An atom of an element has different shells, subshells, and orbitals, and the distribution of electrons in these shells is known as the electronic configuration. The electronic arrangement of any orbital can alternatively be represented using the notation nlx, which stands for “notation for loops.”
where,
No. of primary or principal shells or the number of principal quantum numbers (n).
l is the symbol for a sub-shell or an orbital.
x represents the number of electrons present in that orbital.
The symbol 3p2 indicates that there are two electrons in the p subshell of the third main shell, for example.
For the purpose of retrieving the complete electronic configuration of an atom, these notations are written one after the other in the increasing order of the energy of the orbital. It is always the case that the electrons filling orbitals start from the lowest-energy orbital, with the electrons inhabiting the lower-energy orbitals being the first ones to fill.
The Following Is an Example Of An Electronic Configuration Comprising A Few Elements
In order to make the electrical configuration of the elements as easy and convenient as possible, it is expressed in such a way that the electronic configuration of the noble gas core comes before the electronic configuration of the valence shell electrons in the valence shell. It is represented by the noble gas symbol, which is enclosed in square brackets, followed by the valence shell configuration of the noble gas. The electronic configuration of magnesium is stated as [Ne]3s2, whereas the electronic configuration of calcium is written as [Ar]4s2. There are a set of laws and principles that regulate the filling of electrons into an orbital, and these rules and principles are as follows:
Orbitals that are completely filled and half-filled maintain their stability.
When it comes to writing electronic configuration, almost all of the elements follow the same pattern. When the energies of two subshells differ, it is possible that an electron from the lower energy subshell will travel to the higher energy subshell.
This Is Due to A Combination Of Two Factors
Symmetrical distribution: As we all know, symmetry promotes stability in the distribution of information. It is more stable to have electrons in orbitals in which the subshell is exactly half-filled or totally filled than in other orbitals because of the symmetrical distribution of electrons in these orbitals.
Exchange of energy: Because the electrons in degenerate orbitals have a parallel spin, they have a tendency to exchange their positions with one another. The energy released as a result of this action is referred to as exchange energy. At a point where the orbitals are half-full or totally filled, the number of exchanges is at its highest. As a result, its stability is at its greatest.
Stability Of Orbitals That Are Half Filled and Totally Filled
Degenerate orbitals that are exactly half filled and totally filled have more stability than other partially filled configurations in degenerate orbitals that are not exactly half filled or completely filled. In terms of symmetry and exchange energy, this can be explained in more detail. Because of the symmetrical distribution and exchange energies of d electrons, chromium, for example, has the electronic configuration [Ar]3d5 4s1 rather than [Ar]3d4 4s2 due to the symmetrical distribution and exchange energies of d electrons.
The Distribution of Electrons Is Symmetrical
Stability is achieved by symmetry. The symmetrical distribution of electrons in the half-filled and fully-filled configurations makes them more stable than the asymmetrical distribution of electrons in the unfilled configurations.
Degenerate orbitals such as px, py, and pz are shown to have equal energies, despite the fact that their orientation in space is different. In this symmetrical distribution, the effect of one electron on another is relatively minor, and as a result, the electrons are drawn more strongly to the nucleus, increasing the stability of the nucleus overall.
Exchange of energy: If two or more electrons with the same spin are present in degenerate orbitals, there is a probability that their positions will be switched around. During the exchange process, energy is released, and the energy that is released is referred to as exchange energy. If a greater number of exchanges are conceivable, then a greater amount of exchange energy will be released. Only in the case of half-filled and fully-filled configurations is it possible to make a greater number of swaps.
Conclusion
When compared to alternative arrangements, the perfectly half-filled and fully filled orbitals exhibit superior stability. The factors that contribute to their stability are symmetry and energy exchange. The electrons that are present in the different orbitals of the same subshell are capable of exchanging positions with one another.