
88 CHAPTER 2 Alkanes
The more spherical neopentane boils about 25 °C lower than the straight-chain isomer.
Isopentane is less extended than pentane but more extended than neopentane, and
its boiling point is right between the two, 30 °C.
Symmetry is especially important in determining melting point because highly
symmetric molecules pack well into crystal lattices. (Think of the computer game
Tetris and how easy packing would be if every shape were a highly symmetrical
square.) The better the packing of the lattice, the more energy it takes to break it up.
So neopentane, for example, melts 113 °C higher than pentane does.
CH
4
H
3
C CH
3
Methane
One signal
Ethane
One signal
Propane
Two signals, one for the CH
2
and another for the two
identical CH
3
groups
C
H H
H
3
CCH
3
FIGURE 2.55 Carbon-13 NMR
signals for three alkanes.
2.14 Nuclear Magnetic Resonance Spectroscopy
Spectroscopy is the study of molecules through the investigation of their interaction
with electromagnetic radiation.There are many kinds of spectroscopy (as we shall see in
Chapter 15). One version is called nuclear magnetic resonance (NMR) spectroscopy
and is particularly valuable,both in chemistry as a device for determining molecular struc-
ture and in medicine as an imaging tool.You have heard of this form of spectroscopy before
if you have ever read an article about magnetic resonance imaging (MRI).NMR and MRI
are the same process,but the dreaded word “nuclear”must be hidden from public view.
Although we won’t go into much detail yet, this early introduction to nuclear
magnetic resonance does allow us to address the critical question of difference.When
are two atoms the same and when are they different?
Like electrons, nuclei of many atoms have a property called spin. A nonzero
nuclear spin is necessary for a nucleus to be NMR active and thus detectable by an
NMR spectrometer. The
13
C and
1
H nuclei each have spins of 1/2, just like the
electron.Although
13
C is present in only 1.1% abundance in ordinary carbon,which
is mostly
12
C, that small amount can be detected.
Like the electron, the
13
C and
1
H nuclei can be thought of as spinning in one of
two directions. In the presence of a strong magnetic field, those two spin states differ
in energy, but by only a tiny amount. Nonetheless, transitions between the two states
can be detected by NMR spectrometers tuned to the proper frequency.We’ll have more
to say about those spectrometers and those transitions in Chapter 15, but there is real-
ly not much more to it than that.So we can see a signal whenever a transition between
the lower and the higher energy nuclear spin states is induced.So what? It would seem
that we have simply built a (very expensive) machine to detect carbon or hydrogen in
a molecule,and it would be hardly surprising to find such atoms in organic molecules!
The critical point is that every different carbon (or hydrogen) in a molecule—
every such atom in a different environment, no matter how slightly different—gives a
signal that is different from that of the other carbons (or hydrogens) in the mol-
ecule.The NMR spectrometer can “count”the number of different carbons or hydro-
gens in a molecule by counting the number of signals.That ability can be enormously
useful in structure determination, and NMR spectroscopy is very often used by “the
pros”of structure determination in exactly that way.The array of signals is called the
NMR spectrum of the molecule.
Let’s use Figure 2.55 to look at a few examples. How many signals will a
13
C NMR
spectrometer “see”for methane? One, of course, because there is only one carbon. How