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Packings generations

Molecular modeling techniques are a powerful tool to obtain a very detailed insight in the three-dimensional structure of dendrimer molecules at the atomic level. They have been applied to calculate sizes of the polypropylene imine) dendrimers and radial density profiles in order to estimate the free volume inside the dendrimers, as well as to make predictions about de Gennes dense-packed generations. The molecular modeling work by Coussens and co-workers [20] was focused on the generations 1-5 of the DAB-dendr-(CN)n and DAB-dendr-(NH2)n (n = 4, 8, 16,32, 64). [Pg.614]

Figure 8.7 Performance comparison of the three packing generations specific surface area versus packing factor. Figure 8.7 Performance comparison of the three packing generations specific surface area versus packing factor.
As early as 1983, de Gennes and Hervet [85] proposed a simple equation derived from fundamental principles, to predict the Starburst limited or dense-packed generation mt for PAM AM dendrimers. Based on ideal dendrimer growth, with tertiary amine branch junctures connected by linear, flexible branch cell segments P, this equation relates m, to the branch cell segment length 1 or P ... [Pg.281]

This equation, together with branch cell segment lengths described for PAMAMs (see Sect. 5.2.3.1), predicts occurrence of the dense-packed generation m, between generations 10 and 11. This appears to have been experimentally verified. [Pg.281]

This test is a reference test for the flammability test of individually packed generators. [Pg.312]

Instant hot and cold packs create aqueous solutions that form exothermically or endothermically and therefore release or absorb heat. A hot pack generates heat when a salt such as calcium chloride dissolves in water that is stored in the pack. The calcium chloride dissolves exothermically. A cold pack absorbs heat when a salt such as ammonium nitrate dissolves in water. The ammonium nitrate dissolves endothermically. [Pg.710]

The torque converter is a type of fluid coupling device that hydraulically connects the engine to the transmission—analogous to a mechanical clutch. Used in conjunction with the torque converter is a stator, which essentially assists at low engine speeds, thus increasing acceleration. The vanes inside the converter alter the shape of the fluid path into the stator. The stator captures the kinetic energy of the transmission to enhance torque multiplication. This process will not only increase heat, but also increase shear of the transmission fluid. In addition to torque conversion, at every shift event, clutch packs generate heat, which must be carried away by the transmission fluid. [Pg.105]

Both hot and cold packs depend on large energy changes taking place during a chemical reaction. Cold packs rely on an endothermic reaction, and hot packs generate heat energy from an exothermic reaction. [Pg.216]

Transfer of material between the two columns was automatic by virtue of two intercolumn vapor-transfer lines. The mass flow in these transfer lines was provided by using appropriate lengths of column packing generating appropriate pressure drop to drive the flow see Figure 8). [Pg.350]

Packed generator systems. The traditional acetifler comprises a tall vat packed with an inert material (usually birch twigs or wood shavings) which act as the carrier for the acetobacter culture. The alcoholic substrate is sprayed on the top of the column and allowed to flow down against a stream of air, introduced from the bottom of the vat, into a false bottom and is recirculated for several days until most of the alcohol has been oxidized to acetic add. [Pg.284]

Figure 3.1 Illustration of the Monte Carlo packing-generation method for a system of N = 6 bidisperse frictionless disks (half small and half large with diameter ratio 1.4) in 2D. (a) The x- and y-coordinates for N = 6 random points are first generated in a square cell with periodic boundary conditions and the particles are grown uniformly until the closest pair of disks is in contact, (b) An attempt is made to move each particle randomly from the original (dashed outline) to the new position (shaded disk), and the move is accepted if it does not give rise to particle overlap, (c) The disks are expanded uniformly from the original (dashed outline) to the new size (shaded disk) until the two closest disks touch. This process is repeated for Nj iterations to obtain a single static packing. Figure 3.1 Illustration of the Monte Carlo packing-generation method for a system of N = 6 bidisperse frictionless disks (half small and half large with diameter ratio 1.4) in 2D. (a) The x- and y-coordinates for N = 6 random points are first generated in a square cell with periodic boundary conditions and the particles are grown uniformly until the closest pair of disks is in contact, (b) An attempt is made to move each particle randomly from the original (dashed outline) to the new position (shaded disk), and the move is accepted if it does not give rise to particle overlap, (c) The disks are expanded uniformly from the original (dashed outline) to the new size (shaded disk) until the two closest disks touch. This process is repeated for Nj iterations to obtain a single static packing.
To characterize the structural properties of the packings generated via the Monte Carlo method, we calculated the number of interparticle contacts (defined where 6 is a small cutoff, typically such that fijl(Jij - 1 < 10", where... [Pg.122]


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