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Carbon vibrational energy

Some detailed calculations have been made by Tully [209] on the trajectories for Rideal-type processes. Thus the collision of an oxygen atom with a carbon atom bound to Pt results in a CO that departs with essentially all of the reaction energy as vibrational energy (see Ref. 210 for a later discussion). [Pg.722]

Margottin-Maclou M, Doyennette L and Henry L 1971 Relaxation of vibrational energy in carbon monoxide, hydrogen chloride, carbon dioxide and nitrous oxide App/. Opt. 10 1768-80... [Pg.3015]

Sharma R D and Brau C A 1967 Near-resonant vibrational energy transfer in nitrogen carbon dioxide mixtures Phys. Rev. Lett. 19 1273-5... [Pg.3015]

Yardley J T and Moore C B 1967 Intramolecular vibration-to-vibration energy transfer in carbon dioxide J. Chem. Phys. 46 4491-5... [Pg.3015]

Evidently a large part of the energy liberated in the approach of the carbon atom to ethylene will go into this normal mode — which is the one required for conversion of 30 to 31. Unless the interconversion of vibrational energy is incredibly efficient, one would then expect the initially formed 30 to be converted to 31 even at the lowest temperatures. The fact that allene is formed at -190° is not therefore surprising. On the other hand the existence of a large barrier between 30 and 31 would prohibit rearrangement of 30 if formed under milder conditions free cyclopropyl carbenes do not rearrange to allenes if formed by conventional methods in solution 49). [Pg.26]

The variations in the relative yields of the products with variations in wavelength and temperature have also been interpreted in the same way. An increase in the temperature or a decrease in the wavelength under otherwise constant conditions should increase the vibrational energy possessed by the molecule in the excited state. It has been observed that under these circumstances the ratio of pentenal to carbon monoxide... [Pg.91]

Srinivasan122 has shown that the hydrogen atom transferred to the carbonyl carbon comes from one of the two carbon atoms in the 2 positions. Formation of the pentenal appears to be favored at low vibrational energies since the addition of foreign gas improves the yield which is, nevertheless, always small. Reactions (159) and (160) are the classical steps proposed by Norrish and his coworkers and they are found also with the perfluorocycloketones123. [Pg.55]

They do not spontaneously decompose because the ZPE is not concentrated in just one or a few bonds. An exotic structure could indeed run the risk of decomposing by such concentration of its vibrational energies. A candidate for this is the transition state (which is calculated to be nonplanar) for inversion of methane. Incidentally, this would correspond to racemization if four different hydrogens could be attached to a carbon unfortunately 4H has a halflife of only 10 22 s [1],... [Pg.600]

The unimolecular 1,2-HF and 2,3-HF elimination reactions of CF3CHFCH3 have been characterized using the chemical activation technique for an average vibrational energy of 97 kcalmol-1.36 The transition state for 1,2-HF elimination has a two-fold larger pre-exponential factor than that for 2,3-HF elimination, because three F atoms attached to carbon atoms of the four-membered ring have lower frequencies than those in a CF3 group. [Pg.283]

A molecule can only absorb infrared radiation if the vibration changes the dipole moment. Homonuclear diatomic molecules (such as N2) have no dipole moment no matter how much the atoms are separated, so they have no infrared spectra, just as they had no microwave spectra. They still have rotational and vibrational energy levels it is just that absorption of one infrared or microwave photon will not excite transitions between those levels. Heteronuclear diatomics (such as CO or HC1) absorb infrared radiation. All polyatomic molecules (three or more atoms) also absorb infrared radiation, because there are always some vibrations which create a dipole moment. For example, the bending modes of carbon dioxide make the molecule nonlinear and create a dipole moment, hence CO2 can absorb infrared radiation. [Pg.184]

Figure 2.29 The A symmetric (30) and B symmetric (31) coupled C=C stretching vibrations with their ROA group coupling matrices as implemented in VOAView [65], The volume of the bicoloured spheres is proportional to the vibrational energy and the direction of motion indicated by the colours. The five groups in the group coupling matrices are the the four carbon atoms as indicated, with the fifth group being the remainder of the molecule. Computational parameters vibrations as in Fig. 1 electronic tensors as in Fig. 7 with basis sets as indicated (see Colour Plate section). Figure 2.29 The A symmetric (30) and B symmetric (31) coupled C=C stretching vibrations with their ROA group coupling matrices as implemented in VOAView [65], The volume of the bicoloured spheres is proportional to the vibrational energy and the direction of motion indicated by the colours. The five groups in the group coupling matrices are the the four carbon atoms as indicated, with the fifth group being the remainder of the molecule. Computational parameters vibrations as in Fig. 1 electronic tensors as in Fig. 7 with basis sets as indicated (see Colour Plate section).
This study shows the possibilities and specific feature of IR-pyrolysis for the formation of nanostructured carbon. In such way PAN, thermal transformations of which have been studied in detail [8-11], was chosen as the precursor for preparation of nanostructured carbon materials by carbonization of PAN and its composites with gadolinium chloride under non-coherent IR radiation. Specific action of IR-radiation on vibrational energy of PAN bands macromolecules allows one to decrease extremely time treatment and as a result to make simple, low energy and cost-effective pyrolitic method. [Pg.578]

Chandler DW, Ewing GE. Transfer and storage of vibrational energy in liquids liquid nitrogen and its solutions with carbon monoxide. J Chem Phys 1980 73 4904-4913. [Pg.600]


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See also in sourсe #XX -- [ Pg.137 ]




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