Introduction to spectroscopy
The absorption and emission of electromagnetic radiation of specific energy
(wavelength) is a characteristic feature of many molecules, involving the
movement of electrons between different energy states, in accordance with the
laws of quantum mechanics. Electrons in atoms or molecules are distributed at
various energy levels, but are mainly at the lowest energy level, usually termed
the ground state. When exposed to energy (e.g. from electromagnetic
radiation), electrons may be excited to higher energy levels (excited states),
with the associated absorption of energy at specific wavelengths giving rise to
an absorption spectrum. One quantum of energy is absorbed for a single
electron transition from the ground state to an excited state. On the other
hand, when an electron returns to its ground state, one quantum of energy is
released; this may be dissipated to the surrounding molecules (as heat) or may
give rise to an emission spectrum. The energy change (
ΔE) for an electron
moving between two energy states,
E1 and
E2, is given by the equation:
⇒ Equation [26.3] |
ΔE = E1 − E2 = hν |
where
h is the Planck constant and
ν is the frequency of the
electromagnetic radiation (expressed in Hz or s
−1). By substituting for frequency in [26.3J it IS possible to rearrange this equation to give the
expression:
⇒ Equation [26.4] |
ΔE = |
hc |
λ |