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Radioisotopic/radiometric dating
2
Radioisotopic/radiometric dating
 Many believe in an old earth, i.e., billions
of years old, due to radioisotopic dating
3
Radioisotopic/radiometric dating
 Many believe in an old earth, i.e., billions
of years old, due to radioisotopic dating
 But is this really the case? Is it true that
the earth is billions of years old?
4
Radioisotopic dating
 Some basic concepts
 Carbon 14
 40K-40Ar
 Assumptions
 Closing slides
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Three Types of Radioisotopic
Decay
 Gamma radiation – photon of light emitted;
atom does not lose mass
 Alpha radiation – alpha particle has mass;
when decay happens atom loses mass
7
Half-life
 Parent – the original radioactive element
 Daughter- the resulting element(s) from radioisotopic
decay, or series of decay
 Half-life – the amount of time it takes for parent to decay
to 50:50 parent/daughter ratio; e.g., 1,000,000 atoms of
238U would take 4.5 billion years to get 500,000 atoms
each of 238U and 206Pb (one half-life); and second 4.5
billion yrs would result in 250,000 atoms of 238U and
750,000 atoms of 206Pb (two half-lives)
8
Half-life
 Parent – the original radioactive element
 Daughter- the resulting element(s) from radioisotopic
decay, or series of decay
 Half-life – the amount of time it takes for parent to decay
to 50:50 parent/daughter ratio; e.g., 1,000,000 atoms of
238U would take 4.5 billion years to get 500,000 atoms
each of 238U and 206Pb (one half-life); and second 4.5
billion yrs would result in 250,000 atoms of 238U and
750,000 atoms of 206Pb (two half-lives)
 At this time, unknown what causes an individual
radioactive atom to decay while another does not
9
Half-life
206Pb
206Pb
206Pb
206Pb
206Pb
206Pb
206Pb
206Pb
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
Parent
Daughter
~4,500,000,000 years
Parent
One half-life
10
Half-life
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
238U
Parent
~9,000,000,000 years
Parent
206Pb
206Pb
206Pb
206Pb
206Pb
206Pb
206Pb
206Pb
238U
238U
238U
238U
Daughter
206Pb
206Pb
206Pb
206Pb
Two half-lives
11
206Pb
238U 234Pa
234Th
230Th
234U
214Po
226Ra 214Bi
214Pb
218Po
222Rn
Uranium 238 Decay Series
210Po
210Bi
210Pb
α α α
α α α
α α
β
stable
β
β
β
β
β
4.47 billion yrs 24 days
20 min
1,602 yrs
77,000 yrs
240,000 yrs
6.7 hrs
27 min
3.1 min
3.8 days
138 days
5 days
22 yrs
0.000164 sec
12
206Pb
238U 234Pa
234Th
230Th
234U
214Po
226Ra 214Bi
214Pb
218Po
222Rn
Uranium 238 Decay Series
210Po
210Bi
210Pb
α α α
α α α
α α
β
stable
β
β
β
β
β
4.47 billion yrs 24 days
20 min
1,602 yrs
77,000 yrs
240,000 yrs
6.7 hrs
27 min
3.1 min
3.8 days
138 days
5 days
22 yrs
0.000164 sec
13
 The late Willard F. Libby led team of scientists at University of Chicago
during the post-II War period.
 1949 first measured rate of 14C decay at 5568 ± 30years
 1960 Libby received the Nobel Prize in Chemistry
 Half-life revised to 5730 ± 40 years (Cambridge half-life)
 1950’s used Gas Proportional Counting to measure 14C
 Liquid Scintillation Counting (LSC) uses benzene, acetylene, ethanol,
methanol, and other chemicals.
 Mid-1970’s development of Accelerated Mass Spectroscopy (AMS)
 The Atomic Mass Number is the sum of the number of protons and
neutrons
Carbon 14
14
National Ocean Sciences AMS at Woods Hole Oceanographic
Institution, Massachusetts. Photograph of Staff Physicist Robert
Schneider placing a carousel of graphite targets into the ion source of
the accelerator.
Photo by Tom Kleindinst, 1995
15
 Air/atmosphere carbon molecules:
98.89% 12C
1.11%13C
0.0000000001% 14C, or 1 14C for
every 1,000,000,000,000 12C
16
 Air/atmosphere carbon molecules:
98.89% 12C
1.11%13C
0.0000000001% 14C, or 1 14C for
every 1,000,000,000,000 12C
 12C is stable
17
 Air/atmosphere carbon molecules:
98.89% 12C
1.11%13C
0.0000000001% 14C, or 1 14C for
every 1,000,000,000,000 12C
 12C is stable
 13C is stable
18
 Air/atmosphere carbon molecules:
98.89% 12C
1.11%13C
0.0000000001% 14C, or 1 14C for
every 1,000,000,000,000 12C
 12C is stable
 13C is stable
 14C is unstable; 14C changes back into 14N
19
 Air/atmosphere carbon molecules:
98.89% 12C
1.11%13C
0.0000000001% 14C, or 1 14C for
every 1,000,000,000,000 12C
 12C is stable
 13C is stable
 14C is unstable; 14C changes back into 14N
 Entire inventory of 14C is called the carbon
exchange reservoir.
