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Parallel displacement

The initial near-parallel displacement of the curves in Figure 1.26B raises the question of whether the Schild equation would be obeyed under these conditions. If we consider the two concentrations of agonist that give equal responses before and during the action of the antagonist ([A] and r[A], respectively, where r is the concentration ratio) and repeat the derivation set out in Section 1.5.2 (but using Eq. (1.55) rather than (1.49)), we find that the expression equivalent to the Schild equation is ... [Pg.61]

Note, too, the convergence at low agonist concentrations of the curves plotted in Figure 1.27. The antagonist becomes less active when the response is small, because there are fewer receptors in the AR form available to combine with C. Again, in contrast to the other kinds of antagonism that have been described, there is no initial parallel displacement of the curves (even if many spare receptors are present), and the Schild equation is never obeyed. [Pg.63]

A(0) and A(t) are the total surface area before and after the parallel shift. Equation (115) is exactly the definition of the averaged mean, (//), and Gaussian, (K), curvatures. From Eq. (140), (//) and (K) can be deduced from the area variation of the parallel surfaces with the parallel displacement t as a variant. [Pg.211]

Partial uncompetitive inhibition does not resemble full uncompetitive inhibition in terms of having an ordered mechanism, but it instead represents a very specific form of partial mixed inhibition (discussed later). However, it is sometimes referred to as partial uncompetitive inhibition due to the parallel displacement of Lineweaver-Burk plots in the presence of inhibitor, and it is thus related to full uncompetitive inhibition in the same way that partial competitive inhibition is related to full competitive inhibition. [Pg.122]

Smallest, regularly repeating material portion contained in a parallelepiped from which a crystal is formed by parallel displacements in three dimensions [3]. [Pg.82]

During the process of total reflection at a vacuum boundary, the reflected beam has been observed to be subject to a parallel displacement with respect to the incident beam. For this so-called Goos-Hanchen effect, the displacement was further found to have a maximum for parallel polarization of the incident electric field, and a minimum for perpendicular polarization [24,25]. At an arbitrary polarization angle, however, the displacement does not acquire an intermediate value, but splits into the two values for parallel and perpendicular polarization. This behaviour cannot be explained by conventional electromagnetic theory. [Pg.4]

Reaction of the epoxy alcohol with LiBr forms the halohydrin salt that equilibrates to the equatorial-Br conformer, which then undergoes ring contraction via an /-parallel displacement of Br (Step A). Proton transfer (Step B), although proceeding at a slower rate, leads to another anti-parallel Br displacement (Step C), forming the minor product FI. [Pg.96]

Many different structures can be envisaged for the benzene dimer, but three stand out parallel (P), parallel-displaced (PD) and T-shaped perpendicular (T) while for PD and T there are various orientations possible (See Figure 3-6). [Pg.71]

Sinnokrot, M.O. and Sherrill C.D., Highly Accurate Coupled Cluster Potential Energy Curves for the Benzene Dimer Sandwich, T-Shaped, and Parallel-Displaced Configurations. J. Phys. Chem. [Pg.100]

We are concerned with two coordinate systems X Y Z and XYZ, both centered at 0. XYZ is the space-fixed system whereas X Y Z at any time defines a coordinate system floating with respect to XYZ but fixed relative to its central ion to ligand system, whose ligator Lk is situated upon the Z -axis, having polar coordinates (0, coordinate axes has been shown by parallel displacement, in each case, of the origin of X Y Z from 0 to the point (8k, [Pg.80]

Discrete translations on a lattice. A periodic lattice structure allows all possible translations to be understood as ending in a confined space known as the unit cell, exemplified in one dimension by the clock dial. In order to generate a three-dimensional lattice, parallel displacements of the unit cell in three dimensions must generate a space-filling object, commonly known as a crystal. To ensure that an arbitrary displacement starts and ends in the same unit cell it is necessary to identify opposite points in the surface of the cell. A general translation through the surface then re-enters the unit cell from the opposite side. [Pg.5]

Computational studies on the n-n stacking problem began with the simplest model the benzene dimer. While not the only possible configurations, the benzene dimer structures most studied are the sandwiches 77s (D f) and 77s (T>6 ), the parallel displaced 77pd, and the T-shaped configurations 77t and 77t. ... [Pg.173]

Sinnokrot, M. O. Sherrill, C. D. Highly accurate coupled cluster potential energy curves for the benzene dimer sandwich, T-shaped, and parallel-displaced configurations, 7. Phys. Chem. A 2004,108, 10200-10207. [Pg.194]

Arnstein, S. A. Sherrill, C. D. Substituent effects in parallel-displaced n-ic inteac-tions, Phys. Chem. Chem. Phys. 2008,10, 2646-2655. [Pg.195]

It has been experimentally demonstrated that the principles of temperature and concentration superposition of flow curves are applicable to melted keroplasts. In other words, in the fixed matrix FC compositions with different filler content, tp and T measured at different temperatures, can be interpolated through a flat and parallel displacement along the coordinate axes (in double logarithmic coordinates). [Pg.6]

An off-center specimen also leads to an error in (j). Whatever the displacement of the specimen from the camera center, this displacement can always be broken up into two components, one (A.v) parallel to the incident beam and the other (A> ) at right angles to the incident beam. The effect of the parallel displacement is illustrated in Fig. 11-3(a). Instead of being at the camera center C, the specimen is displaced a distance Ax to the point O. The diffraction lines are registered at D and C instead of at A and B, the line positions for a properly centered specimen. [Pg.353]


See other pages where Parallel displacement is mentioned: [Pg.1656]    [Pg.254]    [Pg.232]    [Pg.232]    [Pg.484]    [Pg.107]    [Pg.241]    [Pg.280]    [Pg.869]    [Pg.209]    [Pg.213]    [Pg.62]    [Pg.350]    [Pg.84]    [Pg.403]    [Pg.404]    [Pg.69]    [Pg.313]    [Pg.186]    [Pg.869]    [Pg.66]    [Pg.23]    [Pg.1477]    [Pg.394]    [Pg.124]    [Pg.124]    [Pg.98]    [Pg.213]    [Pg.144]    [Pg.1977]    [Pg.109]    [Pg.290]   
See also in sourсe #XX -- [ Pg.232 ]

See also in sourсe #XX -- [ Pg.232 ]




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