Isotope 5 Flashcards
3 main types of short-lived isotopes
- Those formed as intermediate daughter products of larger decay chains, e.g. 230Th in the 238U - 206Pb decay series
• Dating and tracing physical processes such as melting - Recently-formed ‘cosmogenic’ isotopes
• Formed at the surface, or in the atmosphere or in space, through spallation and neutron capture processes as a result of cosmic ray bombardment
• Used to give surface exposure ages, sedimentation and sediment tracing in arcs - Extinct short-lived isotope systems
• Can be used to investigate the early solar system (e.g. Hf-W)
Secular equilibrium
Example
o Parent and decay of daughter 1 reach equilibrium after about 5 half-lives of daughter 1 – one decay of each at the same time – rate of decay is matched – will decay away at the same time
o Can be used to date between 0 and 5 half-lives of daughter 1
Short-lived ‘cosmogenic’ radiogenic isotopes
- Generated by high energy cosmic ray bombardment
- NOT stable, decay fairly rapidly
- Exceptionally low abundance of such nuclides
- Requires specialised mass spectrometry
- Atomic decay counting required 1200 tonnes of ice, whereas only 10kg required for Accelerator mass spectrometry
- Ions travel at several % of speed of light, e.g. ~10,000,000 m/s (much faster than conventional mass spectrometry)
- Used to give exposure ages, and applied to sedimentation rates, glacial ice, hydrology and sediment tracing in island arcs
Accelerator Mass Spectrometry
Extremely large, but like all mass spectrometers AMS has 3 main components: Source, Mass analyser (x2) and Detectors.
AMS also has the addition of a tandem accelerator – hence the name.
Why use AMS?
Almost complete elimination of molecular ions and isobars from the mass spectrometry.
How does AMS work?
• The AMS source generates –ve ions, so, for instance, negatively charged 14C ions can be separated from the abundant 14N isobar, which doesn’t form negative ions in the AMS
• The accelerated -ve ions are converted to multiply-charged +ve ions by collisions with gas molecules, which are then accelerated. The ions can travel at several % of the speed of light.
Molecular ions do not exist as multiply charged +ve ions at high energies, so polyatomic interferences are completely eliminated.
• Result is AMS is able to measure single atoms in the presence of 1x1015 (a thousand million million) stable atoms.
Radionuclide examples
Be10 - Exposure dating, ice cores, erosion rates
C14 - Organic matter
Al26 - Exposure dating of rocks
Cl36 - Exposure dating, tracing groundwater flow
Ca41 - Exposure dating of carbonate
I129 - Tracing groundwater
14C
Neutron bombardment:
10N + 147N = 146C + 11H
14C decays to 14N (beta decay) with half-life of 5700 yrs
Living tissue exchanges CO2 with atmosphere and is therefore in equilibrium with the atmosphere
On death, exchange ceases and, over time, 14C decays to 14N
If system remains ‘closed’ then age can be determined using law of radioactive decay:
A = Aoe-λt
(where A0 is initial activity of 14C, t is time and λ is the decay constant)
Applications:
Dendrochronology
Comparison with tree rings aids calibration of 14C dating
Dating of organic material, e.g. charcoal, skin, peat
But only up to 60,000 years old.
10Be
High cosmogenic production rate (0.02 atoms/cm2/sec) and relatively long half-life (1.36 Ma) decaying back to 10B by beta emission.
Produced in the upper atmosphere by spallation reactions with N and O.
Atmospheric residence time for 10Be ~1 year, removed by precipitation.
Also produced in quartz by spallation reactions involving O and interactions with 28Si (10-100 atoms g-1 a-1). Used in conjunction with 26Al to determine exposure ages.
After precipitation will dissolve into seawater and eventually form clay at the bottom of the ocean
Applications:
Erosion studies
Extent of accumulation in soils (and its erosion into rivers) indicates speed of erosion, and uplift.
Tracing sediment subduction in arc magmas
10Be adsorbed onto settling sediment, thus these seds have much higher 10Be than the mantle or mafic oceanic crust
If subducted sediments contribute to arc magmatism, higher 10Be should be present in recent arc lavas
1-2 x 106 atoms/g 10Be in MORB,
up to 24 x 106 atoms/g in arc lavas
Comes into MORB by hydrothermal events
High concentrations into arc magmas by subducting sediment into mantle and it returning to surface within 10 half lives
Only hard proof of mantle recycling
Can’t be used for tracing – OIB are nowhere near subduction zones – takes too long
B/Be vs 10Be
Combined boron and beryllium studies used to trace subduction fluid inputs in arc systems
10Be enriched in sediments. B enriched, relative to Be in altered MORB
Therefore:
high 10Be/9Be ratios and low B/Be ratios indicate largely sediment input (fluid or melt)
Low 10Be/9Be ratios and high B/Be ratios indicate fluid from the mafic part of the oceanic crust
26Al
Product of Ar spallation reactions. Very short half life of 717ka decaying to 26Mg by electron capture.
Used to calculate terrestrial residence ages of meteorites:
After parent body break-up, meteorites are bombarded
by intense cosmic rays
The meteorite becomes saturated in 26Al
After falling to Earth, 26Al production almost ceases due to the protection of the atmosphere and 26Al decreases with time.
Therefore, the measured 26Al activity in the sample can be used to calculate the time at which it arrived on Earth.
Very low 26Al production in materials on Earth’s surface (0.0002 atoms/cm2/sec).
26Al production by spallation reactions involving 28Si in quartz – production rate of about 10-100 atoms g-1 a-1 and as quartz is Al-poor the 26Al/27Al ratio changes sufficiently with time to be measured.
Therefore, used 26Al can be used for exposure ages in quartz-rich materials (in conjunction with 10Be)
36Cl
Produced by spallation reactions with 36Ar in the atmosphere. Half-life is 301Ka.
Also produced between 1952 and 1958 by marine nuclear bomb tests by neutron capture of 35Cl
NOT removed from water (unlike Be).
Therefore, good for tracing groundwater movement, which is no longer in contact with the surface
Cosmogenic 36Cl used for ancient (ka age) systems
Anthropogenic 36Cl used for modern-day systems
Extinct short-lived radioactive decay systems (cosmogenic)
- Formation in a stellar event ‘shortly’ before solar system formation or through spallation near early Sun
- Includes heavier isotopes than currently produced by cosmic bombardment
- Half-lives of hundreds of thousands to tens Ma
- Rapid decay leads to exhaustion of these isotopes ‘soon’ after solar system formation (unlike long-lived radiogenic isotopes)
- Potential for investigating early solar system processes including the age of the solar system and core formation in planetary bodies
- Combined with long-lived U-Th-Pb and Pb-Pb dating, short-lived isotope dating has achieved greater precision and resolution for the age of the earliest solar system materials
- 4568-4571 Ma (CA inclusions (CAIs) in meteorites)
- Earliest meteorites 5-10 Ma later