Dr. Roger C. Wiens
Division of Geological & Planetary Sciences
California Institute of Technology
Radiometric dating--the process of determining the age of rocks from
the decay of their radioactive elements--has been in widespread use for over
half a century. There are over forty such techniques, each using a different
radioactive element or a different way of measuring them. It has become
increasingly clear that these radiometric dating techniques agree with each
other and as a whole, present a coherent picture in which the earth was created
a very long time ago. Many Christians are completely unaware of the great
number of laboratory measurements that have shown these methods to be
consistent, and they are also unaware that Bible-believing Christians are among
those actively involved in radiometric dating. This paper describes in
relatively simple terms how some dating techniques work, how accurately the
half-lives of the radioactive elements and the rock dates themselves are known,
and how dates are checked with one another. In the process the paper refutes
some misconceptions prevalent among Christians today. God has called us to be "wise
as serpents" even in this scientific age. This paper is put out by the
American Scientific Affiliation and the Affiliation of Christian Geologists to
promote greater understanding and wisdom on this issue within the Christian
community.
Introduction
Overview
The Radiometric Clocks
Examples of Dating Methods for Igneous Rocks
Potassium-Argon
Argon-Argon
Rubidium-Strontium
Samarium-Neodymium, Lutetium-Hafnium, and Rhenium-Osmium
Uranium-Lead
Cosmogenic Radionuclides:
Carbon-14, Beryllium-10, Chlorine-369
The Age of the Earth
Can We Really Believe the Dating Systems?
Doubters Still Try
Rightly Handling the Word of Truth
Appendix: Common Misconceptions Regarding Radiometric Dating Techniques
Further Reading
Glossary
Arguments over the age of the earth have sometimes been divisive in the church.
Although the Bible never mentions the earth's age, it is an issue because some
people have tried to calculate the date of creation by adding up the life-spans
of the generations listed in Genesis chapters 5 and 11. Assuming a strictly
literal interpretation of the week of creation, even if some generations were
left out of the genealogies, the earth would be less than ten thousand years
old. Radiometric dating techniques indicate that the earth is thousands of
times older than that--approximately four and a half billion years old. Many
Christians accept this and interpret the Genesis account in less scientifically
literal ways. However, some Christians suggest that the geologic dating techniques
are unreliable, that they are wrongly interpreted, or that they are confusing
at best. Unfortunately, there has not been much literature easily available to
Christians in an understandable form, so that confusion over dating techniques
continues.
The next few pages give a broad overview of radiometric dating techniques, talk
through a few examples, and discuss the degree to which the various dating
systems agree with each other. The goal is to promote greater understanding in
the Christian community on this issue. Many people have been led to be
skeptical of dating without knowing much about it. For example, most people
don't realize that carbon dating is not used on rocks at all. God has called us
to be "wise as serpents" (Matt. 10:16) even in this scientific age.
In spite of this, differences still occur within the body of Christ. A
disagreement over the age of the earth is relatively minor in the whole scope
of Christianity; it is more important to agree on the Rock of Ages than on the
age of rocks. But because God has also called us to wisdom, this issue is
worthy of study.
Rocks are made up of many individual crystals, and each crystal is usually made
up of at least several different chemical elements such as iron, magnesium,
silicon, etc. Most elements in nature are stable and do not change. However,
some elements are not completely stable in their natural state. Some atoms
eventually change from one element to another by a process called radioactive
decay. If there are many atoms of the original element, called the parent
element, the atoms decay to another element, called the daughter element, at a
predictable rate. The passage of time can be charted by the reduction in the
number of parent atoms, and the increase in the number of daughter atoms.
Radiometric dating can be compared to an hourglass. When the glass is turned
over, sand runs from the top to the bottom. You cannot predict exactly when any
one particular grain will get to the bottom, but you can predict from one time
to the next how long the whole pile of sand takes to fall. Once all of the sand
has fallen out of the top, the hourglass will no longer keep time unless it is
turned over again. Similarly, when all the atoms of the radioactive element are
gone, the rock will no longer keep time (unless it receives a new batch of
radioactive atoms).
Unlike the hourglass, where the amount of sand falling is constant right up
until the end, the number of decays from a fixed number of radioactive atoms
decreases as there are fewer atoms left to decay (see Figure 1). If it takes a
certain length of time for half of the atoms to decay, it will take the same
amount of time for half of the remaining atoms, or one-fourth of the original
total, to decay. In the next interval, with only one-fourth remaining, only one
eighth of the original total will decay. By the time ten of these intervals, or
half-lives, have passed, less than one thousandth of the original number of
radioactive atoms is left. Also unlike the hourglass, there is no way to change
the rate at which radioactive atoms decay on earth. If you shake the hourglass,
twirl it, or put it in a rapidly accelerating vehicle, the time it takes the
sand to fall will change. But the radioactive atoms used in dating techniques
have been subjected to heat, cold, pressure, vacuum, acceleration, and strong
chemical reactions without any significant change in their decay rate.1
[http://asa.calvin.edu/ASA/resources/Graphics/WiensFig1.gif]
Figure
1. The rate of loss of sand from the
top of an hourglass compared to the exponential type of decay of radioactive
elements. Most processes we are familiar with are linear, like sand in the
hourglass. In exponential decay, the amount of material decreases by half
during each half-life. After two half-lives only one-fourth is left, after
three half-lives only one eighth is left, etc. As shown in the bottom panel,
the daughter element or isotope amount increases rapidly at first, then more
slowly with each succeeding half-life.
An hourglass will tell time correctly only if it is completely sealed. If it
has a hole allowing the sand grains to escape out the side instead of going
through the neck, it will give the wrong time interval. Similarly, a rock that
is to be dated must be sealed against loss or addition of either the
radioactive daughter or parent. If it has lost some of the daughter element, it
will give an inaccurately young age. As will be discussed later, most dating
techniques have very good ways of telling if such a loss has occurred, in which
case the date is thrown out (and so is the rock!).
An hourglass measures how much time has passed since it was turned over.
(Actually it tells when a specific amount of time, e.g., two minutes, an hour,
etc., has passed, so the analogy is not quite perfect.) Like the hourglass,
radiometric dating of rocks tells how much time has passed since some event occurred.
For igneous rocks the event is usually its cooling and hardening from magma or
lava. For some other materials, the event is the end of a period of metamorphic
heating (in which the rock gets baked underground at generally over a thousand
degrees Fahrenheit). The event in other cases can be the uncovering of a
surface by the scraping action of a glacier, the chipping of a meteorite off an
asteroid, or the length of time a plant or animal has been dead.
