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ETALS

L is Avagadro s constant and k is defined above. It can be seen that there are indeed two corrections to the conductivity at infinite dilution tire first corresponds to the relaxation effect, and is correct in (A2.4.72) only under the assumption of a zero ionic radius. For a finite ionic radius, a, the first tenn needs to be modified Falkenliagen [8] originally showed that simply dividing by a temr (1 -t kiTq) gives a first-order correction, and more complex corrections have been reviewed by Pitts etal [14], who show that, to a second order, the relaxation temr in (A2.4.72) should be divided by (1 + KOfiH I + KUn, . The electrophoretic effect should also... [Pg.585]

Figure A3.14.17. Self-replicating spots in the FIS reaction in a CFUR, comparing an experimental time sequence with numerical simulation based on a simple autocatalytic scheme. (Reprmted with pennission from Lee etal [M], Macmillan Magazines Ltd. 1994.)... Figure A3.14.17. Self-replicating spots in the FIS reaction in a CFUR, comparing an experimental time sequence with numerical simulation based on a simple autocatalytic scheme. (Reprmted with pennission from Lee etal [M], Macmillan Magazines Ltd. 1994.)...
The cross-correlation effects between the DD and CSA interactions also influence the transverse relaxation and lead to the phenomenon known as differential line broadening in a doublet [40], cf Figure Bl.13.8. There is a recent experiment, designed for protein studies, that I wish to mention at tire end of this section. It has been proposed by Pervushin etal [4T], is called TROSY (transverse relaxation optimized spectroscopy) and... [Pg.1513]

Figure Bl.17.3. STEM detectors (a) conventional bright and dark-field detectors, electrons are detected according to their different scattering angles, all other positional infonnation is lost (b) positional detector as developed by Haider and coworkers (Haider etal 1994). Figure Bl.17.3. STEM detectors (a) conventional bright and dark-field detectors, electrons are detected according to their different scattering angles, all other positional infonnation is lost (b) positional detector as developed by Haider and coworkers (Haider etal 1994).
Figure Bl.17.11. Reconstructed density of an a,p-tiibulin protein dimer as obtained from electron crystallography (Nogales etal 1997). Note the appearance of the p-sheets ((a), marked B) and the a-helices ((b), marked H) in the density. In particular the right-handed a-helix H6 is very clear. Pictures by courtesy of E Nogales and Academic Press. Figure Bl.17.11. Reconstructed density of an a,p-tiibulin protein dimer as obtained from electron crystallography (Nogales etal 1997). Note the appearance of the p-sheets ((a), marked B) and the a-helices ((b), marked H) in the density. In particular the right-handed a-helix H6 is very clear. Pictures by courtesy of E Nogales and Academic Press.
Another interesting extension of the FECO teclmique, using a capillary droplet of mercury as the second mirror, was developed by Flom etal [6f]. The light from this special interferometer is analysed in reflection. [Pg.1735]

All static studies at pressures beyond 25 GPa are done with diamond-anvil cells conceived independently by Jamieson [32] and by Weir etal [33]. In these variants of Bridgman s design, the anvils are single-crystal gem-quality diamonds, the hardest known material, truncated with small flat faces (culets) usually less than 0.5 nun in diameter. Diamond anvils with 50 pm diameter or smaller culets can generate pressures to about 500 GPa, the highest static laboratory pressures equivalent to the pressure at the centre of the Earth. [Pg.1958]

Figure B2.3.5. Typical time-of-flight spectra of DF products from the F + D2 reaction [28]- The collision energies and in-plane and out-of-plane laboratory scattered angles are given in each panel. The DF product vibrational quantum number associated with each peak is indicated. Reprinted with pennission from Faiibel etal [28]. Copyright 1997 American Chemical Society. Figure B2.3.5. Typical time-of-flight spectra of DF products from the F + D2 reaction [28]- The collision energies and in-plane and out-of-plane laboratory scattered angles are given in each panel. The DF product vibrational quantum number associated with each peak is indicated. Reprinted with pennission from Faiibel etal [28]. Copyright 1997 American Chemical Society.
In the work of Irvine etal [44], the OH produet was deteeted, as illustrated by the fluoreseenee exeitation speetnun in figure B2.3.15. Sinee the rotational eonstant of OH is imieh larger than that of NO, the speetnun... [Pg.2079]

A recent example of laser flash-lamp photolysis is given by Hippier etal [ ], who investigated the temperature and pressure dependence of the thennal recombmation rate constant for the reaction... [Pg.2126]

These methods try to bracket the transition state from both the reactant and the product side [72, 73]. For example, in the method of Dewar etal [73], two stmctiires, one in the reactant valley and one hi the product valley, are optimized simultaneously. The lower-energy stmcture is moved to reduce the distance separating the two stmctures by a small amount, e.g. by 10%, and its stmcture is reoptimized under the constraint that the distance is fixed. This process is repeated until the distance between the two stmctures is sufficiently small. [Pg.2350]

