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LEAPS

The introduction of automated scanning systems was a great leap forward in the development. That way, the uncertainties of manual probe guidance were eliminated. Usually, these systems were designed for high-frequency surface tests and followed the outer profile of the surface with a probe that could be moved in several axes. A continuous 100 % scan became possible and, as a result, the documentation of the tests with stripchart recorders suggested itself. Now for the first time, wheel testing became retraceable. [Pg.306]

The history of tire diode laser illustrated in figure C2.16.11 shows tire interiDlay of basic device physics ideas and teclmology. A new idea often does not produce a better device right away. It requires a certain leap of faitli to see tire improvement potential. However, once tire belief exists, tire teclmology can be developed to demonstrate its validity. In tire case of diode lasers, tire better teclmology was invariably associated with improved epitaxial growtli. [Pg.2896]

Fig. 1. The time evolution (top) and average cumulative difference (bottom) associated with the central dihedral angle of butane r (defined by the four carbon atoms), for trajectories differing initially in 10 , 10 , and 10 Angstoms of the Cartesian coordinates from a reference trajectory. The leap-frog/Verlet scheme at the timestep At = 1 fs is used in all cases, with an all-atom model comprised of bond-stretch, bond-angle, dihedral-angle, van der Waals, and electrostatic components, a.s specified by the AMBER force field within the INSIGHT/Discover program. Fig. 1. The time evolution (top) and average cumulative difference (bottom) associated with the central dihedral angle of butane r (defined by the four carbon atoms), for trajectories differing initially in 10 , 10 , and 10 Angstoms of the Cartesian coordinates from a reference trajectory. The leap-frog/Verlet scheme at the timestep At = 1 fs is used in all cases, with an all-atom model comprised of bond-stretch, bond-angle, dihedral-angle, van der Waals, and electrostatic components, a.s specified by the AMBER force field within the INSIGHT/Discover program.
An example of a symplectic/time-reversible method is the Verlet (leap-frog) scheme. This method is applicable to separataP Hamiltonian systems of the... [Pg.352]

HyperChem employs the leap frog algorith m to integrate the et uaLioMs of motion. Th is algoritlim updates the positions of atom s and the velocities for the n e.x 1 time step by tli is ca leu la lion (equation 26). [Pg.70]

The leap-frog algorithm uses the simplest central difference I or-m n la for a derivative... [Pg.311]

Our discussion so far has considered the use of SHAKE with the Verlet algorithm Versions have also been derived for other integration schemes, such as the leap-froj algorithm, the predictor-corrector methods and the velocity Verlet algorithm. In the cast of the velocity Verlet algorithm, the method has been named RATTLE [Anderson 1983]... [Pg.389]

Using MRI as a substitute for X ray tomography IS only the first of what are many medical applica tions More he on the horizon If for example the rate of data acquisition could be increased then it would become possible to make the leap from the equivalent of still photographs to motion pictures One could watch the inside of the body as it works— see the heart beat see the lungs expand and con tract—rather than merely examine the structure of an organ... [Pg.546]

In the first time step (At), the velocities advance from time t=0 to (t h-1/2 At). In doing so, they leap over the positions at time t. The current velocities are then calculated using equation 27. This equation supplies only approximate velocities used to calculate energies at time t. [Pg.70]

As described previously, the Leap-frog algorithm for molecular dynamics requires an initial configuration for the atoms and an initial set of velocity vectors. /2- These initial velocities can come... [Pg.312]

At the research level, spectroscopy continues to flourish and is continually developing with occasional quantum leaps. For example, such a leap resulted from the development of lasers. Not all leaps provide suitable material for inclusion in an undergraduate text such as this. Flowever, even in the relatively short period of seven years since the third edition, there have been either new developments or consolidation of rather less recent ones, which are not only of the greatest importance but which can (1 hope ) be communicated at this level. [Pg.472]