There are now well over forty different radiometric dating techniques, each
based on a different radioactive isotope.2 A partial list of the
parent and daughter isotopes and the decay half-lives is given in Table 1.
Notice the large range in the half-lives. Isotopes with long half-lives decay
very slowly, and so are useful for dating correspondingly ancient events.
Isotopes with shorter half-lives cannot date very ancient events because all of
the atoms of the parent isotope would have already decayed away, like an
hourglass left sitting with all the sand at the bottom. Isotopes with
relatively short half-lives are useful for dating correspondingly shorter
intervals, and can usually do so with greater accuracy, just as you would use a
stopwatch rather than a grandfather clock to time a 100-meter dash. On the
other hand, you would use a calendar, not a clock, to record time intervals of
several weeks or more.
Table 1. Some
Naturally-Occurring Radioactive Isotopes and Their Half-Lives
|
Radioactive
Isotope |
Product |
Half-Life |
|
Samarium
- 147 |
Neodymium
- 143 |
106
billion |
|
Rubidium-87 |
Strontium-87 |
48.8
billion |
|
Rhenium-187 |
Osmium-187 |
42
billion |
|
Lutetium-176 |
Hafnium-176 |
38
billion |
|
Thorium-232 |
Lead-208 |
14
billion |
|
Uranium-238 |
Lead-206 |
4.5
billion |
|
Potassium-40 |
Argon-40 |
1.26
billion |
|
Uranium-235 |
Lead-207 |
0.7
billion |
|
Beryllium-10 |
Boron-10 |
1.52
million |
|
Chlorine-36 |
Argon-36 |
300000 |
|
Carbon-14 |
Nitrogen-14 |
5715 |
Half-lives taken from N. E.
Holden, Pure Appl. Chem. 62 (1990): 941-958.
The half-lives have all been measured
directly, either by using a radiation detector to count the number of atoms
decaying in a given amount of time from a known amount of the parent material,
or by measuring the ratio of daughter to parent atoms in a sample that
originally consisted completely of parent atoms. Work on radiometric dating
first started shortly after the turn of the century, but progress was
relatively slow before the late forties. For many of the dating techniques, we
now have had fifty years over which to measure and remeasure the half-lives.
Very precise counting of the decay events or the daughter atoms can be done, so
that while the number of, for example, rhenium-187 atoms decaying in 50 years
is a very small fraction of the total, the resulting osmium-187 atoms can be
very precisely counted.
The uncertainties on the half-lives given in the table are all very small. All
the half-lives are known to better than plus/minus about two percent except for
rhenium (5%), lutetium (3%), and beryllium (3%). There is no evidence of any of
the half-lives changing over time, and such a thing is forbidden by the laws of
physics.
Igneous rocks are good candidates for dating. Recall that for igneous rocks the
event being dated is when the rock was formed from magma or lava. When the
molten material cools and hardens, the atoms are no longer free to move about.
Any daughter atoms from radioactive decays occurring after the rock cools are
trapped where they are made within the rock. These atoms are like the sand
grains accumulating in the bottom of the hourglass. To determine the age of the
rock one needs to measure the number of daughter atoms and the number of
remaining parent atoms, and use the half-life to calculate the time it took to
make those daughter atoms.
However, there is one complication. One cannot always assume that there were no
daughter atoms to begin with. It turns out that there are some cases where one
can make that assumption quite reliably. But usually the initial amount of the
daughter product must be accurately determined. Most of the time one can use
the different amounts of parent and daughter atoms present in different
minerals within the rock to tell how much daughter product was originally
present. Each dating mechanism deals with this problem in its own way. Some
types of dating work better in some rocks; others are better in other rocks,
depending on the rock composition and its age. Let's examine some of the
different dating mechanisms now.
Potassium-Argon. Potassium is an abundant element in the Earth's crust.
One isotope, potassium 40, is radioactive and decays to two different daughter
products, calcium-40 and argon-40, by two different decay methods. This is not
a problem because the production ratio of these two daughter products is
precisely known, and is always constant: 11.2% becomes argon-40 and 88.8%
becomes calcium-40. It is possible to date some rocks by the potassium-calcium
method, but this is not often done because it is hard to determine how much
calcium was initially present. Argon, on the other hand, is a gas. Whenever
rock is melted to become magma or lava, the argon tends to escape. Once the
molten material hardens, it again begins to trap the argon produced from its
potassium. In this way the potassium-argon clock is clearly reset when an
igneous rock is formed.
In its simplest form, the geologist simply needs to measure the relative amounts
of potassium-40 and argon-40 to date the rock. The age is given by a relatively
simple equation:
[http://asa.calvin.edu/ASA/resources/Graphics/WiensEq1.gif]
where t1/2 is the half-life,
and ln is the natural logarithm.
However, in reality there is often a small amount of argon remaining in a rock
when it hardens. This is usually trapped as very tiny air bubbles in the rock.
One percent of the air we breathe is argon. Argon from air bubbles may need to
be allowed for if it is significant compared with the amount of radiogenic
argon. This would most likely be the case in either young rocks that have not
had time to produce much radiogenic argon, or in rocks that are not abundant in
potassium. One must have a way to determine how much air-argon is in the rock.
This is rather easily done because air-argon has a couple of other isotopes,
the most abundant of which is argon-36. The ratio of argon-40 to argon-36 in
air is well known, at 295. Thus, if one measures argon-36 and argon-40, one can
calculate and subtract off the air argon-40 to get an accurate age.
One of the best ways of showing that an age-date is correct is to confirm it
with one or more different dating technique(s). Although potassium-argon is one
of the simplest dating methods, there are still some cases where it does
not agree with other methods. When this does happen, it is usually because the
gas within bubbles in the rock is from deep underground rather than from the
air. This gas can have a higher concentration of argon-40 escaping from the
melting of older rocks. This is called parentless argon-40 because its
parent potassium is not in the rock being dated, and is also not from the air.
In these slightly unusual cases, the date given by the normal potassium-argon
method is too old. However, scientists in the mid-1960s came up with a way
around this problem, the argon-argon method.
Argon-Argon. Although it has been around for over a quarter of a
century, the argon-argon method is seldom discussed by groups critical of
dating methods. This method uses exactly the same parent and daughter isotopes
as the potassium-argon method. In effect, it is a different way of telling time
from the same clock. Instead of simply comparing the total potassium with the
non-air argon in the rock, this method can tell exactly what and how much argon
is directly related to the potassium in the rock.
In the argon-argon method, the rock is placed near the center of a nuclear
reactor for a number of hours. A nuclear reactor emits a very large number of
neutrons, which can change a small amount of the potassium-39 into argon-39.
