Page 79 - Electrical Properties of Materials
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62                            The hydrogen atom and the periodic table

                                   shell in magnesium. Then come aluminium, silicon, phosphorus, sulphur, and
                                   chlorine with one, two, three, four, and five 3p electrons, respectively. Chlorine
                                   is again short of one electron to fill the 3p shell, and so behaves like fluorine.
                                   The 3p shell is completed in argon, which is again inert.
                                     So far everything has gone regularly, and by the rules of the game the next
                                   electron should go into the 3d shell. It does not. Why? Well, why should it? The
                                   electrons in potassium are under no obligation to follow the energy hierarchy
                                   of the hydrogen atom like sheep. They arrange themselves in such a way as to
                                   have the lowest energy. If there were no interaction between the electrons, the
                                                                                     2
                                   energy levels of the element would differ only by the factor Z , conforming
                                   otherwise to that of the hydrogen atom. If the interaction between the electrons
                                   mattered a lot, we should completely abandon the classification based on the
                                   energy levels of the hydrogen atom. As it happens, the electron interactions
                                                                 ∗
     ∗  In the hydrogen-type solutions the en-  are responsible for small quantitative changes that cause qualitative change
     ergy depends only on n, whereas tak-  in potassium—and in the next few elements, called the transition elements.
     ing account of electron interactions the  First the 4s shell is filled, and only after that are the 3d states occupied. The
     energy increases with increasing val-
     ues of l. It just happens that in po-  balance between the two shells remains, however, delicate. After vanadium
     tassium the energy of the 3d level (n =3,  (with three 3d and two 4s electrons) one electron is withdrawn from the 4s
     l = 2) is higher than that of the 4s level  shell; hence chromium has five 3d electrons but only one 4s electron. The same
     (n =4, l =0).
                                   thing happens later with copper, but apart from that everything goes smoothly
                                   up to krypton, where the 4p shell is finally completed.
                                     The regularity is somewhat marred after krypton. There are numerous
                                   deviations from the hydrogen-like structure but nothing very dramatic. It might
                                   be worthwhile mentioning the rare earth elements in which the 4f shell is being
                                   filled while eleven electrons occupy levels in the outer shells. Since chemical
                                   properties are mainly determined by the outer shells, all these elements are
                                   hardly distinguishable chemically.
                                     A list of all these elements with their electron configurations is given in
                                   Table 4.1. The periodic table (in one of its more modern forms) is given in
                                   Fig. 4.5. You may now look at the periodic table with more knowing eyes. If you
                                   were asked, for example, why the alkali elements lithium, sodium, potassium,
                                   rubidium, caesium, and francium have a valency of one, you could answer in
                                   the following way.
                                     The properties of electrons are determined by Schrödinger’s equation. The
                                   solution of this equation for one electron and one proton tells us that the elec-
                                   tron may be in one of a set of discrete states, each having a definite energy
                                   level. When there are many electrons and many protons, the order in which
                                   these states follow each other remains roughly unchanged. We may then derive
                                   the various elements by filling up the available states one by one with elec-
                                   trons. We cannot put more than one electron in a state because the exclusion
                                   principle forbids this.
                                     The energy of the states varies in steps. Within a ‘shell’ there is a slow
     Whenever a new shell is initiated,  variation in energy but a larger energy difference between shells.
     there is one electron with consid-  All the alkali elements start new shells. Therefore each of them may
     erably higher energy than the rest.  lose an electron; each of them may contribute one unit to a new chemical
     Since all electrons strive for lower  configuration; and each of them has a valency of one.
     energy, this electron can easily be  We may pause here for a moment. You have had the first taste of the
     lost to another element.      power of Schrödinger’s equation. You can see now that the solution of all the
                                   basic problems that have haunted the chemists for centuries is provided by
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