20
Cosmic Rays
Upper Atmosphere
Atoms
Neutrons
Lower Atmosphere 14N 14N 14N 12C
12C + neutrons proton
14C
CO2 CO2
14C
12C
14C
12C
14C
12C
21
Cosmic Rays
Upper Atmosphere
Atoms
Neutrons
Lower Atmosphere 14N 14N 14N 12C
12C + neutrons proton
14C
CO2 CO2
14C
12C
14C
12C
14C
12C
22
Cosmic Rays
Upper Atmosphere
Atoms
Neutrons
Lower Atmosphere 14N 14N 14N 12C
12C + neutrons proton
14C
CO2 CO2
14C
12C
14C
12C
14C
12C
23
Cosmic Rays
Upper Atmosphere
Atoms
Neutrons
Lower Atmosphere 14N 14N 14N 12C
12C + neutrons proton
14C
CO2 CO2
14C
12C
14C
12C
14C
12C
24
Cosmic Rays
Upper Atmosphere
Atoms
Neutrons
Lower Atmosphere 14N 14N 14N 12C
12C + neutrons proton
14C
CO2 CO2
14C
12C
14C
12C
14C
12C
25
Cosmic Rays
Upper Atmosphere
Atoms
Neutrons
Lower Atmosphere 14N 14N 14N 12C
12C + neutrons proton
14C
CO2 CO2
14C
12C
14C
12C
14C
12C
26
Cosmic Rays
Upper Atmosphere
Atoms
Neutrons
Lower Atmosphere 14N 14N 14N 12C
12C + neutrons proton
14C
CO2 CO2
14C
12C
14C
12C
14C
12C
27
Cosmic Rays
Upper Atmosphere
Atoms
Neutrons
Lower Atmosphere 14N 14N 14N 12C
12C + neutrons proton
14C
CO2 CO2
14C
12C
14C
12C
14C
12C
28
Cosmic Rays
Upper Atmosphere
Atoms
Neutrons
Lower Atmosphere 14N 14N 14N 12C
12C + neutrons proton
14C
CO2 CO2
14C
12C
14C
12C
14C
12C
29
Known limitations
 Size of sample is important.
 the larger the better
 purification and distillation removes some matter
(LSC)
 AMS better able to handle smaller samples
 Requires great care in collecting and packaging.
Carbon sample location requires careful stratigraphic
examination.
 Upper practical limit of 40,000 – 50,000 years, or 9 -10
half-lives.
 Atmospheric 14C /12C ratio not always constant.
 In general, single dates should not be trusted. Whenever
possible multiple samples should be collected and dated
from associated strata.
(http://id-
archserve.ucsb.edu/Anth3/Courseware/Chronology/08_Radiocarbon_Dating.html#C14Process)
30
Other factors affecting 14C dating
 Plants may discriminate against intake of
14C; plants are known to discriminate
against 13C1
1
. www.plantphys.net/article.php?ch=9&id=135
31
Other factors affecting 14C dating
 Plants may discriminate against intake of
14C; plants are known to discriminate
against 13C1
 Reservoir effects
1
. www.plantphys.net/article.php?ch=9&id=135
32
Other factors affecting 14C dating
 Plants may discriminate against intake of
14C; plants are known to discriminate
against 13C1
 Reservoir effects
 Suess or Industrial effect
1
. www.plantphys.net/article.php?ch=9&id=135
33
Other factors affecting 14C dating
 Plants may discriminate against intake of
14C; plants are known to discriminate
against 13C1
 Reservoir effects
 Suess or Industrial effect
 Atomic bomb effect
1
. www.plantphys.net/article.php?ch=9&id=135
34
Other factors affecting 14C dating
 Plants may discriminate against intake of
14C; plants are known to discriminate
against 13C1
 Reservoir effects
 Suess or Industrial effect
 Atomic bomb effect
 Noah’s flood
1
. www.plantphys.net/article.php?ch=9&id=135
35
14C in coal
 C14 found in coal supposedly millions of
years old
36
14C in fossils
 C14 found in fossilized wood
37
14C in diamonds
 Diamonds are believed to have formed 1-3
billion years ago
 The earth’s mass is about 6x1027 g, which
would be equivalent to about 4.3x1026
atoms of 14C
 It takes 88 half-lives to get to a single atom
of 14C
 88 half-lives is about 500,000 years.
38
The presence of 14C in supposedly
ancient coal, fossil wood, and diamonds
falsifies the notion that the rocks or strata
in which they were found are millions or
years old.
39
K-Ar dating
40
K-Ar dating
 Parent daughter
40K 40Ar
40Ca
41
K-Ar dating
 Parent daughter
40K 40Ar
40Ca
 Half-life of 40K is 1.26 billion years.
42
K-Ar dating
 Parent daughter
40K 40Ar
40Ca
 Half-life of 40K is 1.26 billion years.
 40Ca is rarely used to determine dates
because it is hard to determine the
quantity of calcium initially present.
43
K-Ar dating
 Parent daughter
40K 40Ar
40Ca
 Half-life of 40K is 1.26 billion years.
 40Ca is rarely used to determine dates
because it is hard to determine the
quantity of calcium initially present.
 11.2% of 40K decays to 40Ar
44
K-Ar dating
 Parent daughter
40K 40Ar
40Ca
 Half-life of 40K is 1.26 billion years.
 40Ca is rarely used to determine dates
because it is hard to determine the
quantity of calcium initially present.