Argon-39 is not found in nature because it has a 269-year half-life (the
shortness of this half-life doesn't affect the argon-argon dating method as
long as the measurements are made within about five years of the neutron dose).
The rock is then heated in a furnace to release both the argon-40 and the
argon-39 (representing the potassium) for analysis. The heating is done at
incrementally higher temperatures and at each step the ratio of argon-40 to
argon-39 is measured. If the argon-40 is from decay of potassium within the
rock, it will come out at the same temperatures as the potassium-derived
argon-39 and in a constant proportion. If there is some excess argon-40
in the rock, it will cause a different ratio of argon 40 to argon-39.
Figure 2 is an example of a good argon-argon date. The fact that this plot is
flat shows that essentially all of the argon-40 are from decay of potassium
within the rock. The potassium-40 in the sample is found by multiplying the
argon-39 by a factor based on the neutron exposure in the reactor. When this is
done, the plateau in the figure represents an age date based on the decay of
potassium-40 to argon-40.
[http://asa.calvin.edu/ASA/resources/Graphics/WiensFig2.gif]
Figure
2. A typical argon-argon dating plot.
Each small rectangle represents the apparent age given at one particular
heating-step temperature. The top and bottom parts of the rectangles represent
upper and lower limits for that particular determination. The x-axis gives the
amount of the total argon-39 released from the sample. A good argon-argon age
determination will have many heating steps which all agree with each other. The
"plateau age" is the age given by the average of most of the steps;
in this case it is 136.4 million years. The sample is a Parana continental
flood basalt from Brazil. From S. Turner, et al., Earth and Planetary
Science Letters 121 (1994): 333-348.
There are occasions when the argon-argon dating method does not give an age
even if there is sufficient potassium in the sample and the rock was old enough
to date. This most often occurs if the rock experienced a high temperature
(usually a thousand degrees Fahrenheit or more) at some point since its
formation. If that occurs, some of the argon gas moves around, and the analysis
does not give a smooth plateau across the extraction temperature steps. An
example of an argon-argon analysis which did not yield an age date is shown in
Figure 3. Notice that there is no good plateau in this plot. Sometimes, there
will actually be two plateaus, one representing the formation age, and another
representing the time at which the heating episode occurred. Usually where the
system has been disturbed, there simply is no date given. The important point
to note is that, rather than giving wrong age dates, this system simply does
not give a date if the system has been disturbed. This is also true of
several other igneous rock dating methods, as we will describe below.
[http://asa.calvin.edu/ASA/resources/Graphics/WiensFig3.gif]
Figure
3. An argon-argon plot which gives no
date. Note that the apparent age is different for each temperature step so that
there is no plateau. This sample was struck with a pressure of 420,000
atmospheres to simulate a meteorite impact--an extremely rare event. The impact
heated the rock and caused its argon to be rearranged, so that it could not
give an argon argon date. Before it was smashed, the rock gave an age of around
450 million years, as shown by the dotted line. From A. Deutsch and U.
Schaerer, Meteoritics 29 (1994): 301-322.
Rubidium-Strontium. In nearly all of the dating techniques, except
potassium-argon and the associated argon-argon method, there is always some
amount of the daughter product already in the rock when it cools. Using these
methods is a little like trying to tell time from an hourglass that was turned
over before all of the sand had fallen to the bottom. One can think of ways to
correct for this in an hourglass: One could make a mark on the outside of the
glass where the sand level started from and then repeat the interval with a
stopwatch in the other hand to calibrate it. Or if one is clever she or he
could examine the hourglass's shape and determine what fraction of all the sand
was at the top to start with. By knowing how long it takes all of the sand to
fall, one could determine how long the time interval was. Similarly, there are
good ways to tell quite precisely how much of the daughter product was already
in the rock when it cooled and hardened.
In the rubidium-strontium method, rubidium-87 decays with a half-life of 48.8
billion years to strontium 87. Strontium has several other isotopes that are
stable and do not decay. The ratio of strontium-87 to another stable isotope,
say strontium-86, increases over time as more rubidium-87 turns to
strontium-87. But when the rock first cools, all parts of the rock have the
same (strontium-87/strontium-86) ratio because the isotopes were mixed in the
magma. At the same time, some minerals in the rock have a higher
rubidium/strontium ratio than others. Rubidium has a larger atomic diameter
than strontium, so that rubidium does not fit into the crystal structure of
some minerals as well as it does in others.
Figure 4 is an important type of plot used in rubidium-strontium dating. It
shows the strontium 87/strontium-86 ratio on the vertical axis and the
rubidium-87/strontium-86 ratio on the horizontal axis, that is, it plots a
ratio of the daughter isotope against a ratio of the parent isotope. At first,
all the minerals lie along a horizontal line of constant
strontium-87/strontium-86 but with varying rubidium/strontium. As the rock
starts to age, rubidium gets converted to strontium. The amount of strontium
added to each mineral is proportional to the amount of rubidium present. This
change is shown by the dashed arrows, the lengths of which are proportional to
the rubidium/strontium ratio. The dashed arrows are slanted because the
rubidium/strontium ratio is decreasing in proportion to the increase in
strontium-87/strontium-86. The solid line drawn through the samples will thus
progressively rotate from the horizontal to steeper and steeper slopes.
[http://asa.calvin.edu/ASA/resources/Graphics/WiensFig4.gif]
Figure
4. A rubidium-strontium three-isotope
plot. When a rock cools, all its minerals have the same ratio of strontium 87
to strontium-86, though they have varying amounts of rubidium. As the rock
ages, the rubidium decreases by changing to strontium-87, as shown by the
dotted lines. Minerals with more rubidium gain more strontium-87, while those
with less rubidium do not change as much. At any given time the composition can
be represented as a line through the points. Notice that the line can be
extrapolated back to zero to give the initial strontium-87/strontium-86 ratio.
The age of the rock can be determined from the slope of the line.
A line drawn through the samples at any later time will intersect the
horizontal line at the same point in the lower left-hand corner. This point,
where rubidium-87/strontium-86 equals zero, tells the original
strontium-87/strontium-86 ratio. From that we can determine the original
daughter strontium-87 in each mineral, which is just what we need to know to
determine the correct age.
