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Spheres combinations

Advantages are also found with microelectrodes used at short time scales where time-dependent currents are obtained, as the example in Figure 12.4 shows [56]. Time-dependent currents are proportional to the electrode area. Thus, for the case of a sphere, combination of the expression for the time-dependent current with the resistance shows that the ohmic drop is directly proportional to the radius. Thus, ohmic drop is always minimized by the use of a smaller electrode. [Pg.388]

The word lithosphere is derived from the word sphere, combined with the Greek word lithos which means rock. The lithosphere is the solid outer section of Earth which includes Earth s crust (the skin of rock... [Pg.137]

In order to study the effect of metals distribution on activity and stability, test catalysts were prepared by diluting y-alumina sphere-based catalysts of fixed concentration (a Pt Pd ratio of 2.5 1.0) with bare spheres in varying amounts. The T50 data for these test catalysts for CO oxidation are plotted in Figure 8. Each curve represents the data at a constant total metals concentration when calculated over the entire catalyst—bare sphere combination. The curves demonstrate the effect... [Pg.146]

Manage transportation Providing transportation services to product-producing spheres combining total requirements to gain efficiencies... [Pg.199]

For many practically relevant material/environment combinations, thennodynamic stability is not provided, since E > E. Hence, a key consideration is how fast the corrosion reaction proceeds. As for other electrochemical reactions, a variety of factors can influence the rate detennining step. In the most straightforward case the reaction is activation energy controlled i.e. the ion transfer tlrrough the surface Helmholtz double layer involving migration and the adjustment of the hydration sphere to electron uptake or donation is rate detennining. The transition state is... [Pg.2717]

All that can be concluded from the data given in the preceding example is that the particle is not an unsolvated sphere. However, when an appropriate display of contours is examined for f/fo (e.g.. Ref. 2), the latter is found to be consistent with an unsolvated particle of axial ratio about 4 1 or with a spherical particle hydrated to the extent of about 0.48 g water (g polymer). Of course, there are a number of combinations of these variables which are also possible, and some additional experimental data—such as the intrinsic viscosity—are needed to select that combination which is consistent with all experimental observations. [Pg.628]

Two modifications of the duidized-bed reactor technology have been developed. In the first, two gas-phase duidized-bed reactors coimected to one another have been used by Mobil Chemical Co. and Union Carbide to manufacture HDPE resins with broad MWD (74,75). In the second development, a combination of two different reactor types, a small slurry loop reactor followed by one or two gas-phase duidized-bed reactors (Sphetilene process), was used by Montedision to accommodate a Ziegler catalyst with a special particle morphology (76,77). This catalyst is able to produce PE resins in the form of dense spheres with a diameter of up to 4—5 mm such resins are ready for shipping without pelletization. [Pg.385]

Calculation of Tank Volume A tank may be a sin e geometrical element, such as a cylinder, a sphere, or an ellipsoid. It may also have a compound form, such as a c inder with hemispherical ends or a combination of a toroid and a sphere. To determine the volume, each geometrical element usually must be calculated separately. Calculations for a full tank are usually simple, but calculations for partially filled tanks may be complicated. [Pg.1017]

Column Operation To assure intimate contact between the counterflowing interstitial streams, the volume fraction of liquid in the foam should be kept below about 10 percent—and the lower the better. Also, rather uniform bubble sizes are desirable. The foam bubbles will thus pack together as blunted polyhedra rather than as spheres, and the suction in the capillaries (Plateau borders) so formed vidll promote good liqiiid distribution and contact. To allow for this desirable deviation from sphericity, S = 6.3/d in the equations for enriching, stripping, and combined column operation [Lemhch, Chem. E/ig., 75(27), 95 (1968) 76(6), 5 (1969)]. Diameter d still refers to the sphere. [Pg.2020]