 11.2% of 40K decays to 40Ar
 88.8% of 40K decays to 40Ca
45
 Whole rock dating – the whole of the rock sample is
crushed and dated
 Partial rock dating – rocks are generally composed of
different minerals; these different minerals have
different structures and radioisotopes behave differently
in each mineral
 Note: radioisotopic dating is usually done on igneous and
volcanic rock. Metamorphic and sedimentary rocks are
considered less suitable for dating because their origin is
already preexisting and re-worked rock
46
Date calculation:
t = h x ln[1 + (40Ar)/(0.112 x (40K))]/ln(2)
where:
t = time in years
h = half-life in years
ln = natural logarithm
47
Atmosphere (air) contains 40Ar
-some air 40Ar may be trapped in rocks
-ratio of 40Ar to 39Ar in air is well known at
295:1
-measuring 39Ar and 40Ar, and applying
the ratio one can subtract off air-40Ar
48
Measured K-Ar, Mt. St. Helens
http://www.answersingenesis.org/tj/v10/i3/argon.asp
49
Measured K-Ar, Mt. St. Helens
 Lava solidified in 1986
http://www.answersingenesis.org/tj/v10/i3/argon.asp
50
Measured K-Ar, Mt. St. Helens
 Lava solidified in 1986
 340,000 years ± 600 yrs
http://www.answersingenesis.org/tj/v10/i3/argon.asp
51
Measured K-Ar, Mt. St. Helens
 Lava solidified in 1986
 340,000 years ± 600 yrs
 2,800,000 yrs ± 600,000 yrs
http://www.answersingenesis.org/tj/v10/i3/argon.asp
52
Measured K-Ar, Mt. St. Helens
 Lava solidified in 1986
 340,000 years ± 600 yrs
 2,800,000 yrs ± 600,000 yrs
 Critics claim excess Ar, which is known about
http://www.answersingenesis.org/tj/v10/i3/argon.asp
53
Measured K-Ar, Mt. St. Helens
 Lava solidified in 1986
 340,000 years ± 600 yrs
 2,800,000 yrs ± 600,000 yrs
 Critics claim excess Ar, which is known about
 Biblical creationists question whether dating
works on rocks of unknown ages when it does
not work on rocks of known age
http://www.answersingenesis.org/tj/v10/i3/argon.asp
54
Half-lives of other radioisotopes
Most half-lives taken from Holden, N.E. (1990) Pure appl. Chem. 62, 941-958.
Radioactive Isotope
(Parent)
Product
(Daughter)
Half-Life
(Years)
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-36 300,000
Carbon-14 Nitrogen-14 5715
Uranium-234 Thorium-230 248,000
Thorium-230 Radium-226 75,400
55
Some assumptions
 Decay rate is constant over the determined time
period
56
Decay rate did not change when subject to
extreme changes in temperature,
pressure, magnetism, electrical fields and
chemical alteration.
57
Constant decay rate?
 Anderson and Spangler showed decay process is not random,
therefore, concluded that decay rate is uncertain, putting all
radiometric dating into serious question.
 Working with Cobalt 60 and Cesium 137 they state “The evidence is
inconsistent with the theory of decay independence.”1 Cobalt 60
was significantly influenced by electrical field.
 “…even though holding responsible scientific positions, these
authors admitted to difficulty in getting their work published and
since then have confessed that it has been ‘disregarded, discounted,
disbelieved…by virtually the entire scientific community’ (Anderson
and Spangler, 1974)”2
1 Quoted in Note 11, In the Minds of Men, Ian T. Taylor, TFE Publishing:Toronto, Canada, 3rd edition,
fifth reprint 1994; p. 457.
2 Taylor, ibid., p. 296.
58
 In cautiously worded terms Anderson and Spangler
“writing in American Physical Society Bulletin, 1971,
10:1180 had presented their data to show that the
gamma emission rate of cobalt 60 was significantly
influenced by electrical fields. They concluded that, in
this case, radioactive decay is not independent.” 1
 In 1974, the authors freely expressed their views more
explicitly in the, now defunct, journal Pensée.
1 Taylor, op cit., p.457.
59
Rhenium-187 1
-half-life of 42 billion years
-half-life of 33 years when stripped of electrons
-isolated case
1. Don DeYoung, Thousands…Not Billions, p. 144, with reference to Kerr,
Richard, 1999, Tweaking the Clock of Radioactive Decay, Science 286(5441),
882-883.
60
Solar neutrinos
-seasonal fluctuations
-rates increased when closer to the sun and
decreased when farther from the sun
Brian Thomas, http://www.icr.org/articles/radioactive-decay-rates-not-stable, article
posted August 4, 2009; referencing Mullins, J., 2009, Solar ghosts may haunt
Earth’s radioactive atoms, New Scientist, 2714:42-45.
61
Cavitation
-shock waves produced from the collapse of
vapour bubbles resulting from extremely fast
water flows
-during a 90-minute experiment, radioactive
thorium decay was accelerated by a factor of
10,000 times
Brian Thomas, http://www.icr.org/articles/radioactive-decay-rates-not-stable, article
posted August 4, 2009; referencing Cardone, F., R. Mignani and a. Petrucci,
2009. Piezonuclear decay of thorium. Physics Letters A. 373 (22): 1956-1958.
62
Radioisotopes not found on earth
 Old earth suggested from extinct parent isotopes for
which there is strong evidence that these once existed in
substantial amounts in meteorites, but have since
completely decayed away.
 Extinct Isotope Half-life (years)
 Plutonium-244 82 million
 Iodine-129 16 million
 Palladium-107 6.5 million
 Manganese-53 3.7 million
 Iron-60 1.5 million
 Aluminum-26 700,000
 Calcium-41 130,000
However, can be interpreted as vast quantity of decay
occurred in the past, not necessarily indicative of age.
63
1 4 7 10 13 16 19 22 25 28 31 34 37 40 43 46 49 52 55 58
Time
Decay
Rate
The present
64
Deep Earth Zircons
 Uranium/lead age of 1.5 billion yrs ± 20 million yrs
 Crystals contained too much helium to be million yrs old
 Leak rate of helium out of zircon crystals was unknown
 Predicted and measured helium leak rates agreed at
~6000 yrs
 Helium leak rate concords with Biblical history
D. Russell Humphreys, A Tale of Two Hourglasses, Impact article #402, Institute for Creation
Research, California, December 2006.
65
http://creationontheweb.com/content/view/6193/ accessed December 01, 2008.
Predicted Leak Rates
66
http://creationontheweb.com/content/view/6193/ accessed December 01, 2008.
