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Channel scales

Fig. 8 Emission from formaldehyde-fixed NIF13T3 cells loaded with 100 mM silver nitrate for 20 h. (a) Fluorescence image the inset is the intensity profile along the line drawn across the cell, (b) Merge of (c) and (d). (c) Emission from RNASelect fluorescence (green channel) (d) Emission from silver clusters (red channel)-, Scale bar 30 pm [57]... Fig. 8 Emission from formaldehyde-fixed NIF13T3 cells loaded with 100 mM silver nitrate for 20 h. (a) Fluorescence image the inset is the intensity profile along the line drawn across the cell, (b) Merge of (c) and (d). (c) Emission from RNASelect fluorescence (green channel) (d) Emission from silver clusters (red channel)-, Scale bar 30 pm [57]...
In collaboration with the University of Wageningen, magnetic resonance imaging (MRI) was used to visualize the film flow in the monoliths [15], As shown in Fig. 8.8, liquid (water) was fed onto a complete piece of monolith from which four channels then were prolonged for measurement. In Fig. 8.9, the liquid is represented as light areas in the corners of the four channels. Clearly, the channel walls are not uniformly irrigated. In the corners, the gas-liquid interface is shaped like an arc, whereas between the pockets, only a thin liquid film remains ( 70 pm). This retraction of the film into the corners can be attributed to the high surface tension of the liquid used (water). Additionally, the liquid pockets of one channel have different sizes, and this leads to channel scale maldistribution. [Pg.238]

Fig. 16 (Continued) (e) PCR chamber with exit channel tapering before intersecting with the MR inlet channel (Scale bar. 1 mm), (f) Cross-T intersection (Scale bar 1 mm). The relative sizes of the BR, SW, and BW channels create the difference in volume displacement during the pumping injection and affect how the resistance is dropped under an applied separation voltage. Reproduced from [10] with permission... Fig. 16 (Continued) (e) PCR chamber with exit channel tapering before intersecting with the MR inlet channel (Scale bar. 1 mm), (f) Cross-T intersection (Scale bar 1 mm). The relative sizes of the BR, SW, and BW channels create the difference in volume displacement during the pumping injection and affect how the resistance is dropped under an applied separation voltage. Reproduced from [10] with permission...
Fig. 5 Cryosections of rat brain after administration of 45 and 200 mg of PBCA nanoparticles. Transmitted optical transmission images of the sections (40x). Nano green fluorescence created by the PMl-labeled nanoparticles. Willebrand endothelial cells stained with red fluorescent antibody (von Willebrand factor primary and anti-lgG secondary antibody with fluorescent label). Merge 40x and merge 63 x images merged from the green and red channels. Scale bars 100 mm [45]... Fig. 5 Cryosections of rat brain after administration of 45 and 200 mg of PBCA nanoparticles. Transmitted optical transmission images of the sections (40x). Nano green fluorescence created by the PMl-labeled nanoparticles. Willebrand endothelial cells stained with red fluorescent antibody (von Willebrand factor primary and anti-lgG secondary antibody with fluorescent label). Merge 40x and merge 63 x images merged from the green and red channels. Scale bars 100 mm [45]...
Figure 3 Schematic representation of a chromatographic column with various scales of the relative flow velocity differences a - frans-particle scale b - trans-channel scale c - short-range interchannel scale d - long-range interchannel scale e - transcolumn scale f - trans-pore scale. Figure 3 Schematic representation of a chromatographic column with various scales of the relative flow velocity differences a - frans-particle scale b - trans-channel scale c - short-range interchannel scale d - long-range interchannel scale e - transcolumn scale f - trans-pore scale.
Cha et al. [61] studied the effeet of flow channel scaling on fuel eell performance. In particular, the impact of dimensional seales on the order of 100 micrometers and below has been investigated. A model based on isothermal three-dimensional computational fluid dynamics has been developed which predicts that very small channels result in significantly higher peak power densities compared to their larger counterparts. The experimental results confirm the predicted outcome at relatively large scale. At especially small scale (<100/iW),... [Pg.300]

