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The Reaction Path

It is useful to change from Cartesian coordinates to a mass-scaled coordinate system defined by [Pg.140]

A generahzed transition state is a tentative dynamical bottleneck, and a tentative reaction coordinate is a nearly separable coordinate in a direction from reactants to products. Thermal rate constants are dominated by near-threshold events, and near the reaction threshold, a nearly separable coordinate in a direction from reactants to products is given by following the equations of motion but damping out the velocity along the trajectory. With this damping, the equations of motion can be rewritten for an infinitesimal time interval t as [Pg.141]

The integration constant is zero because of the assumption of infinitesimal velocity (x= 0 at = 0). We can rewrite Eq. [41] in vector form as [Pg.141]

For the geometry x(s) (x hereafter), the gradient is different than zero, and so for the next xi geometry, or in general for a geometry x , with 1, we can apply Eq. [44] and follow the opposite direction of the normalized gradient  [Pg.142]

Then a corrector step is specified as a point at a minimum of a parabolic fit along a line that goes through xi° and parallel to a bisector vector d , which is given by ° [Pg.143]


Having made a choice of the reaction path, we need to choose a reactor type and make some assessment of the conditions in the reactor. This allows assessment of reactor performance for the chosen reaction path in order for the design to proceed. [Pg.18]

Changing the reaction path to reduce or eliminate the formation of unwanted byproducts. [Pg.297]

For very fast reactions, as they are accessible to investigation by pico- and femtosecond laser spectroscopy, the separation of time scales into slow motion along the reaction path and fast relaxation of other degrees of freedom in most cases is no longer possible and it is necessary to consider dynamical models, which are not the topic of this section. But often the temperature, solvent or pressure dependence of reaction rate... [Pg.851]

As a multidimensional PES for the reaction from quantum chemical calculations is not available at present, one does not know the reason for the surprismg barrier effect in excited tran.s-stilbene. One could suspect diat tran.s-stilbene possesses already a significant amount of zwitterionic character in the confomiation at the barrier top, implying a fairly Tate barrier along the reaction path towards the twisted perpendicular structure. On the other hand, it could also be possible that die effective barrier changes with viscosity as a result of a multidimensional barrier crossing process along a curved reaction path. [Pg.857]

To calculate N (E-Eq), the non-torsional transitional modes have been treated as vibrations as well as rotations [26]. The fomier approach is invalid when the transitional mode s barrier for rotation is low, while the latter is inappropriate when the transitional mode is a vibration. Hamionic frequencies for the transitional modes may be obtained from a semi-empirical model [23] or by perfomiing an appropriate nomial mode analysis as a fiinction of the reaction path for the reaction s potential energy surface [26]. Semiclassical quantization may be used to detemiine anliamionic energy levels for die transitional modes [27]. [Pg.1016]

Heidrich D (ed) 1995 The Reaction Path In Chemistry Current Approaches and Perspectives (Boston Kluwer Academic)... [Pg.2328]

The reaction path is defined by Fukui [83] as the line q(.s) leading down from a transition state along the steepest descent direction... [Pg.2353]

These methods, which probably deserve more attention than they have received to date, simultaneously optimize the positions of a number of points along the reaction path. The method of Elber and Karpins [91] was developed to find transition states. It fiimishes, however, an approximation to the reaction path. In this method, a number (typically 10-20) equidistant points are chosen along an approximate reaction path coimecting two stationary points a and b, and the average of their energies is minimized under the constraint that their spacing remains equal. This is obviously a numerical quadrature of the integral s f ( (.v)where... [Pg.2354]

S is the path length between the points a and b. The Euler equation to this variation problem yields the condition for the reaction path, equation (B3.5.14). A similar method has been proposed by Stacho and Ban [92]. [Pg.2354]

B3.5.7.3 BIFURCATION OF THE REACTION PATH AND VALLEY-RIDGE INFLECTION POINTS... [Pg.2354]

D. Heidrich, ed., The reaction path in chemistry, Kluwer Academic Publishers, Dordrecht, 1995,... [Pg.320]

Using the CFTI protocol, we have calculated directly both the derivative of the free energy with respect to the reaction path dA/dX and the 14 individual derivatives dA/d k, k = 1,...,14 with respect to all fixed coordinates along the path ... [Pg.172]

