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Ellipsoidal shapes

The first of these was by Vieillard-Baron [5] who investigated a system of spherocylinders but failed to detect a liquid crystal phase primarily because the anisometry, L/D, of 2 was too small [37]. He also attempted to study a system of 2392 particles with the larger L/D of 5 but these simulations had to be abandoned because of their large computational cost. However, in view of the ellipsoidal shape of the Gay-Berne particles it is the behaviour of hard ellipsoids of revolution which is of primary relevance to us. [Pg.81]

In a steady rotational shear field a spherical micro-organism with a soft wall will be deformed to an ellipsoidal shape. The deformation, M, is defined in... [Pg.110]

Fig. 22. Spherical drop deformed into an ellipsoidal shape in a rotational shear field [76]... Fig. 22. Spherical drop deformed into an ellipsoidal shape in a rotational shear field [76]...
Mature human albumin consists of one polypeptide chain of 585 amino acids and contains 17 disulfide bonds. By the use of proteases, albumin can be subdivided into three domains, which have different functions. Albumin has an ellipsoidal shape, which means that it does not increase the viscosity of the plasma as much as an elongated molecule such as fibrinogen does. Because of its relatively low molecular mass (about 69 kDa) and high concentration, albumin is thought to be responsible for 75-80% of the osmotic pressure of human plasma. Electrophoretic smdies have shown that the plasma of certain humans lacks albumin. These subjects are said to exhibit analbuminemia. One cause of this condition is a mutation that affects spUcing. Subjects with analbuminemia show only moderate edema, despite the fact that albumin is the major determinant of plasma osmotic pressure. It is thought that the amounts of the other plasma proteins increase and compensate for the lack of albumin. [Pg.584]

Our interest is two-fold, we wish to know whether the defect is firstly structurally localised and secondly electronically locaHsed. Our second interest extends to know how important is the continuous surface arising from the spherical shape of Cea or the ellipsoidal shape of C o. [Pg.451]

Figure 4.16 Double bond (a) Lewis model of two tetrahedra sharing an edge, (b) Domain model the two single electron pair domains of the double bond are pulled in toward each other by the attraction of the two carbon cores forming one four-electron double-bond domain with a prolate ellipsoidal shape, thereby allowing the two hydrogen ligands to move apart. Figure 4.16 Double bond (a) Lewis model of two tetrahedra sharing an edge, (b) Domain model the two single electron pair domains of the double bond are pulled in toward each other by the attraction of the two carbon cores forming one four-electron double-bond domain with a prolate ellipsoidal shape, thereby allowing the two hydrogen ligands to move apart.
Let (512, S3) be the coordinates of reflection maxima determined on radial rays in the scattering pattern. Then a linearizing plot of the ellipsoidal shape is... [Pg.225]

The Ulsan carbonates (Fig. 1) have long been interpreted as limestone of Paleozoic age or "age unknown" and as the host of a skarn-type iron (magnetite) deposit due to the intrusion of Cretaceous granitic rocks (Park Park 1980 Choi et al. 1999). However, a Paleozoic marine limestone hypothesis fails to explain the spatial association or the relationship between carbonate and ultramafic rocks in a concentric, ellipsoidal shape surrounded by Cretaceous sedimentary, volcanic, and granitic rocks. The sedimentary hypothesis also fails to explain the isolated exposure of a funnel-shaped Paleozoic marine limestone where no marine limestone has been previously observed within the Mesozoic Kyongsang Basin. [Pg.493]

A better measure of the precision of the parameter estimates for nonlinear models is provided by Eq. (56), which can take into account deviations of the sums-of-squares contours from the ellipsoidal shape. In fact, this equation does provide a rigorous confidence contour for nonlinear models it is only the exact confidence level, a, associated with this contour that is approximated. [Pg.128]

The insight from AFM images may be greatly boosted by sophisticated image analysis. Fritzsche and Henderson [30,31] have extracted cross-sections of nucleosomes at half-maximum height and have fitted them to virtual ellipsoids. These ellipsoids had relatively smooth perimeter and an aspect ratio of 1.2 1.4 moreover, the orientation of the ellipsoids was correlated with the direction of the fiber axis, with more than 50% of nucleosomes aligned with the axis. While this orientation effect may result from surface interactions, as discussed by the authors themselves, it may also represent an actual, and structurally important, feature of fiber structure. Ellipsoid-shaped nucleosomes have been reported in electron EM studies [32,33], and have been predicted in models of chromatin... [Pg.377]

Equation (3-33) shows how the inertia term changes the pressure distribution at the surface of a rigid particle. The same general conclusion applies for fluid spheres, so that the normal stress boundary condition, Eq. (3-6), is no longer satisfied. As a result, increasing Re causes a fluid particle to distort towards an oblate ellipsoidal shape (Tl). The onset of deformation of fluid particles is discussed in Chapter 7. [Pg.44]

The conditions under which fluid particles adopt an ellipsoidal shape are outlined in Chapter 2 (see Fig. 2.5). In most systems, bubbles and drops in the intermediate size range d typically between 1 and 15 mm) lie in this regime. However, bubbles and drops in systems of high Morton number are never ellipsoidal. Ellipsoidal fluid particles can often be approximated as oblate spheroids with vertical axes of symmetry, but this approximation is not always reliable. Bubbles and drops in this regime often lack fore-and-aft symmetry, and show shape oscillations. [Pg.169]

Figure 12.6 Calculated absorption spectra of aluminum spheres, randomly oriented ellipsoids (geometrical factors 0.01, 0.3, and 0.69), and a continuous distribution of ellipsoidal shapes (CDE). Below this is the real part of the Drude dielectric function. Figure 12.6 Calculated absorption spectra of aluminum spheres, randomly oriented ellipsoids (geometrical factors 0.01, 0.3, and 0.69), and a continuous distribution of ellipsoidal shapes (CDE). Below this is the real part of the Drude dielectric function.

See other pages where Ellipsoidal shapes is mentioned: [Pg.679]    [Pg.110]    [Pg.161]    [Pg.258]    [Pg.807]    [Pg.812]    [Pg.204]    [Pg.71]    [Pg.87]    [Pg.91]    [Pg.100]    [Pg.124]    [Pg.63]    [Pg.406]    [Pg.650]    [Pg.45]    [Pg.128]    [Pg.224]    [Pg.199]    [Pg.308]    [Pg.373]    [Pg.273]    [Pg.393]    [Pg.61]    [Pg.72]    [Pg.74]    [Pg.108]    [Pg.232]    [Pg.216]    [Pg.353]    [Pg.354]    [Pg.356]    [Pg.376]    [Pg.466]    [Pg.9]    [Pg.678]    [Pg.596]    [Pg.523]   


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