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Ethylene atoms

It s easy to identify the carbons involved in the double bond in ethylene atoms 1 and 2. In propene, things are slightly more complicated. In this case, the carbon which has three hydrogens attached to it is not involved in the double bond. We can identify this carbon atom as center number 3 by noting that it along with the final three hydrogen atoms all lie in the third quadrant (-X and -Y). Therefore the two carbons of interest are again atoms 1 and 2. [Pg.81]

Fig. 1.10. A titanium atom in a crystal (a) without empty site, (b) with an empty site, (c) with an empty site and an attached propylene monomer. The symbol Et represents an ethylene atom coming from the substitution of a chlorine atom to this radical in a triethyl aluminium molecule (according to P. Rempp). Fig. 1.10. A titanium atom in a crystal (a) without empty site, (b) with an empty site, (c) with an empty site and an attached propylene monomer. The symbol Et represents an ethylene atom coming from the substitution of a chlorine atom to this radical in a triethyl aluminium molecule (according to P. Rempp).
For the MM system and QM/MM interaction, Lennard-Jones parameters (Table 1) for argon were drawn from Maitland et al. [47] and those for the ethylene atoms were drawn from the AMBER ff99 force field [48]. For interactions between distinct atom types, the Lennard-Jones a parameter was chosen to be the arithmetic average of the values for the two atom types, while the parameter was the geometric mean of the two values. [Pg.327]

Table 3.1 Optimized bond lengths R-,j in Angstrom and computed K-,j for 2j + 2 cycloaddition of two ethylenes (atom numbering as in Figure 3.7) ... Table 3.1 Optimized bond lengths R-,j in Angstrom and computed K-,j for 2j + 2 cycloaddition of two ethylenes (atom numbering as in Figure 3.7) ...
Studies to determine the nature of intermediate species have been made on a variety of transition metals, and especially on Pt, with emphasis on the Pt(lll) surface. Techniques such as TPD (temperature-programmed desorption), SIMS, NEXAFS (see Table VIII-1) and RAIRS (reflection absorption infrared spectroscopy) have been used, as well as all kinds of isotopic labeling (see Refs. 286 and 289). On Pt(III) the surface is covered with C2H3, ethylidyne, tightly bound to a three-fold hollow site, see Fig. XVIII-25, and Ref. 290. A current mechanism is that of the figure, in which ethylidyne acts as a kind of surface catalyst, allowing surface H atoms to add to a second, perhaps physically adsorbed layer of ethylene this is, in effect, a kind of Eley-Rideal mechanism. [Pg.733]

As an interesting footnote, Ceyer [291] has found that ethylene is hydrogenated by hydrogen absorbed in the bulk region just below a Ni(l 11) surface. In this case, the surface ethylenes are assumed to by lying flat, with the dissolved H atoms approaching the double bond from underneath. [Pg.733]

Finally, it should also be clear that ER reactions do not necessarily yield a gas-phase product. The new molecule may be trapped on the surface. There is evidence for an ER mechanism in the addition of incident Ft atoms to ethylene and benzene on Cii(l 11) [91], and in the abstraction of Ft atoms from cyclohexane by incident D atoms [92], and the direct addition of Ft atoms to CO on Rii(OOl) [93]. [Pg.914]

Although this reaction appears to involve only two electrons, it was shown by Mulder [57] that in fact two jc and two ct elections are required to account for this system. The three possible spin pairings become clear when it is realized that a pair of carbene radicals are formally involved. Figure 14. In practice, the conical intersection defined by the loop in Figme 14 is high-lying, so that often other conical intersections are more important in ethylene photochemistry. Flydrogen-atom shift products are observed [58]. This topic is further detailed in Section VI. [Pg.350]

The transformation of ethylene to the carbene requires the re-pairing of three electron pairs. It is a phase-preserving reaction, so that the loop is an ip one. The sp -hybridized carbon atom formed upon H transfer is a chiral center consequently, there are two equivalent loops, and thus conical intersections, leading to two enantiomers. [Pg.367]