It also turns out that the slope of the line is proportional to the age of the
rock: the older the rock, the steeper the line. If the slope of the line is m
and the half-life is t1/2, the age t (in years) is given by the equation
[http://asa.calvin.edu/ASA/resources/Graphics/WiensEq2.gif]
For a system with a
very long half-life like rubidium-strontium, the actual numerical value of the
slope will always be quite small. To give an example for the above equation, if
the slope of a line in a plot similar to Fig. 4 is m = 0.05110 (strontium
isotope ratios are usually measured very accurately--to about one part in ten
thousand), we can substitute in the half-life (48.8 billion years) and solve as
follows:
|
|
t
= (48.8) x ln(1.05110)/ln(2) |
|
so
|
t
= 3.51 billion years. |
There are several things that, on rare occasions, can cause problems for the
rubidium-strontium dating method. One possible source of problems is if a rock
contains some minerals that are older than the main part of the rock. Sometimes
magma inside the earth will pick up unmelted minerals from the surrounding rock
as it moves through a magma chamber. Usually a good geologist can distinguish
these "xenoliths" from the younger minerals all around them. If he or
she does happen to use them for dating the rock, the points represented by
these minerals will lie off the line made by the rest of the points. Other
difficulties arise if a rock has undergone metamorphism, that is, if the rock
got very hot, but not hot enough to completely remelt the rock. In these cases,
the dates look confused, and do not lie along a line. Some minerals may have
completely melted, while others did not melt at all, so that some minerals try
to give the igneous age while other minerals try to give the metamorphic age.
In these cases there will not be a straight line, and no date is determined.
In a few, very rare instances, the rubidium-strontium method has given straight
lines that give wrong ages. This can happen when the rock being dated was
formed from magma that was not well mixed, and which had two distinct batches
of rubidium and strontium. One magma batch had rubidium and strontium
compositions near the upper end of a line (such as in Fig. 4), and one batch
had compositions near the lower end of the line. In this case, the minerals all
got a mixture of these two batches, and their resulting composition ended near
a line between the two batches. This is called a two-component mixing line. It
is a very rare occurrence in these dating mechanisms, but at least thirty cases
have been documented among the tens of thousands of rubidium-strontium dates
made. If a two-component mixture is suspected, a second dating method must
confirm or disprove the rubidium-strontium date. The agreement of several
dating methods is the best fail-safe way of dating rocks.
The Samarium-Neodymium, Lutetium-Hafnium, and Rhenium-Osmium Methods.
All these methods work very similarly to the rubidium-strontium method. They
all use three-isotope diagrams similar to Figure 4 to determine the age. The
samarium-neodymium method is the most often-used of these three. It uses the
decay of samarium-147 to neodymium-143, which has a half life of 105 billion
years. The ratio of the daughter isotope, neodymium-143, is plotted against the
ratio of the parent, samarium-147, with neodymium-144 in the denominators. If
different minerals from the same rock plot along a line, the slope is
determined, and the age is given by the same equation as above. The
samarium-neodymium method may be preferred for rocks that have very little potassium
and rubidium, which would make dating by the potassium-argon, argon-argon, and
rubidium-strontium methods difficult. The samarium-neodymium method has also
been shown to be more resistant to being disturbed by metamorphic heating
events, so for some metamorphosed rocks the samarium-neodymium method is
preferred. For a rock of the same age, the slope on the neodymium-samarium
plots will be less than on a rubidium-strontium plot because the half-life is
longer. However, these isotope ratios are usually measured to extreme
accuracy--several parts in ten thousand--so that accurate dates can be obtained
even for ages less than one fiftieth of a half-life, and correspondingly small
slopes.
The lutetium-hafnium method uses the 38 billion year half-life of lutetium-176
decaying to hafnium-176. This dating system is similar in many ways to
samarium-neodymium, as the elements tend to be concentrated in the same types
of minerals. Since samarium-neodymium dating is somewhat easier, the
lutetium-hafnium has not been used in very many cases.
The rhenium-osmium method takes advantage of the fact that the osmium
concentration in most rocks and minerals is very low, so that a small amount of
the parent rhenium-187 can produce a significant change in the osmium isotope
ratio. The half-life for this radioactive decay is 42 billion years. The
nonradiogenic stable isotopes, osmium-186 or -188, are used as the denominator
in the ratios on the three-isotope plots. This method has been useful for
dating iron meteorites, and is now enjoying greater use for dating earth rocks
due to development of easier rhenium and osmium isotope measurement techniques.
Uranium-Lead and related techniques. The uranium-lead method is the
longest-used dating method. It was first used in 1907, some ninety years ago.
The uranium-lead system is more complicated than other parent-daughter systems;
it is actually several dating methods put together. Natural uranium consists
primarily of two isotopes, U-235 and U-238, and these isotopes decay with
different half-lives to produce lead-207 and lead-206, respectively. In
addition, lead-208 is produced by thorium-232. Only one isotope of lead,
lead-204, is not radiogenic. The uranium-lead system has an interesting
complication: none of the lead isotopes is produced directly from uranium and
thorium. Each decays through a series of short-lived radioactive elements that
are produced and almost immediately decay to a lighter element, finally ending
at lead. Since these half-lives are so short compared to uranium and thorium,
they do not affect the overall dating scheme. The result is that one can obtain
three independent estimates of the age of a rock by measuring the lead isotopes
and their parent isotopes, uranium-235 and -238 and thorium-232.
The uranium-lead system in its simpler forms has proved to be less reliable
than many of the other dating systems. This is because both uranium and lead
are less easily retained in many minerals in which they are found. The
intermediate elements in the decay chain do not help matters either. Yet the
fact that there are three dating systems all in one allows scientists to easily
determine whether the system has been disturbed or not. Using slightly more
complicated mathematics, different combinations of the lead isotopes and parent
isotopes can be plotted in a way that minimizes the effects of lead loss. One
of these techniques is called the lead-lead technique because it determines the
ages from the lead isotopes alone. Some of these techniques allow scientists to
chart at what points in time metamorphic heating events have occurred. This
information is also of significant interest to geologists.
The last three radiometric systems listed in Table 1 have far shorter
half-lives than all the rest. Unlike the other radioactive isotopes, carbon-14,
beryllium-10, and chlorine-36 are constantly being replenished in small amounts
by a special mechanism. Cosmic rays--high energy particles and photons in
space--produce these isotopes in air, very high in the earth's atmosphere. Very
small amounts of each of these isotopes are present in the air we breathe and
the water we drink. As a result, living things, both plants and animals, ingest
very small amounts of carbon-14, and lake and sea sediments take up small
amounts of beryllium-10 and chlorine-36.
The cosmogenic dating clocks work somewhat differently than the others.
Carbon-14 in particular is used to date organic material such as bones, wood,
cloth, paper, and other dead tissue from either plants or animals. To a rough
approximation, the ratio of carbon-14 to the stable isotopes, carbon-12 and
carbon-13, is more or less constant in the atmosphere and living organisms.
