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Strained molecules, electron

The electronic spectra of the [2.2]paracyclophanes provide valuable information regarding the extent and mechanisms of transannular electronic interactions in strained 7t-electron systems. A rigid system like the [2.2]paracyclophane molecule is of great value as a model for checking theoretical data with a view to interpretating U V spectra of sterically hindered molecules ( overcrowded compounds ). [Pg.77]

The results for cyclopropane are given as an example for the poor correlation in these highly strained molecules. These extreme molecular structures have an electron distribution that cannot be adequately described using the approximations of the bond polarization model and must be subjected to ab initio calculations. [Pg.98]

Molecular orbital calculations at different levels of sophistication have become an integral part in the characterization of organic radical cations in general, and those of strained molecules in particular. They are used to model the sequence of orbitals in the interpretation of PE spectra, to assign the electronic transitions... [Pg.150]

This example clearly shows the importance of the energy of geometrical distortions upon activation energies, and makes the origin of the high reactivities of strained molecules somewhat more obvious. In two other studies of the influence of geometrical distortions upon reaction rates, we have found that the electronic characteristics of molecules can be profoundly altered by relatively minor geometrical alterations ... [Pg.16]

Figure 12 Computer-generated cage structures of the nonisolable IPR fullerenes Z 6d-C72 and //j-Cgo- The experimentally elusive nature of these molecules is believed to be due to molecular strain and electronic factors, respectively... Figure 12 Computer-generated cage structures of the nonisolable IPR fullerenes Z 6d-C72 and //j-Cgo- The experimentally elusive nature of these molecules is believed to be due to molecular strain and electronic factors, respectively...
A general equation can be derived that describes the variation in direction of the valence electron density about the nucleus. The distortion from sphericity caused by valence electrons and lone-pair electrons is approximated by this equation, which includes a population parameter, a radial size function, and a spherical harmonic function, equivalent to various lobes (multipoles). In the analysis the core electron density of each atom is assigned a fixed quantity. For example, carbon has 2 core electrons and 4 valence electrons. Hydrogen has no core electrons but 1 valence electron. Experimental X-ray diffraction data are used to deri e the parameters that correspond to this function. The model is now more complicated, but gives a better representation of the true electron density (or so we would like to think). This method is useful for showing lone pair directionalities, and bent bonds in strained molecules. Since a larger number of diffraction data are included, the geometry of the molecular structure is probably better determined. [Pg.376]

Hybridization of the carbon to which a proton is attached also influences electron density. As the proportion of s character increases from sp to sp to sp orbitals, bonding electrons move closer to carbon and away from the protons, which then become deshielded. For this reason, methane and ethane resonate at 8 0.23 and 0.86, respectively, but ethene resonates at 8 5.28. Ethyne (acetylene) is an exception in this regard, as we shall see. Hybridization contributes to shifts in strained molecules, such as cyclobutane (8 1.98) and cubane (8 4.00), for which hybridization is intermediate between sp and sp. ... [Pg.63]

In 1967 B. H. Mahan and C. E. Young used a new microwave method to determine the rate constant for thermal electron attachment to molecules. These quantities were determined for SF6 and C7F14 using the ECD and agreed with the values reported using the microwave method at room temperature within the experimental error [37, 38]. In addition, the temperature dependence was determined so that activation energies were obtained. This was especially important in the case of strained molecules such as cyclooctatetrene [34],... [Pg.33]

A well-established approach for studying the bonds in strained molecules is by means of the bond path concept. A bond path corresponds to the ridge of highest electron density that links two nuclei. For many bonds, such as those between the carbons in propane, the bond path is essentially identical with the internuclear axis. In molecules with strained bonds, however, there can be a... [Pg.302]

Figure 4.24 illustrates three kinds of circular DNA, unstrained circle, strained circle, and supercoil. Similarly, Figure 4.18 shows an electron micrograph of a relaxed (unstrained) circle and two supercoiled circles. The unstrained circle contains the same number of twists as linear DNA. It is under no superhelical tension. To make the strained circle, one twist was removed (compared to linear DNA) and the resulting circular DNA is strained because it has the same number of base pairs (105), but fewer numbers of turns (twists). Thus, the strained circle has a higher number of base pairs per turn than the unstrained circle. To relieve the strain, the strained molecule can introduce another superhelical turn within itself, called a writhe. [Pg.498]

Although this reaction is still at an early stage of development, a few modifications have been exploited. These modifications include the extension of the Bellus-Claisen rearrangement to ring strain molecules (such as 2-vinyloxetane, 2-vinyloxirane, and 2-vinylaziridines ) and to tertiary allyl amines, the application of chiral Lewis acid derived from Mgl2 and bis(oxazolinyl)aryl ligands, and the implementation of electron-rich ketene equivalents (e.g., alkoxyketenes, aminoketenes) by the photolysis of chromium carbene complexes. [Pg.308]


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