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Physics of Aquatic Systems
Werner Aeschbach‐HertigInstitut für UmweltphysikUniversität Heidelberg
13. Dating Old Waters
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik2
Contents of Session 13
13.1 Basic principles of 14C dating– Conventional 14C age, calibration of 14C age scale
13.2 Complications of 14C dating of (ground)water– Reservoir effects and carbonate dissolution
13.3 Models for the initial 14C in groundwater– Corrections based on chemistry and stable isotopes
13.4 Other dating methods for old groundwater– Noble gas radioisotopes
Literature (14C): – Mook: Vol. 1, ch. 8 – 9, 12; Vol. 2, ch. 6; Vol. 4, ch. 5– Clark & Fritz, 1997: ch. 5; ch. 8– Kinzelbach et al., 2002. UNEP/DEWA Report RS 02‐2, ch. 7.
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik3
Origin and Distribution of 14C in Nature
from Mook, 2001
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik4
13.1 Basic Principles of 14C Dating I
dN Ndt
λ= −
0
1 ( )ln A ttAλ
⎛ ⎞= − ⎜ ⎟
⎝ ⎠
1 2 5730 yrT =
NdtdNA λ−=≡
( ) 0tN t N e λ−= ⋅
Problem:A0 = ?
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik5
Basic Principles of 14C Dating II
Classical 14C dating on organicmatter:• Carbon in living organism in equilibrium with atmospheric CO2
• No further exchange after death of organism: pure radiodecay• Initial activity A0 = Activity of atmospheric CO2
Complications:
• Atmospheric activity is not constant over time!– Reconstruction of A0(t), i.e., calibration of the 14C age scale, is achieved by 14C measurements on samples of known age
• Organic carbon is isotopically fractionated with respect to air – Corrected based on measurement of stable isotope 13C
• Reservoir effects: Aquatic organisms use dissolved carbon pool in the water (reservoir), whose A0(t) may differ from that of air
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik6
Atmospheric 14C: Anthropogenic effects
from Mook, 2001Suess effect(fossil fuel)
Bomb 14C
2
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik7
Natural variation of 14C for past 50 ka
Tree ringsCoralsCariaco Sediments
Origin of 14C variations: Changes in shielding of cosmic ray flux
Geomagnetic field (long‐term)
Solar activity (short term9
from Hughen et al., 2004, Science 303: 202-207
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik8
Calibration of 14C age
Tree ringsCoralsCariaco sedimentsLake Suigetsu varvesBahamas speleothemsN-Atlantic sediments
from Hughen et al., 2004, Science 303: 202-207
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik9
Non‐uniqueness of 14C age due to calibration
from Mook, 2001
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik10
What is a "conventional 14C age"?
• 14C activity is measured and reported relative to a standard• Standard activity chosen close to natural 14C content of living plants• By definition: 14Ast = 100 pmC (% modern carbon) = 0.95∙14AOx1
(1950) = 0.7459∙14AOx2 (1950) = 13.56 dpm/gC = 0.226 Bq/gC(Ox1, Ox2: International Oxalic Acid standards)
Conventional age:1. A0 = Standard activity in 19502. 14C normalised for isotope fractionation to "biomass" δ13C = ‐25‰3. Original (Libby) half‐life of 5568 a is used (current value: 5730 a)
1 2 14
1950
ln age in C-years before present (BP)ln2
sample
standard
T AA
τ⎛ ⎞
= − =⎜ ⎟⎜ ⎟⎝ ⎠ (present = 1950)
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik11
13.2 Complications of 14C Dating of Water