67
Some assumptions
 Decay rate is constant over the determined time
period
 Neither parent nor daughter material has been
added to or taken away from the sample during
the determined time period
68
238U
238U
238U
238U
238U
238U
206Pb
238U
238U
238U
238U
206Pb
238U
238U
238U
238U
206Pb
206Pb
206Pb
206Pb
206Pb
206Pb
206Pb
206Pb
238U
238U
238U
206Pb
238U
238U
238U
238U
~ 4.5 billion years
206Pb
238U
238U
206Pb
206Pb
206Pb
238U
Time Now
69
Some assumptions
 Decay rate is constant over the determined time
period
 Neither parent nor daughter material has been
added to or taken away from the sample during
the determined time period
 The initial parent/daughter ratio is known (i.e., it
is most often assumed to be zero daughter)
70
Argon-Argon
 40K-39K ratio appears to be constant in the sample
 Sample put in nuclear reactor and bombarded with
neutrons
 39K is turned into 39Ar
 Assumed that newly formed 39Ar is proportional to 39K
71
Wiens calls this a typical argon-argon plot.
But is it typical? Notice also, the Y-axis on the left hand side. From where does
one obtain the age?
Roger C. Wiens, Radiometric Dating A Christian Perspective, revised 2002. Wiens has a PhD in physics
with a minor in geology. He is a firm believer in the radiometric dating method and believes in an old earth.
72
Isochrons
 Iso = same, equal chron = time
 Attempts to address issue of initial amount of daughter
material before any parent material had time to decay
 Attempts to address issue of addition or subtraction of
external radioisotopic material, i.e., whether or not the
sample remained a closed system
 Attempts to address the most likely computed age of a
rock sample, based upon the statistical average of
several radioisotope measurements
73
An ideal isochron
Parent isotope, Rb-87/Sr-86
Daughter
isotope,
Sr-87/Sr-86
Rock when formed
74
Fig. 5. A thin vertical
amphibolite layer
(darker rock) just
upstream of Clear Creek,
Grand Canyon.
Creation 27(3) June-August 2005, p.
46.
75
Creation 27(3) June-August 2005, p. 47.
76
Creation 27(3) June-August 2005, p. 47.
77
“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 human (which implies the
appearance of age). The idea of a false
appearance of great age is a philosophical
and theological matter that we won't go
into here. …
Roger C. Wiens, Radiometric Dating A Christian Perspective, revised 2002. Wiens has a PhD in physics with a
minor in geology. He is a firm believer in the radiometric dating method and believes in an old earth.
78
… The main drawback—and it is a strong
one—is that this makes God appear to be
a deceiver. However, some people have
no problem with this. Certainly whole
civilizations have been incorrect
(deceived?) in their scientific and
theological ideas in the past. Whatever the
philosophical conclusions, it is important
to note that an apparent [emphasis added]
old Earth is consistent with the great
amount of scientific evidence.”
Roger C. Wiens, Radiometric Dating A Christian Perspective, revised 2002. Wiens has a PhD in physics with a
minor in geology. He is a firm believer in the radiometric dating method and believes in an old earth.
79
However, if God stated that He created in
six days, but really took millions and
billions of years, would this not make God
a deceiver?
If God really took millions and billions of
years to make the heavens, earth, and all
creatures, but He said He did it in six
days, would this not make God
incompetent at communicating?
80
 Age is not directly measured
 Amount (or ratio) of parent/daughter, at
the present time, is what is measured
 Heat, pressure, water, chemicals can
affect the parent/daughter ratio
81
Other dating methods
 Thermoluminescence (TL): when individual grains of common minerals,
such as quartz, are heated, they emit light, and this is related to the
radiation ‘stored’ in the crystal structure. By measuring the light emitted
from the mineral grain when it is heated, and measuring the radiation in
the environment where the grain was found, a date is calculated. It is
assumed that the radiation was slowly absorbed from the environment,
building up from zero at a certain time in the past (perhaps when the grain
was last exposed to sunlight).
 Optically-stimulated luminescence (OSL): dates are based on exactly
the same principle and TL. But instead of heating the grain, it is exposed to
light to make it emit its ‘stored’ radiation. The calculated date is based on
the same assumptions, and affected by the same uncertainties, as for TL.
 Electron-spin resonance: dates are based on the same principles as TL
and OSL. However, the ‘stored’ radiation in the sample is measured by
exposing it to gamma radiation and measuring the radiation emitted. The
measuring technique does not destroy the ‘stored’ radiation (as does TL
and OSL), so the measurement can be repeated on the same sample. The
calculated date is based on the same assumptions, and affected by the
same uncertainties, as for TL and OSL.
82
Other dating methods cont’d
 Thorium-uranium (Th/U) dates are based on measuring the isotopes of
uranium and thorium in a sample. It is known that uranium-238 decays
radioactively to form thorium-230 (through a number of steps, including
through uranium-234). The dating calculation assumes that the thorium
and uranium in the sample are related to each other by radioactive decay.
Furthermore, before a date can be calculated, the initial ratios of
230Th/238U and 234U/238U need to be assumed, and it is also assumed
that there has been no gain or loss of uranium or thorium to/from the
environment—i.e. that the system is ‘closed’. However, the bone and soil
must have been ‘open’ to allow these elements to enter and accumulate.
 Protactinium-uranium (Pa/U) dates are based on similar principles as
Th/U dating, but use uranium-235 and protactinium-231 instead. The
isotope 235U decays radioactively to form 231Pa. Again, it is assumed that
the isotopes in the sample are related to each other by radioactive decay.
Also, the initial ration of 231Pa/235U has to be assumed, and it is assumed
that there has been no gain or loss of uranium or protactinium to for from
the environment—i.e. that the system is ‘closed’. Again, any bone sample
containing uranium must have been ‘open’ to allow it to accumulate in the
first place.
83
84
Eisegesis
85
Exegesis
86
Scientist & Bible
87
“When Moses wrote that God created
Heaven and Earth and whatever is in
them in six days, then let this period
continue to have been six days, and
do not venture to devise any
comment according to which six days
were one day. …
Martin Luther cited in E. Plass, What Martin Luther Says: A Practical In-House Anthology
for the Active Christian, Concordia Publishing House, St. Louis, 1991, p. 1523
88
But, if you cannot understand how this
could have been done in six days,
then grant the Holy Spirit the honor
of being more learned than you are.