New to the fourth edition are the topics of laser detection and ranging (LIDAR), cavity ring-down spectroscopy, femtosecond lasers and femtosecond spectroscopy, and the use of laser-induced fluorescence excitation for stmctural investigations of much larger molecules than had been possible previously. This latter technique takes advantage of two experimental quantum leaps the development of very high resolution lasers in the visible and ultraviolet regions and of the supersonic molecular beam. [Pg.472]

The food producing industry has responded to consumer demand for foods with lower fat content (Table 1). Foods with low or no cholesterol claims leaped 78% from 1980 to 1990, in spite of the fact that many of the principal food producers reduced the amount of new product introductions during 1989 and 1990 (7). Table 2 indicates the change in the market for various food industry segments, especially those suspected as fat problem generators, including dairy and meat foods. Many low fat and low cholesterol foods were created by a dding claims to food that have always been low in fat and/or cholesterol. [Pg.116]

Once a direction is estabflshed for the next poiat ia the space of the variables of optimization (whether by random search, by systematic evaluation of gradients, or by any other methods of making perturbations), it is possible to take a jump ia the directioa of the improvement much greater than the size of the perturbations. This could speed up the process of finding the optimum and reduce computer time. If such a leap is successful, the next iteration may take a bigger leap and so on, until the improvement stops. Then one could reverse the direction and decrease the size of the step until the optimum is found. [Pg.79]

Figure 1 A stepwise view of the Verlet integration algorithm and its variants, (a) The basic Verlet method, (b) Leap-frog integration, (c) Velocity Verlet integration. At each algorithm dark and light gray cells indicate the initial and calculating variables, respectively. The numbers in the cells represent the orders m the calculation procedures. The arrows point from the data that are used in the calculation of the variable that is being calculated at each step. Figure 1 A stepwise view of the Verlet integration algorithm and its variants, (a) The basic Verlet method, (b) Leap-frog integration, (c) Velocity Verlet integration. At each algorithm dark and light gray cells indicate the initial and calculating variables, respectively. The numbers in the cells represent the orders m the calculation procedures. The arrows point from the data that are used in the calculation of the variable that is being calculated at each step.
Modifications to the basic Verlet scheme have been proposed to tackle the above deficiencies, particularly to improve the velocity evaluation. One of these modifications is the leap-frog algorithm, so called for its half-step scheme Velocities are evaluated at the midpoint of the position evaluation and vice versa [12,13]. The algorithm can be written as... [Pg.46]

Figure lb gives a graphical representation of the steps involved in the leap-frog propagation. The current velocity v , which is necessary for calculating the kinetic energy, can be calculated as... [Pg.46]

The main disadvantage of this algorithm is that it is computationally a little more expensive than the simpler Verlet or leap-frog algorithms (though the added accuracy often outweighs this slight overhead). [Pg.48]

Crystal growth. As we saw in the preceding section, before World War II the dislocation pioneers came to the concept through the enormous disparity between calculated and measured elastic limiting stresses that led to plastic deformation. The same kind of disparity again led to another remarkable leap of imagination in postwar materials science. [Pg.115]

Operators should be trained to look before they leap when they find valves wrongly set. See also Section 3.3.5 (a). Other accidents that occurred because operators failed to carry out simple tasks are described in Sections 13.5 and 17.1. [Pg.90]

Confirming its structure required isolating enough Cgo to apply modern techniques of structure determination. A quantum leap in fullerene research came in 1990 when a team led by Wolfgang Kratschmer of the Max Planck Institute for Nuclear Physics in Heidelberg and Donald Huffman of the University of Arizona successfully prepared buckmin-sterfullerene in amounts sufficient for its isolation, purification, and detailed study. Not only was the buckminsterfullerene structure shown to be correct. [Pg.436]


See other pages where LEAPS is mentioned: [Pg.271]    [Pg.5]    [Pg.25]    [Pg.244]    [Pg.333]    [Pg.311]    [Pg.370]    [Pg.370]    [Pg.370]    [Pg.436]    [Pg.311]    [Pg.94]    [Pg.116]    [Pg.46]    [Pg.46]    [Pg.47]    [Pg.47]    [Pg.816]    [Pg.1138]    [Pg.148]    [Pg.101]    [Pg.782]    [Pg.107]   


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