Once a living thing dies, it no longer takes in carbon from food or air, and
the amount of carbon-14 starts to drop with time. How far the
(carbon-14/carbon-12) ratio has dropped indicates how old the sample is. Since
the half-life of carbon-14 is less than 6,000 years, it can only be used for dating
material less than about 40,000 years old. Dinosaur bones do not have carbon-14
(unless contaminated), as the dinosaurs became extinct over 60 million years
ago, but some other animals that are now extinct, such as North American
mammoths, can be dated by carbon-14. Also, some materials from prehistoric
times, as well as biblical events, can be dated by carbon-14.
The carbon-14 system has been carefully calibrated with nonradiometric age
indicators. For example growth rings in trees, if counted carefully, are a
reliable way to determine the age of a tree. Each growth ring only collects
carbon from the air and nutrients during the year it is made. To calibrate
carbon-14, one can analyze carbon from several center rings of a tree, and then
count the rings inward from the living portion to determine the actual age.
This has been done for the "Methuselah of trees," the bristlecone
pines, which grow very slowly and live up to 6,000 years. Scientists have
extended this calibration even further. These trees grow in a very dry region
near the California-Nevada border. Dead trees in this dry climate take many
thousands of years to decay. Growth ring patterns based on wet and dry years
can be correlated between living and long dead trees, extending the ring count
back to about 10,000 years ago.
There are other ways of extending farther back in time. One of the best known
is the seasonal variations in oxygen isotopes in polar ice from Greenland and
Antarctica. Because winter ice has a greater concentration of the lighter
isotope, oxygen-16, each winter's deposit makes an invisible layer in the ice,
something like a tree ring, which is detectable by isotope analysis. This
record goes back about 100,000 years.
While the ice cores are not so easy to compare with carbon 14 dates, the tree
rings are very easy to use since trees contain a lot of carbon. The comparison
of radiocarbon ages of tree rings with their known ages has revealed variations
of up to 12% between the predicted and actual ages. The variations occur because
the source of carbon-14 at the top of the atmosphere is slightly variable. This
phenomenon is quite well understood, and affects only the clocks that rely on
cosmic ray production (e.g., carbon-14, beryllium-10, and chlorine-36).
Carbon-14 dates of less than about 10,000 years are corrected for this effect,
and there is no reason to believe that older radiocarbon dates are altered to
any larger degree. In summary, thousands of radiocarbon dates are obtained each
year on organic matter less than about forty thousand years old. It has proved
to be a reliable clock for such time scales. A research journal by the name Radiocarbon,
published since 1959, is devoted exclusively to this study and is available in
many geology and archeology libraries around the country.
|
Some
of the oldest rocks on earth are found in Western Greenland. Because of their
great age, they have been especially well studied. The table below gives the
ages, in billions of years, from twelve different studies using five
different techniques on one particular rock formation in Western Greenland,
the Amitsoq gneisses. |
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|
||||||||||||||||||||||||||||
|
Note
that scientists give their results with a stated uncertainty. They take into
account all the possible errors and give a range within which they are 95%
sure that the actual value lies. The top number, 3.60±0.05, refers to the
range from 3.55 to 3.65 billion years. The size of this range is every bit as
important as the actual number. One number with a small uncertainty range is
more accurate than a number with a larger range. For the numbers given above,
one can see that all of the ranges overlap and agree between 3.62 and 3.65
billion years as the age of the rock. Several studies also showed that,
because of the great ages of these rocks, they have been through several mild
metamorphic heating events that disturbed the ages given by potassium-bearing
minerals. |
||||||||||||||||||||||||||||
We now turn our attention to what the dating
systems tell us about the age of the earth. The most obvious constraint is the
age of the oldest rocks. These have been dated at up to about four billion
years. But actually only a very small portion of the earth's rocks are that
old. From satellite data we know that the earth's surface is constantly
rearranging itself little by little as earthquakes occur. Such rearranging
cannot occur without some of the earth's surface disappearing under other parts
of the earth's surface, remelting some of the rock. So it appears that none of
the rocks have survived from the creation of the earth without undergoing
remelting, metamorphism, or erosion, and all we can say--from this line of
evidence--is that the earth appears to be at least as old as the four billion-year-old
rocks.
When scientists began systematically dating meteorites, they learned a very
interesting thing: nearly all of the meteorites had practically identical ages,
at 4.56 billion years. These meteorites are chips off the asteroids. When the
asteroids were formed in space, they cooled relatively quickly (some of them
may never have gotten very warm), so all of their rocks were formed within a
few million years. The asteroids' rocks have not been remelted ever since, so
the ages have generally not been disturbed. Meteorites which show evidence of
being from the largest asteroids have slightly younger ages. The moon is larger
than the largest asteroid. The oldest rocks we have from the moon do not exceed
4.1 billion years, though a larger sampling might yield some slightly older
ages. Most scientists think that all the bodies in the solar system were
created about the same time. There is evidence from the uranium, thorium, and
lead isotopes that links the earth's age with that of the meteorites. This
would make the earth about 4.5-4.6 billion years old.
Notice one other important detail about radioactive isotopes. Most of the
naturally-occurring radioactive isotopes mentioned above have very long
half-lives, on the order of billions of years. The only ones with shorter
half-lives are those which have a source constantly replenishing them, such as
the carbon-14, beryllium-10 and chlorine-36 produced by cosmic rays. We can
make hundreds of other radioactive isotopes with half-lives shorter than a billion
years, but they do not occur naturally on earth. Occasionally there is evidence
that these isotopes existed at some point in the past, but have since decayed
completely away. The longest half-lives of this group of "extinct"
radionuclides are close to a hundred million years. Why do we find almost no
short-lived radionuclides and so many long-lived ones? This is what one would
expect to find if God had created the earth approximately four and a half
billion years ago. The earth is old enough that radioactive isotopes with
half-lives of up to a hundred million years decayed away, but not so old that
radioactive isotopes with half-lives close to a billion years are gone.
Some Christians question whether we can believe something so far back in the
past. My answer is that it is similar to believing in other things of the past.
It only differs in degree. Why do you believe Abraham Lincoln ever lived?
Because it would take an extremely elaborate scheme to make up his existence,
including forgeries, fake photos, and many other things, and besides, there is
no good reason to simply have made him up. Well, the situation is very similar
for the dating of rocks, only we have rock records rather than historical
records. Consider the following:
The last two points deserve more attention. Some Christians have argued that
something may be slowly changing with time so that all the ages look older than
they really are. The only two quantities in the exponent of a decay rate
equation are the half-life and the time. So for ages to appear longer than
actual, all the half-lives would have to be changing in sync with each other.
One could consider that time itself was changing if that happened (Remember
that our clocks are now standardized to atomic clocks!). And such a thing would
have to have occurred without our detection in the last 80 years, which is
already 4% of the way back to the time of Christ.
