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Four-Atom Expansions

The expansion of a cyclopropane to a seven-membered ring can be efficiently achieved through a divinylcyclopropane rearrangement. Examples of this transformation have emerged from the groups of Wender, Marino (Eq. 24), Piers (Eq. 25), White (Eq. 26), Harvey (Eq. 27), Barluenga (Eq. 28), Wulff, Davies, and others.  [Pg.13]

Divinylcyclopropane rearrangements have been utilized as the key step in the synthesis of a variety of natural products, including the total [Pg.13]

The reaction between cyclopropylcarbene-tungsten complexes and alkynes has been studied by Herndon (Eq. 31). Both inter- and [Pg.14]


If we substitute the atomic orbital expansion, we obtain a series of two-electron integrals, each of which involves four atomic orbitals ... [Pg.65]

Ring expansion of cycloalkanones.1 The hypoiodite reaction can also be used for a four-atom ring expansion of cyclic ketones via the corresponding lactols (cf., 13, 150). [Pg.174]

Application of the three and four atom HYBO functional form to the formulation of th( interaction of larger systems is not straightforward. Howc ver, since the MBE expansion of the interaction of large systems is, in general, truncated to the four body terms one can easily assemble the related force field by composing related HYBO three and four atom blocks. [Pg.376]

Consider an atom in a cell, Cq. The interactions with atoms in nearby cells are calculated using the usual pairwise formulae. There are 27 such cells (i e. the cell in which the atom is positioned and the surrounding 26 cells). The interaction between the atom and all of the atoms in each of the faraway cells is then calculated using the multipole expansion. The potential due to a faraway cell will be approximately constant for all atoms in the cell of current interest, Cq (the cells are usually small, containing on average four atoms). Thus the potential due to each faraway cell can be represented as a Taylor series expansion about the centre of Cq. If there are M cells in total then there are M — 27 faraway cells then the calculation of these cell-cell interactions for the entire system will be of order M(M —27). As the number of cells is approximately equal to the number of atoms, this still leaves us with a quadratic dependency upon the number of atoms present (though it does now vary as about N /16, if there is an average of four atoms per cell). [Pg.342]

The angle 6 is the bond angle defined by three atoms ky, and k are constants. The torsional term torsion four-atom term for units of the form A—B—C—D, is usually written as a Fourier-series expansion, where the periodicity takes the values 1, 2 and 3, and to is the dihedral angle between the ABC and BCD planes ... [Pg.24]

All the calculations are performed in momentum space and (unless otherwise stated) plane waves with kinetic energy up to 9.15 Ry are included in the expansions of the wave functions. Only those with kinetic energy S 2.55 Ry are dealt with exact, the remaining ones are treated by Lowdin perturbation theory up to second order. This corresponds to approximately 21 + 125 waves when working with the two-atoms cells, 43 + 240 when working with the doubled (four atoms) ui it cells, 85 + 500 on quadrupled cells, etc. Two to five special k-points are used for Brillouin zone integration (corresponding to (222) in the notation of... [Pg.232]

Both the selection of classes of appropriate features, and how the bin distribution is accomplished, are the subjects of current research. One recent approach that holds promise is the expansion of 3D feature keys to include pharmacophoric or stereophoric features as surrogates for the macromolecular receptor site. Each of these features is comprised of a collection of three or four atomic environments (selected from a list including hydrogen-bond donors, acceptors, etc.) in association with interatomic distance ranges. Another theme is the introduction of a 3D surface descriptor as the basis for matching. [Pg.2776]

DMBE The double many-body expansion (DMBE) is a function in which, like MBE, the various 2-, 3-,. .., //-atom terms are combined to represent the potential for an //-atom system. It is based on partitioning the energy into an extended-Hartree-Fock-type term (EHF) and a dynamical correlation (DC) energy (resulting from the DC of the electrons) both of these terms are represented by MBEs. For example, the DMBE potential for a four-atom system has the form... [Pg.3060]


See other pages where Four-Atom Expansions is mentioned: [Pg.13]    [Pg.13]    [Pg.88]    [Pg.356]    [Pg.149]    [Pg.150]    [Pg.3]    [Pg.23]    [Pg.251]    [Pg.411]    [Pg.412]    [Pg.435]    [Pg.822]    [Pg.423]    [Pg.145]    [Pg.894]    [Pg.135]    [Pg.285]    [Pg.290]    [Pg.134]    [Pg.894]    [Pg.752]    [Pg.476]    [Pg.68]    [Pg.169]    [Pg.71]    [Pg.455]    [Pg.251]    [Pg.22]    [Pg.265]    [Pg.181]    [Pg.429]    [Pg.374]    [Pg.556]    [Pg.378]    [Pg.103]    [Pg.2466]    [Pg.2468]    [Pg.3158]    [Pg.219]   


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Ring expansions, four atom

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