How can water be dated by 14C?• Only dissolved carbon can be dated!• Usually dissolved inorganic carbon (DIC) is used, rarely DOC• Total Dissolved Inorganic Carbon is present in several forms:
TDIC = CO2(aq) + H2CO3 + HCO3‐ + CO3
2‐
• TDIC is not in immediate equilibrium with the atmosphere and influenced by the complex carbonate chemistry
Ocean• Large TDIC‐reservoir, slow exchange, and upwelling of older carbon lead to a decreased activity: Asurf < 100 pmC
• Typical (but variable!): Asurf ~ 95 pmC ↔ τsurf ~ 400 yr
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik12
14C‐Dating of the Deep Ocean
from Broecker, 1995, The Glacial World according to Wally
3
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik13
Lakes and Groundwater: "Hardwater" Effects
Fresh water may dissolve old calcite (Ca12CO3) Hard (carbonate‐rich) water can have ATDIC << 100 pmCEffect depends on geological setting (presence of carbonate)Correction can be many ka for "hardwater" lakes and groundwater
14C ages of groundwater are not conventional ages:– 14C activity of TDIC is not normalised for isotope fractionation– The more precise half‐life of 5730 a is used
Why is groundwater 14C dating special?– Main problem is the origin of TDIC to determine A0
– δ13C is used to estimate A0 (mixing of different carbon sources)– High resolution ages are useless because of mixing
05730 a lnln2
AA
τ ⎛ ⎞= ⎜ ⎟⎝ ⎠
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik14
Carbonate Geochemistry
( )2CO g
3CaCO
-3HCO
2 3H CO
( )2CO aq
2-3CO
Soil CO2
Dissolved CO2
Carbonic acid
Bicarbonate
Carbonate
Calcite
soil
air
grou
ndw
ater
rock
( ) ( )2 2CO g CO aq↔
( )2 2 2 3CO aq H O H CO+ ↔
+ -2 3 3H CO H + HCO↔
- + 2-3 3HCO H + CO↔
2+ 2-3 3CaCO Ca + CO↔
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik15
Reaction Constants in the Carbonate System
( )2CO g
3CaCO
-3HCO
2 3H CO
( )2CO aq
2-3CO
[ ]2
2 3 1.470
CO
H COK = 10
P−=
Note 1: [x] denotes the molar (mol/l) activity of compound xNote 2: Dissolved CO2 is denoted as H2CO3, although in reality [CO2 (aq)] >> [H2CO3]Note 3: All reaction constants depend on T, values given at 25°C
Solubility, Henry's law
[ ]
+3 6.35
12 3
H HCOK = 10
H CO
−−
⎡ ⎤ ⎡ ⎤⎣ ⎦ ⎣ ⎦ = First dissociation const.
+ 23 10.33
23
H COK = 10
HCO
−−
−
⎡ ⎤ ⎡ ⎤⎣ ⎦ ⎣ ⎦ =⎡ ⎤⎣ ⎦
Second dissociation const.
3
+ 2 8.48CaCO 3K = Ca CO 10− −⎡ ⎤ ⎡ ⎤ =⎣ ⎦ ⎣ ⎦ Solubility product
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik16
Distribution of Carbonate Species in Water
Carbonate speciation depends on pH = ‐log[H+]
from Clark & Fritz, 1997
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik17
Description of the Carbonate SystemCarbonate system is defined by pH and concentration of 1 species.In practice, often well‐measurable sum parameters are used:– TDIC = ΣCO2 = mCO2 + mHCO3
‐ + mCO32‐
– Alk = mHCO3‐ + 2mCO3
2‐ (carbonate alkalinity)
with: mX = molal concentration (mol/kg) of compound X
Alkalinity is a measure of the buffering capacity of water, formally the equivalent sum of bases titratable with strong acids:
– Total Alk = mHCO3‐ + 2mCO3
2‐ + mB(OH)4‐ + mH3SiO4‐ +…
– Usually: Total Alk ≈ mHCO3‐ + 2mCO3
2‐ = Carbonate Alk
Alkalinity can be measured by titration in the fieldAt given T, all species can be calculated from pH and Alk or TDIC
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik18
Calcite Dissolution
Calcite dissolution is enhanced by CO2 (H2CO3):
( ) 2+ -2 2 3 3CO g + H O + CaCO Ca + 2HCO→
Asoil gas = 100 pmC Acalcite = 0 pmC
Calcite dissolution produces 50:50 mixture of young and old carbon!
