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Pi-electron energy

HMO calculations of the pi electronic energies of the radicals were done using the values of coulomb and bond integrals suggested by Streitwieser (5). The only exception to these integral values was for the case of a heteroatom (with lone electron pair) bonded to the radical center carbon. The bond integrals for this case were chosen to be one-half the values suggested by Streitwieser ... [Pg.417]

Markovic, S. (2003) Approximating the total pi-electron energy of phenylenes in terms of spectral moments. Indian J. Chem., 42, 1304—1308. [Pg.1113]

Molecular-Orbitals— Total Pi-Electron Energy of Alternant Hydrocarbons. [Pg.198]

Figure Bl.23.5. Schematic illustration of tlie TOE-SARS spectrometer system. A = ion gun, B = Wien filter, C = Einzel lens, D = pulsing plates, E = pulsing aperture, E = deflector plates, G = sample, PI = electron multiplier detector with energy prefilter grid and I = electrostatic deflector. Figure Bl.23.5. Schematic illustration of tlie TOE-SARS spectrometer system. A = ion gun, B = Wien filter, C = Einzel lens, D = pulsing plates, E = pulsing aperture, E = deflector plates, G = sample, PI = electron multiplier detector with energy prefilter grid and I = electrostatic deflector.
Fig. 3.31. Distributions (i)/(Ee) dEe of electron energy (E ) for a low-pressure HF-plasma (suffix pi, Maxwellian with temperature = 80000 K) and an electron beam (suffix eb, simplified to Gaussian shape with 40 eV half-width) (ii) rTx (Ej) ofthe Ej dependent electron impact ionization cross-section for X=Ti... Fig. 3.31. Distributions (i)/(Ee) dEe of electron energy (E ) for a low-pressure HF-plasma (suffix pi, Maxwellian with temperature = 80000 K) and an electron beam (suffix eb, simplified to Gaussian shape with 40 eV half-width) (ii) rTx (Ej) ofthe Ej dependent electron impact ionization cross-section for X=Ti...
By following the same arguments as before, we conclude that the conformation will be lower in energy than the Cee conformation. The same analysis can be used to compare the relative energetics of the and Cx conformations. In conclusion, we can say that the C conformation will be favored over the Cee and Cx conformations due to a larger pi attractive nonbonded interaction which obtains in the 6 pi electron aromatic geometry of the conformation. [Pg.87]

Aromatics are in a sense unique in their catalytic cracking reactions. The aromatic ring contains the equivalent of six double bond or pi electrons, which are, however, mutually stabilized by strong resonance energy. We may postulate an association between a carbonium ion and these electrons in a generalized sense ... [Pg.10]

Fig. 5.13 Correct molecular orbital energy levels For early elements of the first long row. Some mixing (hybridization) has occurred between the 2r and 2p orbitals. Note that it is somewhat more difficult to keep books" and determine the bond order here ihan in Fig. 5.12 3o- and are clearly bonding (they lie below the atomic orbitals contributing i0 them) 4(7, and 5trR are essentially nonbonding since they lie between the atomic orbitals contributing to them and roughly symmetrically spaced about the center of gravity." The maximum net bond order is therefore one cr bond plus two 7r bonds. The electronic configuration shown is for the Bz molecule. Note the unpaired pi electrons. Fig. 5.13 Correct molecular orbital energy levels For early elements of the first long row. Some mixing (hybridization) has occurred between the 2r and 2p orbitals. Note that it is somewhat more difficult to keep books" and determine the bond order here ihan in Fig. 5.12 3o- and are clearly bonding (they lie below the atomic orbitals contributing i0 them) 4(7, and 5trR are essentially nonbonding since they lie between the atomic orbitals contributing to them and roughly symmetrically spaced about the center of gravity." The maximum net bond order is therefore one cr bond plus two 7r bonds. The electronic configuration shown is for the Bz molecule. Note the unpaired pi electrons.
The behavior of pyridine in substitution reactions can be understood on the basis of its resonance structures (la-d) and on the basis of the electron-density distribution at the various ring positions as derived from molecular-orbital-theoretical calculations, An example of the published pi-electron density distribution is shown in II, The resonance energy of pyridine is 35 kcal/mole (versus 39 kcal/mole for benzene). [Pg.1384]

The spectrum of naphthalene is shown above. Its broad bands reflect the absorption of energy by the extended pi-electron system. [Pg.654]

PEDOT PEELS PEG PEG-Si PEI PEO PEP PER PET PG PG-zb Ph phim PHMA PI pia PIXIES poly-(3,4-ethylenedioxythiophene) parallel electron energy loss spectroscopy poly(ethylene glycol) 2-[methoxypoly(ethyleneoxy)propyl]trimethoxysilane poly(ethylene imine) poly(ethylene oxide) poly(ethylene-aZf-propylene) photoelectrorheological (effect) positron emission tomography adaptor protein G Fc domain of PG phenyl benzimidazolate poly(w-hexyl methacrylate) polyisoprene V-4-pyridyl isonicotinamide protein imprinted xerogels with integrated emission sites... [Pg.813]


See other pages where Pi-electron energy is mentioned: [Pg.290]    [Pg.537]    [Pg.544]    [Pg.546]    [Pg.554]    [Pg.233]    [Pg.238]    [Pg.1]    [Pg.892]    [Pg.290]    [Pg.537]    [Pg.544]    [Pg.546]    [Pg.554]    [Pg.233]    [Pg.238]    [Pg.1]    [Pg.892]    [Pg.527]    [Pg.527]    [Pg.528]    [Pg.11]    [Pg.340]    [Pg.134]    [Pg.635]    [Pg.636]    [Pg.228]    [Pg.123]    [Pg.194]    [Pg.587]    [Pg.79]    [Pg.17]    [Pg.177]    [Pg.181]    [Pg.41]    [Pg.290]    [Pg.411]    [Pg.411]    [Pg.411]    [Pg.715]    [Pg.510]    [Pg.659]    [Pg.256]    [Pg.215]    [Pg.222]    [Pg.119]   
See also in sourсe #XX -- [ Pg.647 , Pg.649 ]

See also in sourсe #XX -- [ Pg.601 , Pg.614 , Pg.618 ]




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