Electrochemical Impedance Spectroscopy (EIS) consists in measuring the voltage response to sinusoidal current perturbation with different frequencies. This method can yield important information about mass transport limitations, but the interpretation of the results must be done very carefully. In particular, it has been shown that the cell global impedance spectrum is strongly affected by gas consumption along the channels [22]. Even on the scale of a differential cell, local effects on the rib/channel scale can dominate the resulting spectrum [23]. [Pg.1668]

Droplet-based microfluidic system behavior is impacted by multiphase flow characteristics, interfacial tension, and the wetting and physical properties of the liquids. At different channel scales and fluid velocities, the system can be influenced by balancing inertial, viscous, or gravitational forces against the interfacial forces. In these cases, other dimensionless numbers are relevant. For example, the ratio of interfacial and gravitational force is given by the Bond number (Bo),... [Pg.435]

A new dimension to acid-base systems has been developed with the use of zeolites. As illustrated in Fig. XVIII-21, the alumino-silicate faujasite has an open structure of interconnected cavities. By exchanging for alkali metal (or NH4 and then driving off ammonia), acid zeolites can be obtained whose acidity is comparable to that of sulfuric acid and having excellent catalytic properties (see Section XVIII-9D). Using spectral shifts, zeolites can be put on a relative acidity scale [195]. An important added feature is that the size of the channels and cavities, which can be controlled, gives selectivity in that only... [Pg.719]

Consider a triatomic system with the three nuclei labeled A, Ap, and Ay. Let the arrangement channel -1- A A be called the X arrangement channel, where Xvk is a cyclic permutation of apy. Let Rx,r be the Jacobi vectors associated with this arrangement channel, where r is the vector from A to and the vector from the center of mass of AyA to A . Let R i, rx be the corresponding mass-scaled Jacobi coordinates defined by... [Pg.206]

Nevertheless, the technique suffers from a severe time scale problem -the trajectories are computed for (at most) a few nanoseconds. This is far too short compared to times required for many processes in biophysics. For example, the ii to T conformational transition in hemoglobin lasts tens of microseconds [1], and the typical time for ion migration through the gramicidin channel is hundreds of nanoseconds. This limits (of course) our ability to make a meaningful comparison to experiments, using MD. [Pg.263]

Here f denotes the fraction of molecules diffusely scattered at the surface and I is the mean free path. If distance is measured on a scale whose unit is comparable with the dimensions of the flow channel and is some suitable characteristic fluid velocity, such as the center-line velocity, then dv/dx v and f <<1. Provided a significant proportion of incident molecules are scattered diffusely at the wall, so that f is not too small, it then follows from (4.8) that G l, and hence from (4.7) that V v° at the wall. Consequently a good approximation to the correct boundary condition is obtained by setting v = 0 at the wall. ... [Pg.27]

Now suppose, as before, that distance is measured on a scale whose unit is comparable with the dimensions of che flow channel, and let v° be some characteristic mass mean velocity in the system, like introduced above... [Pg.28]

Let H and L be two characteristic lengths associated with the channel height and the lateral dimensions of the flow domain, respectively. To obtain a uniformly valid approximation for the flow equations, in the limit of small channel thickness, the ratio of characteristic height to lateral dimensions is defined as e = (H/L) 0. Coordinate scale factors h, as well as dynamic variables are represented by a power series in e. It is expected that the scale factor h-, in the direction normal to the layer, is 0(e) while hi and /12, are 0(L). It is also anticipated that the leading terms in the expansion of h, are independent of the coordinate x. Similai ly, the physical velocity components, vi and V2, ai e 0(11), whei e U is a characteristic layer wise velocity, while V3, the component perpendicular to the layer, is 0(eU). Therefore we have... [Pg.178]

