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Many shells

Many shell-and-tube condensers use copper alloy tubes, such as admiralty brasses (those containing small concentrations of arsenic, phosphorus, or antimony are called inhibited grades), aluminum brasses, and cupronickel austenitic stainless steel and titanium are also often used. Utility surface condensers have used and continue to use these alloys routinely. Titanium is gaining wider acceptance for use in sea water and severe service environments but often is rejected based on perceived economic disadvantages. [Pg.7]

In order to restria attention to a smgle shell of scatterers, one selects a limited range of the R-space data for back-transformation to k-space, as illustrated m Figure 3B,C. In Ae ideA case, this procedure allows one to anAyze each shell separately, AAough in practice many shells cannot be adequately separated by Fourier tering (9). [Pg.32]

How many shells are occupied by electrons in a gold atom, Au (atomic number 79) ... [Pg.176]

How many shells are needed to account for the seven periods of the periodic table ... [Pg.212]

How many shells are completely filled in an argon atom, Ar (atomic number 18) ... [Pg.212]

The submatrix elements that enter into the left sides of these equations can be expressed in terms of complex CFP [112]. Using these coefficients the many-shell wave function for N electrons (N = Ni + N2 +...+ Nu) is composed of the antisymmetric wave functions of (N — 1) electrons... [Pg.189]

How many shells are there in the spool The number of rings seen in the averaged axial projection is 11 (Fig. 9e), whereas the number of shells required to accommodate the T7 genome, given geometrically... [Pg.316]

Here we discuss thermal emission from Cas A, which directly connects to nucleosynthetic products. Many shell-type SNRs, including Cas A, also show non-thermal synchrotron X-rays - see [115]. [Pg.257]

MultiwaUed carbon nanotubes (MWNT) consist of a concentric arrangement of single-walled nanotubes with a usually constant distance of layers. There are examples with just two nanotubes fit one into another (sodouble-walled nanotubes, DWNTs) as well as species with many shells (more than 50). The latter measure many nanometers in diameter and may be so hard to distinguish from classical carbon fibers that only electron microscopy can reveal the difference. Common MWNTs, however, possess a smaller number of concentric tubes. The nomenclature of MWNT indicates the intercalation of the inner tubes by the notation (wi,mi) (n2,m2i (n3,m3) ...,starting from the central tube. [Pg.135]

As can be seen in Figure 2-50, the first time the correction factor F is equal to or greater than 0.8 an exit is made and the corrected MTD is calculated. From the. 2n that is used in computing the correction factor it is known how many shells in series are to be used. For example, if is used, then four shells in series with a total of eight or more tube passes are required. [Pg.74]

How can we attach a physical interpretation to the eigenvalues of the matrix equation if they are to be changed at will The interpretation of the many-shell effective Hartree-Fock matrix is deferred until Chapter 23. [Pg.205]

Special form for half-closed case of the effective many-shell Hamiltonian. Given a stack of individual shell Fock matrices in H and a stack of shell R matrices in R, forms the single effective Hamiltonian for the combined set of shells the original McWeenyan. [Pg.226]

The effective Hartree-Fock matrix equation for a many-shell system has been derived in Chapter 14 and used in several applications open shells and some MCSCF models. So far, it has been seen simply as the formally correct equation to generate SCF orbitals for these many-sheU structures without any interpretation. In particular, the fact that the effective Hartree-Fock matrix (the McWeenyan ) contains many arbitrary parameters has not been addressed, nor has the practical problem of the actual grounds for the choice of values for these parameters been systematised. In looking at this problem we must bear two points in mind ... [Pg.293]

This fact is extremely useful in the development of many-shell SCF theories as we see in this chapter, but it is also necessary to proceed with caution to ensure that an equation does not have its domain of validity inadvertently reduced by the action of projection operators. [Pg.597]

Solves the spin-restricted many-shell Haxtree-Fock problem. [Pg.600]

If we therefore apply the many-shell formalism to the closed-shell HF problem we obtain the effective Fock matrix... [Pg.676]

With this analysis of the simple one-shell case the interpretation of the many-shell case is much more straightforward. [Pg.677]

There were many shells fired during the dispersion testing that must have left many isolated dud or UXO rounds. For example, on fired Stokes mortars at Camp Simms several unexploded (dud) shells were found resulting from failure to detonate on impact. A similar number of exploded Stokes mortars were also found. Although the final numbers are not in yet, an approximate 50% dud ratio is emerging. Similarly, one of three Livens projectiles was a dud. This is extremely high, most likely due to the early developmental stage of the mortar at this time. [Pg.130]

The level order in many -shell nuclei seems to be well described by an inter-... [Pg.9]

With many shells, shell covers, and head covers... [Pg.111]

Synatschke CV, Schacher EH, Eortsch M, Drechsler M, Muller AHE (2011) Double-layered micellar interpolyelectrolyte complexes-how many shells to a core Soft Matter 7 1714-1725. doi 10.1039/c0sm01195a... [Pg.81]


See other pages where Many shells is mentioned: [Pg.121]    [Pg.122]    [Pg.166]    [Pg.23]    [Pg.121]    [Pg.428]    [Pg.352]    [Pg.675]    [Pg.677]    [Pg.677]    [Pg.132]    [Pg.52]    [Pg.81]    [Pg.153]    [Pg.155]    [Pg.166]    [Pg.798]    [Pg.119]    [Pg.323]    [Pg.327]   


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Energy expression many-shell system

Hartree-Fock equation many shells

Many-body inner shell

Many-body outer shell

Many-body perturbation theory open-shell

Many-body perturbation theory open-shell molecules

Open-shell many body formalism

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