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Field equation

Bobrowiez F W and Goddard W A III 1977 The self-eonsistent field equations for generalized valenee bond and open-shell Hartree-Foek wave funetions Modern Theoretical Chemistry vo 3, ed H F III Sehaefer (New York Plenum) pp 97-127... [Pg.2196]

In stead, these m eth od s solve the poten tial energy surface by using a force field equation (see Molecular Mechanics" on page2] i.The force field equation represen ts electron ic energy implicitly th roil gh param eteri/ation. [Pg.12]

Drowicz F W and W A Goddard IB 1977. The Self-Consistent Field Equations for Generalized Valence Bond and Open-Shell Hartree-Fock Wave Functions. In Schaeffer H F III (Editor). Modem Theoretical Chemistry III, New York, Plenum, pp. 79-127. [Pg.180]

A6-12 function (also known as a Lennard-Jones function) frequently simulates van der Waals interactions in force fields (equation 11). [Pg.26]

The force field equations for MM+, AMBER, BIO+, and OPLS are similar in the types of terms they contain bond, angle, dihedral, van derWaals, and electrostatic. There are some differences in the forms of the equations that can affect your choice of force field. [Pg.101]

Upon substitution of the displacement field. Equation (4.163), in the stress-displacement relations and subsequently in the stress-equilibrium differential equations. Equation (4.164), the displacement-equilibrium equations are, for each layer,... [Pg.265]

The thermodynamic quantities and correlation functions can be obtained from Eq. (1) by functional integration. However, the functional integration cannot usually be performed exactly. One has to use approximate methods to evaluate the functional integral. The one most often used is the mean-field approximation, in which the integral is replaced with the maximum of the integrand, i.e., one has to find the minimum of. F[(/)(r)], which satisfies the mean-field equation... [Pg.692]

This is commonly known as the high field equation. It is of similar form to the Tafel equation for activation controlled electrochemical reactions with... [Pg.130]

Using this new variable, the mean-field equation can be written as... [Pg.337]

Most traditional models focus on looking for equilibrium solutions among some set of (pre-defined) aggregate variables. The LEs are effectively mean-field equations, in which certain variables (i.e. attrition rate) are assumed to represent an entire force, the equilibrium state is explicitly solved for and declared the battle outcome. In contrast, ABMs focus on understanding the kinds of emergent patterns that might arise while the overall system is out of (or far from) equilibrium. [Pg.601]

These field equations are derivable from the following lagrangian density... [Pg.580]

Equation (10-22) will be a (formal) solution of (10-1) if the Heisenberg operator in(x) satisfies the free field equation... [Pg.584]

In (11-56) and (11-57) above, iftln and free field equations ... [Pg.648]

These satisfy free-field equations and free-field commutation rules, e.g. [Pg.654]

This is verified by applying U(a,A) to the left and U(a,A) l to the right of both sides of Eqs. (11-142) and (11-97), mid making use of the transformation properties of (11-184) and (11-185) of the fields. Equations (11-241) and (11-242) were to be expected. They guarantee that four-vector, respectively. We are now in a position to discuss the transformation properties of the one-particle states. Consider the one-negaton state, p,s,—e>. Upon taking the adjoint of Eq. (11-241) and multiplying by ya we obtain... [Pg.676]

Hence the transformation (ll-263)-(l1-266) with j> a = 1 and rjP fixed, is not the only one which produces a negaton-positon field operator for which the commutation rules and field equations are invariant. An U (it) satisfying... [Pg.681]

The mapping (7) introduces the unknown interface shape explicitly into the equation set and fixes the boundary shapes. The shape function h(x,t) is viewed as an auxiliary function determined by an added condition at the melt/crystal interface. The Gibbs-Thomson condition is distinguished as this condition. This approach is similar to methods used for liquid/fluid interface problems that include interfacial tension (30) and preserves the inherent accuracy of the finite element approximation to the field equation (27)... [Pg.308]

The transformed field equations, boundary conditions and the Gibbs-Thomson... [Pg.308]

Under the conditions of a static electric field, the Maxwell s field equations reduce to the Poisson equation [111,112,172,261], given by... [Pg.559]


See other pages where Field equation is mentioned: [Pg.315]    [Pg.400]    [Pg.222]    [Pg.461]    [Pg.1183]    [Pg.2369]    [Pg.147]    [Pg.689]    [Pg.192]    [Pg.126]    [Pg.12]    [Pg.379]    [Pg.363]    [Pg.359]    [Pg.150]    [Pg.353]    [Pg.690]    [Pg.510]    [Pg.460]    [Pg.551]    [Pg.601]    [Pg.604]    [Pg.645]    [Pg.649]    [Pg.692]    [Pg.701]    [Pg.310]    [Pg.311]    [Pg.308]    [Pg.559]    [Pg.560]    [Pg.139]   
See also in sourсe #XX -- [ Pg.325 ]

See also in sourсe #XX -- [ Pg.182 ]




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Basic equations for gravity and magnetic fields

Butler-Volmer equation-high field approximation

Conservation Equations in a Flow Field

Constant field equation,

Corrections to Mobility Equations in the High-Field Regime

Coupled field equations

Diffusion Equation for Two-component Gas Mixture (Without and With a Potential Field)

Dirac equation fields

Dirac equation for the electron in an external field

Dirac equation in an external field

Dirac equation in external electromagnetic fields

Dirac equation modified fields

Dirac field-free equation

Einstein field equations

Einstein gravitational field equations

Electric field Maxwell equations

Electromagnetic field equations

Electromagnetic field theory equations

Electromagnetic fields vector wave equations

Field Vectors and the Maxwell Equations

Field and Davidson equation

Field equations allowing for magnetic currents and charges

Field equations and boundary conditions

Field wave equations

Force field equation

Free-space Maxwell equations electromagnetic field

General Self-Consistent-Field Equations and Atomic Spinors

Goldman constant field equation

Goldman-Hodgkin-Katz constant field equation

High-field equation

Hilbert-Einstein field equations

Homogeneous field equation

Laws high field equation

Liouville equation electric field

Magnetic field, Schrodinger equation

Magnetic fields equation

Master equations fields

Maxwell s field equations

Mean field approximation differential equation

Mean velocity field transport equation

Mean-field transition temperature equation

Null-field equations for distributed sources

Null-field equations for localized sources

Proca field equations

Proca field equations gauge invariance

Projective field equations

Reaction-diffusion equation with electric field

Response equations field wave functions

Schrodinger equation field-dependent

Schrodinger equation force field methods

Schrodinger equation self-consistent field

Schrodinger equation self-consistent field theory

Schroedinger wave equation field

Self-consistent field equations, trial

Self-consistent field method Hartree equations

Self-consistent field method Hartree-Fock equations

Self-consistent-field equation

Singlet Field Equation

Solutions of the Differential Equations for Flow Processes with Variable External Stress and Field

Solutions of the Dirac equation in field-free space

Symmetric states field equations

The Levy-Leblond equation in a central field

The Levy-Leblond equation in a magnetic field

The Schrodinger equation in a magnetic field

Time dependent self consistent field equations

Time-dependent self-consistent field Hartree-Fock equation

Uniqueness theorem field equations

Vector fields Yang-Mills equations

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