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Molecule projections

Fig.4 Spin density in the DPPH molecule projected onto a plane containing the two N-atoms of the hydrazyl group. Densities are given in units of e/X negative spin densities are indicated by broken lines. Fig.4 Spin density in the DPPH molecule projected onto a plane containing the two N-atoms of the hydrazyl group. Densities are given in units of e/X negative spin densities are indicated by broken lines.
In order to understand the potency of a given molecule, project scientists must first understand the nature of the measurement used to generate the potency value. If the molecule in question is from a literature report, there may be no in-house data to examine, and in that case the synthesis of the compound and the development of an assay usually becomes a critical first step to understanding the project landscape at that point. More commonly, however, the compound in question has been identified in some type of in-house screening process. These can take many forms, but they can broadly be grouped into two major categories ... [Pg.147]

For this study, p-xylene and triisopropylcyclohexane (TIPcyC6) were the two molecular probes chosen, using toluene as a solvent. Their molecular dimensions were obtained from the shadow of the three-dimensional molecule projected onto a plane according to the method of Rohrbaurgh et al. [5] (Table 2). A molecular probe is considered not to penetrate into a cylindrical pore if two of its dimensions are greater than the pore diameter [6], As the free diameter of the window of the supercage of the Y zeolite is equal to 0.74 nm, it is considered that only TIPCyC6 cannot penetrate into the zeolite microporosity. [Pg.219]

Problem 11-26. From the vector of general displacements of the three atoms of the water molecule, project out the unique normal mode of B2 symmetry. [Pg.114]

Figure 2. The H Ru fCO) molecule, projected onto one of its large open faces (cf. Ref. 27,28). Figure 2. The H Ru fCO) molecule, projected onto one of its large open faces (cf. Ref. 27,28).
Figure 21. The [( -CsMe IrClJzin-Cl) . molecule, projected onto its Ir(fi-Cl)2lr plane (see Ref. 58). Note the obtuse Ir-Cl-Ir angles. Figure 21. The [( -CsMe IrClJzin-Cl) . molecule, projected onto its Ir(fi-Cl)2lr plane (see Ref. 58). Note the obtuse Ir-Cl-Ir angles.
The distances between saturated hydrocarbon molecules in crystals can be calculated by the use of these radii, with consideration also of the possibility of molecular or group rotation. Another factor must be introduced for aromatic molecules.64 The double bonds in these molecules project above and below the plane of the ring in such a way as to give to the ring an effective thickness of about 3.4 A, as observed in anthracene, durene, hexamethylbenzene, benzbisantkrene, and many other aromatic hydrocarbons. The same value is also found between the layer of graphite. [Pg.262]

FIGURE 4. Hexacyclopropylethane (22) molecule projected down the central C—C bond. Drawn after Reference 57... [Pg.149]

Fig. 5. Hexamethylbenzene, showing a single layer of molecules projected on to the (001) plane. The contour lines are drawn at 1 oA 2 intervals. (Brockway and Robertson, J. Chem. Soc., 1939, p. 1330.)... Fig. 5. Hexamethylbenzene, showing a single layer of molecules projected on to the (001) plane. The contour lines are drawn at 1 oA 2 intervals. (Brockway and Robertson, J. Chem. Soc., 1939, p. 1330.)...
If the selfconvolution of the electron density of a molecule (projected onto z) is denoted M(z) and the point-distribution function prescribing how the molecules are repeated along z by D(z), the desired Patterson function is their convolution... [Pg.272]

The final vector comprising of the seven invariant moments represents the distribution of the property P on the bidimensional map. This representation was used to compare bidimensional molecule projections by Carbo similarity index and Hodgkin similarity index. [Pg.420]

Each mitochondrion (plural mitochondria) is bounded by two membranes (Figure 2.24a). The smooth outer membrane is relatively porous, because it is permeable to most molecules with masses less than 10,000 D. The inner membrane, which is impermeable to ions and a variety of organic molecules, projects inward into folds that are called cristae (singular crista). Embedded in this membrane are structures composed of molecular complexes and called respiratory assemblies (described in Chapter 10) that are responsible for the synthesis of ATP. Also present are a series of proteins that are responsible for the transport of specific molecules and ions. [Pg.53]

Figure 8a. The structure of platinum phthalocyanine. Electron density map of the molecule projected on a plane inclined at angle of 26.5 to the plane of the molecule. Figure 8a. The structure of platinum phthalocyanine. Electron density map of the molecule projected on a plane inclined at angle of 26.5 to the plane of the molecule.
The active site zinc ion (see Fig. 11) is located in a shallow cleft which runs across the surface of the protein to the opening of a pocket in the enzyme surface. Note that the three zinc hgands contributed by the protein are positioned away from the cleft, while the inner sphere water molecule projects out into the cleft. The cleft is hned with several highly polar residues in the vicinity of the metal ion which are beheved to participate in substrate binding and/or catalysis. The pocket adjacent to the metal ion is lined with nonpolar (hydrophobic) residues. Both the cleft and the pocket are filled with water molecules which appear to be arranged in an ice-hke array. [Pg.109]

The aim of the projects 1.12 to 1.15 is to examine the convergence of MP perturbation series for very simple molecules (Projects 1.12 and 1.13) and to analyze the effect that the introduction of correlation energy has on the description of simple organic reactions (Project 1.14) and on geometry optimizations (Project 1.15). [Pg.421]

Delgado reports a QSPR model [49] for the prediction of log(l/S) for a set of 50 chlorinated hydrocarbons including chlorinated benzenes, dibenzo-p-dioxins and PCBs. The model involves only two molecular descriptors, one geometry-dependent descriptor and one charged partial surface area (CPSA) descriptor. The geometric descriptor is the area of the shadow of the molecule projected on a plane defined by the X and Y axes XY shadow) the CPSA descriptor is the surface weighted atomic partial negative surface area (WNSA-3). The model has a squared correlation coefficient of 0.97 and standard deviation of 0.45 log units. [Pg.23]

Fig. 31. Heptasilapropellane molecule, projected to the perpendicular molecular axis (above left) and along the molecular axis (above right). Sketches showing variations in the bond lengths (A) and bond angles with mean values stated for all three six-membered rings appear below... Fig. 31. Heptasilapropellane molecule, projected to the perpendicular molecular axis (above left) and along the molecular axis (above right). Sketches showing variations in the bond lengths (A) and bond angles with mean values stated for all three six-membered rings appear below...

See other pages where Molecule projections is mentioned: [Pg.1135]    [Pg.95]    [Pg.74]    [Pg.864]    [Pg.212]    [Pg.70]    [Pg.255]    [Pg.252]    [Pg.253]    [Pg.101]    [Pg.905]    [Pg.674]    [Pg.833]    [Pg.175]    [Pg.116]    [Pg.207]    [Pg.150]    [Pg.214]    [Pg.301]    [Pg.266]    [Pg.221]    [Pg.322]    [Pg.398]    [Pg.391]    [Pg.359]    [Pg.347]    [Pg.141]    [Pg.233]    [Pg.415]    [Pg.261]   
See also in sourсe #XX -- [ Pg.333 ]




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