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Centroid volume

A perpendicular line drawn through the centroid volume will thus define two regions of equal area, as illustrated in figure lb. There are several ways of determining the centroid elution volume and these will be discussed in Section 3. [Pg.377]

Fig. 1. Chromatograms illustrating difference between a small zone (a) and a large zone (b) size exclusion experiment. In the saull zone experiment, the elution volume, V, is taken as the apex of the peak In a large zone experiment, the elutxon volume is the centroid volume, V, of the leading boundary. The shaded areas represent the volume loaded onto the column in each case. Fig. 1. Chromatograms illustrating difference between a small zone (a) and a large zone (b) size exclusion experiment. In the saull zone experiment, the elution volume, V, is taken as the apex of the peak In a large zone experiment, the elutxon volume is the centroid volume, V, of the leading boundary. The shaded areas represent the volume loaded onto the column in each case.
The steps involved in data reduction are outlined in Table 1. The centroid volume, V, is determined for each concentration by one of the methods described above. These values of V are plotted as a function of concentration with the elution values of the standard proteins used to calibrate the column indicated on the ordinate. If V decreases with increasing concentration, this Indicates that the protein is self-associating under the experimental conditions and that an equilibrium exists. No decrease in V means that the protein is not self-associating and the experiment is over. The next step is to calculate for each value of V using equation (8) and to decide on a plausible self-association model to fit the data. Examination of the plot of V as a function of concentration should aid in this decision. For example, if all of the data points fall between the monomer and dimer elution points (as determined from the column calibration), then the equilibrium is probably a monomer-dimer selfassociation. [Pg.385]

The foregoing are volume integrals evaluated over the entire volume of the rigid body and dw is an infinitesimal element of weight. If the body is of uniform density, then the center of gravity is also called the centroid. Centroids of common lines, areas, and volumes are shown in Tables 2-1, 2-2, and 2-3. For a composite body made up of elementary shapes with known centroids and known weights the center of gravity can be found from... [Pg.142]

It is worth noting what determines elastic resistance to shear. Both shape changes and volume changes are determined by the behavior of the valence electrons in materials, but in quite different ways. Volume changes affect the average distances between the electrons, and between the valence electrons and their associated positive nuclei. Shear changes have little, or no, effect on these average distances because small shears do not affect volumes. However, shear causes a shift in the centroid of the electrons relative to the nucleus. [Pg.197]

We have recently demonstrated the ability of six resorcin[4]arenes and eight water molecules to assemble in apolar media to form a spherical molecular assembly which conforms to a snub cube (Fig. 9.3). [10] The shell consists of 24 asymmetric units - each resorcin[4]arene lies on a four-fold rotation axis and each H2O molecule on a three-fold axis - in which the vertices of the square faces of the polyhedron correspond to the corners of the resorcin[4]arenes and the centroids of the eight triangles that adjoin three squares correspond to the water molecules. The assembly, which exhibits an external diameter of 2.4 nm, possesses an internal volume of about 1.4 A3 and is held together by 60 O-H O hydrogen bonds. [Pg.145]

Based on the flow analysis network, Wang etal., [18] and Osswald [11] developed the finite element/control volume appproach (FEM-CVA) for injection and compression molding, respectively. Similar to FAN, FEM-CVA assigns a fill factor to every nodal point or nodal control volume. The nodal control volumes are constructed by connecting element centroids to element midsides, as shown in Fig. 9.28. [Pg.493]

Based on the control volume approach and using the three-dimensional finite element formulations for heat conduction with convection and momentum balance for non-Newtonian fluids presented earlier, Turng and Kim [10] and [17] developed a three-dimensional mold filling simulation using 4-noded tetrahedral elements. The nodal control volumes are defined by surfaces that connect element centroids and sides as schematically depicted in Fig. 9.33. [Pg.497]

The element side surfaces are formed by lines that connect the centroid of the triangular side and the midpoint of the edge. Kim s definition of the control volume fill factors are the same as described in the previous section. Once the velocity field within a partially filled mold has been solved for, the melt front is advanced by updating the nodal fill factors. To test their simulation, Turng and Kim compared it to mold filling experiments done with the optical lenses shown in Fig. 9.34. The outside diameter of each lens was 96.19 mm and the height of the lens at the center was 19.87 mm. The thickest part of the lens was 10.50 mm at the outer rim of the lens. The thickness of the lens at the center was 6 mm. The lens was molded of a PMMA and the weight of each lens was 69.8 g. [Pg.497]

We wish to point out, that by use of a suitable fiber which further broadens the spectrum, this fs laser frequency measurement technique has now been simplified to a setup with a single laser, as described elsewhere in this volume [6]. With the technique of Fig. 6, the 15 — 25 transition frequency was measured twice, first with a GPS referenced commercial Cs clock [29], and second with a transportable Cs atomic fountain clock constructed by A. Clairon and coworkers in Paris [30]. A total of 614 spectral lines was recorded in the latter measurement during ten days, and fitted with the described line shape model [13]. After adding a correction of 310 712 233(13) Hz to account for the hyperfine splitting of the 15 and 25 levels, we obtain for the hyperfine centroid [28] ... [Pg.27]

Now consider a ring-shaped differential volume element of radius r, thickness dr, and length dx oriented coaxially with the tube, as shown in Fig. 8-17. The volume clement involves only pressure and viscous effects and thus the pressure and shear forces must balance each other. The pressure force acting on a submerged plane surface is the product of the pressure at the centroid of the surface and the surface area. A force balance on the volume element in the flow direction gives... [Pg.481]

CN - coordination number Nf- average number of faces of the VDPs N t, - average number of non-bonding contacts per one U-O bond PVdp -volume of the VD polyhedron Svdp - total area of faces of the VDP Rsd- radius of the sphere with volume equal to that of the VDP Da -vector that originates in the U atom and ends in the centroid of the VD polyhedron G3-the second moment of inertia, which describes deviation of the VD polyhedron from ideal sphere A - difference between the shortest and the longest bonds in the coordination polyhedron p - total number of faces. Standard deviations are given in parentheses. [Pg.42]

In an FV method, the whole solution domain is subdivided into a finite number of contiguous control volumes. The computational node is located at the centroid of each control volume, whereas the node is located at the grid in the FD method. The FV method uses the integral form of the conservation equation... [Pg.255]

Figure 2.1 An eleniontul volume of fluid, fixed in space, through which dirfu.sion is occurring in all directions. At the centroid of the element, flic [mrlicle (lux in the x direction is given by Jx. The flux across one face. A BC D, is shown. Figure 2.1 An eleniontul volume of fluid, fixed in space, through which dirfu.sion is occurring in all directions. At the centroid of the element, flic [mrlicle (lux in the x direction is given by Jx. The flux across one face. A BC D, is shown.
Averaging the pore scale transport process over the REV and assigning the average properties to the centroid of the REV results in continuous functions in space of the hydrodynamic properties and state variables. As for the flow equation (1), differential calculus can be applied to establish mass and momentum balance equations for infinitesimal small soil volume and time increments. For the case of inert solute transport in a macroscopic homogeneous soil, the general continuity equation applies ... [Pg.75]


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