• Open system: Constant supply of soil CO2 (unsaturated zone)– 14C‐active soil CO2 is dominant reservoir
• Closed system: Closed off from soil CO2 (saturated zone)– 14C‐dead CaCO3 is dominant reservoir
4
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik19
13.3 Models for A0 in Groundwater
Components or "endmembers" used in the models:t: Total carbon (TDIC) with measured conc., activity, isotope ratiog: Gaseous CO2 (soil air),usually with Ag = 100 pmC, δ13Cg = ‐25 ‰s: Solid calcite, usually with As = 0 pmC, δs = δ13Cs = 0 ‰
1) Vogel model: empirical value– Constant A0 of 85 ± 5 pmC– Based on young groundwater samples from NW Europe– No physical basis, not universally applicable
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik20
Models for A0 in Groundwater
2) Tamers model: Chemical balance (chemical dilution)– Idea: TDIC = CO2 + HCO3
‐, half of HCO3‐ from dead calcite
with: mX = molal concentration (mol/kg) of compound XAg = activity of soil gas CO2, usually 100 pmC
– Assumes stoichiometric dissolution, no other reactions – Yields A0 ≈ 50 pmC for most natural groundwaters– Oversimplified
( )( )
-2 3
0 g-2 3
CO aq + 0.5 HCOA = A
CO aq HCOm m
m m⋅
+
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik21
δ13C of Natural Carbon Compounds/Reservoirs
from Clark & Fritz, 1997
Idea: Use δ13C to distinguish contributions from soil gas and calcite
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik22
Models for A0 in Groundwater
3) Pearson model: Isotopic mixing balance– Idea: 14A0 and δ13C result from mixing of soil gas and calcite
with: As = activity of solid calcite, usually taken as 0 pmCδt = measured δ13C of TDICδg = δ13C of soil gas CO2, usually taken as ‐25 ‰δs = δ13C of solid calcite, usually taken as 0 ‰
– Pure isotope mixing, no reference to chemistry– Does not include isotope fractionation effects!
( )t s0 g s s
g s
δ - δA = A - A + Aδ - δ
⋅
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik23
Isotopic Composition of Carbon Components
from Mook, 2001
t s0 g
g s
δ - δA = Aδ - δ
⋅
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik24
Isotope Fractionation in the Carbonate System
from Clark & Fritz, 1997
5
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik25
Models for A0 in Groundwater
4) Fontes & Garnier model: Chemical & isotopic balance– Idea: Partial isotope exchange between soil CO2 and carbonate
( )t g s g sC C C C C q q= + = + − +
with: Ct , Cs = molal concentrations of total and solid‐derived Cq = fraction of solid‐derived C at equilibrium with soil CO2ε = δ13C fractionation between CO2 gas and solid carbonate
Open system:
Cg
δg
Cs - qq
δsδg - ε
soil CO2 solid carbonate
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik26
This part is identical to Tamers with
Models for A0 in Groundwater
Fontes & Garnier modelIsotope mass balance equations for 13C and 14C:
( ) ( ) t t s s t s g g sC C C C qδ δ δ δ ε δ= + − + − −
( ) ( )0 0.2t s s t s g g sC A C A C C A q A Aε= + − + − −
assuming ε14C(%) = 0.2ε13C(‰)
( ) ( ) ( )
0 1
1 0.2
δ δ δ
εδ ε δ
⎛ ⎞= − + +⎜ ⎟⎝ ⎠
− − −+ − − ⋅
− −
s sg s
t t
t s t s s t gg s
g s
C CA A AC C
C C C CA A
Eliminating q from the above equations yields the final model equation:
-S 3C = 0.5 HCO⋅m
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik27
Models for A0 in Groundwater
Fontes & Garnier model: Closed system– Model also describes carbonate dissolution in closed system
Mathematically equivalent to open system with q' = ‐q
Closed system:
Cg- q'
δg
Csq'
δsδs + ε
soil CO2 solid carbonate
