
750 CHAPTER 15 Analytical Chemistry: Spectroscopy
15.10 Summary
New Concepts
This chapter recapitulates the ideas introduced in Chapter 4 in
the discussion of column chromatography, and introduces the
much more versatile separation methods of gas chromatography
and high-performance liquid chromatography. All chromatogra-
phy works in much the same way: The components of a mixture
are forced to partition themselves between a moving phase and
a stationary phase.The more a given component exists in the
moving phase, the faster it moves through the column; the more
strongly it is absorbed by the stationary phase, the longer it
remains on the column.
In mass spectrometry, a molecule is first ionized by bom-
bardment with high-energy electrons. The molecular ion so
formed can undergo numerous fragmentation reactions before
it passes, along with the daughter ions formed through frag-
mentation, into a region between the poles of a magnet. Ions
are separated by mass, and focused on a detector. The mass
spectrometer gives the molecular weight of a molecule, provided
that the molecular ion can be detected, and high-resolution
mass spectrometry can determine the molecular formula of an
ion. Structural information can often be gained through an
analysis of the important daughter ions in the fragmentation
pattern. The presence of chlorine or bromine in a molecule can
be deduced from the appearance of signals from M 2 isotopes.
Infrared spectroscopy detects vibrational excitation of
chemical bonds. Functional groups have characteristic vibra-
tional frequencies in the IR region that depend on the masses
of the atoms in the bond and on the force constant of the bond.
Analysis of an IR spectrum gives information on the kinds of
functional groups present.
Nuclear magnetic resonance spectroscopy detects the energy
absorbed in the transition from a low-energy state in which the
nuclear spin is aligned with an external magnetic field to a slight-
ly higher energy state in which it is aligned against the external
field.The
1
H NMR spectra can be integrated to reveal the rela-
tive number of hydrogens in each peak. Hydrogens,
13
C, and
some other nuclei have characteristic absorptions (the chemical
shift, δ), which depend critically on the surrounding chemical
environment. Hydrogen nuclei are coupled to adjacent hydrogens
through a coupling constant, J. The number of lines observed for
a particular hydrogen depends on the number of other nuclei to
which it is coupled. For first-order spectra, the number of lines
equals n 1, where n is the number of equivalent coupled nuclei.
Key Terms
base peak (p. 702)
chemical shift (δ) (p. 718)
coupling constant (J) (p. 718)
daughter ion (p. 702)
decoupling (p. 739)
DEPT (distortionless enhancement with
polarization transfer) (p. 741)
diastereotopic (p. 721)
enantiotopic (p. 721)
first-order spectrum (p. 735)
force constant (p. 708)
fragmentation pattern (p. 702)
gas chromatography (GC) (p. 697)
GC/IR (p. 699)
GC/MS (p. 699)
high-performance liquid chromatography
(HPLC) (p. 697)
homotopic (p. 721)
infrared (IR) spectroscopy (p. 707)
integral (p. 718)
Karplus curve (p. 731)
long-range coupling (p. 731)
M 1 peak (p. 700)
mass spectrometry (MS) (p. 699)
molecular ion (p. 700)
n 1 rule (p. 729)
off-resonance decoupling (p. 740)
parent ion (p) (p. 702)
ppm scale (p. 716)
radical cation (p. 699)
tetramethylsilane (TMS) (p. 716)
vinylic hydrogen (p. 724)
wavenumber (p. 708)
Common Errors
Practice, practice, practice! The successful interpretation of
spectra requires it. The most common error is not to realize this
fact. The memorization of tables of data will not make you into
a spectroscopist, but working lots and lots of problems will. See
Section 15.8 for some hints on solving problems.
A central question in this chapter, and in all of chemistry, is,
What’s different? A common error is missing the symmetry of
a molecule and not noticing when two hydrogens are equivalent
or when they are not. This chapter offers a device that is useful
in making such distinctions.