It would not be inconsistent with the scientific evidence to conclude that God
made everything relatively recently, but with the appearance of great age, just
as Genesis 1 and 2 tell of God making Adam as a fully grown man (which implies
the appearance of age). That is a philosophical and theological matter which we
won't go into here, though it has some shades of the Abraham Lincoln example.
We only note here that an apparent old earth is consistent with the
great amount of scientific evidence.
Some doubters have tried to dismiss geologic dating with a sleight of hand by
saying that no rocks are completely closed systems (that is, that no rocks are
so isolated from their surroundings that they have not lost or gained some of
the isotopes used for dating). Speaking from an extreme technical viewpoint
this might be true--perhaps one atom out of one trillion of a certain isotope
has leaked out of nearly all rocks, but such a change would make an
unmeasurably small change in the result. The real question to ask is: "Is
the rock sufficiently close to a closed system that the results will be the
same as a really closed system?" Since the early 1960s many books have
been written on this subject. These books detail experiments showing, for a
given dating system, which minerals work all of the time, which minerals work
under some certain conditions, and which minerals are likely to lose atoms and
give incorrect results. Understanding these conditions is part of the science
of geology. Geologists are careful to use the most reliable methods whenever
possible, and as discussed above, to test for agreement between different
methods.
Some people have tried to defend a young earth position by saying that the
half-lives of radionuclides can in fact be changed, and that this can be done
by certain little-understood particles such as neutrinos, muons, or cosmic
rays. This is stretching it. While certain particles can cause nuclear changes,
they do not change the half-lives. The nuclear changes are well understood and
are nearly always very minor in rocks. In fact the main nuclear changes in
rocks are the very radioactive decays we are talking about.
There are only three quite technical instances where a half-life changes, and
these do not affect the dating techniques we have discussed.
1. According to theory, a certain type decay called electron-capture decay is
most likely to show changes with pressure or chemical combination, and that
should be most pronounced for very light elements. The synthetic isotope,
beryllium-7, has indeed been shown by several people to change by up to a
fraction of a percent. In one such experiment, beryllium-7 was subjected to
270,000 atmospheres of pressure, which would only occur at depths greater than
450 miles inside the earth. All known rocks, with the possible exception of
diamonds, are from much shallower depths. In fact, beryllium-7 is not used for
dating rocks, as it has a half-life of only 54 days, and heavier nuclei are
even less subject to these minute changes, so that the dates of rocks made by
electron-capture decays would only be off by at most a few hundredths of a
percent.
2. Cosmic rays are very, very high-energy atomic nuclei flying through space.
The electron-capture decay mentioned above does not take place in cosmic rays
until they slow down. This is because the fast moving cosmic rays do not have
electrons. All normal matter, such as everything on earth, the moon,
meteorites, etc. always has electrons, so this instance does not affect things
we date.
3. The last case also involves very fast-moving matter. It has been
demonstrated by atomic clocks in rapid very fast spacecraft. These atomic
clocks slow down very slightly (only a second or so per year) as predicted by
Einstein's theory of relativity. No rocks in our solar system are going fast
enough to make a noticeable change in their dates.
These cases are very specialized, and all are well understood. None of these
cases alter the dates of rocks either on earth or other places in the solar
system. The conclusion again is that half-lives are completely reliable in
every context, including the dating of rocks on earth and even on other
planets.
As Christians it is very important that we understand God's Word correctly. Yet
from the middle ages until the 1700s, people insisted that the Bible taught
that the earth, not the sun, was the center of the solar system. It wasn't that
people just thought it had to be that way; they actually quoted Scriptures:
"The earth is firmly fixed; it shall not be moved" (Psalm
104:5), or "the sun stood still" (Joshua 10:13; why should it
say the sun stood still if it is the earth's rotation that causes day
and night?), and many other passages. I am afraid the debate over the age of
the earth has many similarities. But I am optimistic. Today there are many
Christians who accept the reliability of geologic dating, but do not compromise
the spiritual and historical inerrancy of God's word. While a full discussion
of Genesis 1 is not given here, references are given below to books which deal
with that issue.
As scientists, we deal daily with what God has revealed about himself through
the created universe. The psalmist marveled at how God, Creator of the
universe, could care about humankind: "When I consider Your heavens,
the work of Your fingers, the moon and the stars, which You have set in place,
what is man that You are mindful of him, the son of man that You care for him?"
(Psalm 8:3-4). Near the beginning of the twenty-first century we can marvel
even more, knowing how vast the universe is, how ancient the rocks and hills
are, and how carefully our environment has been designed. Truly God is more
awesome than we can imagine!
There are several misconceptions that seem especially prevalent among
Christians. Most of these topics are covered in the above discussion, but they
are reviewed briefly here for clarity.
1. Radiometric dating is based on index fossils.
This is not at all true, though it has actually been suggested. Radiometric
dating is based on the half-lives of the radioactive isotopes. These half-lives
have been measured over the last 40-80 years. They are not calibrated at all by
fossils.
2. The decay rates are poorly known, so the dates are inaccurate.
Most of the decay rates used for dating rocks are known to within 2 percent.
Uncertainties are only slightly higher on rhenium (5%), lutetium (3%), and
beryllium (3%). Such small uncertainties are no reason to dismiss radiometric
dating. Whether a rock is 100 million years or 102 million years old does not
make a great deal of difference.
3. A small error in the half-lives leads to a very large error in the date.
Since exponents are used in the dating equations, it is possible for people to
think this might be true, but it is not. If a half-life is off by 2%, it will
only lead to a 2% error in the date.
4. Decay rates can be affected by the physical surroundings.
This is not true in dating rocks. Radioactive atoms used for dating have been
subjected to heat, cold, pressure, vacuum, acceleration, and strong chemical
reactions without any measurable change. The only exceptions, which are not
relevant to dating rocks, are discussed under the section, "Doubters Still
Try," above.
5. No one has measured the decay rates directly; we only know them from
inference.
Decay rates have been directly measured over the last 50-80 years. In some
cases a batch of the pure parent material is weighed and set aside for a long
time, and then the resulting daughter material is weighed. In many cases it is
easier to detect radioactive decays by the energy burst each decay gives off.
For this, a batch of the pure parent material is carefully weighed and then put
in front of a Geiger counter which counts the number of decays over a long time.
6. The decay rates might be slowing down over time, leading to incorrect old
dates.
