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Trajectory Orthogonal

Under the title Shear Fracture, Cook (Ref 4, p 346) noted that under conditions in which the tensile forces cannot develop or are restricted, a type of fracturing that can be associated with trajectories of maximum shear stress may develop. Rinehart 8t Pearson (Ref 1) detonated a 1/8 inch layer of expl on the cylindrical surface of a 2)4 inch OD aluminum (24S-T) cylindrical block with a 3/4 inch cylindrical relief hole drilled thru the longitudinal axis. The shock wave moving in toward the relief hole developed at each point of the block two mutually orthogonal trajectories of maximum shear stress. The trajectories, where the shear stress was maximal, spread out in 8 to 12 curved continuous lines from points on the surface of the relief hole. The shear fraction patterns observed along trajectories of maximum shear resembled the "Luder s... [Pg.544]

Figure 4 Schematic of the model-based optimization process, where performance depends on two variables (Vi and V2). Model-based methods would explore the entire oval domain, seeking the global best. Common OVAT practices only explore a few points along orthogonal trajectories. Abbreviation OVAT, one variable at a time. Figure 4 Schematic of the model-based optimization process, where performance depends on two variables (Vi and V2). Model-based methods would explore the entire oval domain, seeking the global best. Common OVAT practices only explore a few points along orthogonal trajectories. Abbreviation OVAT, one variable at a time.
Examples.—(1) Let xy — C he a system of rectangular hyperbolas, to find the orthogonal trajectory, first eliminate C by differentiation with respect to xt thus we obtain, xdyfdx + y = 0. If two curves are at right angles... [Pg.395]

The differential equation of the one family is obtained from that of the other by substituting dyjdx for - dxjdy. Hence the equation to the orthogonal trajectory of the system of rectangular hyperbolas is, xdx + ydy = 0, or x2 - y2 = Gy a system of rectangular hyperbolas whose axes coincide with the asymptotes of the given system. For polar coordinates it would have been necessary to substitute — (drjr)dd for rdOJdr. [Pg.395]

Collard K, Hall GG (1977) Orthogonal trajectories of the electron density. Int J Quant Chem... [Pg.49]

Helical undulators build on this principle by using two orthogonal magnetic field arrays [82, 83]. These permit transverse excursions in perpendicular x and y directions. If the arrays have a relative longitudinal shift, this introduces a phase to the induced perpendicular excursions and when the phase is 90° the electron trajectory can follow left- or right-handed corkscrew paths The emitted radiation is correspondingly right- or left-handed CPL. [Pg.300]

US studies can produce informative free energy landscapes but assume that degrees of freedom orthogonal to the surface equilibrate quickly. The MD time needed for significant chain or backbone movement could exceed the length of typical US simulations (which are each typically on the nanosecond timescale). However, in spite of this caveat, US approaches have been very successful. One explanation for this success lies in the choice of initial conditions US simulations employ initial coordinates provided by high-temperature unfolding trajectories, which themselves have been found to yield predictive information about the nature of the relevant conformational space. [Pg.488]

At any given instant the equation S(x, t) = const, defines a surface in Euclidean space. As t varies the surface traces out a volume. At each point of the moving surface the gradient, VS is orthogonal to the surface. In the case of an external scalar potential the particle trajectories associated with S are given by the solutions mx = VS. It follows that the mechanical paths of a moving point are perpendicular to the surface S = c for all x and t. A family of trajectories is therefore obtained by constructing the normals to a set of... [Pg.106]

