Transcript Chapter 3

Quaternary Environments
Dating Methods I
Accuracy Versus Precision
Precision means that the samples have
low amount of error associated with the
dating
 Accuracy means that the samples are
dated to the true age of the sample
 We strive for both accuracy and precision
in dating techniques

Accuracy Versus Precision
Relative Versus Absolute Dating

Relative Dating
 Principle

of Superposition
Absolute Dating
 Provides
solid chronological dates (within
error bars) that are related to a calendar year
scale
Methods

Radioisotopic Methods


Paleomagnetic Methods


Relies on past reversals of the Earth’s magnetic field
Organic and Inorganic Chemical Methods


Based on rate of atomic disintegration
Based on time-dependent chemical changes in a
sample
Biological Methods

Based on the growth of an organism
Using Radioactivity in Dating

Radiometric dating
 Useful
radioactive isotopes for providing ages
 87Rb/87Sr
 232Th/208Pb
 238U/206Pb
 40K/40Ar
 235U/207Pb
 14C/14N
– 47.0 billion years
– 12.1 billion years
– 4.5 billion years
– 1.3 billion years
– 713 million years
– 5,730 years (5,570 Libby years)
Sources of Error


A closed system is required
To avoid potential problems, only fresh,
unweathered samples should be used
Using Radioactivity in Dating

Reviewing basic atomic structure
 Nucleus
– positively charged particles with mass
 Neutrons – neutral particles with mass
 Electrons – negatively charged particles that
orbit the nucleus
 Protons
Using Radioactivity in Dating

Reviewing basic atomic structure
 Atomic
number
 An
element’s identifying number
 Equal to the number of protons in the atom’s
nucleus
 Mass
number
 Sum
of the number of protons and neutrons in an
atom’s nucleus
 Identifies an isotope
Using Radioactivity in Dating

Reviewing basic atomic structure
 Isotope
 Variant
of the same parent atom
 Differs in the number of neutrons
 Results in a different mass number than the
parent atom
Using Radioactivity in Dating

Radioactivity
 Spontaneous
changes (decay) in the structure
of atomic nuclei

Types of radioactive decay
 Alpha
emission
 Emission
of 2 protons and 2 neutrons (an alpha
particle)
 Mass number is reduced by 4 and the atomic
number is lowered by 2
Using Radioactivity in Dating

Types of radioactive decay
 Beta
emission
 An
electron (beta particle) is ejected from the
nucleus
 Mass number remains unchanged and the atomic
number increases by 1
Using Radioactivity in Dating

Types of radioactive decay
 Electron
 An
capture
electron is captured by the nucleus
 The electron combines with a proton to form a
neutron
 Mass number remains unchanged and the atomic
number decreases by 1
Common Types of Radioactive
Decay
Using Radioactivity in Dating
Parent – an unstable radioactive isotope
 Daughter product – the isotopes resulting
from the decay of a parent
 Half-life – the time required for one-half of the
radioactive nuclei in a sample to decay

Using Radioactivity in Dating

Radiometric dating
 Principle
 The
of radioactive dating
percentage of radioactive atoms that decay
during one half-life is always the same (50
percent)
 However, the actual number of atoms that decay
continually decreases
 Comparing the ratio of parent to daughter yields
the age of the sample
Radioactive decay curve
Radiocarbon Dating

Dating with 14C
 Half-life
of 5730 years
 Used to date very recent events
14C is produced in the upper atmosphere
 Useful tool for anthropologists, archeologists,
and geologists who study very recent Earth
history
Sources of Error in 14C Dating

Problems of Sample Selection and
Contamination
 Young
carbon effects
 Old carbon effects
Variation in 14C content in the ocean
reservoir
 Fractionation Effects

14C
Age of Sea Water
Radiocarbon Variation Over the
Last 2000 years
Calibration Curve Showing
Departure
Calibrated Curve
Radiocarbon Plateaus
14C
Bomb Spike
Potassium Argon Dating (40K/40Ar)
Instrumental in dating sea-floor basalts
and providing the timing of magnetic
reversals
 Used in dating lava flows
 Also for dating metamorphic events