Some fraction of such events will lead to the system remaining on the Odd surface until, further along the reaction path, the Odd surface again intersects the Even surface on the product side at which time quenching to produce ground-state products can occur. [Pg.294]

Molecular mechanics methods are not generally applicable to structures very far from equilibrium, such as transition structures. Calculations that use algebraic expressions to describe the reaction path and transition structure are usually semiclassical algorithms. These calculations use an energy expression fitted to an ah initio potential energy surface for that exact reaction, rather than using the same parameters for every molecule. Semiclassical calculations are discussed further in Chapter 19. [Pg.53]

The Reaction Path in chemistry Current Approaches and Perspectives D. Heidrich, Ed., Kluwer, Dordrecht (1995). [Pg.163]

Attention should be paid to the fact that the ratio of Pd and phosphine ligand in active catalysts is crucial for determining the reaction paths. It is believed that dba is displaced completely with phosphines when Pd2(dba)3 is mixed with phosphines in solution. However the displacement is not eom-plcte[16]. Also, it should be considered that dba itself is a monodentate alkene ligand, and it may inhibit the coordination of a sterically hindered olefinic bond in substrates. In such a case, no reaction takes place, and it is recommended to prepare Pd(0) catalysts by the reaction of Pd(OAc)2 with a definite amount of phosphinesflO]. In this way a coordinatively unsaturated Pd(0) catalyst can be generated. Preparation of Pd3(tbaa)3 tbaa == tribenzylidene-acetylacetone) was reported[17], but the complex actually obtained was Pd(dba)2[l8],... [Pg.3]

The issue of regioselectivity arises with arylhydrazones of unsymmetrical ketones which can form two different enehydrazine intermediates. Under the conditions used most commonly for Fischer cyclizations, e g. ethanolic HCI, the major product is usually the one arising from the more highly substituted enehydrazine. Thus methyl ketones usually give 2-methy indoles and cycliz-ation occurs in a branched chain in preference to a straight chain. This regioselectivity is attributed to the greater stability of the more substituted enhydrazine and its dominance of the reaction path. [Pg.56]

The reaction path shows how Xe and Clj react with electrons initially to form Xe cations. These react with Clj or Cl- to give electronically excited-state molecules XeCl, which emit light to return to ground-state XeCI. The latter are not stable and immediately dissociate to give xenon and chlorine. In such gas lasers, translational motion of the excited-state XeCl gives rise to some Doppler shifting in the laser light, so the emission line is not as sharp as it is in solid-state lasers. [Pg.130]

Figure 2.7 shows a representation of this situation. The ordinate is an energy axis and the abscissa is called the reaction coordinate and represents the progress of the elementary step. In moving from P to H, the particle simply moves from one equilibrium position to another. In the absence of any external forces, the energy of both the initial and final locations should be the same as shown by the solid line in Fig. 2.7. Between the two minima corresponding to the initial and final positions is the energy barrier arising from the dislodging of the particles neighboring the reaction path from their positions of minimum energy. Figure 2.7 shows a representation of this situation. The ordinate is an energy axis and the abscissa is called the reaction coordinate and represents the progress of the elementary step. In moving from P to H, the particle simply moves from one equilibrium position to another. In the absence of any external forces, the energy of both the initial and final locations should be the same as shown by the solid line in Fig. 2.7. Between the two minima corresponding to the initial and final positions is the energy barrier arising from the dislodging of the particles neighboring the reaction path from their positions of minimum energy.

See other pages where The Reaction Path is mentioned: [Pg.782]    [Pg.830]    [Pg.830]    [Pg.831]    [Pg.837]    [Pg.842]    [Pg.848]    [Pg.851]    [Pg.855]    [Pg.855]    [Pg.856]    [Pg.2312]    [Pg.2333]    [Pg.2350]    [Pg.2350]    [Pg.2353]    [Pg.2353]    [Pg.2353]    [Pg.2353]    [Pg.2353]    [Pg.2354]    [Pg.2354]    [Pg.2354]    [Pg.302]    [Pg.164]    [Pg.177]    [Pg.46]    [Pg.304]    [Pg.305]    [Pg.23]    [Pg.154]    [Pg.46]   


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