For you are to deal with the Scripture
in such a way that you bear in mind
that God Himself says what is written.
But since God is speaking, it is not
fitting for you wantonly to turn His
Word in the direction you wish to go.”
Martin Luther cited in E. Plass, What Martin Luther Says: A Practical In-House Anthology
for the Active Christian, Concordia Publishing House, St. Louis, 1991, p. 1523
89
90
Acknowledgments
Answers In Genesis
Creation Ministries International
Institute for Creation Research
91
The End

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Radioisotopic or radiometric dating.pptx

  • 2. 2 Radioisotopic/radiometric dating  Many believe in an old earth, i.e., billions of years old, due to radioisotopic dating
  • 3. 3 Radioisotopic/radiometric dating  Many believe in an old earth, i.e., billions of years old, due to radioisotopic dating  But is this really the case? Is it true that the earth is billions of years old?
  • 4. 4 Radioisotopic dating  Some basic concepts  Carbon 14  40K-40Ar  Assumptions  Closing slides
  • 6. 6 Three Types of Radioisotopic Decay  Gamma radiation – photon of light emitted; atom does not lose mass  Alpha radiation – alpha particle has mass; when decay happens atom loses mass
  • 7. 7 Half-life  Parent – the original radioactive element  Daughter- the resulting element(s) from radioisotopic decay, or series of decay  Half-life – the amount of time it takes for parent to decay to 50:50 parent/daughter ratio; e.g., 1,000,000 atoms of 238U would take 4.5 billion years to get 500,000 atoms each of 238U and 206Pb (one half-life); and second 4.5 billion yrs would result in 250,000 atoms of 238U and 750,000 atoms of 206Pb (two half-lives)
  • 8. 8 Half-life  Parent – the original radioactive element  Daughter- the resulting element(s) from radioisotopic decay, or series of decay  Half-life – the amount of time it takes for parent to decay to 50:50 parent/daughter ratio; e.g., 1,000,000 atoms of 238U would take 4.5 billion years to get 500,000 atoms each of 238U and 206Pb (one half-life); and second 4.5 billion yrs would result in 250,000 atoms of 238U and 750,000 atoms of 206Pb (two half-lives)  At this time, unknown what causes an individual radioactive atom to decay while another does not
  • 11. 11 206Pb 238U 234Pa 234Th 230Th 234U 214Po 226Ra 214Bi 214Pb 218Po 222Rn Uranium 238 Decay Series 210Po 210Bi 210Pb α α α α α α α α β stable β β β β β 4.47 billion yrs 24 days 20 min 1,602 yrs 77,000 yrs 240,000 yrs 6.7 hrs 27 min 3.1 min 3.8 days 138 days 5 days 22 yrs 0.000164 sec
  • 12. 12 206Pb 238U 234Pa 234Th 230Th 234U 214Po 226Ra 214Bi 214Pb 218Po 222Rn Uranium 238 Decay Series 210Po 210Bi 210Pb α α α α α α α α β stable β β β β β 4.47 billion yrs 24 days 20 min 1,602 yrs 77,000 yrs 240,000 yrs 6.7 hrs 27 min 3.1 min 3.8 days 138 days 5 days 22 yrs 0.000164 sec
  • 13. 13  The late Willard F. Libby led team of scientists at University of Chicago during the post-II War period.  1949 first measured rate of 14C decay at 5568 ± 30years  1960 Libby received the Nobel Prize in Chemistry  Half-life revised to 5730 ± 40 years (Cambridge half-life)  1950’s used Gas Proportional Counting to measure 14C  Liquid Scintillation Counting (LSC) uses benzene, acetylene, ethanol, methanol, and other chemicals.  Mid-1970’s development of Accelerated Mass Spectroscopy (AMS)  The Atomic Mass Number is the sum of the number of protons and neutrons Carbon 14
  • 14. 14 National Ocean Sciences AMS at Woods Hole Oceanographic Institution, Massachusetts. Photograph of Staff Physicist Robert Schneider placing a carousel of graphite targets into the ion source of the accelerator. Photo by Tom Kleindinst, 1995
  • 15. 15  Air/atmosphere carbon molecules: 98.89% 12C 1.11%13C 0.0000000001% 14C, or 1 14C for every 1,000,000,000,000 12C
  • 16. 16  Air/atmosphere carbon molecules: 98.89% 12C 1.11%13C 0.0000000001% 14C, or 1 14C for every 1,000,000,000,000 12C  12C is stable
  • 17. 17  Air/atmosphere carbon molecules: 98.89% 12C 1.11%13C 0.0000000001% 14C, or 1 14C for every 1,000,000,000,000 12C  12C is stable  13C is stable
  • 18. 18  Air/atmosphere carbon molecules: 98.89% 12C 1.11%13C 0.0000000001% 14C, or 1 14C for every 1,000,000,000,000 12C  12C is stable  13C is stable  14C is unstable; 14C changes back into 14N
  • 19. 19  Air/atmosphere carbon molecules: 98.89% 12C 1.11%13C 0.0000000001% 14C, or 1 14C for every 1,000,000,000,000 12C  12C is stable  13C is stable  14C is unstable; 14C changes back into 14N  Entire inventory of 14C is called the carbon exchange reservoir.
