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Hamilton formulation

To develop a system of mechanics from here without the introduction of any other concepts, apart from energy, some general principle that predicts the course of a mechanical change is required. This could be like the Maupertuis principle of least action or Fermat s principle of least time. It means that the actual path of the change will have an extreme value e.g. minimum) of either action or time, compared to all other possible paths. Based on considerations like these Hamilton formulated the principle that the action integral... [Pg.101]

The main advantage of the Lagrange and Hamilton formulations is that any set of non-redundant variables can be used, while the Newton formulation focuses on spatial coordinates and corresponding velocities. The main difference between the Lagrange and Hamilton formulations is that the former is a single second-order differential equation, while the latter is a coupled set of first-order differential equations. Depending on the system, one of them may be easier to solve than the other. [Pg.453]

For considering mechanics problems, the formula based on the energy, which is a conserved quantity, is usually superior to that based on the Lagrangian mentioned above. W.R. Hamilton formulated an EOM based on the energy, which excels in its applicability to mechanics problems. With the general momentum pi, the total differential of the time-independent Lagrangian is given as... [Pg.14]

The aim of this section is to show how the modulus-phase formulation, which is the keytone of our chapter, leads very directly to the equation of continuity and to the Hamilton-Jacobi equation. These equations have formed the basic building blocks in Bohm s formulation of non-relativistic quantum mechanics [318]. We begin with the nonrelativistic case, for which the simplicity of the derivation has... [Pg.158]

These difficulties have led to a revival of work on internal coordinate approaches, and to date several such techniques have been reported based on methods of rigid-body dynamics [8,19,34-37] and the Lagrange-Hamilton formalism [38-42]. These methods often have little in common in their analytical formulations, but they all may be reasonably referred to as internal coordinate molecular dynamics (ICMD) to underline their main distinction from conventional MD They all consider molecular motion in the space of generalized internal coordinates rather than in the usual Cartesian coordinate space. Their main goal is to compute long-duration macromolecular trajectories with acceptable accuracy but at a lower cost than Cartesian coordinate MD with bond length constraints. This task mrned out to be more complicated than it seemed initially. [Pg.122]

Just as single reference Cl can be extended to MRCI, it is also possible to use perturbation methods with a multi-detenninant reference wave function. Formulating MR-MBPT methods, however, is not straightforward. The main problem here is similar to that of ROMP methods, the choice of the unperturbed Hamilton operator. Several different choices are possible, which will give different answers when the tlieory is carried out only to low order. Nevertheless, there are now several different implementations of MP2 type expansions based on a CASSCF reference, denoted CASMP2 or CASPT2. Experience of their performance is still somewhat limited. [Pg.132]

It applies for both formulations above that the expansion in principle contains an infinite number of terms. The convergence to a few lowest order terms relies on the ability to orderly separate influences of the dominant rf irradiation terms (through a suitable interaction frame) from the less dominant internal terms of the Hamiltonian. In principle, this may be overcome using the spectral theorem (or the Caley-Hamilton theorem [57]) providing a closed (i.e., exact) solution to the Baker-Campbell-Hausdorf problem with all dependencies included in n terms where n designates the dimension of the Hilbert-space matrix representation (e.g., 2 for a single spin-1/2, 4 for a two-spin-1/2 system) [58, 59]. [Pg.9]

Steels MD, Hamilton M McLean PC (1992). The consequences of a change in formulation of methadone prescribed in a drug clinic. British Journal of Addiction, 87, 1549-54 Steinberg KL, Roffman RA, Carroll KM, Kabela E, Kadden R, Miller M Duresky D (2002). Tailoring cannabis dependence treatment for a diverse population. Addiction, 97, 135-42... [Pg.170]

Hamilton and coworkers designed a rocket propellant formulation based on BAMO-AMMO Copolymer TPE and 80% total solids (AP and Al) and it was directly cast into a phenolic case and required no liner or insulation. The results of firing of a 18 kg test motor exhibited completely acceptable ballistic properties. The authors claimed it to be the 1st demonstration of a high energy TPE motor firing [158]. Prior to this, Wardle and his team reported BAMO-AMMO copolymer and CL-20-based potentially attractive high energy ETPE gun propellants. [Pg.265]

