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Configuration a and

In contrast to this the austenite - martensite transition temperature depends on the concentration of vacancies. The configurations A and E show a transition temperature of 10 K, while in C and D the bcc structure already occurs at 100 K. [Pg.98]

The rate equations determine the rate of change of the probability of a particular configuration, a, within an ensemble of growing crystals. They must include the rate constants for adding or subtracting units, which are assumed to obey microscopic reversibility. The net flux between configurations a and a which occur with probability P(a) and P(a ) respectively, and differ by one unit is ... [Pg.298]

Fig. 8. Scheme of the electronic structure of (A) [3Fe-4S] centers and (B) [4Fe-centers according to the standard model. The thin and thick dashed fines indicate the Emtiferromagnetic and double exchEmge coupling, respectively. Configurations a and b correspond to the two possible locations of the excess electron in the mixed-valence pair. In part (B), the local spin values are Sc = Sd = 2 in the case of [4Fe-4S] centers and Sc = Sd = i in the case of [4Fe-4S] + centers. [Pg.441]

A reference configuration with total baryon number Ni> = 1.51 Nq (where Nq is the total baryon number of the sun) is chosen and the case with (configurations A and B in Fig. 13) and without antineutrinos (/ in Fig. 13) are compared. A mass defect can be calculated between the configurations with trapped antineutrinos and without it at a constant total baryon number and the result is shown in Fig. 14). The mass defect could be interpreted as an energy release if the configurations A, B with antineutrinos are initial states and the configuration / without them is the final state of a protoneutron star evolution. [Pg.397]

Measurements on single crystals of lower symmetry doped with NpO or PuOl" " should remove this uncertainty but no such experiment has been performed so far. However, the distinction between configurations (a) and (b) has been possible in an electron paramagnetic resonance study at 20 K on a single uniaxial crystal of RbU02(N03)3 doped with plutonyl ions. This study conclusively showed that the ground state is H4 with gy = 5.4 and g = 0 28). [Pg.388]

Figure 8. (+)-(55)-l,6-spiro[4,4]nonadiene configuration (A) and schematic representation of the puckering of the various conformations (B). (Reproduced with permission from tef. 78. Copyright 1979 American Chemical Society.)... [Pg.158]

It is interesting to note that the relative probability of finding the system with the configuration a and b in the equilibrium state is, according to (3)... [Pg.11]

Fig. 7. This diagram resembles Fig. 5. However, the energy surface is lowered for the isomeric configurations a and b as well as for the activated molecule in the presence of the catalyst. Hence the normal molecules will be more strongly adsorbed than in the case shown in Fig. 5. The activation energy is lowered by a larger amount than the energy of the normal molecules, so that the surface still has a conventional catalytic action. Fig. 7. This diagram resembles Fig. 5. However, the energy surface is lowered for the isomeric configurations a and b as well as for the activated molecule in the presence of the catalyst. Hence the normal molecules will be more strongly adsorbed than in the case shown in Fig. 5. The activation energy is lowered by a larger amount than the energy of the normal molecules, so that the surface still has a conventional catalytic action.
Monosaccharides commonly form internal hemiacetals or hemiketals, in which the aldehyde or ketone group joins with a hydroxyl group of the same molecule, creating a cyclic structure this can be represented as a Haworth perspective formula. The carbon atom originally found in the aldehyde or ketone group (the anomeric carbon) can assume either of two configurations, a and /3, which are interconvertible by mutarotation. In the linear form, which is in equilibrium with the cyclized forms, the anomeric carbon is easily oxidized. [Pg.247]

The dihydroxo-bridged binuclear complexes are among the most common, structurally well-characterized polynuclear complexes. For symmetrical bidentate nonbridging ligands, LL, the cation (LL)2M(OH)2M(LL)2"+ may exist in three isomeric forms a meso isomer (A,A) with configuration A and A, respectively, at the two metal centers, and a racemic pair of isomers (A,A and A, A) with configuration A or A at each of the two metal centers (cf. Fig. 2). If the bidentate... [Pg.66]

These excited states do not all contribute equally and each configuration will interact differently with any given substrate. For example, the most important interactions for configurations (a) and (b) are... [Pg.126]

In the basis of these orthonormal symmetry-adapted functions, matrix elements of the invariant Hamiltonian are given for two different configurations A and B by... [Pg.50]

