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To a considerable degree, we can predict relative reactivities, provided we use common sense to limit our efforts to reasonable situations. In the preceding section, we argued that reactions in which atoms or radicals combine can well be expected to be extremely fast because each entity has a potentially bonding electron in an outer unfilled shell, and bringing these together to form a bond does not require that other bonds be broken:
Figure 4-6). As CH4 and Cl⋅ get closer together, the new bond starts to form and the old bond starts to break. At the top of the barrier, the hydrogen will be bonded partly to chlorine and partly to carbon, [Cl−−−H−−−CH3], and this we call the activated complex or transition state. The concept of the transition state is an important one, which we will use repeatedly later in connection with many other kinds of reactions. The value of the concept lies in the fact that the reacting system, when it reaches the top of the barrier, can be though of as a chemical entity with a particular, even if not well-defined, structure and definite thermodynamic properties.
The difference between the average energy of the reactants and the energy of the transition state is called the activation energy (Figure 4-4). We expect this energy to be smaller (lower barrier) if a weak bond is being broken and a strong bond is being made. The perceptive reader will notice that we are suggesting a parallel between reaction rate and ΔH0 because ΔH0 depends on the difference in strengths of the bonds being broken and formed. Yet previously , we pointed out that the energy barrier for a reaction need bear no relationship to how energetically feasible the reaction is, and this is indeed true for complex reactions involving many steps. But our intuitive parallel between rate and ΔH0ΔH0 usually works quite well for the rates of individual steps. This is borne out by experimental data on rates of removal of a hydrogen atom from methane by atoms or radicals (X⋅), such as F⋅, Cl⋅, Br⋅, HO⋅, H2N⋅, which generally parallel the strength of the new bond formed:
Similarly, if we look at the H−C bond-dissociation energies of the hydrocarbons shown in Table 4-6, we would infer that Cl⋅ would remove a hydrogen most rapidly from the carbon forming the weakest C−H bond and, again, this is very much in accord with experience. For example, the chlorination of methylbenzene (toluene) in sunlight leads to the substitution of a methyl hydrogen rather than a ring hydrogen for the reason that the methyl C−H bonds are weaker and are attacked more rapidly than the ring C−H bonds. This can be seen explicitly in the ΔH0 values for the chain-propagation steps calculated from the bond-dissociation energies of Table 4-6.
Methyl substitution (observed):
Ring substitution (not observed):
The ΔH0 of ring-hydrogen abstraction is unfavorable by +7kcal because of the high C−H bond energy (110kcal). Thus this step is not observed. It is too slow in comparison with the more favorable reaction at the methyl group even though the second propagation step is energetically favorable by −37kcal and presumably would occur very rapidly. Use of bond-dissociation energies to predict relative reaction rates becomes much less valid when we try to compare different kinds of reactions. To illustrate, ethane might react with F⋅ to give fluoromethane or hydrogen fluoride:
It is not a good idea to try to predict the relative rates of these two reactions on the basis of their overall ΔH0 values because the nature of the bonds made and broken is too different.
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علامات بسيطة في جسدك قد تنذر بمرض "قاتل"
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أول صور ثلاثية الأبعاد للغدة الزعترية البشرية
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مستشفى العتبة العباسية الميداني في سوريا يقدّم خدماته لنحو 1500 نازح لبناني يوميًا
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