60 Chapter 2 Atoms: A Quest for Understanding
34
35
Cl
37
Cl
80
60
40
20
0
100
35 36 37 38
Atomic weight (amu)
Relative intensity
FIGURE 2.22
The mass spectrum of chlorine. From this
spectrum we can determine the relative
abundances of
35
CI (75.77%) and
37
CI
(24.23%).
more than otherwise identical ions with a single positive charge because of the
greater interaction between their charge and the magnetic field. Within a very
short distance, the original coherent beam of ions spreads out into beams of dis-
tinct ions, each with a different mass-to-charge ratio.
At the end of the mass spectrometer, the beams of ions are detected. The re-
sults are displayed in a
mass spectrum, as shown in Figure 2.22. Each line on the
spectrum indicates the relative quantity of the different ion beams that result
from the original sample. Using a standard that produces an ion beam with a
known mass, we can reproduce the scale on the bottom of the mass spectrum.
In much the same way, we use a standard to determine the masses of the
atoms in the periodic table. Which element is used as the standard? The most
abundant isotope of carbon,
12
C, is defined as exactly 12 atomic mass units (amu).
12
C = 12.000000000 amu
An atomic mass unit, an arbitrary unit used to set the masses reported in the
periodic table, is currently defined as follows:
1 amu = 1.66053873 × 10
−27
kg 1 kg = 6.02214198 × 10
26
amu
1 g = 6.02214198 × 10
23
amu
Strictly speaking, the amu is not an SI unit, but its use remains sufficiently com-
mon among scientists that we will use it in this textbook.
A detailed look at the mass of individual isotopes shows that they are typically
not integer values. That is, the isotope
63
Cu does not have a mass of exactly 63.
Only
12
C is defined with an exact mass. The isotope
63
Cu has a mass number of 63
but a mass of 62.9296011 amu. The isotope
96
Mo has a mass of 95.9046789 amu.
Precise measurements have shown that neither a proton (roughly 1.0073 amu)
nor a neutron (roughly 1.0087 amu) has a mass of 1 amu. Therefore, the isotope
238
U, which has an atomic mass of 238.0508 amu, has an atomic mass lower than
the sum of the protons and neutrons, which have a total mass of 239.9418 amu,
as shown.
Mass of 92 individual protons of
238
U
= 92 × 1.0073 amu = 92.6716 amu
Mass of 146 individual neutrons of
238
U
= 146 × 1.0087 amu = 147.2702 amu
Total mass of individual protons and neutrons of
238
U = 239.9418 amu
Where did the rest of the mass go? When the nuclei of elements formed from
the individual neutrons and protons, some of the mass—a different amount for
each isotope of each element—was released as energy (see Section 5.7).
Unfortunately, the individual masses don’t translate accurately into masses
that we can measure for a macroscopic quantity of an element found on a labo-
ratory shelf. The presence of isotopes complicates the mass even more. To illus-
trate this, assume we have a bottle of carbon powder. What mass should we use
for the typical carbon atom found in this bottle, given that three different iso-
topes of carbon exist: carbon-12, carbon-13, and carbon-14? Fortunately, in na-
ture, the relative abundance of each isotope remains largely constant. In addition,
the relative natural abundances of each of the isotopes of the elements have been
determined by scientists using mass spectrometers. Knowing the percentages of
each of the isotopes (and their masses), scientists have calculated the weighted
average mass of each element, and that is the atomic mass listed for it in the
periodic table. For our bottle of carbon powder, we would use 12.011 amu as the
average mass.
To better understand the concept of weighted average, we can draw an
analogy to a student grade point average (GPA). Let’s look at an “A student” who
completed 10 credits of coursework in a semester. If 5 credits were A grades (4.0,
on a scale of 0.0 to 4.0), 3 credits were B (3.0), and 2 credits were C (2.0), then her