Quantitative Formulations. Computer simulations (213) have been used to put the Gurney-Mott mechanism on a more quantitative basis. Hamilton s recent formulation (214) uses "a more analytical approach. ., that gives a maximum insight into the concepts involved." The method is based on the principle that when there is a branch in a sequence of events allowing two or more possible pathways, a particular event j will be selected with probability p given by... [Pg.370]

Hamilton s original formulation contained the assumption that the individual silver atom center is highly unstable, an assumption not supported by molecular orbital calculations. [Pg.371]

In gas-solid flows well beyond the Stokes regime, the effect of convective acceleration of the gas surrounding the particle is important. To incorporate this effect into the preceding formulation, modifications of the expressions for the Stokes drag, carried mass, and Basset force in the BBO equation are necessary [Odar and Hamilton, 1964]. The modified BBO equation takes the form [Hansell et al., 1992]... [Pg.108]

The Hamiltonian formulation plays an important role in connection with quantum mechanics. The Hamilton operator of quantum mechanics H is constructed from the Hamilton function of classical mechanics H by replacing the momenta by operators. If Cartesian coordinates are used, these operators are given by pi = —ihd/dqi. [Pg.73]

The Hamilton-Jacobi form of the classical equations of motion has been shown to have provided the basis for the quantum-mechanical formulations according to Sommerfeld, Heisenberg, Schrodinger and Bohm. Each of these formulations inspired its own peculiar interpretation of quantum effects, despite their common basis. Each of the different points of view still has its adherents and the debates about their relative merits continue. Closer scrutiny shows that the Sommerfeld and Heisenberg systems assume quanta to be particles in the classical sense, although Heisenberg considered electronic positions to be fundamentally unobservable. [Pg.85]

Schrodinger s equation is the wave-mechanical analogue of Hamilton s formulation of the classical laws of motion. Hamilton s function ... [Pg.276]

To quantize the dynamics of the particles first requires that we express the velocities of the particles in terms of canonical momenta. In the presence of electromagnetic fields, the canonical momenta are not merely m dx-Jdt). Rather, in order to incorporate Lorentz s velocity-dependent forces into Hamilton s formulation of classical mechanics, the canonical momenta are given by [2]... [Pg.8]

Special techniques are required to describe the symmetry of fields. Since fields are defined in terms of continuous variables it is desirable to formulate suitable transformations of dynamic variables pertaining to fields, in terms of continuous parameters. This is done by using Hamilton s principle and defining quantities such as momentum densities for any field. The most useful parameter to quantify the symmetry of a field is the Lagrangian density (T 3.3.1). [Pg.17]

Although a powder neutron diffraction analysis of PtF carried out by Ibers and Hamilton soon confirmed the formulation tentatively provided by the X-ray data (Ref. 13), they were obliged to tilt the O2 and three-fold disorder it in order to arrive at a suitable 0-0 distance. Recently (see Ref. 121), using anhydrous liquid HF as a solvent, we succeeded in growing single crystals of O RuF. With the more favorable heavy atom scattering factors of this salt we were able to prove the Ibers and Hamilton conjecture and also derive the 0-0 distance directly from the refinement. [Pg.3]

X-ray powder dilTiaction data provided powerful structural evidence to support the formulation for the first O2 salt [1], O2 PtFg" The light-atom placement was not sufficiently precise to settle this fonmilation by itself, however, and it was only the combination of this structural information with the magnetic and chemical properties of Oi PtF that established it N.K. Jha prepared a sample of OjPtF for the neutron diffraction structure which rvas carried out by Ibers and Hamilton [2]. They had to... [Pg.33]

In order to obtain a more compact formulation of the mixed quantum-classical equations we use a Hamilton-Jacobi-like formalism for the propagation of the quantum degree of freedom as in earlier studies [23], A similar approach has been introduced by Nettesheim, Schiitte and coworkers [54, 55, 56], TTie formalism presented here is based on recent investigations of the present authors [23], This formalism can be summarized as follows. Starting from the Hamiltonian Eqn. (2.2) and averaging over the x- and y-mode, respectively, gives... [Pg.137]

The mixed quantum-classical equations of motion can now be formulated in the form of Hamilton s equations... [Pg.138]

Gennery AR, O Sullivan JJ, Hasan A, Hamilton JR, Dark JH. Changing cyclosporin A formulation an analysis in paediatric cardiac transplant recipients. PediatrTransplant 1999 3 215-218. [Pg.664]


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See also in sourсe #XX -- [ Pg.453 ]




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Hamilton

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