Tris-chelate complexes exist in enantiomeric configuration A and D about the metal atom, and when the chelating ligand is unsymmetrical, there are also geometrical isomers, cis and trans. Each geometrical isomer exists in enantiomeric forms thus there are four different molecules. In the case of tris complexes with symmetrical ligands, the process of inversion (interconversion of enantiomers) is important. When the metal ions are of the inert type, it is often possible to resolve the complex then the process of racemisation can be followed by measurement of optical rotation as a function of time. Possible pathways for racemisation fall into two broad classes those without bond rupture and those with bond rupture. [Pg.230]

The configurations of SO3 adsorbed on Pt (111) surface are shown in Figure 6.2, and its adsorption energy and geometric data are shown in Table 6.1. Figure 6.2 shows two such configuration A and B where three atoms from the molecule SO3 are bound to Pt surface in both cases, and a fourth atom remains unbound to the Pt surface in each case. In configuration A, two O atoms and one S atom are bound to... [Pg.64]

The S center in configuration B is approximately tetrahedrally bound to three O atoms and apart from surface Pt atom. Here the O-S-O angle is 106°. This angle is close to that of a tetrahedral configuration. Therefore the formations of adsorbed SO3 in both configurations A and B are similar. The S-O bond with the surface bound is 1.669 A, which is longer than that of the calculated S-O bond of the gas phase and is similar to that of the S-O bound to Pt surface in configuration A, 1.69 A. [Pg.66]

The projected DOS of S and O atomic orbital components in configurations A and B are shown in Figure 6.5(a) and (b), which display direct comparison between Pt (111) surface and S03 molecule, and S03 adsorbed on Pt (111) surface. In Figure 6.5(a), O component of S03 molecule is divided into two atoms and one atom in order to compare 0(1) and 0(2) with O component in SO3 molecule. [Pg.67]

The structure of the simple hydroxamate complex tris(benzohy-droxamato) iron (III) (R = , R = H in Figure 1) has shown the most stable crystalline form of the solid to be the racemic cis isomer (11). (The convention for symbols of absolute configurations A and A are those of the IUPAC Proposal (12). The cis isomer is defined as the isomer... [Pg.40]

In a derivation, quite analogous to that on p. 132 but now for two different configurations A and B, there arises the determinant ... [Pg.201]

We have seen (p. 201) that when the wave function, which represents the stationary state, can be regarded as composed of two wave functions, corresponding to two configurations A and B, 9 = CAenergy difference between A and B. [Pg.256]

Rotamers around C(l)—C(2) in 418 are separated by very low energy barriers and are not distinguishable by NMR spectroscopy. Enaminoesters with R4 = R5 can adopt either the E or the Z configuration (A and B Scheme 10) around C(2)=C(3). Secondary enaminoesters (R4 H R5 = H) can exist in forms C-E and in the tautomeric imino form F. Isomers similar to J-L (Scheme 5) with R1 = OAlkyl, which are sterically very crowded, have not been observed. The imino form (F) exists when severe steric hindrance prevents planarity and conjugation of 418. [Pg.353]

FIGURE 5. Electrostatic potentials of vinylamine with respect to a positive point charge. Equipotential curves through planes parallel to the CCN plane at a distance d— 1.220 A for non-planar equilibrium configuration (a) and d = 1.292 A for the all planar structure (b). All energies in kcalmol-1. Reproduced by permission of Helvetica Chimica Acta from Reference 23... [Pg.711]


See other pages where Configuration a and is mentioned: [Pg.582]    [Pg.222]    [Pg.430]    [Pg.444]    [Pg.354]    [Pg.387]    [Pg.12]    [Pg.59]    [Pg.39]    [Pg.278]    [Pg.346]    [Pg.120]    [Pg.53]    [Pg.475]    [Pg.20]    [Pg.615]    [Pg.616]    [Pg.703]    [Pg.344]    [Pg.63]    [Pg.67]    [Pg.74]    [Pg.77]    [Pg.77]    [Pg.78]    [Pg.394]    [Pg.180]    [Pg.966]    [Pg.55]   
See also in sourсe #XX -- [ Pg.3 , Pg.1034 , Pg.1160 ]

See also in sourсe #XX -- [ Pg.3 , Pg.1034 , Pg.1160 ]

See also in sourсe #XX -- [ Pg.3 , Pg.1034 , Pg.1160 ]

See also in sourсe #XX -- [ Pg.3 , Pg.980 ]

See also in sourсe #XX -- [ Pg.3 , Pg.1030 , Pg.1180 ]

See also in sourсe #XX -- [ Pg.3 , Pg.953 ]




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