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Shells, electrons and

Figure Bl.24.14. A schematic diagram of x-ray generation by energetic particle excitation, (a) A beam of energetic ions is used to eject inner-shell electrons from atoms in a sample, (b) These vacancies are filled by outer-shell electrons and the electrons make a transition in energy in moving from one level to another this energy is released in the fomi of characteristic x-rays, the energy of which identifies that particular atom. The x-rays that are emitted from the sample are measured witli an energy dispersive detector. Figure Bl.24.14. A schematic diagram of x-ray generation by energetic particle excitation, (a) A beam of energetic ions is used to eject inner-shell electrons from atoms in a sample, (b) These vacancies are filled by outer-shell electrons and the electrons make a transition in energy in moving from one level to another this energy is released in the fomi of characteristic x-rays, the energy of which identifies that particular atom. The x-rays that are emitted from the sample are measured witli an energy dispersive detector.
In these approximations for the K series the value 1 is subtracted from the atomic number Z to correct for the screening of the nuclei by the remaining K-shell electron. For the L series the screening effect of the two K-shell electrons and the seven remaining L-shell electrons must be taken into consideration by subtracting 7.4. [Pg.196]

Note that the occurrence of a maximum oxidation state, corresponding to the removal of all the valence shell electrons and the adoption of a configuration, does not occur after manganese. In Chapter 9 we see how this reflects the contraction of the poorly penetrating 3d orbitals as the nuclear charge increases and it becomes progressively more difficult to remove electrons. [Pg.18]

There is no clear rigorous definition of an atom in a molecule in conventional bonding models. In the Lewis model an atom in a molecule is defined as consisting of its core (nucleus and inner-shell electrons) and the valence shell electrons. But some of the valence shell electrons of each atom are considered to be shared with another atom, and how these electrons should be partitioned between the two atoms so as to describe the atoms as they exist in the molecule is not defined. [Pg.276]

In this equation, Z is the effective nuclear charge, which takes into account the fact that an outer electron is screened from experiencing the effect of the actual nuclear charge by the electrons that are closer to the nucleus (see Section 2.4). In principle, the Allred-Rochow electronegativity scale is based on the electrostatic interaction between valence shell electrons and the nucleus. [Pg.89]

For the S03 molecule, the structure we draw first by considering the number of valence shell electrons and the octet rule is... [Pg.113]

Fig. 7.16. Binding energies of (a) K shell electrons and (b) L shell electrons as a function of atomic number. The graphs were constructed from data tabulated in Ref. [56]. Fig. 7.16. Binding energies of (a) K shell electrons and (b) L shell electrons as a function of atomic number. The graphs were constructed from data tabulated in Ref. [56].
For a better understanding of the energy level splitting of triplet and singlet levels Ti and Si, let us neglect the closed-shell electrons and consider just a two-electron system ... [Pg.10]

Look at their positions in the periodic table. The group 4A element germanium has four valence-shell electrons and thus has four relatively low ionization energies, whereas the group 5A element arsenic has five valence-shell electrons and has five low ionization energies. [Pg.208]

Group 2A elements tend to lose both of their ns2 valence-shell electrons and adopt a noble gas electron configuration. [Pg.230]

It is not clear whether an increase in the effective nuclear charge is reasonable. In principle, such an increase could be explained by an increased covalency between the inner shell electrons and the ligands, leading to a charge transfer from inner shells to the ligands and thus to an increase of the effective nuclear charge Z for the f-electrons. This effect could be called anti-screening . [Pg.534]

Although structures for many chemical species can be described using only single bonds, this is not possible for many others. For the relatively simple C02 molecule, the structure can be determined as follows. The carbon atom has four valence shell electrons and each oxygen atom has six, so 16 valence shell electrons must be distributed to provide an octet around each atom. For three atoms, eight electrons around each would require a total of 24 electrons if there were no shared electrons. Because only 16 electrons are available, eight must be shared so they contribute to the octet of more than one atom. [Pg.51]

When sulfur bums in air, the product is S02. The three atoms have a total of 18 valence shell electrons, and by following the procedure described previously, it found that six electrons must be shared. This means that there will be three bonds to the central atom. However, for it to have an octet of electrons, it must also have an unshared pair of electrons. The structures that show these features are... [Pg.52]

The cyanamide ion, CN22-, contains 16 valence shell electrons and has the linear structure... [Pg.181]


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See also in sourсe #XX -- [ Pg.15 ]

See also in sourсe #XX -- [ Pg.12 ]




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Valence-shell electron pair repulsion, and

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