If we consider the first ionization energy of lithium,
we find that its value, at 5.39 eV, would have to result from an
effective nuclear charge of 0.63. This implies that there is a higher
degree of screening than can be explained, as perfect screening
would result in a Zeff value of one. In fact, the ground
state electronic configuration of lithium is 1s22s1,
and the least tightly bound electron is in the 2s orbital, where
Zeff = 1.26.
The electronic configuration 1s3 is prohibited
by the Pauli exclusion principle, which
is stated simply as:
No individual orbital may be occupied
by more than two electrons, and if two electrons do occupy a single
orbital, then their spins must be paired.
Many experiments, such as spectroscopic and magnetic
measurements, have shown that every electron has an intrinsic rotation
or angular momentum known as spin.
The spin direction of an electron can have only two possible values.
These are described by the spin angular momentum
quantum number, ms.
| The values
of the electron spin quantum number |
| ms = +1/2 |
also denoted by α,
or spin-up |
| ms = -1/2 |
also denoted by β,
or spin-down |
An electron is therefore fully described by the
set of four quantum numbers, n, l, ml, and ms.
This leads to the alternative statement of the Pauli exclusion
principle:
No two electrons in an atom may
have the same values for all four quantum numbers n, l, ml,
and ms.
The most important consequence of the Pauli exclusion
principle for atoms is that each set of orbitals with a given n
and l, known as a subshell (a shell
refers to a given value of n), can hold a maximum of (4l+2) electrons,
ie. two for an s subshell, 6 for a p subshell, and 10 for a d subshell.
The building-up principle
In the lithium atom, the third electron is in the
n = 2 shell. It occupies the 2s orbital, and not a 2p orbital, giving
the 1s22s1 ground state electronic configuration.
Why should this be so?
The order in which the orbitals are occupied, such
that the 2s orbital is occupied before the 2p orbital, is known
as the building up principle, or the
aufbau principle. This can be used
to predict the ground-state electronic configuration of a species,
which can be confirmed by spectroscopic measurements.
The building up principle gives the order of occupation
of the orbitals, determined by a combination of the principle quantum
number and the penetration and shielding effects, as:
1s 2s 2p 3s 3p 4s 3d 4p ...
This gives the ground state electronic configurations
of the neutral atoms shown in the table.
| Ground-state
electron configurations of neutral atoms |
| H |
1s1 |
| He |
1s2 = [He] |
| |
|
| Li |
[He]2s1 |
| Be |
[He]2s2 |
| B |
[He]2s22p1 |
| C |
[He]2s22p2 |
| N |
[He]2s22p3 |
| O |
[He]2s22p4 |
| F |
[He]2s22p5 |
| Ne |
[He]2s22p6 = [Ne] |
| |
|
| Na |
[Ne]3s1 |
| Mg |
[Ne]3s2 |
| Al |
[Ne]3s23p1 |
| Si |
[Ne]3s23p2 |
| P |
[Ne]3s23p3 |
| S |
[Ne]3s23p4 |
| Cl |
[Ne]3s23p5 |
| Ar |
[Ne]3s23p6 = [Ar] |
| |
|
| K |
[Ar]4s1 |
| Ca |
[Ar]4s2 |
| Sc |
[Ar]3d14s2 |
| Ti |
[Ar]3d24s2 |
| V |
[Ar]3d34s2 |
| Cr |
[Ar]3d54s1 |
| Mn |
[Ar]3d54s2 |
| Fe |
[Ar]3d64s2 |
| Co |
[Ar]3d74s2 |
| Ni |
[Ar]3d84s2 |
| Cu |
[Ar]3d104s1 |
| Zn |
[Ar]3d104s2 |
| Ga |
[Ar]3d104s24p1 |
| Ge |
[Ar]3d104s24p2 |
| As |
[Ar]3d104s24p3 |
| Se |
[Ar]3d104s24p4 |
| Br |
[Ar]3d104s24p5 |
| Kr |
[Ar]3d104s24p6
= [Kr] |
If we consider the carbon atom, we see that there
are two electrons in the 2p subshell. This subshell has three
orbitals, and so the two electrons may occupy different orbitals,
or be paired in one on the orbitals. The actual occupancy is each
electron in a different orbital, as dictated by Hund's
rule:
When more than one orbital has
the same energy, electrons occupy separate orbitals and do so with
parallel spins (ie. both α, or
spin up)
The electrons occupy different orbitals because the
electrostatic repulsion between electrons in different orbitals
is lower than that between repulsion between electrons in the same
orbital, and so occupying different orbitals is a lower energy,
and more stable, configuration. The reduced repulsion when the electrons
are in different orbitals results from the fact that the orbitals
occupy different regions of space.
|