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Triangular

Thomas A. Albright, Jeremy K. Burdett, and Myung-Hwan Whangbo. [Pg.78]

Assembly of the orbital interaction diagram for equilateral triangular H3 (Dsh) from those of H2 + H. [Pg.79]

5 MOLECULAR ORBITAL CONSTRUCTION FROM FRAGMENT ORBITALS [Pg.80]

An orbital correlation diagram linking the level structures of linear and equilateral [Pg.81]


The discussion here is confined to the more common type of foam, the polyederschaum and their interesting geometric aspects. If three bubbles are joined, as in Fig. XIV-13, the three separating films or septa meet to form a small triangular column of liquid (perpendicular to the paper in the figure)... [Pg.519]

Fig. XVII-18. Contours of constant adsorption energy for a krypton atom over the basal plane of graphite. The carbon atoms are at the centers of the dotted triangular regions. The rhombuses show the unit cells for the graphite lattice and for the commensurate adatom lattice. (From Ref. 8. Reprinted with permission from American Chemical Society, copyright 1993.)... Fig. XVII-18. Contours of constant adsorption energy for a krypton atom over the basal plane of graphite. The carbon atoms are at the centers of the dotted triangular regions. The rhombuses show the unit cells for the graphite lattice and for the commensurate adatom lattice. (From Ref. 8. Reprinted with permission from American Chemical Society, copyright 1993.)...
Figure A2.3.28 Square and triangular lattices and their duals. The square lattice is self-dual. Figure A2.3.28 Square and triangular lattices and their duals. The square lattice is self-dual.
Figure A3.10.9 STM images of Si(l 11) surfaces before (a) and after (b) etching by bromine at 675 K. In (a) the (7 X 7) reconstmcted surface is seen. In (b), the rest layer consisting of triangular arrays of Si atoms has been exposed by etehing [28], Both images show a 17 x 17 mn area. Figure A3.10.9 STM images of Si(l 11) surfaces before (a) and after (b) etching by bromine at 675 K. In (a) the (7 X 7) reconstmcted surface is seen. In (b), the rest layer consisting of triangular arrays of Si atoms has been exposed by etehing [28], Both images show a 17 x 17 mn area.
Pulsed-force mode AFM (PFM-AFM) is a method introduced for fast mapping of local stiffness and adliesion with lower required data storage than recording force-distance curves at each point on the x-y plane [115]. A sinusoidal or triangular modulation is applied between the tip and sample (either via lever or sample piezo) at a lower frequency than that of either the piezo or cantilever resonance frequency. Tip and sample then come... [Pg.1700]

Salsburg Z W, Jacobson J D, Fickett W and Wood W W 1959 Application of the Monte Carlo method to the lattice gas model. Two dimensional triangular lattice J. Chem. Phys. 30 65-72... [Pg.2280]

Figure 4. Triangular phase diagram, showing partitions of R q, and Rq, at fixed... Figure 4. Triangular phase diagram, showing partitions of R q, and Rq, at fixed...
Figure 3. Relaxed triangular plot [68] of the U3 ground-state potential energy surface using hyperspherical coordinates. Contours, are given by the expression (eV) — —0.56 -t- 0.045(n — 1) with n = 1,2,..,, where the dashed line indicates the level —0.565 eV. The dissociation limit indicated by the dense contouring implies Li2 X Sg ) -t- Li. Figure 3. Relaxed triangular plot [68] of the U3 ground-state potential energy surface using hyperspherical coordinates. Contours, are given by the expression (eV) — —0.56 -t- 0.045(n — 1) with n = 1,2,..,, where the dashed line indicates the level —0.565 eV. The dissociation limit indicated by the dense contouring implies Li2 X Sg ) -t- Li.
In the remainder of this section, we focus on the two lowest doublet states of Li3. Figures 3 and 4 show relaxed triangular plots [68] of the lower and upper sheets of the 03 DMBE III [69,70] potential energy surface using hyper-spherical coordinates. Each plot corresponds to a stereographic projection of the... [Pg.585]

Figure 11. Perspective view [60] of a relaxed triangular plot [68] for the two DMBE adiabatic potential energy surfaces of H3 using hyperspherical coordinates. Figure 11. Perspective view [60] of a relaxed triangular plot [68] for the two DMBE adiabatic potential energy surfaces of H3 using hyperspherical coordinates.
The discretization of a problem domain into a finite element mesh consisting of randomly sized triangular elements is shown in Figure 2,1. In the coarse mesh shown there are relatively large gaps between the actual domain boundary and the boundary of the mesh and hence the overall discretization error is expected to be large. [Pg.19]

Standard procedures for the derivation of the shape functions of common types of finite elements can be illustrated in the context of two-dimensional triangular and rectangular elements. Let us, first, consider a triangular element having three nodes located at its vertices as is shown in Figure 2.6. [Pg.23]

In the outlined procedure the derivation of the shape functions of a three-noded (linear) triangular element requires the solution of a set of algebraic equations, generally shown as Equation (2.7). [Pg.24]

Shape functions of the described triangular element are hence found on the basis of Equation (2.11) as... [Pg.24]

The number of terms of a complete polynomial of any given degree will hence correspond to the number of nodes in a triangular element belonging to this family. An analogous tetrahedral family of finite elements that corresponds to complete polynomials in terms of three spatial variables can also be constructed for three-dimensional analysis. [Pg.24]


See other pages where Triangular is mentioned: [Pg.71]    [Pg.145]    [Pg.214]    [Pg.285]    [Pg.370]    [Pg.390]    [Pg.403]    [Pg.405]    [Pg.405]    [Pg.123]    [Pg.342]    [Pg.517]    [Pg.649]    [Pg.935]    [Pg.1681]    [Pg.1702]    [Pg.2]    [Pg.29]    [Pg.586]    [Pg.486]    [Pg.158]    [Pg.276]    [Pg.442]    [Pg.19]    [Pg.23]    [Pg.24]    [Pg.30]    [Pg.30]    [Pg.31]    [Pg.31]    [Pg.32]    [Pg.32]    [Pg.33]    [Pg.34]   
See also in sourсe #XX -- [ Pg.33 ]




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