Species such as carp, salmon, trout, channel catfish, and tilapia have been bred for many generations in captivity though they usually differ httle in appearance or genetically from their wild counterparts. A few exceptions exist, such as the leather carp, a common carp strain selectively bred to produce only one row of scales, and the Donaldson trout, a strain of rainbow trout developed over numerous generations to grow more rapidly to larger size and... [Pg.21]

Gate oxide dielectrics are a cmcial element in the down-scaling of n- and -channel metal-oxide semiconductor field-effect transistors (MOSEETs) in CMOS technology. Ultrathin dielectric films are required, and the 12.0-nm thick layers are expected to shrink to 6.0 nm by the year 2000 (2). Gate dielectrics have been made by growing thermal oxides, whereas development has turned to the use of oxide/nitride/oxide (ONO) sandwich stmctures, or to oxynitrides, SiO N. Oxynitrides are formed by growing thermal oxides in the presence of a nitrogen source such as ammonia or nitrous oxide, N2O. Oxidation and nitridation are also performed in rapid thermal processors (RTP), which reduce the temperature exposure of a substrate. [Pg.348]

Radiation Damage. It has been known for many years that bombardment of a crystal with energetic (keV to MeV) heavy ions produces regions of lattice disorder. An implanted ion entering a soHd with an initial kinetic energy of 100 keV comes to rest in the time scale of about 10 due to both electronic and nuclear coUisions. As an ion slows down and comes to rest in a crystal, it makes a number of coUisions with the lattice atoms. In these coUisions, sufficient energy may be transferred from the ion to displace an atom from its lattice site. Lattice atoms which are displaced by an incident ion are caUed primary knock-on atoms (PKA). A PKA can in turn displace other atoms, secondary knock-ons, etc. This process creates a cascade of atomic coUisions and is coUectively referred to as the coUision, or displacement, cascade. The disorder can be directiy observed by techniques sensitive to lattice stmcture, such as electron-transmission microscopy, MeV-particle channeling, and electron diffraction. [Pg.394]

Fig. 20. Scaling of channel enthalpy extraction for the various MHD faciUties discussed in text ( ) achieved, and (e) predicted where O is the average gas conductivity in mho/m B, the average magnetic field in T M, the channel Mach number E, the average channel active length, m and P, the average... Fig. 20. Scaling of channel enthalpy extraction for the various MHD faciUties discussed in text ( ) achieved, and (e) predicted where O is the average gas conductivity in mho/m B, the average magnetic field in T M, the channel Mach number E, the average channel active length, m and P, the average...
Whereas considerable progress has been made towards achieving acceptable channel performance (power and enthalpy extraction) and durabiUty, as of this writing performance and durabiUty have not been demonstrated simultaneously. A larger scale demonstration plant has been proposed in the United States by the MHD Development Corp. (112). [Pg.433]


See other pages where Channel scales is mentioned: [Pg.213]    [Pg.242]    [Pg.242]    [Pg.331]    [Pg.420]    [Pg.1114]    [Pg.2598]    [Pg.140]    [Pg.300]    [Pg.266]    [Pg.307]    [Pg.554]    [Pg.348]    [Pg.245]    [Pg.25]    [Pg.213]    [Pg.242]    [Pg.242]    [Pg.331]    [Pg.420]    [Pg.1114]    [Pg.2598]    [Pg.140]    [Pg.300]    [Pg.266]    [Pg.307]    [Pg.554]    [Pg.348]    [Pg.245]    [Pg.25]    [Pg.336]    [Pg.769]    [Pg.2498]    [Pg.2892]    [Pg.2954]    [Pg.10]    [Pg.203]    [Pg.432]    [Pg.437]    [Pg.546]    [Pg.8]    [Pg.282]    [Pg.518]    [Pg.318]    [Pg.355]    [Pg.373]    [Pg.479]   
See also in sourсe #XX -- [ Pg.6 ]




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