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Contoured surface

These are typical of ionic liquids and are familiar in simulations and theories of molten salts. The indications of structure in the first peak show that the local packing is complex. There are 5 to 6 nearest neighbors contributing to this peak. More details can be seen in Figure 4.3-3, which shows a contour surface of the three-dimensional probability distribution of chloride ions seen from above the plane of the molecular ion. The shaded regions are places at which there is a high probability of finding the chloride ions relative to any imidazolium ion. [Pg.160]

Figure 5 Free energy surface at l l(Fig. 5a) [22, 24, 28] and 1 3 (Fig. 5b) [23, 24, 33] stoichiometries in the vicinity of disordered state ( f=0.0) at T—. 7Q and 1.6, respectively. The solid line in left-hand (right-hand) figure indicates the kinetic path evolving towards the L q LI2 ordered phase when the system is quenched from T—2.5 (3.0) down to 1.70 (1.60), while the broken lines are devolving towards disordered phase. The open arrows on the contour surface designate the direction of the decrease of free energy, and the arrows on the kinetic path indicate the direction of time evolution or devolution. Figure 5 Free energy surface at l l(Fig. 5a) [22, 24, 28] and 1 3 (Fig. 5b) [23, 24, 33] stoichiometries in the vicinity of disordered state ( f=0.0) at T—. 7Q and 1.6, respectively. The solid line in left-hand (right-hand) figure indicates the kinetic path evolving towards the L q LI2 ordered phase when the system is quenched from T—2.5 (3.0) down to 1.70 (1.60), while the broken lines are devolving towards disordered phase. The open arrows on the contour surface designate the direction of the decrease of free energy, and the arrows on the kinetic path indicate the direction of time evolution or devolution.
We need ways to visualize electrons as particle-waves delocalized in three-dimensional space. Orbital pictures provide maps of how an electron wave Is distributed In space. There are several ways to represent these three-dimensional maps. Each one shows some important orbital features, but none shows all of them. We use three different representations plots of electron density, pictures of electron density, and pictures of electron contour surfaces. [Pg.475]

Orbital density pictures are probably the most comprehensive views we can draw, but they require much time and care. An electron contour drawing provides a simplified orbital picture. In this representation, we draw a contour surface that encloses almost all the electron density. Commonly, almost all means 90%. Thus, the electron density is high inside the contour surface but very low outside the surface. Figure 7-19c shows a contour drawing of the 2s orbital. [Pg.476]

A useful analogy for understanding the value of contour surfaces is a swarm of bees around a hive. At any one time, some bees will be off foraging for nectar, so a contour surface drawn around all the bees might cover several acres. This would not be a very useful map of bee density. A contour surface containing 90% of the bees, on the other hand, would be just a bit bigger than the hive itself This would be a very useful map of bee density, because anyone inside that contour surface would surely interact with bees. [Pg.476]

C07-0084. The conventional method of showing the three-dimensional shape of an orbital is an electron contour surface. What are the limitations of this representation ... [Pg.495]

The rate constants for deblocking and cure can be obtained by monitoring the concentration of free isocyanate during cure. In the absence of actual concentration data it is possible to obtain good values for the rate constants using a normalization procedure. In addition to the normalization procedure used in this work it is possible to define other normalization functions which may produce significant changes in the contour surface over which the search occurs. [Pg.253]

The first graphical representation using MATLAB software is that of a two-dimensional contour surface plot of the data from Table 75-1 [2], This Figure 75-3 plot can represent multiple levels of j-axis data (absorbance) by the use of contours and color schemes. The MATLAB commands for generating this image are given in Table 75-2 where A represents the raster data matrix shown in Table 75-1. [Pg.505]

M. Mrksich, C.S. Chen, Y. Xia, L.E. Dike, D.E. Ingber, and G.M. Whitesides, Controlling cell attachment on contoured surfaces with self-assembled monolayers of alkanethiolates on gold. Proc. Natl. Acad. Sci. U.SA 93, 10775-10778 (1996). [Pg.401]

To get the orbital shape it is necessary to draw contour surfaces of constant probability density. For the py orbital the cross section in the yz plane is first obtained and rotated about the y-axis. In the yz plane, (j) = 7t/2, sin > = 1, and hence... [Pg.218]

Fig.4 (see p. 74/75) shows all localized orbitals for the ground state of the BH molecule and the 12 excited state of B2.37) These are again rotationally symmetric orbitals, i.e., sigma type orbitals, and the complete contour surfaces can be obtained by spinning around the indicated axis. In all orbitals shown the outermost contour corresponds to a wavefunction value of 0.025 Bohr-3/2. For all valence shell orbitals the increment from one contour to another is 0.025 Bohr-3/2. For the inner shells the increment is again 0.2 Bohr 3/2, but only three contours and the wavefunction values at the nuclear positions are shown. [Pg.51]

The analytical expressions of the various wave functions, for the ground state (n = 1) and for orbitals 2p and 3d, are listed in figure 1.15. The same figure also shows the form (actually, the contour surface) attained by the five ADs of sub-level 3d and, for comparative purposes, the three ADs of sublevel 2p and the AD s for the ground state (n = 1). The orientation of the atomic orbitals depends on angular factor xf/i and not on principal quantum number n. Orbitals of the same / thus have the same orientation, regardless of the value of n. [Pg.65]