This allows for the equivalence between crossed cylinders and the particle on a plane problem. Likewise, the mechanics of two spheres can be described by an equivalently radiused particle-on-a-plane problem. The combination of moduli and the use of an effective radius greatly simplifies the computational representation and allows all the cases to be represented by the same formula. On the other hand, it opens the possibility of factors of two errors if the formula are used without realizing that such combinations have been made. Readers are cautioned to be aware of these issues in the formulae that follow. [Pg.146]

One should perhaps mention some other closures that are discussed in the literature. One possibility is to combine the PY approximation for the hard core part of the potential and then use the HNC approximation to compute the corrections due to the attractive forces. Such an approach is called the reference hypernetted chain or RHNC approximation [48,49]. Recently, some new closures for a mixture of hard spheres have been proposed. These include one by Rogers and Young [50] (RY) and the Martynov-Sarkisov [51] (MS) closure as modified by Ballone, Pastore, Galli and Gazzillo [52] (BPGG). The RY and MS/BPGG closure relations take the forms... [Pg.149]

When the four previous equations are combined with the relation for the initial diameter of the sphere (Dq) [Eq. (6.2.6)], the fireball s temperature and maximum diameter can be calculated. From this model, it follows that the temperature of the fireball, and thus its emissive power, is independent of initial fuel mass. [Pg.173]

During the actual preparation of the GPC/SEC gel, there are several noteworthy items in the procedure. When combining aqueous and organic phases, always pour the organic phase into the water phase as the reverse procedure produces very large particles. This mixture must be held at 40°C to prevent the initiator from starting the reaction before the right size particles are formed. Rotor speed determines the particle size of the spheres the faster the speed the smaller the particles. Constant torque mixers produce the best results with more narrow particle-size distributions. The initial mixture should be stirred at 300-400 rpm to ensure a particle-size distribution from 2 to 20 yam. [Pg.164]

Methods for evaluating the effect of a solvent may broadly be divided into two types those describing the individual solvent molecules, as discussed in Section 16.1, and those which treat the solvent as a continuous medium. Combinations are also possible, for example by explicitly considering the first solvation sphere and treating the rest by a continuum model. Each of these may be subdivided according to whether they use a classical or quantum mechanical description. [Pg.392]

An analytical solution to this has already been attempted [25]. According to this model, the minimum concentration of fines would be that quantity required to coat each coarse particle with a monolayer of fines. Treating the particles as perfect spheres, the fractional change in combined particle volume due to additional film of fines is then ... [Pg.709]

We have used the multisublattice generalization of the coherent potential approximation (CPA) in conjunction with the Linear-MufRn-Tin-Orbital (LMTO) method in the atomic sphere approximation (ASA). The LMTO-ASA is based on the work of Andersen and co-workers and the combined technique allows us to treat all phases on equal footing. To treat itinerant magnetism we have employed for the local spin density approximation (LSDA) the Vosko-Wilk-Nusair parameterization". [Pg.14]

In the relativistic KKR method the trial function inside the MT-sphere is chosen as a linear combination of solutions of the Dirac equation in the center-symmetrical field with variational coefficients C7 (k)... [Pg.141]


See other pages where Spheres combinations is mentioned: [Pg.580]    [Pg.37]    [Pg.255]    [Pg.464]    [Pg.154]    [Pg.255]    [Pg.222]    [Pg.437]    [Pg.217]    [Pg.7]    [Pg.1409]    [Pg.83]    [Pg.251]    [Pg.580]    [Pg.37]    [Pg.255]    [Pg.464]    [Pg.154]    [Pg.255]    [Pg.222]    [Pg.437]    [Pg.217]    [Pg.7]    [Pg.1409]    [Pg.83]    [Pg.251]    [Pg.236]    [Pg.1710]    [Pg.2412]    [Pg.2421]    [Pg.319]    [Pg.10]    [Pg.106]    [Pg.454]    [Pg.213]    [Pg.224]    [Pg.521]    [Pg.116]    [Pg.311]    [Pg.889]    [Pg.232]    [Pg.45]    [Pg.445]    [Pg.144]    [Pg.604]   
See also in sourсe #XX -- [ Pg.127 ]




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