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Standard approximation

The velocity Verlet algorithm may be derived by considering a standard approximate decomposition of the Liouville operator which preserves reversibility and is symplectic (which implies that volume in phase space is conserved). This approach [47] has had several beneficial consequences. [Pg.2251]

A burette reading will indicate the actual pointage of the bath compared to the standard (approximately 3-6) for a concentration of 3-5%. Obtain the standard pointage from the chemical manufacturer. [Pg.401]

Furthermore, one can infer quantitatively from the data in Fig. 13 that the quantum system cannot reach the maximum herringbone ordering even at extremely low temperatures the quantum hbrations depress the saturation value by 10%. In Fig. 13, the order parameter and total energy as obtained from the full quantum simulation are compared with standard approximate theories valid for low and high temperatures. One can clearly see how the quasi classical Feynman-Hibbs curve matches the exact quantum data above 30 K. However, just below the phase transition, this second-order approximation in the quantum fluctuations fails and yields uncontrolled estimates just below the point of failure it gives classical values for the order parameter and the herringbone ordering even vanishes below... [Pg.116]

MicroEnv is calculated using standard approximations used in classical molecular mechanics (i.e., pair potentials and analytical expressions for strain energy190) ... [Pg.116]

Shizgal et al. start with the Boltzmann transport equation and after a number of standard approximations write it in the space-independent form as follows ... [Pg.261]

A simple and successful approximation for the excess free energy functional is to first assume that the excess free energy functional is only a functional of the average site density profile, denoted p(r), and then invoke standard approximations, similar to those used for simple liquids, for FEX- With a judicious choice of Fkx[Pm], the free energy functional can be exactly decomposed as... [Pg.123]

The summation starts in -me2, and the energy in the current units is just m. To simplify the iterative process, a standard approximation neglects the vacuum polarization effects giving a simpler structure of the four-current [5,7] ... [Pg.140]

Of course, one is not really interested in classical mechanical calculations. Thus in normal practice the partition functions used in TST, as discussed in Chapter 4, are evaluated using quantum partition functions for harmonic frequencies (extension to anharmonicity is straightforward). On the other hand rotations and translations are handled classically both in TST and in VTST, which is a standard approximation except at very low temperatures. Later, by introducing canonical partition functions one can direct the discussion towards canonical variational transition state theory (CVTST) where the statistical mechanics involves ensembles defined in terms of temperature and volume. There is also a form of variational transition state theory based on microcanonical ensembles referred to by the symbol p,. Discussion of VTST based on microcanonical ensembles pVTST is beyond the scope of the discussion here. It is only mentioned that in pVTST the dividing surface is... [Pg.187]

In the infrared detection system, the sample is weighed into a special ceramic boat which is then placed into a combustion furnace at 1371°C (2500°F) in an oxygen atmosphere. Most of the sulfur present is converted to sulfur dioxide, which is then measured with an infrared detector after moisture and dust are removed by traps. The calibration factor is determined using standards approximating the material to be analyzed. [Pg.298]

Figure 6. 10-15% SDS polyacrylamide gel of lane 1 — untreated E, coli extract (0 mM KCl) lane 2 — the peak GUS fraction from the HPLC separation of untreated extract lane 3 — Sigma SDS-7 molecular weight standards (approximate molecular weights of 4 standards are indicated on the right hand edge of the figure) lane 4 — BPA-1000 treated E. coli extract (4000 ppm BPA-1000 and 300 mM KCl) lane 5 — the peak GUS fraction from the HPLC separation of BPA-1000 treated extract. GUS migrates slightly slower than the 66,000 molecular weight standard. Figure 6. 10-15% SDS polyacrylamide gel of lane 1 — untreated E, coli extract (0 mM KCl) lane 2 — the peak GUS fraction from the HPLC separation of untreated extract lane 3 — Sigma SDS-7 molecular weight standards (approximate molecular weights of 4 standards are indicated on the right hand edge of the figure) lane 4 — BPA-1000 treated E. coli extract (4000 ppm BPA-1000 and 300 mM KCl) lane 5 — the peak GUS fraction from the HPLC separation of BPA-1000 treated extract. GUS migrates slightly slower than the 66,000 molecular weight standard.
In the original formulation of the R12 method [23], which is often referred to as "the standard approximation" or SA, a large uncontracted OBS was needed as the RI basis, strongly limiting the applicability of the R12 method to relatively small systems. Klopper and Samson [26] later pioneered the use of a separate RI basis set and considerably improved the applicability and accuracy of MP2-R12. Valeev developed an alternative formulation of the RI procedure [27] known as the complementary auxiliary basis set (CABS) approach, which had smaller RI errors. Ten-no, on the other hand, proposed the use of a numerical quadrature for the same purpose [28]. Kedzuch et al. later used the CABS approach to develop a particularly elegant and practical formalism for the MP2-R12 energies [30]. [Pg.137]