Potassium Argon Dating (40K/40Ar)
 39K
and 41K, Stable
 40K unstable and 0.012% of all potassium
 40K decays to 40Ca and 40Ar
 Ca is common in rocks and is therefore
not useful in dating
 Measure the amount of 40Ar in the lab and
the amount of 40K is also measured from
the sample
Potassium Argon Dating (40K/40Ar)



Long half-life makes this useful over long time scales but not
really usable at less than 100,000 years
Optimal time range is around 30 ma and up to 1 ba rocks
can be dated
Dating is done on sanidine, plagioclase, biotite, hornblende,
and olivine in volcanic rocks and glauconite, feldspar, and
sylvite in sedimentary rocks
Problems of 40K/40Ar

Assumptions



Checks


No Ar was left in the rock at formation
System has remained closed since formation
The ratio of 36Ar to 40Ar is known in the atmosphere
and can be measured in the rock to determine
atmospheric contamination
Problem

Loss of Ar due to diffusion, recrystallization, solution,
and chemical reactions
40Ar/39Ar



Dating
A problem with 40K/40Ar dating is that K and Ar are
measured at different places in the rock
This can be solved by irradiating the samples and
converting 39K to 39Ar
With the known ratio of 40K to 39K, the amount of 40K can
be calculated from the same lattice structure as the 39Ar
Uranium Series Dating
 238U




and 235U have a decay process that cascades
through a series of elements
Each decay stage can be used as a dating tool
Thermal Ionization Mass Spectrometry (TIMS) allows
very accurate estimates from small samples
U series are useful in dating corals and speleothems
Mollusks seem to be an open system in relation to U and
are not generally conducive to U series dating
Problems of U Series Dating

Assumes the initial 230Th/234U, 234U/238U,
and 231Pa/235U ratios
 Likely
in ocean sediments but more in flux in
the atmosphere

Assumes a closed system
Luminescence Dating Principles
and Applications



Light emitted from a mineral crystal (usually
quartz or feldspars) when exposed to heat or
light
The light emitted is related to the amount of
ionizing radiation that the sample has been
exposed to from sediment
The clock is set to zero by heating or optical
bleaching

Therefore Loess and fluvial sediments make good
candidates for luminescence dating
Luminescence

Thermoluminescence (TL Dating)
 When

the light is emitted as a result of
thermal hearting
 First published Wintle and Huntley 1979
Optical and Infrared Stimulated Luminescence
(OSL and IRSL Dating)
 Visible or infrared energy emitted in response
to radiation
Problems in TL Dating



Assumes that the relationship between the radiation
dose and the resulting luminescence is a linear
relationship; not always the case
 <5,000 yrs the rate of electron accumulation is slow,
possibly needing to exceed a threshold
 Some minerals may reach saturation >300,000 yrs
Anomalous Fading – Minerals do not hold the electrons
beyond a few weeks
Variations in environmental dose; related to moisture
content for one example
Optical and Infrared Stimulated
Luminescence (OSL and IRSL Dating)



Zero in the modern sediments
Sensitive to light bleaching setting the system to zero
Multiple measurements are possible because short
stimulation to the light source does not deplete the
potential luminescence
Fission Track Dating




Uranium will decay through fission, splitting the
nucleus and shooting the two halves into the
mineral
The results are fission tracks from 10-20μm in
length
Some glassy minerals will loose their fission
tracks through heating, setting the clock to zero
Different minerals have different annealing
temperatures
Fission Track Dating




The samples are polished and etched with a
chemical that brings out the tracks
The tracks are counted, then the sample is
heated, annealing the tracks. Then the sample
is irradiated with a slow neutron beam and the
tracks from the fission of 235U are counted
The number of induced tracks is proportional to
the amount of 238U in the sample
The known fission rate of 238U is used to
calculate the age of the sample
Fission Track Dating





Can be used in apatite, micas, sphene, and
zircons
Can also be used in rocks such as volcanic ash,
obsidian, basalts, granites, tuffs, and
carbonatites
Ranges from 103 to 108 years
The error associated with this technique is hard
to determine and is seldom reported
Repeat measures are the best, but are seldom
undertaken because of time constraints
Dendrochronology
Temperate trees produce annual rings.
 The trees are recording all of the
environmental variables that affect tree
growth.
 Can be used to date objects with annual
resolution back 10,000 years in the best
circumstances.

Neutron capture (A)
and Beta emission (B)