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Electrons in Atomic Shells

As discussed in many introductory chemistry textbooks, electrons on atoms behave according to the rules of quantum mechanics. Their states are described by products of one-electron wavefunctions known as orbitals. One does not have to refer to atomic orbitals for a discussion of the chemical bond ° but they are essential in systematic descriptions of atomic spectra. A qualitative understanding of optical [Pg.34]

The molar volume is proportional to r r = ar N. However, the lattice energy is given in the variable r and not in the volume V. This can be expressed as [Pg.35]

Electrons on atoms are described by an orbital scheme. Briefly, atoms have electrons in shells around the nucleus and each electron in an atom has a unique set of four quantum numbers. No two sets are the same. Electron orbitals are solutions of the Schrodinger equation for one electron in the field of a central charge, the (screened) nucleus. The electronic state of an atom that has more than one valence electron is a combination of products of such orbitals with the right symmetry. Mathematical details are not important here but three points should be noted because they are significant for the color of materials  [Pg.35]

Orbitals have levels which represent the energy necessary to remove the electron from the orbital to infinity at rest is equal to the ith ionization potential, which is the energy needed to remove an electron from an orbital at energy level e ). [Pg.35]

Optical transitions occur between stationary states involving many electrons and cannot in general be described by the excitation of single electrons that change orbitals. The selection rules determine the intensities of the optical transitions and these rules are a simple consequence of the symmetries of the initial and final states. [Pg.36]


The electron density is probed by electromagnetic waves, as in optics. In fact, the same theory of light diffraction and dispersion is relevant to the X-ray diffraction for wavelengths comparable to the size of atoms. For X-rays, the wavelength Xx 0.5-1 A depends on material of the anticathode in an X-ray tube. In a synchrotron, the electromagnetic wave spectrum is very large and determined by the speed of moving electrons. From the experiment we can find the density (or number) of electrons in atomic shells. [Pg.75]


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