Fig. 7.1 The electron density p(t) is displayed in the and Fig. 7.1 The electron density p(t) is displayed in the and <rv symmetry planes of BF3 in (a) and (b), respectively. The density is a maximum at the position of each nucleus (values of p greater than 2.5 au are not shown in the relief maps) and has a saddle between B and each of the F nuclei. The minimum in p at a saddle point denotes the position of a bond critical point (BCP). The trajectories traced out by the vectors Vp are illustrated in (c) and (d) for the same planes as in (a) and (b). All the paths in the neighborhood of a given nucleus terminate at the maximum value of p found at each nucleus and define the atomic basin. (a) and (b) show two orthogonal views of the same BCP. They indicate that p is a minimum at the BCP along the internuclear axis, the curvature is positive, and two trajec-...
Figure 7. A "snapshot" of a typical cellulosic chain trajectory taken from a Monte Carlo sample of cellulosic chains, all based on die conformational energy map of Fig. 6. Filled circles representing glycosidic oxygens, linked by virtud bonds spanning the sugar residues (not shown), allow one to trace the instantaneous chain trajectory in a coordinate system that is rigidly fixed to the residue at one end of the chain. Projections of the chain into three mutually orthogonal planes assist in visualization of the trajectory in three dimensions. Figure 7. A "snapshot" of a typical cellulosic chain trajectory taken from a Monte Carlo sample of cellulosic chains, all based on die conformational energy map of Fig. 6. Filled circles representing glycosidic oxygens, linked by virtud bonds spanning the sugar residues (not shown), allow one to trace the instantaneous chain trajectory in a coordinate system that is rigidly fixed to the residue at one end of the chain. Projections of the chain into three mutually orthogonal planes assist in visualization of the trajectory in three dimensions.
If one plots classical trajectories on a potential energy surface with /"j and as orthogonal coordinates then the cross terms in the kinetic energy lead to an apparently strange motion, the trajectory not being one expected for a particle moving freely on the surface (for which there would be no cross term). This in illustrated by Fig. 2a. [Pg.100]

This type of mass spectrometer, which is not widely used, allows mass determination with a high precision. An ion cyclotron resonance spectrometer is basically an ion trap ions formed by electron impact, for example, are subjected to the orthogonal magnetic field B, which induces cyclotronic movement in the. rv plane (Fig. 16.8). The radius of the circular movement, which depends on kinetic energy, is given by equation (16.2). If the velocity v is small and the magnetic field B is intense, the radius of the trajectory will be small and the ions will be trapped in the ionisation... [Pg.299]

A very perceptive treatment of chemical reaction dynamics, called the reaction path Hamiltonian analysis, states that the reactive trajectory is determined as the minimum energy path, and small displacements from that path, on the potential-energy surface [64-71]. The usual analysis keeps the full dimensionality of the reacting system, albeit with a focus on motion along and orthogonal to the minimum energy path. It is also possible to define a reaction path in a reduced dimensionality representation. [Pg.259]

The 2P shape resonance in e-Be scattering has served as the test case for almost all the theoretical approaches to the treatment of electron scattering resonances and the earliest applications of the dilated electron propagator have also focused on this system /21,26,40/. Theta trajectories from different decouplings of the bi-orthogonal dilated electron propagator are displayed in fig. 4. The optimal value of a = 0.75 has been determined through a separate a-trajectory /26/. [Pg.244]


See other pages where Trajectory Orthogonal is mentioned: [Pg.158]    [Pg.111]    [Pg.47]    [Pg.395]    [Pg.249]    [Pg.117]    [Pg.17]    [Pg.22]    [Pg.158]    [Pg.111]    [Pg.47]    [Pg.395]    [Pg.249]    [Pg.117]    [Pg.17]    [Pg.22]    [Pg.302]    [Pg.677]    [Pg.371]    [Pg.30]    [Pg.76]    [Pg.407]    [Pg.808]    [Pg.235]    [Pg.14]    [Pg.67]    [Pg.712]    [Pg.468]    [Pg.307]    [Pg.202]    [Pg.859]    [Pg.182]    [Pg.75]    [Pg.186]    [Pg.29]    [Pg.244]    [Pg.221]    [Pg.230]    [Pg.81]    [Pg.201]    [Pg.238]    [Pg.247]   
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