DFT calculations [17,331,332] of 02/Pt(l 11) find the two different molecular precursors defined in the discussions above and observed by STM [153,326]. However, DFT calculations of 02 dissociation on surfaces are problematical and two different standard approximations for the exchange correlation functional (PW91 and RPBE) get somewhat different results. The DFT calculations are in only fair agreement with experiments. Most troubling is that all DFT barriers to dissociation from both molecular precursors are significant, 0.6-0.9 eV relative to the 02+ Pt(lll) asymptote. This is qualitatively inconsistent with experiment, which shows that thermal dissociation is energetically favored over desorption. [Pg.222]

The standard approximations in TDDFT are the local density approximation (LDA) for vXCCT and the related adiabatic LDA (ALDA) for f . Within LDA, the potential is taken from the model of the homogeneous electron gas [43], with the dominant exchange part vxJA of vx A being only the 1/3 power of pa... [Pg.60]

Sulfur Standard (approximately 100 mg/kg) Transfer 0.1569 g of w-butyl sulfide, accurately weighed, into a tared 500-mL volumetric flask. Dilute to the mark with isooctane, and reweigh. Calculate the sulfur concentration (5), in percent,... [Pg.891]

Ion exchange was performed by crushing and sieving the zeolite to between 70-200 mesh (Tyler standard). Approximately 50 grams was placed into an Erlenmeyer flask, 250 ml of IN NaCl solution was added and the slurry was agitated for 16 hours. [Pg.335]

Commercially available aqueous standard stock solutions or solutions prepared from analytical reagent grade chemicals may be used. Dilute these to give calibration standards approximately in the range given in Section IV.A.l. [Pg.293]

Standard approximate methods, e.g., the Percus-Yevick or hyper-chain approximations, are applicable for systems with the Gibbs distribution and are based on the distinctive Boltzmann factor like exp —U r)/ ksT)), where U(r) is the potential energy of interacting particles. The basic kinetic equation (2.3.53) has nothing to do with the Gibbs distribution. The only approximate method neutral with respect to the ensemble averaging is the Kirkwood approximation [76, 77, 87]. [Pg.124]

In the case of an analysis that requires a protocol to be developed, it is necessary to include the preparation of standards and the recording of data relating to these standards (approximately half a day) and a subsequent manual check of a few analysis points on the sample. [Pg.169]

The coefficients A and B are obtained by applying a least-squares procedure, and the standard approximation error (SAE)... [Pg.315]

We will not go into details of a microscopic modeling of these reactions here but rather parameterize the reaction rates by standard approximations. We adopt the Tafel relation, given at the cathode side by... [Pg.511]

We further neglect the commutator [fC, ri2 ] > which is justified in the so-called standard approximation A [11]. (For a two-electron closed-shell singlet state a formulation in which K does not arise is always exactly possible [10]). This allows us to rewrite (53) as... [Pg.30]

Within the standard approximation we assume that the given basis is saturated at the one-electron level, which implies that the Hartree-Fock equations are solved exactly and that a Brillouin theorem holds even for virtual orbitals that are not represented in the given basis. Then one can replace (64) by the equivalent expression... [Pg.32]

As to the evaluation of B h [as defined by (74)], there is a difference between the two variants A and B of the standard approximation. Approximation A is only used in the context of MP2-R12 as an alternative to approximation B, while in treatments on a higher level of approximation only approximation B is applied. In approximation B all those terms — that arise in the summation over the complete basis — are neglected that in atomic theory decrease as (L + l)-7 or faster, while in approximation A even terms that decrease as (L + 1) 5 are neglected, where L is the highes orbital angular momentum contained in the Cl expansion. Note that the error of a conventional Cl without rl2 terms goes as (L + 1) 3. [Pg.34]

Let us return to the problem of solving the response of the quantum mechanical system to an external electric field. The zeroth-order wave function of the quantum mechanical system is obtained by use of any of the standard approximate methods in quantum chemistry and the coupling to the field is described by the electtic dipole operator. There exist a number of ways to determine the response functions, some of which differ in formulation only, whereas others will be inherently different. We will give a short review of the characteristics of tire most common formulations used for the calculation of molecular polarizabilities and hyperpolarizabilities. The survey begins with the assumption that the external perturbing fields arc non-oscillatory, in which case we may determine molecular properties at zero frequencies, and then continues with the general situation of time-dependent fields and dynamic properties. [Pg.31]

We have introduced the notation qs to signify the value of the coordinate q at the saddle point, and will similarly find it convenient to introduce q to denote the coordinate for the well under consideration. As yet, our statements are general and involve no approximations other than those present in transition state theory itself A standard approximation at this point is to note that in the vicinity of the well it is appropriate to represent the energy surface as a quadratic function in the variable q, and in addition it is asserted that one may make the transcription... [Pg.350]


See other pages where Standard approximation is mentioned: [Pg.253]    [Pg.118]    [Pg.109]    [Pg.15]    [Pg.148]    [Pg.149]    [Pg.124]    [Pg.60]    [Pg.146]    [Pg.245]    [Pg.691]    [Pg.695]    [Pg.891]    [Pg.5]    [Pg.245]    [Pg.118]    [Pg.15]    [Pg.34]    [Pg.40]    [Pg.83]    [Pg.356]    [Pg.342]   
See also in sourсe #XX -- [ Pg.137 ]




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Adiabatic approximation standard techniques

Gibbs free standard energy approximation

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