The method has severe limitations for systems where gradients on near-atomic scale are important (as in the protein folding process or in bilayer membranes that contain only two molecules in a separated phase), but is extremely powerful for (co)polymer mixtures and solutions [147, 148, 149]. As an example Fig. 6 gives a snapshot in the process of self-organisation of a polypropylene oxide-ethylene oxide copolymer PL64 in aqueous solution on its way from a completely homogeneous initial distribution to a hexagonal structure. [Pg.27]

The full ab-initio molecular dynamics simulation revealed the insertion of ethylene into the Zr-C bond, leading to propyl formation. The dynamics simulations showed that this first step in ethylene polymerisation is extremely fast. Figure 2 shows the distance between the carbon atoms in ethylene and between an ethylene carbon and the methyl carbon, from which it follows that the insertion time is only about 170 fs. This observation suggests the absence of any significant barrier of activation at this stage of the polymerisation process, and for this catalyst. The absence or very small value of a barrier for insertion of ethylene into a bis-cyclopentadienyl titanocene or zirconocene has also been confirmed by static quantum simulations reported independently... [Pg.434]

Fig. 2. Time-evolution of the methyl/ethyl C-C distances for both the zirconocene and the corresponding titanocene catalyst. The two curves starting at around 3.2 A represent the distance between the methyl carbon atom and the nearest-by ethylene carbon atom in the zirconocene-ethylene and the titanocene-ethylene complex, respectively. The two curves starting at around 1.35 A reflect the ethylene internal C-C bond lengths in the two complexes. Fig. 2. Time-evolution of the methyl/ethyl C-C distances for both the zirconocene and the corresponding titanocene catalyst. The two curves starting at around 3.2 A represent the distance between the methyl carbon atom and the nearest-by ethylene carbon atom in the zirconocene-ethylene and the titanocene-ethylene complex, respectively. The two curves starting at around 1.35 A reflect the ethylene internal C-C bond lengths in the two complexes.
Fig. 3. Time evolution of the distance between the Zr atom and each of the three hydrogen atoms belonging to the methyl group (the original methyl group bonded to the Zr) in the zirconocene-ethylene complex. The time-evolution of one of the hydrogen atoms depicted by the dotted curve shows the development of an a-agostic interaction. Later on in the simulation (after about 450 fs) one of the other protons (broken curve) takes over the agostic interaction (which is then a 7-agostic interaction). Fig. 3. Time evolution of the distance between the Zr atom and each of the three hydrogen atoms belonging to the methyl group (the original methyl group bonded to the Zr) in the zirconocene-ethylene complex. The time-evolution of one of the hydrogen atoms depicted by the dotted curve shows the development of an a-agostic interaction. Later on in the simulation (after about 450 fs) one of the other protons (broken curve) takes over the agostic interaction (which is then a 7-agostic interaction).
HMO theory is named after its developer, Erich Huckel (1896-1980), who published his theory in 1930 [9] partly in order to explain the unusual stability of benzene and other aromatic compounds. Given that digital computers had not yet been invented and that all Hiickel s calculations had to be done by hand, HMO theory necessarily includes many approximations. The first is that only the jr-molecular orbitals of the molecule are considered. This implies that the entire molecular structure is planar (because then a plane of symmetry separates the r-orbitals, which are antisymmetric with respect to this plane, from all others). It also means that only one atomic orbital must be considered for each atom in the r-system (the p-orbital that is antisymmetric with respect to the plane of the molecule) and none at all for atoms (such as hydrogen) that are not involved in the r-system. Huckel then used the technique known as linear combination of atomic orbitals (LCAO) to build these atomic orbitals up into molecular orbitals. This is illustrated in Figure 7-18 for ethylene. [Pg.376]

Sodium me/aperiodate (NalO ) in cold aqueous solution readily oxidises 1,2-diols with splitting of the molecule and the consequent formation of aldehydes or ketones thus ethylene glycol gives formaldehyde and pinacol gives acetone. In the case of a 1,2,3-triol, the central carbon atom of the triol... [Pg.145]

Figure 4-5 The Geometry of Ethylene with all Atoms at their Equilibrium Positions in the MM3 Eorce Eield. Figure 4-5 The Geometry of Ethylene with all Atoms at their Equilibrium Positions in the MM3 Eorce Eield.
Procedure, a) Using the procedure shown in constructing the ethylene input file, construct an approximate input file for HjO. The atom type for oxygen is 6. The approximate input geometry can be taken as in File 4-.5, where all of the c-eourdinates are set at 0. Go to the tinker directory in the MS-DOS operating system and create an input (ile for your II2O calculation. Be sure the extension of the input file is. xyz. Rename or edit the (ile as neeessaiy. [Pg.110]