  • 20. 20 Cosmic Rays Upper Atmosphere Atoms Neutrons Lower Atmosphere 14N 14N 14N 12C 12C + neutrons proton 14C CO2 CO2 14C 12C 14C 12C 14C 12C
  • 21. 21 Cosmic Rays Upper Atmosphere Atoms Neutrons Lower Atmosphere 14N 14N 14N 12C 12C + neutrons proton 14C CO2 CO2 14C 12C 14C 12C 14C 12C
  • 22. 22 Cosmic Rays Upper Atmosphere Atoms Neutrons Lower Atmosphere 14N 14N 14N 12C 12C + neutrons proton 14C CO2 CO2 14C 12C 14C 12C 14C 12C
  • 23. 23 Cosmic Rays Upper Atmosphere Atoms Neutrons Lower Atmosphere 14N 14N 14N 12C 12C + neutrons proton 14C CO2 CO2 14C 12C 14C 12C 14C 12C
  • 24. 24 Cosmic Rays Upper Atmosphere Atoms Neutrons Lower Atmosphere 14N 14N 14N 12C 12C + neutrons proton 14C CO2 CO2 14C 12C 14C 12C 14C 12C
  • 25. 25 Cosmic Rays Upper Atmosphere Atoms Neutrons Lower Atmosphere 14N 14N 14N 12C 12C + neutrons proton 14C CO2 CO2 14C 12C 14C 12C 14C 12C
  • 26. 26 Cosmic Rays Upper Atmosphere Atoms Neutrons Lower Atmosphere 14N 14N 14N 12C 12C + neutrons proton 14C CO2 CO2 14C 12C 14C 12C 14C 12C
  • 27. 27 Cosmic Rays Upper Atmosphere Atoms Neutrons Lower Atmosphere 14N 14N 14N 12C 12C + neutrons proton 14C CO2 CO2 14C 12C 14C 12C 14C 12C
  • 28. 28 Cosmic Rays Upper Atmosphere Atoms Neutrons Lower Atmosphere 14N 14N 14N 12C 12C + neutrons proton 14C CO2 CO2 14C 12C 14C 12C 14C 12C
  • 29. 29 Known limitations  Size of sample is important.  the larger the better  purification and distillation removes some matter (LSC)  AMS better able to handle smaller samples  Requires great care in collecting and packaging. Carbon sample location requires careful stratigraphic examination.  Upper practical limit of 40,000 – 50,000 years, or 9 -10 half-lives.  Atmospheric 14C /12C ratio not always constant.  In general, single dates should not be trusted. Whenever possible multiple samples should be collected and dated from associated strata. (http://id- archserve.ucsb.edu/Anth3/Courseware/Chronology/08_Radiocarbon_Dating.html#C14Process)
  • 30. 30 Other factors affecting 14C dating  Plants may discriminate against intake of 14C; plants are known to discriminate against 13C1 1 . www.plantphys.net/article.php?ch=9&id=135
  • 31. 31 Other factors affecting 14C dating  Plants may discriminate against intake of 14C; plants are known to discriminate against 13C1  Reservoir effects 1 . www.plantphys.net/article.php?ch=9&id=135
  • 32. 32 Other factors affecting 14C dating  Plants may discriminate against intake of 14C; plants are known to discriminate against 13C1  Reservoir effects  Suess or Industrial effect 1 . www.plantphys.net/article.php?ch=9&id=135
  • 33. 33 Other factors affecting 14C dating  Plants may discriminate against intake of 14C; plants are known to discriminate against 13C1  Reservoir effects  Suess or Industrial effect  Atomic bomb effect 1 . www.plantphys.net/article.php?ch=9&id=135
  • 34. 34 Other factors affecting 14C dating  Plants may discriminate against intake of 14C; plants are known to discriminate against 13C1  Reservoir effects  Suess or Industrial effect  Atomic bomb effect  Noah’s flood 1 . www.plantphys.net/article.php?ch=9&id=135
  • 35. 35 14C in coal  C14 found in coal supposedly millions of years old
  • 36. 36 14C in fossils  C14 found in fossilized wood
  • 37. 37 14C in diamonds  Diamonds are believed to have formed 1-3 billion years ago  The earth’s mass is about 6x1027 g, which would be equivalent to about 4.3x1026 atoms of 14C  It takes 88 half-lives to get to a single atom of 14C  88 half-lives is about 500,000 years.
  • 38. 38 The presence of 14C in supposedly ancient coal, fossil wood, and diamonds falsifies the notion that the rocks or strata in which they were found are millions or years old.
  • 40. 40 K-Ar dating  Parent daughter 40K 40Ar 40Ca
  • 41. 41 K-Ar dating  Parent daughter 40K 40Ar 40Ca  Half-life of 40K is 1.26 billion years.
  • 42. 42 K-Ar dating  Parent daughter 40K 40Ar 40Ca  Half-life of 40K is 1.26 billion years.  40Ca is rarely used to determine dates because it is hard to determine the quantity of calcium initially present.
