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Asymmetric stationary solution

The first two plots correspond to low ei (ei = 0.02). For small e2 (e2 = 0.02) the extremum corresponding to stable solutions is such that Avj = 7T (<7i = 0, <72 = 7r). In this solution, the periapses are anti-aligned. When e2 is larger (e2 = 0.04 in the right-hand plot), the extremum seen in the left-hand plot becomes a saddle point and a bifurcation gives rise to two extrema symmetric with respect to the saddle. These extrema correspond to asymmetric stationary solutions where Aw = <72 — <7i... [Pg.278]

However, in this case it is no longer possible to prove that J = 0. One cannot exclude the possibility of a constant flow from — oo to +00, as in the asymmetric random walk. Such solutions would describe, for instance, diffusion in an open system, such as diffusion through a medium between two reservoirs with different densities. The stationary solution is no longer unique, but depends on the current J, which depends on additional information concerning the physical problem one is dealing with. See Exercise. [Pg.141]

Gil-Av et al. argued that the separation of the antipodes on a suitable asymmetric stationary phase would involve reversible association between the enantiomers and the asymmetric stationary phase molecules. The two antipodes would form diastereoisomeric interaction with somewhat different interatomic distances. Hence, there would be different polar, dispersive and/or steoric interactions between substituents situated round the asymmetric centers of the solute and stationary phase molecules, respectively. Such differences would effect the standard free energy of distribution and the magnitude of the distribution coefficients of the enantiomers. Gil-Av et al. used A-TFA-D-isoleucine lauryl ester and A-TFA-L-isoleucine lauryl ester as the stationary phase which were coated on the walls of a capillary column 100 m long, 250 pm I.D. and was shown to have an efficiency of about 98,000 theoretical plates. The samples of the derivatized amino acids were injected with a split ratio of 1 100. The separation was carried out isothermally at 90°C and the analysis time was just over 4 hours. The results obtained for the... [Pg.108]

Nonideal asymmetrical chromatographic bands showing (a) fronting and (b) tailing. Also depicted are the corresponding sorption isotherms showing the relationship between the concentration of solute in the stationary phase as a function of its concentration in the mobile phase. [Pg.555]

The isomerism of a- and jS-glucose is to be attributed to the spatially different arrangement of the H and OH-groups attached to the asymmetric carbon atom 1. This atom is asymmetric in the cyclic lactol formula (Tollens). The mutarotation of the sugars, i.e. the gradual change to the final stationary value of the optical rotation, is to be explained by an equilibrium occurring in solution between the various... [Pg.395]

B Feibush. Interaction between asymmetric solutes and solvents. A-Lauroyl-valyl-t-butylamide as a stationary phase in gas liquid chromatography. J Chem Soc Chem Commun 544, 1971. [Pg.121]

In an N-NDR model Christoph et al. [35, 37] found stable target patterns coexisting with the pulse solution for values of the external voltage for which the stationary state is also unstable with respect to homogeneous perturbations. In contrast, the asymmetric target patterns and the more complex motions observed during H2 oxidation on Pt ring electrodes (cf. Fig. 56) have not yet been reproduced in simulations. [Pg.180]

Note that co-elution of the analyte and IPR in the form of an ion-pair is not a rule. A dynamic distribution equilibrium of both the IPR and analyte between the plug of injected sample and the stationary phase may also involve a separation of the ion-pair partners if their retention free energies are very different. Moreover, since the hydrophobicities of the analyte and the ion-pair between analyte and IPR differ, a split, broad, or asymmetric peak may also be observed. This happens if the rate of interconversion between the free and paired analyte is slow compared to the chromatographic retention time scale and this downside can be observed in Figure 11.1 [25]. In this case, the analyte-IPR ion-pair would not be detected via MS [26]. Interestingly, analyte retention increased with the alkyl chains of the IPR in the reconstitution solution, similar to traditional IPC [26]. [Pg.127]

B. Feibush and E. GU-Av, Interaction between asymmetric solutes and solvents. Peptide derivatives as stationary phases in gas liquid partition chromatography. Tetrahedron 26 (1970), 1361. [Pg.1043]

Figure 8. Loci of the stationary corotation solutions of the 2/1 resonance for several mass ratios m2/mi. Top figures correspond to the symmetric solutions of the two left-hand side plots in Figure 6. The points corresponding to two early determinations of the elements of Gliese 876 are shown in one of these plots. The bottom figure corresponds to the asymmetric solutions of the two right-hand side plots in Figure 6. The line across these curves shows the values of the eccentricities for which 0.63(1 + ei) = (1 — e2). In all panels, the thick line shows the boundary between the domains of symmetric and asymmetric solutions. Figure 8. Loci of the stationary corotation solutions of the 2/1 resonance for several mass ratios m2/mi. Top figures correspond to the symmetric solutions of the two left-hand side plots in Figure 6. The points corresponding to two early determinations of the elements of Gliese 876 are shown in one of these plots. The bottom figure corresponds to the asymmetric solutions of the two right-hand side plots in Figure 6. The line across these curves shows the values of the eccentricities for which 0.63(1 + ei) = (1 — e2). In all panels, the thick line shows the boundary between the domains of symmetric and asymmetric solutions.
Fig. 8.26 Sketch of the solute drag effect produced by the segregation of dopants to the grain boundaries, a Symmetrical distribution of the dopant in the region of a stationary grain boundary, b For a moving boundary, the dopant distribution becomes asymmetrical if the diffusion coefficient of the dopant atoms across the boundary is different from that of the host atoms. The as5nnmetrical distribution produces a drag on the boundary, c Breakaway of the boundary from the dopant leaving a solute cloud behind. Reproduced with permission from [4]. Cop5urght 2003, CRC Press... Fig. 8.26 Sketch of the solute drag effect produced by the segregation of dopants to the grain boundaries, a Symmetrical distribution of the dopant in the region of a stationary grain boundary, b For a moving boundary, the dopant distribution becomes asymmetrical if the diffusion coefficient of the dopant atoms across the boundary is different from that of the host atoms. The as5nnmetrical distribution produces a drag on the boundary, c Breakaway of the boundary from the dopant leaving a solute cloud behind. Reproduced with permission from [4]. Cop5urght 2003, CRC Press...
The main result of the above described experiments consists in the possibility of non-stationary synthesis of ATP from ADP and P in homogeneous solutions of the coupling factors of chloroplasts at acid-base shift, with the yield of about 6 mol ATP per mol protein in the absence of any asymmetric membrane structure. [Pg.2007]


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