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Cross-section area, geometrical

K depends upon geometrical configuration, cross-sectional area and length of ZnO Block... [Pg.624]

Observe that this is a geometric property, not to be confused with the modulus of the material, which is a material property. I, c, Z, and the cross-sectional areas of some common cross-sections are given in Fig. 3-1, and the mechanical engineering handbooks provide many more. The maximum stress and defection equations for some common beamloading and support geometries are given in Fig. 3-2. Note that for the T- and U-shaped sections in Fig. 3-1 the distance from the neutral surface is not the same for the top and bottom of the beam. It may occasionally be desirable to determine the maximum stress on the other nonneutral surface, particularly if it is in tension. For this reason, Z is provided for these two sections. [Pg.145]

Where u, is the mobile phase velocity at the column outlet, Fg the column volumetric flow rate, and Ag the column cross-sectional area available to the mobile phase. In a packed bed only a fraction of the column geometric cross-sectional area is available to the mobile phase, the rest is occupied by the solid (support) particles. The flow of mobile phase in a packed bed occurs predominantly through the interstitial spaces the mobile phase trapped within the porous particles is largely stagnant (37-40). [Pg.528]

The total cross section for collision with a fast particle is never greater than twice the geometrical cross-sectional area of the nucleus and therefore, fast particle cross-sections are rarely much larger than 10- 4 cm (radii of the heaviest nuclei are about 10- cjjij Hence a cross-section of 10-24 considered as... [Pg.193]

At energies on either side of 8.8 eV a small aluminum sphere presents a much smaller target to incident photons. At 5 eV, for example, the absorption efficiency of a sphere with x = 0.3 is about 0.1 as far as absorption is concerned, the sphere is much smaller than its geometrical cross-sectional area. The field lines of the Poynting vector, shown in Fig. 12.46, are what are to be... [Pg.340]

Under this condition, there is complete depletion of O2 at the electrode next to the porous layer of Fig.6a or inside the cavity of Fig.6b. The constant depends on the diffusion constant of O2 (in its particular carrier gas), Dq, and the geometrical characteristics of the diffusion barrier. In the device of Fig.6b (sensor with integral cavity), the diameter of the aperture C (usually greater than 50 microns) is much larger than the mean free path of the gas molecules at 1 atm (about 1 micron) and bulk diffusion dominates. In this case(ll-12). D0 - K Ta/P and cr - (DgA)/(kTd), where K] is a constant, P is the absolute pressure, a is a constant having a value between 1.5 and 2 and A and d are the cross-sectional area and length of the aperture C. Representative values for D0 are about 1.5 cm2/s at 700 °C and 0.15 cm2/s at 20 °C. Since Pg — cP with c the percentage of O2 molecules in the gas, we have... [Pg.143]

This choice of physical quantities reflects the experience of the authors however, a different selection may also lead to satisfactory results. For example, for a column of circular cross-section, a geometric choice could have been diameter, D, instead of area moment of inertia, /. Flowever, I is more general and works for every cross-sectional... [Pg.180]

Now that the physical configuration has been clarified, we can consider in detail the mathematical model for the process. First, we find a relationship between the flow rate and the geometrical and operational variables. Neglecting leakage flow between the screws, as well as that between the screws and the barrel, this is simply given by multiplying the velocity Vi with the cross-sectional area of the melt-filled channel, Am, as shown in Fig. 6.48... [Pg.306]

Furthermore, it is dear that the scale-up of an injector inherently lessens its efficiency. This is caused by the fact that the dispersing effect of the liquid propulsion jet is restricted to its circumference which, in the case of geometrically similar scale-up, increases only linearly (u = Jtd) while its cross-sectional area increases quadratically (S = it d2/4). This means that with increasing diameter of the device, an increasingly smaller fraction of the liquid throughput is dispersed The dispersion efficiency of injectors inherently diminishes with increasing scale. [Pg.164]

The optical properties of spherical particles at wavelength X change drastically around size parameter, x = 2ita/X 1 particles with x 1 are in the geometric limit, and their absorption cross-sections scale with the cross-sectional area Cabs a2. Particles with size parameters 1 have absorption cross-sections that roughly scale as particle volume CabS a3. The scattering properties of both large... [Pg.195]

It cannot therefore be assumed that each particle obstructs the light with its geometric cross-sectional area. These effects are compensated for by inclusion of an extinction coefficient (/Q in the equation, making the apparent area K times the geometric area. [Pg.372]

If the cross-sectional area of the container is A, the depth to be used in Stokes equation, from geometrical considerations, is [53] ... [Pg.383]

This prevents water penetration and only the exterior of the electrode is exposed to electrolytes. When used with 30 nm sized carbon black powder, the conductive area of the electrode in contact with the electrolyte consists of less than 1 % of the geometric cross-sectional area of the electrode. This has been compared with an ensemble of microelectrodes. These CCEs showed an improvement of up to three orders of magnitude in terms of Faradaic signal-to-noise compared with glassy carbon electrodes [218]. In addition, the sol gel method of preparation affords a variety of structural configurations and it has been shown that CCEs can be produced by thick film and ink jet technology, which allows for their mass production [219]. [Pg.2849]

The net result of absorption and scattering is extinction, while the light that is not extinct is said to be transmitted. In terms of the extinction efficiency, Q, which is defined as the ratio of the radiant power scattered and absorbed by a particle to the radiant power geometrically incident on the particle (proportional to the cross-sectional area). Therefore the extinction efficiency per cross-sectional area of the particle is the sum of its scattering and absorption efficiency per cross-sectional area, and Q, respectively ... [Pg.34]


See other pages where Cross-section area, geometrical is mentioned: [Pg.268]    [Pg.591]    [Pg.278]    [Pg.24]    [Pg.27]    [Pg.58]    [Pg.440]    [Pg.67]    [Pg.72]    [Pg.340]    [Pg.204]    [Pg.61]    [Pg.56]    [Pg.273]    [Pg.36]    [Pg.228]    [Pg.7]    [Pg.8]    [Pg.420]    [Pg.162]    [Pg.323]    [Pg.25]    [Pg.55]    [Pg.279]    [Pg.107]    [Pg.518]    [Pg.596]    [Pg.199]    [Pg.46]    [Pg.289]    [Pg.274]    [Pg.532]    [Pg.68]    [Pg.141]    [Pg.238]    [Pg.36]    [Pg.1563]   
See also in sourсe #XX -- [ Pg.323 ]




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Cross-sectional area

Geometric cross section

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