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Force computation

Additionally, to optimize task 4, we applied a conventional, atom pair interaction based multiple-time-step scheme to the force computation within Ihe innermost distance class. Here, for atom pairs closer than 5 A, the Coulomb sum is calculated every step, and for all other atom pairs the Coulomb sum is extrapolated every second step from previously explicitly calculated forces. [Pg.83]

Fig. 5. Theory vs. experiment rupture forces computed from rupture simulations at various time scales (various pulling velocities Vcant) ranging from one nanosecond (vcant = 0.015 A/ps) to 40 picoscconds (vcant = 0.375 A/ps) (black circles) compare well with the experimental value (open diamond) when extrapolated linearly (dashed line) to the experimental time scale of milliseconds. Fig. 5. Theory vs. experiment rupture forces computed from rupture simulations at various time scales (various pulling velocities Vcant) ranging from one nanosecond (vcant = 0.015 A/ps) to 40 picoscconds (vcant = 0.375 A/ps) (black circles) compare well with the experimental value (open diamond) when extrapolated linearly (dashed line) to the experimental time scale of milliseconds.
In the context of molecular simulation, particularly biomolecular modelling, a critical aspect for numerical simulation is the presence of long-range Coulombic forces which render the force computations much more costly... [Pg.349]

Moving responsibility for the force computation away from the patches required a move away from pure message-driven execution to dependency-driven execution in which patches control the data (atomic coordinates) needed for compute objects to execute. A compute object, upon creation, registers this dependency with those patches from which it needs data. The patch then triggers force calculation by notifying its dependent compute objects when the next timestep s data is available. Once a compute object has received notification from all of the patches it depends on, it is placed in a prioritized queue for eventual execution. [Pg.478]

The complexity of the force computation function described here is computed by counting the number of force terms evaluated by each processor. The cost of force computation for processor i, which is denoted by C is,... [Pg.488]

As before, let Cj, denote tbe cost of force computation on processor i, 0 < i < P — 1). Processor i is assigned U rows of the force matrix and for load balance - , lp will satisfy h algorithm computes a priori the row assignment so that the load sent to processors is balanced. Some typical values are listed in Table 6. [Pg.488]

The time complexity of this algorithm shows that the force computation does not involve any extra overheads and therefore, the speedup should be equal to P and efficiency 100% in theory. [Pg.489]

Force computation at time t.M is a diagonal matrix with atom masses. F is the vector of mechanical forces F(r) = — W. /... [Pg.144]

This famous electrostatic theorem states that the intemuclear forces, which drive the formation and breakage of bonds, are equal to the forces computed from electrostatics. Of course, the simplicity of this formula hides a formidable difficulty p(r ) depends itself on the positions of all atoms, it is an unknown functional of the electron-nuclei potential vext(r) ... [Pg.333]

In practice, even the requirement for a "full range of frequencies" is sometimes eased because we can identify the particular features of response important to a particular force computation. The principal limitation to the language of dielectric response is its restriction to electric fields weak enough to provoke only a linear response. This weak-field condition poses no limitation to computing forces between materials in their thermal-equilibrium states. [Pg.242]

This transform provides the needed conversion between measurements conducted at real frequencies < R and the e(/ ) used in force computation. Except for the case of conductors, in which e( 0) = oo, e(0) is finite. In the entire lower half of the... [Pg.246]

Because of the wide range of possible velocities, valence electron energy loss spectra have proven most useful for gathering data used in van der Waals force computation. [Pg.250]

On the positive- axis used in force computation, e(i ) is a reassuringly sedate function ... [Pg.257]

The slowly decreasing form of this last relation shows why incompleteness of spectral information need not always impede force computation. Even limited data can often give an adequate idea of the magnitude of forces. [Pg.272]

A true test of the significance of different forces computed between similar pairs of surfaces (e.g., those pairs in Fig. 1) is whether these different forces lead to different rates of deposition. Toward this end, the rate of deposition of spherical hydrosol particles onto a rotating disk collector... [Pg.123]

For three-dimensional crystals the lattice summation converges only slowly, and in any brute-force computational scheme one must make sure that, as one sums outward from the "zeroth unit cell" at the center of the crystal, the ions included at any stage should have as close to zero net charge as possible. For some crystals the Madelung constants a have been evaluated (Table 8.4), using component potentials obtained by summing certain infinite series. [Pg.481]

