absorption spectrum. It must be noted, however, that when a large change
occurs (e.g. due to an alteration in the electronic structure of a molecule) the less
energetic changes, such as the vibration of bonds and rotation of the molecule,
will happen as well, leading to more complex spectra.Quantum theory shows that atoms exist only in discrete states, each of which
possesses a characteristic energy, defined by quantum numbers, which charac-
terize the atomic state. Transitions may occur only between these levels, and
even then some transitions are unfavorable. Electrons occupy atomic orbitals
with characteristic spatial distributions around the nucleus.
The discrete energy levels arise naturally as the allowed solutions of the wave
equations for the system under consideration. Electronic energy levels in atoms
may be accounted for by solving the Schrödinger wave equation.
Atoms have electronic energy levels and atomic orbitals that are defined by
three quantum numbers that can have integer values:n principal quantum number,
l orbital angular momentum quantum number,
m magnetic quantum number, and
ms electronic spin quantum number which can be +1/2 or -1/2 only.The energy of an orbital is mostly dependent on its principal quantum number
n. In fact, for hydrogen, the energy depends only on n. There are only certain
allowed values of the other quantum numbers. For example, l may take integer
values from 0 to (n– 1); m values from +l to -land ms+1/2 or –1/2.
The different orbitals are described by symbols:s (sharp) for l = 0
p (principal) for l = 1
d (diffuse) for l= 2
f ( fundamental) for l = 3For atoms other than hydrogen, the other quantum numbers modify the energy
slightly. For example, the 3p level where n =3, l =1 has a higher energy than the
3 s with n =3, l =0. These are often referred to as subshells.
The atoms of the various elements are built up by adding electrons into the
next empty level with the lowest energy, remembering that each level mayAtomic energy
levels
E1 – Electromagnetic radiation and energy levels 191
Table 2. The regions of the electromagnetic spectruma
Wavelength range Frequency (Hz) Region Spectra
100–1 m 3–300 ¥ 106 Radiofrequency Nuclear magnetic resonance
1–0.1 m 0.3–3 ¥ 109 Radiofrequency Electron spin resonance
100–1 mm 3–300 ¥ 109 Microwave Rotational
1–0.02 mm 0.3–15 ¥ 1012 Far infrared Vibrational
20–2 mm 15–150 ¥ 1012 Infrared (IR) Vibrational
2–0.8 mm 150–375 ¥ 1012 Near infrared Vibrational
800–400 nm 375–750 ¥ 1012 Visible Electronic
400–150 nm 750–2000 ¥ 1012 Ultraviolet (UV) Electronic
150–2 nm 2–150 ¥ 1015 Vacuum UV Electronic
2–0.1 nm 150–3000 ¥ 1015 X-ray Inner shell electronic
0.1–0.0001 nm 3–3000 ¥ 1018 g-ray Nuclear reactions
aThe regions overlap considerably, and the range is approximate.