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Atomic Orbitals
Light has wave properties, which we characterize by frequency and wavelength,
and particle properties as shown by the the photoelectric effect.
In 1923 a French physicist Louis de Broglie postulated, by analogy with
light, that matter must have both particle and wave properties. De Broglie
proposed that a particle with a mass m moving at a speed u will
have a wavelength given by
= h / m · u
The mathematical description of atomic structure based on the wave properties
of subatomic particles is called quantum mechanics. A model of the
hydrogen atom based on the wave nature of the electron was developed principally
by the Austrian physicist Erwin Schrodinger. Mathematical equations
describing the nature of electron waves in atoms that give acceptable
(acceptable here means physically reasonable) solutions to the Schrodinger
equation are known as wave functions. In order to obtain one of
these wave functions, we must assign integral values known as quantum numbers
to three quantities in the wave equation, similar to the integral value of n
required in the Bohr equation for the hydrogen atom.
A given set of these three quantum numbers yields a wave function for an
electron called an atomic orbital. Although they are only
mathematical expressions, atomic orbitals allow us to visualize a
three-dimensional region in an atom in which there is a high probability of
finding electrons. A fourth quantum number refers to a magnetic property
of electrons called spin. A description of the quantum numbers follows
- Principal Quantum Number (n) The first or principal quantum number
designates the main or principal energy level. This is the most
important quantum number because values of the other two depend on the value
assigned to n. In the case of the hydrogen atom n is the only quantum
number determining the energy ( given by the Bohr formula).
The value of n must be a positive integer n = 1, 2, 3,.... The
size of an orbital depends on n. Energy levels are sometimes called
shells and designated by letters, K (n=1), L (n=2), M (n=3), N (n=4),
.....
- Angular Momentum Quantum Number (l) (Azimuthal
Quantum Number) The angular momentum quantum number designates the
particular energy sublevel or subshell within a principal energy
level. It can have positive integral values from zero to one less than
the value of n. That is l = 0, 1, 2, ...,(n-1). This
quantum number distinguishes orbitals of given n having different
shapes. The different sublevels are usually denoted by a letter as
follows
| Letter |
s |
p |
d |
f... |
| l |
0 |
1 |
2 |
3... |
- Magnetic Quantum Number (ml)
This quantum number designates a particular orbital within a given
sublevel. It distinguishes orbitals of given n and l (
of given energy and shape) but having a different orientation in
space. The allowed values for this quantum number are integers from -l
to +l including zero. Each orbital of a given sublevel has
the same energy. In a sublevel l there will be 2l + 1
orbitals.
The quantum numbers n, l and ml arise from
Schrodinger's treatment of the electron in a hydrogen atom as a matter wave; by
analogy, this concept can be applied to electrons in other atoms as well.
Although these three quantum numbers are sufficient to fully characterize the
orbitals in an atom, there is a need for a fourth quantum number to describe the
electrons that occupy these orbitals.
- Spin Quantum Number (ms) This quantum number
refers to the two possible orientations of the spin axis of an
electron. The name, electron spin quantum number, implies that
electrons have a spinning motion. There is however no way to attach a
precise physical reality to electron spin. What we do know is that
experiments have shown that electrons give atoms properties that can be
explained by assuming that the electron is spinning. The possible
values of the electron spin quantum number are +1/2 and -1/2.
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