  • 43. 43 K-Ar dating  Parent daughter 40K 40Ar 40Ca  Half-life of 40K is 1.26 billion years.  40Ca is rarely used to determine dates because it is hard to determine the quantity of calcium initially present.  11.2% of 40K decays to 40Ar
  • 44. 44 K-Ar dating  Parent daughter 40K 40Ar 40Ca  Half-life of 40K is 1.26 billion years.  40Ca is rarely used to determine dates because it is hard to determine the quantity of calcium initially present.  11.2% of 40K decays to 40Ar  88.8% of 40K decays to 40Ca
  • 45. 45  Whole rock dating – the whole of the rock sample is crushed and dated  Partial rock dating – rocks are generally composed of different minerals; these different minerals have different structures and radioisotopes behave differently in each mineral  Note: radioisotopic dating is usually done on igneous and volcanic rock. Metamorphic and sedimentary rocks are considered less suitable for dating because their origin is already preexisting and re-worked rock
  • 46. 46 Date calculation: t = h x ln[1 + (40Ar)/(0.112 x (40K))]/ln(2) where: t = time in years h = half-life in years ln = natural logarithm
  • 47. 47 Atmosphere (air) contains 40Ar -some air 40Ar may be trapped in rocks -ratio of 40Ar to 39Ar in air is well known at 295:1 -measuring 39Ar and 40Ar, and applying the ratio one can subtract off air-40Ar
  • 48. 48 Measured K-Ar, Mt. St. Helens http://www.answersingenesis.org/tj/v10/i3/argon.asp
  • 49. 49 Measured K-Ar, Mt. St. Helens  Lava solidified in 1986 http://www.answersingenesis.org/tj/v10/i3/argon.asp
  • 50. 50 Measured K-Ar, Mt. St. Helens  Lava solidified in 1986  340,000 years ± 600 yrs http://www.answersingenesis.org/tj/v10/i3/argon.asp
  • 51. 51 Measured K-Ar, Mt. St. Helens  Lava solidified in 1986  340,000 years ± 600 yrs  2,800,000 yrs ± 600,000 yrs http://www.answersingenesis.org/tj/v10/i3/argon.asp
  • 52. 52 Measured K-Ar, Mt. St. Helens  Lava solidified in 1986  340,000 years ± 600 yrs  2,800,000 yrs ± 600,000 yrs  Critics claim excess Ar, which is known about http://www.answersingenesis.org/tj/v10/i3/argon.asp
  • 53. 53 Measured K-Ar, Mt. St. Helens  Lava solidified in 1986  340,000 years ± 600 yrs  2,800,000 yrs ± 600,000 yrs  Critics claim excess Ar, which is known about  Biblical creationists question whether dating works on rocks of unknown ages when it does not work on rocks of known age http://www.answersingenesis.org/tj/v10/i3/argon.asp
  • 54. 54 Half-lives of other radioisotopes Most half-lives taken from Holden, N.E. (1990) Pure appl. Chem. 62, 941-958. Radioactive Isotope (Parent) Product (Daughter) Half-Life (Years) 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-36 300,000 Carbon-14 Nitrogen-14 5715 Uranium-234 Thorium-230 248,000 Thorium-230 Radium-226 75,400
  • 55. 55 Some assumptions  Decay rate is constant over the determined time period
  • 56. 56 Decay rate did not change when subject to extreme changes in temperature, pressure, magnetism, electrical fields and chemical alteration.
  • 57. 57 Constant decay rate?  Anderson and Spangler showed decay process is not random, therefore, concluded that decay rate is uncertain, putting all radiometric dating into serious question.  Working with Cobalt 60 and Cesium 137 they state “The evidence is inconsistent with the theory of decay independence.”1 Cobalt 60 was significantly influenced by electrical field.  “…even though holding responsible scientific positions, these authors admitted to difficulty in getting their work published and since then have confessed that it has been ‘disregarded, discounted, disbelieved…by virtually the entire scientific community’ (Anderson and Spangler, 1974)”2 1 Quoted in Note 11, In the Minds of Men, Ian T. Taylor, TFE Publishing:Toronto, Canada, 3rd edition, fifth reprint 1994; p. 457. 2 Taylor, ibid., p. 296.
  • 58. 58  In cautiously worded terms Anderson and Spangler “writing in American Physical Society Bulletin, 1971, 10:1180 had presented their data to show that the gamma emission rate of cobalt 60 was significantly influenced by electrical fields. They concluded that, in this case, radioactive decay is not independent.” 1  In 1974, the authors freely expressed their views more explicitly in the, now defunct, journal Pensée. 1 Taylor, op cit., p.457.
  • 59. 59 Rhenium-187 1 -half-life of 42 billion years -half-life of 33 years when stripped of electrons -isolated case 1. Don DeYoung, Thousands…Not Billions, p. 144, with reference to Kerr, Richard, 1999, Tweaking the Clock of Radioactive Decay, Science 286(5441), 882-883.
  • 60. 60 Solar neutrinos -seasonal fluctuations -rates increased when closer to the sun and decreased when farther from the sun Brian Thomas, http://www.icr.org/articles/radioactive-decay-rates-not-stable, article posted August 4, 2009; referencing Mullins, J., 2009, Solar ghosts may haunt Earth’s radioactive atoms, New Scientist, 2714:42-45.
  • 61. 61 Cavitation -shock waves produced from the collapse of vapour bubbles resulting from extremely fast water flows -during a 90-minute experiment, radioactive thorium decay was accelerated by a factor of 10,000 times Brian Thomas, http://www.icr.org/articles/radioactive-decay-rates-not-stable, article posted August 4, 2009; referencing Cardone, F., R. Mignani and a. Petrucci, 2009. Piezonuclear decay of thorium. Physics Letters A. 373 (22): 1956-1958.
  • 62. 62 Radioisotopes not found on earth  Old earth suggested from extinct parent isotopes for which there is strong evidence that these once existed in substantial amounts in meteorites, but have since completely decayed away.  Extinct Isotope Half-life (years)  Plutonium-244 82 million  Iodine-129 16 million  Palladium-107 6.5 million  Manganese-53 3.7 million  Iron-60 1.5 million  Aluminum-26 700,000  Calcium-41 130,000 However, can be interpreted as vast quantity of decay occurred in the past, not necessarily indicative of age.
  • 63. 63 1 4 7 10 13 16 19 22 25 28 31 34 37 40 43 46 49 52 55 58 Time Decay Rate The present
  • 64. 64 Deep Earth Zircons  Uranium/lead age of 1.5 billion yrs ± 20 million yrs  Crystals contained too much helium to be million yrs old  Leak rate of helium out of zircon crystals was unknown  Predicted and measured helium leak rates agreed at ~6000 yrs  Helium leak rate concords with Biblical history D. Russell Humphreys, A Tale of Two Hourglasses, Impact article #402, Institute for Creation Research, California, December 2006.