Note that the strict foiiriat of the ethylene output file was not followed in adding new atoms. Be careful of your connected atom list to the right of the input file it is a rich source of potential errors. Use your graph to keep the numbering straight. [Pg.111]

What is the MM3 enthalpy of formation at 298.15 K of styrene Use the option Mark all pi atoms to take into account the conjugated double bonds in styrene. Is the minimum-energy structure planar, or does the ethylene group move out of the plane of the benzene ring ... [Pg.168]

It is a property of linear, homogeneous differential equations, of which the Schroedinger equation is one. that a solution multiplied by a constant is a solution and a solution added to or subtracted from a solution is also a solution. If the solutions Pi and p2 in Eq. set (6-13) were exact molecular orbitals, id v would also be exact. Orbitals p[ and p2 are not exact molecular orbitals they are exact atomic orbitals therefore. j is not exact for the ethylene molecule. [Pg.177]

By the criterion of Exercise 2-9, is an eigenvalue of the matrix in a and p. There are two secular equations in two unknowns for ethylene. For a system with n conjugated sp carbon atoms, there will be n secular equations leading to n eigenvalues . The family of , values is sometimes called the spectrum of energies. Each secular equation yields a new eigenvalue and a new eigenvector (see Chapter 7). [Pg.186]

These absorptions are ascribed to n-n transitions, that is, transitions of an electron from the highest occupied n molecular orbital (HOMO) to the lowest unoccupied n molecular orbital (LUMO). One can decide which orbitals are the HOMO and LUMO by filling electrons into the molecular energy level diagram from the bottom up, two electrons to each molecular orbital. The number of electrons is the number of sp carbon atoms contributing to the n system of a neuhal polyalkene, two for each double bond. In ethylene, there is only one occupied MO and one unoccupied MO. The occupied orbital in ethylene is p below the energy level represented by ot, and the unoccupied orbital is p above it. The separation between the only possibilities for the HOMO and LUMO is 2.00p. [Pg.197]

Within the predictive capabilities of the models, reactivity is given by bThe larger r- the more reactive the molecule (or ion or radical). Note that the tenriinal carbon atoms in buta-1,3-diene are predicted by Iltiekcl theoiy to be slightly more reactive than the carbon atoms in ethylene. Qualitative eoirelation with experience is seen fur sume alkenes and free radicals in Fig. 7-3,... [Pg.217]

Assuming a 2sf 2pf electron distribution for the carbon atoms, calculate the energy of fomiation of ethylene from the gaseous atoms. [Pg.230]

Using Program SCF for ethylene and 1,3,5-hexatriene, list the electron repulsion integrals in the foiiii Yjj, Yj2, and so on. Take the coordinates from Figure 8-6. Try small variations in the atomic coordinates to see what their influence is on Yy. [Pg.260]

Polyamides from diamines and dibasic acids. The polyamides formed from abphatic diamines (ethylene- to decamethylene-diamine) and abphatic dibasic acids (oxabc to sebacic acid) possess the unusual property of forming strong fibres. By suitable treatment, the fibres may be obtained quite elastic and tough, and retain a high wet strength. These prpperties render them important from the commercial point of view polyamides of this type are cabed nylons The Nylon of commerce (a 66 Nylon, named after number of carbon atoms in the two components) is prepared by heating adipic acid and hexamethylenediamine in an autoclave ... [Pg.1019]


See other pages where Ethylene atoms is mentioned: [Pg.8]    [Pg.197]    [Pg.329]    [Pg.8]    [Pg.197]    [Pg.329]    [Pg.815]    [Pg.855]    [Pg.366]    [Pg.385]    [Pg.145]    [Pg.434]    [Pg.436]    [Pg.377]    [Pg.637]    [Pg.236]    [Pg.450]    [Pg.90]    [Pg.111]    [Pg.154]    [Pg.209]    [Pg.216]    [Pg.221]    [Pg.252]    [Pg.257]    [Pg.149]   
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