1.8 Units 25
EXAMPLES 1.19Molecular properties: wavelength, frequency, and energy
The wavelength λand frequency νof electromagnetic radiation are related to the
speed of light by
c 1 = 1 λν (1.14)
(see Example 3.7), wherec 1 = 1 2.99792 1 × 110
8
1 m 1 s
− 1
1 ≈ 131 × 110
8
1 m 1 s
− 1
. The energy of
a photon is related to the frequency of its associated wave via Planck’s constant
h 1 = 1 6.62608 1 × 110
− 34
Js:
E 1 = 1 hν (1.15)
In a spectroscopic observation of the transition between two states of an atom or
molecule, the frequency of the radiation emitted or absorbed is given byhν 1 =|∆E|,
where∆E 1 = 1 E
2
1 − 1 E
1
is the energy of transition between states with energies E
1
and E
2
.
Different spectroscopic techniques are used to study the properties of atoms and
molecules in different regions of the electromagnetic spectrum, and different units
are used to report the characteristics of the radiation in the different regions. The
values of frequency and wavelength are usually recorded in multiples of the SI units of
hertz (Hz 1 = 1 s
− 1
) and metre (m), respectively, but a variety of units is used for energy.
For example, the wavelength of one of the pair of yellow D lines in the electronic
spectrum of the sodium atom isλ 1 = 1 589.76 nm 1 = 1 5.8976 1 × 110
− 7
m. By equation (1.14),
this corresponds to frequency
and by equation (1.15), the corresponding energy of transition is
∆E 1 = 1 hν 1 = 1 (6.62608 1 × 110
− 34
J s) 1 × 1 (5.0833 1 × 110
14
s
− 1
) 1 = 1 3.368 1 × 110
− 19
J
Energies are often quoted in units of the electron volt, eV, or as molar energies in
units ofkJ mol
− 1
. The value of eV is the product of the protonic charge e(see Table 1.4)
and the SI unit of electric potentialV 1 = 1 J C
− 1
(Table 1.2): eV 1 = 1 1.60218 1 × 110
− 19
J. The
corresponding molar energy is
eV 1 × 1 N
A
1 = 1 (1.60218 1 × 110
− 19
J) 1 × 1 ( 6.02214 1 × 110
23
mol
− 1
)
= 1 96.486 kJ mol
− 1
(1.16)
whereN
A
is Avogadro’s constant. For the sodium example,
∆E 1 = 1 3.368 1 × 110
− 19
J 1 = 1 2.102 eV 1 ≡ 1 202.8 kJ mol
− 1
Very often, the characteristics of the radiation are given in terms of the wavenumber
(1.17)
ν
λ
ν
===
1
c
E
hc
∆
ν
λ
==
×
×
=×
−
−
c 2 99792 10
5 8975 10
5 0833
81
7
.
.
.
m s
m
110
14 1
s
−