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1- , bond dissociation from

Bond Dissociation from the T State For the T state, reaction that cannot be observed for the Tj states can be expected. A bond dissociation process is one of the reactions, which can be expected for the T states. Here, we introduce the formation of naphthylmethyl radical from the T states [67],... [Pg.72]

We introduced two examples of three-color three-laser photolysis. The former example employed the third laser as an excitation source to evaluate the amount of intermediates generated by the first and second lasers irradiation. On the other hand, the latter example used the second and third lasers to promote bond dissociation from the respective T and D states. The role of each laser is quite different. These examples indicate that one can control reactions by selecting laser wavelength and delay time based on the properties of each intermediate. [Pg.103]

Figure 5 Potential energy curves for the bond dissociation from Si of the benzylammon-ium ion (a) before interaction between the aromatic ring and the a bond and (b) after interaction. (Modified from Ref. 47.)... Figure 5 Potential energy curves for the bond dissociation from Si of the benzylammon-ium ion (a) before interaction between the aromatic ring and the a bond and (b) after interaction. (Modified from Ref. 47.)...
The synthetic potential of the C-Si bond cleavage from allyl- and benzylsilane radical-cations produced by photoreaction of electron-deficient iminium salts has been extensively investigated [25]. When a benzylsilane or allylsilane is irradiated in the presence of an iminium salt such as 27, a one-electron oxidation of the silane to the excited iminium salt produces a radical/radical-cation pair. Subsequent C-Si bond dissociation from the silane radical-cation by the loss of TMS+ leads to an... [Pg.235]

A simple example would be in a study of a diatomic molecule that in a Hartree-Fock calculation has a bonded cr orbital as the highest occupied MO (HOMO) and a a lowest unoccupied MO (LUMO). A CASSCF calculation would then use the two a electrons and set up four CSFs with single and double excitations from the HOMO into the a orbital. This allows the bond dissociation to be described correctly, with different amounts of the neutral atoms, ion pair, and bonded pair controlled by the Cl coefficients, with the optimal shapes of the orbitals also being found. For more complicated systems... [Pg.300]

The heats of formation of the gaseous atoms, 4, are not very different clearly, it is the change in the bond dissociation energy of HX, which falls steadily from HF to HI, which is mainly res ponsible for the changes in the heats of formation. 6. We shall see later that it is the very high H—F bond energy and thus the less easy dissoeiation of H—F into ions in water which makes HF in water a weak aeid in comparison to other hydrogen halides. [Pg.73]

Electron affinity and hydration energy decrease with increasing atomic number of the halogen and in spite of the slight fall in bond dissociation enthalpy from chlorine to iodine the enthalpy changes in the reactions... [Pg.315]

A more useful quantity for comparison with experiment is the heat of formation, which is defined as the enthalpy change when one mole of a compound is formed from its constituent elements in their standard states. The heat of formation can thus be calculated by subtracting the heats of atomisation of the elements and the atomic ionisation energies from the total energy. Unfortunately, ab initio calculations that do not include electron correlation (which we will discuss in Chapter 3) provide uniformly poor estimates of heats of formation w ith errors in bond dissociation energies of 25-40 kcal/mol, even at the Hartree-Fock limit for diatomic molecules. [Pg.105]

Even within a particular approximation, total energy values relative to the method s zero of energy are often very inaccurate. It is quite common to find that this inaccuracy is almost always the result of systematic error. As such, the most accurate values are often relative energies obtained by subtracting total energies from separate calculations. This is why the difference in energy between conformers and bond dissociation energies can be computed extremely accurately. [Pg.8]

In this section you have seen how heats of com bustion can be used to determine relative stabilities of isomeric alkanes In later sections we shall expand our scope to include the experimentally determined heats of certain other reactions such as bond dissociation energies (Section 4 16) and heats of hydrogenation (Section 6 2) to see how AH° values from various sources can aid our understanding of structure and reactivity... [Pg.86]

The same conclusion is reached using bond dis sociation energies The following equation shows the bond dissociation energies of the reactants and prod ucts taken from Table 4 3... [Pg.174]

Bromination of methane is exothermic but less exothermic than chlorination The value calculated from bond dissociation energies is AH° = -30 kJ Al though bromination of methane is energetically fa vorable economic considerations cause most of the methyl bromide prepared commercially to be made from methanol by reaction with hydrogen bromide... [Pg.174]

Resonance theory can also account for the stability of the allyl radical. For example, to form an ethylene radical from ethylene requites a bond dissociation energy of 410 kj/mol (98 kcal/mol), whereas the bond dissociation energy to form an allyl radical from propylene requites 368 kj/mol (88 kcal/mol). This difference results entirely from resonance stabilization. The electron spin resonance spectmm of the allyl radical shows three, not four, types of hydrogen signals. The infrared spectmm shows one type, not two, of carbon—carbon bonds. These data imply the existence, at least on the time scale probed, of a symmetric molecule. The two equivalent resonance stmctures for the allyl radical are as follows ... [Pg.124]

Because these stability measurements pertain to the gas phase, it is important to consider the effects that solvation might have on the structure-stability relationships. Hydride affinity values based on solution measurements can be derived from thermodynamic cycles that relate hydrocarbon p T, bond dissociation energy and electrochemical potentials. The hydride affinity, AG, for the reaction... [Pg.279]

From this value and known C—H bond dissociation energies, pK values can be calculated. Early application of these methods gave estimates of the p/Ts of toluene and propene of about 45 and 48, respectively. Methane was estimated to have a pAT in the range of 52-62. Electrochemical measurements in DMF have given the results shown in Table 7.3. These measurements put the pK of methane at about 48, with benzylic and allylic stabilization leading to values of 39 and 38 for toluene and propene, respectively. The electrochemical values overlap with the pATdmso scale for compounds such as diphenyl-methane and triphenylmethane. [Pg.410]

Table 12.4. Substituent Effects on Radical Stability from Measurements of Bond Dissociation Energies and Theoretical Calculations of Radical Stabilization Energies... Table 12.4. Substituent Effects on Radical Stability from Measurements of Bond Dissociation Energies and Theoretical Calculations of Radical Stabilization Energies...

See other pages where 1- , bond dissociation from is mentioned: [Pg.3767]    [Pg.4250]    [Pg.118]    [Pg.53]    [Pg.3766]    [Pg.4249]    [Pg.268]    [Pg.449]    [Pg.151]    [Pg.151]    [Pg.815]    [Pg.73]    [Pg.114]    [Pg.328]    [Pg.324]    [Pg.136]    [Pg.172]    [Pg.446]    [Pg.220]    [Pg.209]    [Pg.172]    [Pg.96]    [Pg.14]    [Pg.14]    [Pg.525]    [Pg.694]   


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