Each processor is assigned a predetermined set of force computations, involving a force decomposition of the workload that remains in effect during the simulation. [Pg.261]

Twenty years ago Car and Parrinello introduced an efficient method to perform Molecular Dynamics simulation for classical nuclei with forces computed on the fly by a Density Functional Theory (DFT) based electronic calculation [1], Because the method allowed study of the statistical mechanics of classical nuclei with many-body electronic interactions, it opened the way for the use of simulation methods for realistic systems with an accuracy well beyond the limits of available effective force fields. In the last twenty years, the number of applications of the Car-Parrinello ab-initio molecular d3mam-ics has ranged from simple covalent bonded solids, to high pressure physics, material science and biological systems. There have also been extensions of the original algorithm to simulate systems at constant temperature and constant pressure [2], finite temperature effects for the electrons [3], and quantum nuclei [4]. [Pg.643]

Solubility in DMSO is less intuitive than aqueous solubility, based on examination of the chemical structure. Chemists can usually differentiate between compounds that are soluble or insoluble in water, but it is much harder to predict compounds that are soluble or insoluble in DMSO (Balakin, 2003). Solubility in DMSO is determined by a subtle balance of oppositely-directed inter- and intramolecular forces. Computational models have been developed to predict DMSO solubility with greater than a 90% success rate (Balakin, 2003 Balakin et al., 2004 Japertas et al., 2004 Lu and Bakken, 2004 Delaney, 2005). Software can be used to provide an alert to a compound with a low DMSO solubility... [Pg.117]

Kennedy, I.H., Thin films solid electrolyte systems. Thin Solid Films 43 (1977) 41-92. Skliar, M. and Tathireddy, R, Approximation of evolutional system using singular forcing, Comput. Chem. Eng. 26 (2002) 1013—1021. [Pg.91]

In the case of the protonated Schiff base model, the forces computed from the LR-TDDFT Sj PES lead to a single bond rotation instead of double bond isomerization. This failure might be related to the local approximation of the exchange-correlation functional or, as suggested by the significantly different results obtained with P-TDDFT, to a breakdown of the linear response approximation. Further investigations in this respect are needed. P-TDDFT and ROKS correctly... [Pg.137]

This has opened the way to a systematic, quantum chemical definition and description of functional groups, to macromolecular shape analysis, to macromolec-ular force computations, and to shape-code-based macromolecular similarity analysis [20-25],... [Pg.347]

Current prediction techniques allow a detailed and reasonable structure to be generated only for small or constrained systems. Five- or 10-residue protein loops or molecules such as enkephalin represent the limit of current techniques. A larger database of protein conformational motifs may increase the success of prediction, but brute force computational approaches will remain impractical for some time. The incorporation of a priori knowledge, whether at an atomic level or through abstraction at a higher level of organization, appears to be the best means available to understand and predict protein conformation. [Pg.74]

The Somoyai function is defined in terms of the electronic density function and the composite nuclear potential, providing a 3D shape representation of the bonding pattern within the molecule under study. Some of the topological techniques of molecular shape analysis have been reviewed, with special emphasis on applications to the Somoyai function. A combination of a family of recently introduced ab initio quality macromolecular electronic density computation methods with the electrostatic Hellmann-Feynman theorem provides a new technique for the computation of forces acting on the nuclei of large molecules. This method of force computation offers a new approach to macromolecular geometry optimization. [Pg.40]


See other pages where Force computation is mentioned: [Pg.299]    [Pg.100]    [Pg.108]    [Pg.440]    [Pg.152]    [Pg.154]    [Pg.268]    [Pg.36]    [Pg.248]    [Pg.253]    [Pg.267]    [Pg.330]    [Pg.66]    [Pg.413]    [Pg.90]    [Pg.266]    [Pg.268]    [Pg.486]    [Pg.8]    [Pg.306]    [Pg.103]    [Pg.193]    [Pg.119]    [Pg.22]    [Pg.184]    [Pg.191]   
See also in sourсe #XX -- [ Pg.403 ]




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