While we cannot rule out that this could possibly have happened in the past,
there is no evidence that anything of the sort has happened in the past
century. And the following argument makes this suggestion meaningless in terms
of apparent ages: Since the different dating methods are in good agreement, all
of the half-lives must have slowed down the same amount together. Such an
occurrence would be the same as if time itself slowed down. But everything
still appears very old, so why complicate things by making this suggestion in
the first place?
7. There is little or no way to tell how much of the decay product was
originally in the rock, leading to anomalously old ages.
A good part of this work is devoted to explaining how one can tell how much of
a given element or isotope was originally present. Usually it involves using
more than one sample from a given rock. By comparing the ratios of parent and
daughter isotopes relative to a stable isotope for samples with different
relative amounts of the parent isotope, one can determine how much of the
daughter isotope would be present if there had been no parent isotope. This is
the same as the initial amount (it would not change if there was no parent
isotope to decay). Figure 4 and the accompanying explanation tell how this is
done most of the time. While this is not absolutely 100% foolproof, comparison
of several dating methods will always show whether the given date is reliable.
8. There are only a few different dating techniques.
We have listed eleven different radiometric dating techniques and discussed
them. These make up only the tip of the iceberg. There are over forty different
radiometric dating techniques in use, and there are many other dating
techniques making use of rare stable isotopes, yearly variations such as tree
rings and ice cores, and other reliable methods.
9. "Radiation halos" in rocks prove that the earth was young.
This refers to tiny halos of crystal damage surrounding spots where radioactive
elements are concentrated in certain rocks. Halos thought to be from polonium,
a short-lived element produced from the decay of uranium, have been found in
some rocks. A plausible explanation for a halo from such a short-lived element
is that these were not produced by an initial concentration of the radioactive
element. Rather, as water seeped through cracks in the minerals, a chemical
change caused newly-formed polonium to drop out of solution at a certain place
and almost immediately decay there. A halo would build up over a long period,
although the center of the halo never contained more than a few atoms of
polonium at one time. "Hydrothermal" effects can act in ways that at
first seem strange, such as the well-known fact that gold--a chemically
unreactive metal with very low solubilities--is concentrated along quartz veins
by the action of water over long periods of time. Other researchers have found
halos produced by an indirect radioactive decay effect called hole diffusion,
which is an electrical effect in a crystal. These results suggest that the
halos in question are not from short-lived isotopes after all.
At any rate, halos from uranium inclusions are far more common. Because of
uranium's long half-lives, these halos take at least several hundred million
years to form. Because of this, most people agree that halos provide compelling
evidence for a very old earth.
10. Only atheists and liberals are involved in radiometric dating.
The fact is that there are many Bible-believing Christians who are involved in
radiometric dating, and who can see its validity firsthand. Most of the members
of the Affiliation of Christian Geologists are firmly convinced that
radiometric dating shows evidence that God created the earth billions, not
thousands, of years ago.
11. Different dating techniques usually give conflicting results.
This is not true at all. The fact that dating techniques most often agree with
each other is why scientists tend to trust them in the first place. Nearly
every college and university library in the country has periodicals such as Science,
Nature, and specific geology journals which give the results of dating
studies. The public is usually welcome to (and should!) browse in these
libraries. So the results are not hidden; people can go look at the results for
themselves. In 1994 alone, at least 450 research articles were published,
essentially all favoring a very old earth. Besides the scientific periodicals
which carry up-to-date research reports, specific suggestions are given below
of books for further reading.
Van Till Howard J., Young Davis
A., and Menninga, Clarence. (1988) Science Held Hostage. InterVarsity,
Downers Grove, IL, 189 pp.
This book talks about the misuse
of science by both hard-line atheists and by young-earth creationists. A good
deal of the book is devoted to refuting young-earth arguments, including a
substantial section on the Grand Canyon geology. Its authors are well-known
Christians in Geology and Physics.
Ross, Hugh. (1994) Creation and
Time: A Biblical and Scientific Perspective on the Creation-Date Controversy.
NavPress, Colorado Springs, CO.
Hugh Ross has a Ph.D. in Astronomy
and he defends modern science and an old age for the universe, refutes common
young-earth arguments, and firmly believes in the inerrancy of the Bible.
Young, Davis A. (1982) Christianity
and the Age of the Earth. Zondervan, Grand Rapids, MI (now available
through Artisan Sales, Thousand Oaks, CA).
Davis Young has a Ph.D. in Geology
and teaches at Calvin College. He argues for an old earth and refutes many of
the common young-earth claims (including their objections to radiometric
dating).
Strahler, Arthur N. (1987) Science
and Earth History: The Evolution/Creation Controversy. Prometheus Books,
Buffalo, pp. 129-138.
This book was not written by a
Christian, but is included here because it is a very thorough and comprehensive
refutation of young-earth evidences. The only negative aspect is that at one
point Strahler throws in a bit of his own theology--his arguments against the
need for a God. This book is long and in small print; it covers a wealth of
information.
Wiester, John. (1983) The
Genesis Connection. Interdisciplinary Biblical Research Institute,
Hatfield, PA, 254 pp.
John Wiester has taught Geology at
Westmont and Biola University, and is active in the American Scientific
Affiliation, an organization of scientists who are Christians. This book
discusses many scientific discoveries relating to the age of the earth and how
these fit into the context of Genesis 1.
Stoner, Don. (1992) A New
Look at an Old Earth. Schroeder, Paramount, CA, 191 pp.
A persuasive book written for the
Christian layman. Stoner uses arguments both from the theological and the
scientific side. He talks somewhat philosophically about whether God deceives
us with the Genesis account if the earth is really old. Stoner also tries to
discuss the meaning of the Genesis 1 text.
Dickin, Alan. (1995) Radiometric
Isotope Geology. Cambridge University Press, 452 pp.
This is the most up-to-date and
comprehensive textbook on radiometric dating techniques.
The following books are popular college-level Geology texts that deal in depth
with various dating techniques. Geologic Time is very easy to read and
has been around for some time. The text by Dalrymple is meant to be relatively
easy to read, but is also very comprehensive. The Faure texts are regular
textbooks for Geology, including more mathematics and more details.
Dalrymple, G. Brent. (1991) The
Age of the Earth. Stanford University Press, 474 pp.
Eicher, Don L. (1976) Geologic
Time, 2nd edition. Prentice-Hall, Englewood Cliffs, NJ, 150 pp.
Faure, Gunter. (1986) Principles of Isotope Geology, 2nd edition. Wiley,
New York, 464 pp.
Faure, Gunter. (1991) Principles
and Applications of Inorganic Geochemistry: A Comprehensive Textbook for
Geology Students. MacMillan Pub. Co., New York, 626 pp.