  • 67. 67 Some assumptions  Decay rate is constant over the determined time period  Neither parent nor daughter material has been added to or taken away from the sample during the determined time period
  • 69. 69 Some assumptions  Decay rate is constant over the determined time period  Neither parent nor daughter material has been added to or taken away from the sample during the determined time period  The initial parent/daughter ratio is known (i.e., it is most often assumed to be zero daughter)
  • 70. 70 Argon-Argon  40K-39K ratio appears to be constant in the sample  Sample put in nuclear reactor and bombarded with neutrons  39K is turned into 39Ar  Assumed that newly formed 39Ar is proportional to 39K
  • 71. 71 Wiens calls this a typical argon-argon plot. But is it typical? Notice also, the Y-axis on the left hand side. From where does one obtain the age? Roger C. Wiens, Radiometric Dating A Christian Perspective, revised 2002. Wiens has a PhD in physics with a minor in geology. He is a firm believer in the radiometric dating method and believes in an old earth.
  • 72. 72 Isochrons  Iso = same, equal chron = time  Attempts to address issue of initial amount of daughter material before any parent material had time to decay  Attempts to address issue of addition or subtraction of external radioisotopic material, i.e., whether or not the sample remained a closed system  Attempts to address the most likely computed age of a rock sample, based upon the statistical average of several radioisotope measurements
  • 73. 73 An ideal isochron Parent isotope, Rb-87/Sr-86 Daughter isotope, Sr-87/Sr-86 Rock when formed
  • 74. 74 Fig. 5. A thin vertical amphibolite layer (darker rock) just upstream of Clear Creek, Grand Canyon. Creation 27(3) June-August 2005, p. 46.
  • 77. 77 “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 human (which implies the appearance of age). The idea of a false appearance of great age is a philosophical and theological matter that we won't go into here. … Roger C. Wiens, Radiometric Dating A Christian Perspective, revised 2002. Wiens has a PhD in physics with a minor in geology. He is a firm believer in the radiometric dating method and believes in an old earth.
  • 78. 78 … The main drawback—and it is a strong one—is that this makes God appear to be a deceiver. However, some people have no problem with this. Certainly whole civilizations have been incorrect (deceived?) in their scientific and theological ideas in the past. Whatever the philosophical conclusions, it is important to note that an apparent [emphasis added] old Earth is consistent with the great amount of scientific evidence.” Roger C. Wiens, Radiometric Dating A Christian Perspective, revised 2002. Wiens has a PhD in physics with a minor in geology. He is a firm believer in the radiometric dating method and believes in an old earth.
  • 79. 79 However, if God stated that He created in six days, but really took millions and billions of years, would this not make God a deceiver? If God really took millions and billions of years to make the heavens, earth, and all creatures, but He said He did it in six days, would this not make God incompetent at communicating?
  • 80. 80  Age is not directly measured  Amount (or ratio) of parent/daughter, at the present time, is what is measured  Heat, pressure, water, chemicals can affect the parent/daughter ratio
  • 81. 81 Other dating methods  Thermoluminescence (TL): when individual grains of common minerals, such as quartz, are heated, they emit light, and this is related to the radiation ‘stored’ in the crystal structure. By measuring the light emitted from the mineral grain when it is heated, and measuring the radiation in the environment where the grain was found, a date is calculated. It is assumed that the radiation was slowly absorbed from the environment, building up from zero at a certain time in the past (perhaps when the grain was last exposed to sunlight).  Optically-stimulated luminescence (OSL): dates are based on exactly the same principle and TL. But instead of heating the grain, it is exposed to light to make it emit its ‘stored’ radiation. The calculated date is based on the same assumptions, and affected by the same uncertainties, as for TL.  Electron-spin resonance: dates are based on the same principles as TL and OSL. However, the ‘stored’ radiation in the sample is measured by exposing it to gamma radiation and measuring the radiation emitted. The measuring technique does not destroy the ‘stored’ radiation (as does TL and OSL), so the measurement can be repeated on the same sample. The calculated date is based on the same assumptions, and affected by the same uncertainties, as for TL and OSL.
  • 82. 82 Other dating methods cont’d  Thorium-uranium (Th/U) dates are based on measuring the isotopes of uranium and thorium in a sample. It is known that uranium-238 decays radioactively to form thorium-230 (through a number of steps, including through uranium-234). The dating calculation assumes that the thorium and uranium in the sample are related to each other by radioactive decay. Furthermore, before a date can be calculated, the initial ratios of 230Th/238U and 234U/238U need to be assumed, and it is also assumed that there has been no gain or loss of uranium or thorium to/from the environment—i.e. that the system is ‘closed’. However, the bone and soil must have been ‘open’ to allow these elements to enter and accumulate.  Protactinium-uranium (Pa/U) dates are based on similar principles as Th/U dating, but use uranium-235 and protactinium-231 instead. The isotope 235U decays radioactively to form 231Pa. Again, it is assumed that the isotopes in the sample are related to each other by radioactive decay. Also, the initial ration of 231Pa/235U has to be assumed, and it is assumed that there has been no gain or loss of uranium or protactinium to for from the environment—i.e. that the system is ‘closed’. Again, any bone sample containing uranium must have been ‘open’ to allow it to accumulate in the first place.
  • 83. 83
  • 87. 87 “When Moses wrote that God created Heaven and Earth and whatever is in them in six days, then let this period continue to have been six days, and do not venture to devise any comment according to which six days were one day. … Martin Luther cited in E. Plass, What Martin Luther Says: A Practical In-House Anthology for the Active Christian, Concordia Publishing House, St. Louis, 1991, p. 1523
  • 88. 88 But, if you cannot understand how this could have been done in six days, then grant the Holy Spirit the honor of being more learned than you are. For you are to deal with the Scripture in such a way that you bear in mind that God Himself says what is written. But since God is speaking, it is not fitting for you wantonly to turn His Word in the direction you wish to go.” Martin Luther cited in E. Plass, What Martin Luther Says: A Practical In-House Anthology for the Active Christian, Concordia Publishing House, St. Louis, 1991, p. 1523
  • 89. 89
  • 90. 90 Acknowledgments Answers In Genesis Creation Ministries International Institute for Creation Research