Smoothed contour surface maps (contour maps where the areas between the isolines are filled with colours) were produced. [Pg.386]

Groenewold, G. H. Rehm, B. W. 1982. Instability of contoured surface-mined landscapes in the northern Great Plains causes and implications. [Pg.205]

Fig. 3. Early method of contour surface mining. This was the predominant way of mining throughout Appalachia until passage of stringent legislation that ushered in a new integrated mining technique. [Caterpillar Ini)... Fig. 3. Early method of contour surface mining. This was the predominant way of mining throughout Appalachia until passage of stringent legislation that ushered in a new integrated mining technique. [Caterpillar Ini)...
The theory suggests that the behavior of each electron in an atom can be described by a wave function (i//), which is a function of the space coordinates of the electron and thus has spatial characteristics. These one electron wave functions are called atomic orbitals (AOs). Atomic orbitals describe electron densities in the atom at various distances and directions from the nucleus. By choosing a low constant absolute value for the wave function, a contour surface can be constructed. The probability of finding an electron ([Pg.5]

Figure 5.1 Seasonable February morning in Maine. Lines of constant temperature (isotherms) allow plotting a two-dimensional function without using the third dimension. This is a contour map of t(x,y), giving the temperature t at all locations x,y). Along each contour line lie all points having the same temperature. A planar contour map of a function of two variables takes the form of contour lines on the plane. In contrast, a contour map of a function of three variables takes the form of contour surfaces in three dimensions (see Plate 2). Figure 5.1 Seasonable February morning in Maine. Lines of constant temperature (isotherms) allow plotting a two-dimensional function without using the third dimension. This is a contour map of t(x,y), giving the temperature t at all locations x,y). Along each contour line lie all points having the same temperature. A planar contour map of a function of two variables takes the form of contour lines on the plane. In contrast, a contour map of a function of three variables takes the form of contour surfaces in three dimensions (see Plate 2).
In X-ray crystallography, 2-A model" means that analysis included reflections out to a distance in the reciprocal lattice of 1/(2 A) from the center of the diffraction pattern. This means that the model takes into account diffraction from sets of equivalent, parallel planes spaced as closely as 2 A in the unit cell. (Presumably, data farther out than the stated resolution was unobtainable or was too weak to be reliable.) Although the final 2-A map, viewed as an empty contour surface, may indeed not allow us to discern adjacent atoms, structural constraints on the model greatly increase the precision of atom positions. The main constraint is that we know we can fit the map with groups of atoms — amino-acid residues — having known connectivities, bond lengths, bond angles, and stereochemistry. [Pg.163]

T can be calculated (7). Therefore, it is possible to carry out relaxation time measurements in such a way as to obtain xfa, the volume fraction of the solvent bouijid to the contour surface of the tactoid. Indeed, in that case T. appears as a linear function of the content in solid (Figure 2) because x x l. If the interlayer water were taking part in the exchange (that s, if T T ) the slope (xfa + x.) of the linear relationship would be larger than that observed. On th other hand, if x was changing with the solid content, then T would not be linear with respect to the concentration in solid. [Pg.363]

To summarize at this point, it is reiterated that wavefunction tjr r,6,three-dimensional shape of each orbital can be represented by a contour surface, on which every point has the same value off. The three-dimensional shapes of nine hydrogenic orbitals (2s, 2p, and 3d) are displayed in Fig. 2.1.5. In these orbitals, the nodal surfaces are located at the intersections where f changes its sign. For instance, for the 2p orbital, the yz plane is a nodal plane. For the 3d y orbital, the xz and yz plane are the nodal planes. [Pg.38]

The distribution of flow about a circular opening under suction has been investigated by the author (1939) and the flow pattern is as shown in Figure 129. The various contours are expressed as percentages of the velocity at the tip. Furthermore, when the coordinates are expressed in terms of the tip diameter, the contours for all openings are identical and their absolute values are functions of the velocity at the opening. Thus, what is important to consider is the ratio Q/A At, where A is the area of the pipette opening. Let us assume for the sake of a concrete example that Q = 10 cu cm, A = 0.01 sq cm, and At = 2 sec. Then the flow at the pipette tip is 500 cu cm per sec. It may be shown that this volume is confined within the 0.5 percent velocity contour. This conforms with a velocity contour surface of 0.005 X 500 = 2.5 cm per sec. Hence all particles... [Pg.484]

A more limited number of formulations available than with liquids or pastes Parts that must generally be designed to hold the melt before it cures to a solid Difficulties that can occur in application of solids to vertical or contoured surfaces Heat required to make the solid epoxy adhesives flow and cure... [Pg.244]

An electron density contour surface piece with a larger Betti number usually (but not necessarily) has the larger surface area. If this is the case, then the sequence of Betti numbers in the above ordering is the same as the decreasing sequence of the Betti numbers. [Pg.211]


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Contour

Contour surface plot

Contour surfaces

Electron density contour surfaces

Excited state surface equipotential contours

Fluorescence surface contour plot

Isodensity contour surface

Molecular Contour Surfaces

Molecular isodensity contour surface

Molecular isodensity contour surface concept

Potential energy surfaces contour plot

Response surface models contour plot

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