are able to reproduce self-oscillations (the limit cycle), the extended system could be presented as a set of non-linear oscillators continuously distributed in space. Diffusion acts to conjunct these local oscillations and under certain conditions it can result in the synchronisation of oscillations. Thus, autowave solutions could be interpreted as a result of a weak coupling (conjunction) of local oscillators when they are not synchronised completely. The stationary spatial distributions in an initially homogeneous systems can also arise due to diffusion, which makes homogeneous solutions unstable. [Pg.471]

To separate space diffusion, we represent the distribution function as... [Pg.231]

Finite-space diffusion takes place during the charging of insertion electrodes at moderate frequencies, transforming into mainly capacitive behavior within the limit of very low frequencies, in contrast to the semi-infinite diffusion for solution redox-species (except for thin-layer solution electrochemistry) electrochemical impedance spectroscopy becomes a very useful diagnostic tool for the characterization of insertion mechanisms ... [Pg.355]


See other pages where Space diffusion is mentioned: [Pg.524]    [Pg.187]    [Pg.13]    [Pg.86]    [Pg.41]    [Pg.42]    [Pg.45]    [Pg.45]    [Pg.174]    [Pg.217]    [Pg.53]    [Pg.123]    [Pg.244]    [Pg.336]    [Pg.340]    [Pg.21]    [Pg.35]    [Pg.440]    [Pg.198]    [Pg.1257]   
See also in sourсe #XX -- [ Pg.21 ]




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Anomalous diffusion space

Diffusion equation space-fractional

Diffusion half-space

Diffusion in free space

Diffusion in phase space

Diffusion in the extracellular space

Diffusion real space

Diffusion space function

Diffusion space number

Energy-space diffusion

Mixed phase-and physical-space diffusion

Phase-space diffusion

Physical-space diffusion

Reaction space, proton diffusion between

Reaction space, proton diffusion between membranes

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