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Light atoms

These hold quite well for light atoms but become less dependable with greater nuclear charge. The tenu mtercombination bands is used for spectra where the spin quantum number S changes for example, singlet-triplet transitions. They are very weak in light atoms but quite easily observed in heavy ones. [Pg.1134]

Quasiclassical calculations are similar to classical trajectory calculations with the addition of terms to account for quantum effects. The inclusion of tunneling and quantized energy levels improves the accuracy of results for light atoms, such as hydrogen transfer, and lower-temperature reactions. [Pg.168]

The densities of common engineering materials are listed in Table 5.1 and shown in Fig. 5.12. These reflect the mass and diameter of the atoms that make them up and the efficiency with which they are packed to fill space. Metals, most of them, have high densities because the atoms are heavy and closely packed. Polymers are much less dense because the atoms of which they are made (C, H, O) are light, and because they generally adopt structures which are not close-packed. Ceramics - even the ones in which atoms are packed closely - are, on average, a little less dense then metals because most of them contain light atoms like O, N and C. Composites have densities which are simply an average of the materials of which they are made. [Pg.57]

Since such heavy metals contain many more electrons than the light atoms, H, N, C, O, and S, of the protein, they scatter x-rays more strongly. All diffracted beams would therefore increase in intensity after heavy-metal substitution if all interference were positive. In fact, however, some interference is negative consequently, following heavy-metal substitution, some spots measurably increase in intensity, others decrease, and many show no detectable difference. [Pg.380]

Moderators. Neutrons are most effectively slowed by collisions with nuclei of about the same mass. Thus the best moderators are those light atoms which do not capture neutrons. These are H, " He, Be and C. Of these He, being a gas, is insufficiently dense and Be is expensive and toxic, so the common moderators are highly purified graphite or the more expensive heavy water. In spite of its neutron-absorbing properties, which as mentioned above must be offset by using enriched fuel, ordinary water is also used because of its cheapness and excellent neutronmoderating ability. [Pg.1260]

Because the sequence of neutron captures inevitably leads to looFrn which has a fission half-life of only a few seconds, the remaining three actinides, loiMd, 102N0 and losLr, can only be prepared by bombardment of heavy nuclei with the light atoms jHe to foNe. This raises the mass number in multiple units and allows the f Fm barrier to be avoided even so, yields are minute and are measured in terms of the number of individual atoms produced. [Pg.1262]

Thus, it is possible to make a very important assumption that chain-type compounds decompose forming gaseous niobium-containing components, while island-type compounds release upon thermal decomposition only light atoms and molecules into the gaseous phase [383]. [Pg.209]

Oxyfluoride compounds that crystallize in island-type structures decompose and release light atoms into the gaseous phase ... [Pg.216]

Yilmaz, H., Phys. Rev. 100, 1148, "Wave functions and transition probabilities for light atoms." A perturbation expansion based on the functions of Morse-Young-Haurwitz. [Pg.345]

From this discussion the biggest effects clearly arise when hydrogen or deuterium is attached to a light atom. The effect for the substitution of l3C for l2C, for example, amounts to less than 4 percent. (See Problem 9-13.)... [Pg.216]

Figure 1. Molecular graphics (ANIMOL) views of the dihydro-xybenzenes. The gray atoms are carbons, the dark atoms are oxygens and the light atoms are hydrogens. a) ortho b) meta c) para. Figure 1. Molecular graphics (ANIMOL) views of the dihydro-xybenzenes. The gray atoms are carbons, the dark atoms are oxygens and the light atoms are hydrogens. a) ortho b) meta c) para.

See other pages where Light atoms is mentioned: [Pg.407]    [Pg.454]    [Pg.994]    [Pg.1133]    [Pg.1628]    [Pg.1628]    [Pg.1823]    [Pg.1823]    [Pg.2077]    [Pg.2251]    [Pg.261]    [Pg.167]    [Pg.261]    [Pg.323]    [Pg.177]    [Pg.381]    [Pg.103]    [Pg.516]    [Pg.517]    [Pg.857]    [Pg.441]    [Pg.173]    [Pg.166]    [Pg.207]    [Pg.208]    [Pg.216]    [Pg.836]    [Pg.74]    [Pg.318]    [Pg.664]    [Pg.666]    [Pg.692]    [Pg.710]    [Pg.712]    [Pg.725]    [Pg.206]    [Pg.257]    [Pg.1017]   
See also in sourсe #XX -- [ Pg.170 , Pg.172 , Pg.173 , Pg.174 , Pg.176 ]




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ATOMS CAN BE IDENTIFIED BY THE LIGHT THEY EMIT

Atom light induced

Atomic frame light

Atomic orbital calculations, light

Atomic systems light mapping

Atoms identifying with light

Demonstrations Light from Excited Atoms

Electrons on Atoms and Interaction with Light

General features of late potential energy surfaces where the attacking atom is light

Interstitial light atom

Lamb Shift in Light Muonic Atoms

Light Muonic Atoms

Light atom anomaly

Light atom attack

Light atom transfer

Light atomic spectrum

Light dispersion from atoms

Light from atom-molecule

Light, Photon Energies, and Atomic Spectra

Reflection of atoms by light

Sodium atom light emission from

Sodium atoms polarized light

Spin-orbit effects light atoms

Studies of Light Halo Nuclei from Atomic Isotope Shifts

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