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Exact 2-component

The unitary transformation required for the block diagonalization of the relativistic Fock operator can be obtained in one step if a matrix representation of the Fock operator is available this is achieved by the so-called eXact-2-Component (X2C) approach [725-728,731-734]. An important characteristic of the X2C approach is its noniterative construction of the key operator X of Eq. (11.2). In this noniterative construction scheme, the matrix operator X is obtained from the electronic eigenvectors of the relativistic (modified) Roothaan Eq. (14.13),... [Pg.537]

Turning now to the 2-component relativistic Hamiltonians we observe that the eXact 2-Component (X2C) Hamiltonians reproduces the DC orbital energies quite well, although there is a difference of about 10 Ei, for the lsi/2 level. This discrepancy stems entirely from picture change errors in the two-electron operator since the one-electron X2C Hamiltonian by construction reproduces exactly the positive-energy spectrum of the parent 4-component Hamiltonian. In the present calculations the one-electron X2C Hamiltonian... [Pg.69]

X2C ( eXact 2-Component ) is an umbrella acronym [56] for a variety of methods that arrive at an exactly decoupled two-component Hamiltonian, with X2C referring to one-step approaches [65]. Related methods to arrive at formally exact two-component relativistic operators are, for example, infinite-order methods by Barysz and coworkers (BSS = Barysz Sadlej Snijders, lOTC = infinite-order two-component) [66-69] and normalized elimination of the small component (NESC) methods [70-77]. We discuss here an X2C approach as it has been implemented in a full two-component form with spin-orbit (SO) coupling and transformation of electric property operators to account for picture-change (PC) corrections [14],... [Pg.312]

The exact components of the matrix of hydrodynamic resistance for a two-particle chain are shown in Appendix F. [Pg.25]

In summary, it seems likely that below a few centimeters depth in LIS sediments, Mn comes into fairly rapid equilibrium with solid-phase components such as MnCOs, although at present the exact components remain unknown. [Pg.382]

The phases that are found on a phase diagram are made up of various combinations of components. Components are simply the chemical substances sufficient for this purpose. A component can be an element, such as carbon, or a compound, such as sodium chloride. The exact components chosen to display phase relations are the simplest that allow aU phases to be described. [Pg.91]

The pathogenesis of metal fume fever and ODTS is considered to be based on a non-specific, i.e. non-allergic, activation of macrophages or pulmonary epithelial cells with local and systemic release of pyrogenic and chemotactic mediators. The mechanism of polymer fume fever is unknown, and the exact components of the fume that cause the toxicity are also unknown. It has been shown that the heating rate of PTFE influences the type and quantity of thermal decomposition products, some of which appear to be extremely toxic. [Pg.69]

Standardize designs and define the exact components to be used... [Pg.270]

To carefully delineate the exact components of the precursor, it was dissected into two constituent parts silatrane glycol and alumatrane, which were synthesized as shown [Reactions (3) and (4)] in one step from Si02 and Al(OH)3 respectively (n,i2). [Pg.137]

In general, the final network design should be achieved in the minimum number of units to keep down the capital cost (although this is not the only consideration to keep down the capital cost). To minimize the number of imits in Eq. (7.1), L should be zero and C should be a maximum. Assuming L to be zero in the final design is a reasonable assumption. However, what should be assumed about C Consider the network in Fig. 7.16, which has two components. For there to be two components, the heat duties for streams A and B must exactly balance the duties for streams E and F. Also, the heat duties for streams C and D must exactly balance the duties for streams G and H. Such balemces are likely to be unusual and not easy to predict. The safest assumption for C thus appears to be that there will be one component only, i.e., C = 1. This leads to an important special case when the network has a single component and is loop-free. In this case, ... [Pg.215]

The TBP (True Bolling Point) distillation gives an almost exact picture of a crude petroieum by measuring the boiling points of the components making up the crude whence its name. [Pg.331]

When the two components are mixed together (say in a mixture of 10% ethane, 90% n-heptane) the bubble point curve and the dew point curve no longer coincide, and a two-phase envelope appears. Within this two-phase region, a mixture of liquid and gas exist, with both components being present in each phase in proportions dictated by the exact temperature and pressure, i.e. the composition of the liquid and gas phases within the two-phase envelope are not constant. The mixture has its own critical point C g. [Pg.100]

This is exact—see Problem 11-8. Notice that Eq. 11-14 is exactly what one would write, assuming the meniscus to be hanging from the wall of the capillary and its weight to be supported by the vertical component of the surface tension, 7 cos 6, multiplied by the circumference of the capillary cross section, 2ar. Thus, once again, the mathematical identity of the concepts of surface tension and surface free energy is observed. [Pg.13]

All standard states, both for pure substances and for components in mixtures and solutions, are defined for a pressure of exactly 1 atmosphere. However the temperature must be specified. (There is some movement towards metricating this to a pressure of 1 bar = 100 kPa = 0.986 924 atm. This would make a significant difference only for gases at J= 298 K, this would decrease a p by 32.6 J moT )... [Pg.367]

Since H=K. + V, the canonical ensemble partition fiinction factorizes into ideal gas and excess parts, and as a consequence most averages of interest may be split into corresponding ideal and excess components, which sum to give the total. In MC simulations, we frequently calculate just the excess or configurational parts in this case, y consists just of the atomic coordinates, not the momenta, and the appropriate expressions are obtained from equation b3.3.2 by replacing fby the potential energy V. The ideal gas contributions are usually easily calculated from exact... [Pg.2246]

Vn is often called the barrier of rotation. This is intuitive but misleading, because the exact energetic barrier of a particular rotation is the sum of all V components and other non-bonding interactions with the atoms under consideration. The multiplicity n gives the number of minima of the function during a 360° rotation of the dihedral angle o). The phase y defines the exact position of the minima. [Pg.343]

Imposition of no-slip velocity conditions at solid walls is based on the assumption that the shear stress at these surfaces always remains below a critical value to allow a complete welting of the wall by the fluid. This iraplie.s that the fluid is constantly sticking to the wall and is moving with a velocity exactly equal to the wall velocity. It is well known that in polymer flow processes the shear stress at the domain walls frequently surpasses the critical threshold and fluid slippage at the solid surfaces occurs. Wall-slip phenomenon is described by Navier s slip condition, which is a relationship between the tangential component of the momentum flux at the wall and the local slip velocity (Sillrman and Scriven, 1980). In a two-dimensional domain this relationship is expressed as... [Pg.98]

The double bond in ethylene is stronger than the C—C single bond in ethane but It IS not twice as strong Chemists do not agree on exactly how to apportion the total C=C bond energy between its ct and rr components but all agree that the rr bond is weaker than the ct bond... [Pg.191]

The vapor pressure ratio measures the intrinsic tendency of component 1 to enter the vapor phase relative to component 2. Likewise, ri measures the tendency of Mi to add to Mi - relative to M2 adding to Mi-. In this sense there is a certain parallel, but it is based on Mi - as a reference radical and hence appears to be less general than the vapor pressure ratio. Note, however, that ri = l/r2 means kn/ki2 = k2i/k22- In this case the ratio of rate constants for monomer 1 relative to monomer 2 is the same regardless of the reference radical examined. This shows the parallelism to be exact. [Pg.430]


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