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Chapter 6 Reference: The Energy Stored in a Nucleus
The nuclei of atoms remain intact during a
chemical reaction. This suggests that much larger
quantities of energy are required for nuclear changes.
Experimentally, this has proven to be true. Nuclear
reactions usually involve energy changes that are
over a million times greater than those found in
chemical reactions. This enormous factor accounts
for the interest in nuclear reactions as a source of
energy.
One such nuclear reaction is represented by the
following equation:
+ → + + 3 + energy
Focusing on the “+ energy” term in the equation,
the numerical value is on the order of 4.5 x 109
kcal/mole of uranium. Compare this to the molar
heat of combustion of carbon at about 94 kcal/mole.
In this case, the energy produce from the nuclear
reaction is on the order of 107 times greater than that
produced from the chemical reaction.
Looking at the nuclear reaction above, the symbol
is the isotopic notation representing the neutron,
one of the fundamental particles present in the
nucleus of the atom. (Reminder: the superscript
refers to the mass number and the subscript refers to
the atomic number.) In the overall reaction, instead
of producing new kinds of substances by the
rearranging and recombining of atoms, the element
uranium has combined with a neutron and split into
two other elements – barium and krypton – plus three
more neutrons. Atoms of a given element are
characterized by their atomic number, the number of
units of positive charge on the nucleus. For one
element to change into another element, the nucleus
must be altered. In the above example, the uranium
nucleus, when reacting with the neutron, splits of
fissions into two other nuclei and, in addition,
releases three more neutrons. The above reaction is
used in an atomic pile, the energy source of a nuclear
power plant. The example shown is only one of the
ways the uranium nucleus can divide. Lanthanum
and bromine nuclei are also produced, cerium and
selenium, and so on, each pair of fission products
being such that the sum of their atomic numbers is
always 92.
In order to determine the products of a nuclear
reaction, it is necessary to pay attention to the
superscripts and subscripts shown with each isotope.
The subscripts refer to the atomic number, or the
number of units of positive charge in the nucleus.
The zero subscript attached to the neutron denotes the
lack of charge on this on this particle. Looking at
just the subscripts,
+ → + + 3
Notice that the sum on each side of the equation is
identical: 92 + 0 = 56 + 36 + (3 x 0). This is
another way of expressing the law of conservation of
charge. (Reminder: Since a neutral atom has the
same number of electrons as it has protons, the
charge from the electrons is also conserved)
In the model of the atom, the nucleus is pictured as
being made up of protons and neutrons. These two
kinds of particles are given the general name
nucleon. The mass number of a nucleus is equal to
the number of nucleons present for a particular
isotope. The superscripts in the equation represent
the mass numbers:
+ → + + 3
The mass numbers are also conserved:
235 + 1 = 141 + 92 + (3 x 1)
This may be rephrased in terms of a rule: The total
number of nucleons in unchanged during nuclear
reactions.
The nuclear reaction is really representing the nuclei
and the particles associated with them. It does not
tell anything about what compound of uranium was
bombarded with neutrons or what compound of
barium is formed. A nuclear equation summarizes
only the nuclear changes. During the nuclear change,
there is much disruption of the other atoms present
due to the tremendous amounts of energy released
Exact Mass Relationships
Although the mass numbers of the proton and
neutron are both one, the masses of these
fundamental particles are not identical. The mass of
one mole of protons is 1.00762 grams whereas the
mass of mole of neutrons is 1.00893 grams. Further
investigation shows that the experimentally measured
mass of the nucleus of any given isotope is not the
exact sum of the masses of protons and neutrons
confined in the nucleus. For example, the mass of
the nucleus of the uranium isotope of mass number
235 is less than the sum of the masses of 92 protons
and 143 neutrons.
One of the consequences of the special theory of
relativity formulated by Albert Einstein in 1905 was
that we came to realize that mass and energy are one
and the same. Although this was a very radical
notion at the time Einstein first presented his theory,
the equation relating mass to energy, E = mc2, has
become very familiar to many since the successful
application of nuclear energy became a part of
modern technology in the 1940’s. In this equation, c
is the speed of light, 3.00 x 1010
cm/second. A small
amount of mass, m, is equivalent to a tremendous
amount of energy. The proportionality constant, c2,
relating mass to energy is numerically, 9.00 x 1020
.
The idea of the relationship between mass and
energy can be used in several ways. The mass of the
nucleus is less than the masses of the 92 protons
and 143 neutrons postulated to be in it. The
difference in mass represents the binding energy
which holds the nucleons together in the nucleus.
The nuclear binding energy can be used as a way to
express the implied decrease in mass. Going back
to a chemical reaction, the combustion of carbon,
C (s) + O2 (g) → CO2 (g) H = -94 kcal
The mass change associated with an energy change
on the order of 102 kcal is about 5 x 10
-9 grams. This
is a quantity far too small to be detected on any
balance capable of weighing out the 12 grams of
carbon and 32 grams of oxygen consumed in the
reaction. Since the chemical “mass defects” are too
small to measure, the amounts are not used for
chemical reactions.
If we wish to gain some idea of the alteration of
mass in a nuclear change, we cannot use the fission
reaction because the exact masses of the nuclei
involved are not known. Let us look at another type
of reaction of possible importance in the production
of nuclear energy:
This reaction is called fusion since nuclei are
combining to form a heavier nucleus. The energy
associated with this change is 4.05 x 108 kcal/mol of
nuclei.
Let us do a little work with the exact masses of the
nuclei. We will simplify it a bit by using the exact
masses of the atoms. This will make no difference,
since the masses of the atoms differ from the nuclear
masses by the masses of the electrons present in each
atom. Since charge is conserved, the number and
character of the electrons does not change between
reactants and products, so there is no difference in the
mass of the electrons. Thus, for the hydrogen-to-
helium reaction:
Reactants: 2.01471 g/mol
3.01701
Sum: 5.03178
Products: 4.00390 g/mol
1.00893
Sum: 5.01283
Mass difference: 5.03178 – 5.01283 = 0.01895 g/mol
Compare this mass difference of 0.02 g/mol for the
nuclear reaction with the approximate 5 x 10-9
g/mol
for the chemical reaction of combustion of carbon.
As a reminder, in nuclear reactions, changes in the
nuclei take place. In a chemical reaction, the nuclei
remain intact and the changes are explainable in
terms of the electrons outside of the nucleus.
Nuclear Decay
Nuclear decay is the spontaneous decomposition
of an unstable nucleus that results in the emission of
ionizing particles and/or radiation. Several types of
decay occur. In all cases, the same rules apply to
these types of nuclear reactions as apply to fission
and fusion: the charge and total number of nucleons
are conserved in a nuclear reaction. For further
information on the types of radioactive decay, refer to
pages 860-862 in your Ebbing/Gammon textbook and
pages 685 – 687 in the Holt textbook.