Electronic media: There is a site on the
world wide web called Talk.Origins at
"http://rumba.ics.uci.edu:8080/". Information on radiometric dating
can be found under several FAQ (frequently asked questions) subheadings. The
information can also be accessed by anonymous ftp to "ics.uci.edu:/pub/origins".
American Scientific Affiliation
http://ursa.calvin.edu/chemistry/ASA/
Affiliation of Christian Geologists
http://www.ksu.edu/~kbmill/acghome.html
Science & Christianity Resource List
http://hercules.geology.uiuc.edu/~Schimmri/christianity/scichr
Reasons to Believe
http://www.reasons.org/reasons/index.html
Acknowledgments: Several members of the Affiliation of Christian
Geologists and other Christians involved in the sciences reviewed this paper
and/or made contributions. The following people are sincerely thanked for their
contributions: Drs. Jeffery Greenberg and Stephen MosHier (Wheaton College),
John Wiester (Westmont College), Dr. Davis Young (Calvin College), Dr. Elaine
Kennedy (Loma Linda University), Steven Schimmrich (U. of Illinois), Kenneth
VanDellen (Macomb Community College), Dr. Guillermo Gonzalez (U. Texas,
Austin), Ronald Kneusel, and James Gruetzner (U. New Mexico).
About the author: Dr. Wiens received a bachelor's degree in Physics at
Wheaton College and his Ph.D. at the University of Minnesota doing research on
meteorites and moon rocks. He spent two years at Scripps Institution of
Oceanography (La Jolla, CA) where he studied isotopes of helium, neon, argon,
and nitrogen in terrestrial rocks. He is presently a staff scientist in the
Geological and Planetary Sciences Division at Caltech, where he is continuing
to study meteorites and is involved in a space mission to return to earth a
sample of solar wind. He has published over a dozen scientific research papers
and has also published articles in Christian magazines. Dr. Wiens became a
Christian at a young age, and has been a member of Mennonite Brethren, General
Conference Baptist, and Conservative Congregational churches.
Atom The smallest unit that
materials can be divided into. An atom is about ten billionths of an inch in
diameter and consists of a nucleus of nucleons (protons and neutrons)
surrounded by electrons.
Closed system A system
(rock, planet, etc.) which has no influence or exchange with the outside world.
In reality there is always some exchange or influence, but if this amount is
completely insignificant for the process under consideration (e.g., for dating,
if the loss or gain of atoms is insignificant) for practical purposes the
system can be considered closed.
Cosmic rays Very high
energy particles which fly through space. They are stopped by the earth's
atmosphere, but in the process, they constantly produce carbon-14,
beryllium-10, chlorine-36, and a few other radioactive isotopes in small
quantities.
Cosmogenic Produced by
bombardment of cosmic rays. Carbon-14 is said to be cosmogenic because it is
produced by cosmic rays.
Daughter The element or isotope which is produced by radioactive decay.
Decay The change from one
element or isotope to another. Only certain isotopes decay. The rest are said
to be stable.
Electron-capture decay The
only type of radioactive decay that requires the presence of something--an
electron--outside the atom's nucleus. Electron capture decay of light atoms--those
having the fewest electrons--can be very slightly affected by extremely high
pressures or certain chemical bonds, so as to change their half-lives by a
fraction of a percent. But no change in the half-lives of elements used for
radiometric dating has ever been verified.
Element A substance that
has a certain number of protons in the nucleus and unique properties. Elements
may be further broken down into isotopes, which have nearly all of the same
properties except for their mass and their radioactive decay characteristics.
Half-life The amount of time it takes for half the atoms of a
radioactive isotope to decay.
Ice core Long sections of
ice brought up by special drilling rigs on the ice sheets of Greenland and
Antarctica.
Igneous rock Rock formed
from molten lava. The other two types of rock are sedimentary, formed by the
cementing together of soil or sand, and metamorphic rocks reformed by heat over
long periods of time.
Isotope Atoms of a given
element that have the same atomic mass. Most elements have more than one
isotope. Most radioactive elements used for dating have one radioactive isotope
and at least one stable isotope. For example carbon-14 (which weighs 14 atomic
mass units) is radioactive, while the more common isotopes, carbon-12 and
carbon-13 are not.
Lead-lead dating A
variation on the uranium-lead technique in which only the isotopes of lead need
to be measured.
Magma Hot molten material
from which rocks are formed. When magma erupts on the surface of the earth, it
is called lava.
Metamorphism The heating of
rocks over long time periods at temperatures which are hot enough to change the
crystal structure but not hot enough to completely melt the rock. Metamorphism
tends to alter or reset the radiometric time clocks, though some radiometric
techniques are more resistant to resetting than others.
Nucleons Neutrons and protons, which make up the nucleus of an atom.
Parent The element or isotope which decays. The element it produces is
called the daughter.
Radioactive Subject to
change from one element to another. During the change, or decay, energy is
released either as light or energetic particles.
Radiocarbon Carbon-14,
which is used to date dead plant and animal matter. Radiocarbon is not used for
dating rocks.
Radiometric dating
Determination of a time interval (e.g., the time since formation of a rock) by
means of the radioactive decay of its material. Radiometric dating is one
subset of the many dating methods used in geology.
Three-isotope plot In
dating, this is a plot in which one axis represents the parent isotope and the
other axis represents the daughter isotope. Both parent and daughter isotopes
are ratioed to a daughter element isotope that is not produced by radioactive
decay. This type of plot gives the age independent of the original amounts of
the isotopes.
Tree ring A ring visible in
the stump or sawed section of a tree which indicates how much it grew in a
year. The age of a tree can be determined by counting the growth rings.
Two-component mixing The
mixing of two different source materials to produce a rock. On rare occasions
this can result in an incorrect age for certain techniques that use
three-isotope plots. Two component mixing can be recognized if more than one
dating technique is used, or if surrounding rocks are dated.
Xenolith Literally, a
foreign chunk of rock within a rock. Some rocks contain pieces of older rocks
within them. These pieces were ripped off the magma chamber in which the main
rock formed and were incorporated into the rock without melting. Xenoliths do
not occur in most rocks, and they are usually recognizable by eye where they do
occur. If unrecognized, they can result in an incorrect date for a rock (the
date may be of the older xenolith).
1 In only a couple of special cases have any decay rates been observed to vary,
and none of these special cases apply to the dating techniques discussed here.
These exceptions are discussed later.
2 The term isotope subdivides elements into groups of atoms that have the same
atomic weight. For example carbon has isotopes of weight 12, 13, and 14 times
the mass of a nucleon, referred to as carbon-12, carbon-13, or carbon-14
(abbreviated as 12C, 13C, 14C). It is only the carbon-14 isotope that is
radioactive.