Detailed x-ray diffraction studies on polar liquid crystals have demonstrated tire existence of multiple smectic A and smectic C phases [M, 15 and 16]. The first evidence for a smectic A-smectic A phase transition was provided by tire optical microscopy observations of Sigaud etal [17] on binary mixtures of two smectogens. Different stmctures exist due to tire competing effects of dipolar interactions (which can lead to alternating head-tail or interdigitated stmctures) and steric effects (which lead to a layer period equal to tire molecular lengtli). These... [Pg.2546]

Bruohez M etal 1998 Semioonduotor nanoorystals as fluoresoent biologioal labels Science 281 2013... [Pg.2925]

INDO/1 and /lNDO/.Sarc Dr. Michael /erner s INDO versions and used for m olecular syslein s w ith transition m etals,/INDO/1 is expected to give gcom dries of m oicculcs, and /INDO/S is param -clrixcd to give UV spectra. [Pg.127]

Th e ability to perform m oleciilar orbital (MO ) calculation s on m et-als is extremely useliil because molecular mechanics methods are gen erally unable to treat m etals. This is becau se m etals h ave a wide range of valences, oxidation states, spin multiplicities, and have 1111 usual bonding situations (e.g.. d%-p% back bonding). In addition. the 11 on direction al n at are o ( m etallic hon din g is less am en a-ble to a ball and spring interpretation. [Pg.151]

I done as follows [Essex etal. 1994]. Molecular axes are defined for each CH2 unit in the as shown in Figure 7.19. These molecular axes are defined for the nth CH2 unit as s ... [Pg.412]

These subjects have been reviewed up the year 1975 in various works. Prij s Card Index (363) of thiazole compounds provides swift access to information on individual compounds. Syntheses of thiazoles have been carefully reviewed by Wiley etal. (361), and in 1957 the subject was dealt with in an excellent survey by Sprague and Land (448). [Pg.167]

Pugmire etal. have published calculated electron densities for pyrazine (68JA697), quinoxaline (69JA6381) and phenazine and the calculated total electron densities a + v) are shown in (10), (11) and (12). [Pg.159]

The behaviour under electron impact of IV- and C-trimethylsilylpyrazoles (mono-, di-and tri-substituted) has been studied by Birkofer et al. (740MS 8)347). Loss of a methyl radical followed by loss of HCN is the most common fragmentation feature of these compounds. When more than one trimethylsilyl group is present, a neutral fragment CaHgSi is expelled. Mass spectrometry of pyrazolium salts has been studied by Larsen etal. (8i OMS377, 830MS52). [Pg.204]

Other extensive tables are given by Angus, S., International Theimodynamic Tables of the Fluid State—6, Nitrogen, Perganion, 1977 (244 pp.) Hanley, H. J. M., R. D. McCarty, etal.,y, Fhys. Chem. Ref Data, 3 (1974) 979-1019. [Pg.301]

FIG. 6-61 Terminal velocities of spherical particles of different densities settling in air and water at 70°F under the action of gravity. To convert fhs to m/s, multiply by 0.3048. (From Lapple, etal.. Fluid and Particle Mechanics, University of Delaware, Newark, 1951, p. 292. )... [Pg.680]

FIG. 14-58 Typical holdup data for random packings and the air-water system. The raschig rings are of ceramic material. To convert pounds per hour per fr to Idlograms per second per m , multiply hy 0.001.356 to convert inches to millimeters, miinltiplyhy 25.4. [Shulman etal., AIChE J. i, 247 (I.9.5.5).]... [Pg.1393]

FIG. 18-108 Bomb filter for small-scale pressure filtration tests. [Silverhlatt etal., Cbem. Eng., 81(9), 132 (1974), hy permission.]... [Pg.1706]


See other pages where ETALS is mentioned: [Pg.263]    [Pg.665]    [Pg.1112]    [Pg.1298]    [Pg.1394]    [Pg.1505]    [Pg.1685]    [Pg.1707]    [Pg.2159]    [Pg.2206]    [Pg.2344]    [Pg.2820]    [Pg.282]    [Pg.377]    [Pg.138]    [Pg.286]    [Pg.286]    [Pg.288]    [Pg.289]    [Pg.289]    [Pg.290]    [Pg.290]    [Pg.951]    [Pg.151]    [Pg.45]    [Pg.45]    [Pg.45]    [Pg.268]   


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ETAL ANODES

ETAL CLEANERS AND POLISHES

ETAL COMPLEX EQUILIBRIA

ETAL ENOLATES

ETAL IMPURITIES

ETAL INDUCED RADICAL REACTIONS

ETAL SURFACE TREATMENTS

ETAL TREATMENTS

ETAL-MATRIX COMPOSITES

ETAL-ORGANIC COMPOUNDS

ETAL-PROMOTED COUPLING REACTIONS

ETALLIC BONDS

ETALLIC COATINGS

Etale Group Schemes

Etale coverings of formal schemes

Etale finite group scheme

Etale morphisms

Etale morphisms of formal schemes

Etale topology

M etallization

Protocol of Haab etal

SUBSTITUTION REACTION WITH ETALS

Siegmar Diele and Petra Goring etal-containing Liquid Crystals

Snyder etal

Thayer, John S., Not for Synthesis Only The Reactions of Organic Halides with etal Surfaces

Transition etals

Yang etal

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