Electron Configuration
From MyMCAT
Contents |
Introduction
Electron configuration describes the arrangement of electrons in an atom, molecule, or other physical structure (e.g., a crystal). The very first model of an atom's electron configuration was proposed by Niels Bohr. His model was that of an electron in orbit around a nucleus just as a planet orbits a star. The model described quite well the observation that each atom can have multiple orbitals and that with either the absorption or release or energy, electrons could be moved between orbitals.
This model intuitively makes sense, electrons are negative and spin around a positive center, but it fails to explain many phenomena. Why don't the electrons just fall in to the nucleus? Why don't the absorption spectra of the elements correlate with orbital size? and why are the orbitals fixed in energy?
The reason for the failures in Bohr's model is because electrons do not orbit in the sense that we accustomed to. According to Heisenberg, at the microscopic scale, all elementary particles can exhibit both particle-like and wave-like properties. Thus, electrons can act like waves, and as such, electrons interact with each other in complex ways and the states of electrons are no longer viewed as simple particles in orbit, but instead by complex functions of interacting waves. These properties impose certain constraints on how electrons exist and also helps explain why the periodic table is organized the way it is.
The view of electron configuration today is now of electrons in a "blurry" cloud around the nucleus with unknown positions and velocities. An orbital is no longer a simple ring around the nucleus, but instead a region in space where there is a high probability that the electron will be located at any given time (but we have no guarantee of where the electron precisely is). The use of four quantum numbers helps us explain this new view.
Quantum Numbers
In the quantum mechanical view of electron configuration, electrons exist only at specific energy levels (they are quantized) and the shape of an orbital is a probabilistic interpretation of where the electrons are most likely to exist in space around the nucleus. Orbitals, instead of referring to a path the electron would take around the nucleus now refer to regions where there is a high probability the electron is present.The state of each electron in an atom is given by four quantum numbers. Three of these properties describe where the electron is in space around the nucleus and the fourth is independent of the others describing instead how electrons in an orbital are behaving.
| Name: | Denoted: | Value: | Description: |
|---|---|---|---|
| The Principal Quantum Number | n | integer, 1 or more | This number partially defines the overall energy of the orbital and the general distance the orbital is from the nucleus. (In the classical/Bohr view you could consider this analogous to how far away the orbit was from the nucleus) |
| The Azimuthal Quantum Number | l | integer, 0 to n-1 | This number describes the orbital's angular momentum, or otherwise known as the orbital. By convention, letters have been assigned to the integer values (s=0, p=1, d=2, f=3, ...). It however can also be interpreted as the number of nodes in the density plot of the wave function which is describing the electron. Together the Principal and Azimuthal numbers describe the overall energy that an orbital has. |
| The magnetic Quantum Number | ml | integer, -l to +l, including zero. | This number indicates the spatial orientation of a given orbital type (previously described by the other two numbers). Each unique orientation will share the same energy level for a given n and l value. |
| spin quantum number | ms | +½ or -½ (sometimes called "up" and "down") | Spin is an intrinsic property of the electron and independent of the other numbers. |
Putting it all together then, we can discuss any electron in terms of these four numbers. For example, we could say that hydrogen's one electron exists in a n=1, l=0, m=0, s=+½ state, or simply it is in a "1s" orbital (where the s implies l=0 and we are ignoring the spin as it often is not important to an electrons orbital state). Any combination of these numbers describes a valid orbital so long as the basic rules above are not broken. In the next two sections however, we will see that some additional rules are necessary to accurately describe multiple electrons and energy states of an atom.
Pauli Exclusion Principle
When we are working with multiple electrons (basically anything beyond neutral hydrogen) it becomes important to ensure there are no conflicts in electron configuration. Specifically, the Pauli Exclusion Principle states that every electron in an atom must have a unique set of quantum numbers. Therefore, if an element has 5 electrons, no two of these electrons can share the same four numbers. What does this mean? Well if one electron in an atom is in the 2s orbital with a spin of +½, then only one other electron can be in the 2s orbital with a spin of -½ and ALL the remaining electrons must be in different orbitals.
This Pauli Exclusion Principle also allows one to determine how many electrons can exist at a given energy level. For example, in the 3p state, n=3 and l=1. ml thus, can have the values from -l to l, or -1,0, and 1 implying there are three different orbitals at this state. Additionally, ms can be either +½ or -½. This means that the electrons can have anyone of 3 magnetic quantum numbers and 2 spins for a total of 6 different possibilities. Thus, the 3p orbitals can hold up to 6 electrons without violating the Pauli exclusion principle.
The Aufbau Principle
Now that we have described the quantum numbers and the requirement of each electron having a unique set of quantum numbers lets look at all the electrons in an atom. How do we decide which orbital each electron should go into? The theory is quite simple, but in practice can often be difficult to determine, but generally, electrons enter into each state in order of increasing energy; i.e., the first electron goes into the lowest-energy state, the second into the next lowest, and so on. The Aufbau principle describes this order and with a few exceptions is generally correct.When determining the overall energy of an orbital both the principal (ie the shell) and azimuthal (ie the subshell) quantum numbers must be taken into account. Simply stated, the sum of "n" and "l" (the principle and azimuthal quantum numbers) provides a rough approximation of the energy, and thus in comparing two orbitals, the lower n+l orbital is filled first. If the n+l values are the same, the one with the lower principle quantum number is filled first. (This rule is often referred to as the n+l rule.)
For example, n = 3 and l = 0 (3s) has the same n+l as n = 2 and l = 1 (2p) both are n+l = 3 so the "rule" guides you to complete the 2p orbitals before filling the 3s.
The complete order of orbital filling can easily be derived for the whole set of possible orbitals by using the n+l rule: 1s, 2s, 2p, 3s, 3p, 4s, 3d... The order can also however be visually mapped out and described in the diagram to the right. Furthermore, one can determine the filling order by referring to the periodic table. Each row down the periodic table increases the n value, and each "block" is a different l value. The s block is the two leftmost columns, the p block is the 6 rightmost columns, the transition metals are the d block, etc.
This figure shows the orbitals organized by the aufbau principle. The superscript (top) numbers state how many electrons are in that orbital, while the subscript (bottom) numbers state how many electrons in total there from 1s to the current orbital. An atom in its ground state will always fill the maximum value possible for each orbital as it increases whereas atoms which are excited with extra energy often skip orbitals and contain electrons at higher than normal orbital states.
If a atom's electron configuration is to written out, often it is written as simply a noble gas configuration plus some additional orbitals. This reduces the number of orbitals to write and emphasizes only the valence shell electrons.

