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Energy maximum

Figure 14.5 Illustration of the linear and quadratic synchronous transit methods. Energy maxima and minima are denoted by and , respectively... Figure 14.5 Illustration of the linear and quadratic synchronous transit methods. Energy maxima and minima are denoted by and , respectively...
Make a graph of potential energy versus angle of bond rotation for propane, and assign values to the energy maxima. [Pg.98]

An explanation of the relationship between reaction rate and intermediate stability was first advanced in 1955. Known as the Hammond postulate, the argument goes like this transition states represent energy maxima. They are high-energy activated complexes that occur transiently during the course of a reaction and immediately go on to a more stable species. Although we can t... [Pg.197]

The transition state, on the other hand, is a species that reacts without further activation. It cannot be diverted to an alternative product, nor will it succumb to trapping. An intermediate, at a free-energy minimum, is both preceded and followed by a transition state. Both of the transition states lie at free-energy maxima. [Pg.127]

Full 360° rotation leads to three identical staggered structures which are energy minima, and three identical eclipsed structures which are energy maxima. The difference in energy between eclipsed and staggered structures of ethane, termed the barrier to rotation, is known experimentally to be 2.9 kcal/mol (12 kJ/mol). Note, that any physical measurements on ethane pertain only to its staggered structure, or... [Pg.1]

In this case, the geometrical coordinate connecting stable forms is not specified in detail (as in the previous two examples), but is referred to simply as the reaction coordinate . Also the energy maxima have been designated as transition states as an indication that their structures may not be simply described (as the energy maxima for rotation in ethane and /7-butane). [Pg.3]

The populations of the eclipsed forms of butane, like the eclipsed forms of ethane, are small and represent energy maxima for the molecule as rotation occurs about the central C-C bond. The energy differences between the butane conformations are represented diagrammatically in Figure 5-8. The valleys correspond to staggered forms and the energy difference between the anti and gauche forms is 0.8-0.9 kcal mole-1. [Pg.124]

Figure 4.2 shows the reaction coordinate diagram for this mechanism. The carbocation is a real intermediate and thus lies at an energy minimum energy maxima occur both when the C—X bond is stretched, and when the C—Y bond is formed. This process will be considered in detail in Chapter 5. A number of modifications of the original Ingold Sw 1 mechanism must be made to accommodate the results of more recent investigations. [Pg.173]

Looking for stereo irrelevancy we find that the ability of the human auditory system to discriminate the exact location of audio sources decreases at high frequencies [Blauert, 1983], The cues to get spatial impression are mainly taken from the energy maxima in space at each frequency. [Pg.50]

The third problem is introduced by the possibility of two ratedetermining steps with nearly equal energy maxima. Competitive carbon-hydrogen bond rupture in aromatic substitution reactions must, in some instances, adversely affect the quality of the correlations. Clearly, the influence of substituents on the rate of formation of the benzenium ion and its rate of decomposition are often opposed. [Pg.134]

All the staggered conformations about the C-2—C-3 bond of 2,2-dimethylpropane are equivalent to one another and of equal energy they represent potential energy minima. All the eclipsed conformations are equivalent and represent potential energy maxima. [Pg.52]

Figures 8.3 and 8.4 show potential energy maxima at inter-particle separations of a few nanometres. Surface roughness of at least up to this magnitude is, therefore, unlikely to invalidate these potential energy calculations. Figures 8.3 and 8.4 show potential energy maxima at inter-particle separations of a few nanometres. Surface roughness of at least up to this magnitude is, therefore, unlikely to invalidate these potential energy calculations.
The magnitude of p(s) corresponds to the number of energy states (allowed -points) per unit energy. Maxima (peaks) in p(e) correspond to portions of the band structure which are relatively flat (In the example in Fig. 3.1, the relationship between the band structure and the p(e) (or DO VS), for tram- polyacetylene is presented.)... [Pg.22]

Pour cold water in the ultrasonic bath (30-50 kHz) half of its depth and switch it on. Observe the places of maximum agitation on the water surface to determine the horizontal X and Y coordinates of the energy maxima. Place a stainless steel coil connected to a cold water tap in the bath and circulate water. Adjust the vertical Z coordinate of the energy maximum by adding water slowly so as to obtain a geyser at the surface (ultrasonic fountain). [Pg.310]

Fig. 10.17. Transition states of the selectivity-determining step of a stereogenic addition of a hydride donor to an a-chiral carbonyl compound (the energy profile would be allowed to contain additional local energy maxima provided that they do not have a higher energy than the two highest maxima shown in the figure). Fig. 10.17. Transition states of the selectivity-determining step of a stereogenic addition of a hydride donor to an a-chiral carbonyl compound (the energy profile would be allowed to contain additional local energy maxima provided that they do not have a higher energy than the two highest maxima shown in the figure).

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See also in sourсe #XX -- [ Pg.62 ]

See also in sourсe #XX -- [ Pg.87 ]




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