( )t g s g sC C C C q q C′ ′= + = − + +
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik28
Models for A0 in Groundwater
Fontes & Garnier model– Widely used, probably best of the "simple" models– Includes chemical and isotopic balance– Applies for both open and closed conditions:
• Calcite dissolution in unsaturated zone during recharge• Calcite dissolution in confined part of aquifer• Combination of both processes
– Does not include more complex chemical reactions• Incongruent dissolution (dissolution and re‐precipitation)• Addition of C from other sources (e.g. oxidation of organic C by sulphate reduction, geogenic CO2)
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik29
Effect of Carbonate Dissolution along Flow Path
from Kendall & McDonnell, 1998
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik30
Models for A0 in Groundwater5) NETPATH: Complete chemical and isotopic modeling– USGS developed software to model geochemical and isotopic evolution along a flow path in groundwater
– Plummer, L. N. et al. 1994. An interactive code (netpath) for modeling net geochemical reactions along a flow path, Version 2.0. Water‐Resources Investigations Report 94‐4169, U.S. Geological Survey, Reston, Virginia.
– available at: http://water.usgs.gov/software/netpath.html
– Allows modeling of geochemically complex systems– Any possible reactions can be implemented– Requires some knowledge of aquatic geochemistry and experience in use of the program
– Does not always yield unequivocal results
6
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik31
The Effect of Mixing on 14C Ages
Usually only piston‐flow 14C ages are calculated and reported!– Useful first approximation for confined aquifers– Dispersion model would probably be more appropriate
true age
14C age
The piston flow 14C‐ageunderestimates the true meanage of a mixed water parcel
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik32
13.4 Other Dating Methods for old Groundwater
10-3 10-1 101 103 105 107
age [yr]
222RnSF6CFCs
4He
39Ar
3H-3He
3H
85Kr
40Ar36Cl81Kr
14C
Here: NG radio‐isotopes 39Ar & 81Kr
Old: 36Cl and 81KrIntermediate: 39Ar39Ar closes gap from 50 – 1000 yr !
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik33
Properties of 39Ar and 81Kr
• Noble gas isotopes: conservative, except for radioact. decay• Small but ± constant cosmogenic source, simple behaviour
Property 39Ar 81Kr
Half‐life [yr] 269 229'000
Decay constant [s‐1] 8.17∙10‐11 9.59∙10‐14
Production (in atmosphere) 40Ar(n,2n)39Ar Spallat. 82‐86Kr80Kr(n,γ)81Kr
Isotope conc. in air [iX/X] 8.1∙10‐16 5.2∙10‐13
Absolute conc. in air [atoms m‐3] 2.0∙108 1.6∙107
Absolute conc. in water [atoms/L] ≈ 7000 ≈ 1000
⇒ Potentially very good dating tracers, but very low abundance
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik34
Analytical Methods for 39Ar and 81Kr
1. Low‐Level Counting (LLC): Count decaying atoms– best labs have background count rate ≈ 0.1 cpm– Required sample size for signal of 0.1 cpm (modern samples, 100 % efficiency!): Min. sample size 39Ar 81Kr
Air volume [L] 100 1∙106
Water volume [L] 3000 2∙107
2. Accelerator Masss Spectrometry (AMS): Count all atoms– Conventional MS impossible due to extremely low abundance– Conventional AMS impossible because negative NG ions unstable– Cyclotron‐AMS possible, but enormously complex and costly
Difficult for 39Ar, impossible for 81Kr!
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik35
New Detection Method for NG Radioisotopes
Atom Trap Trace Analysis (ATTA)Chen et al., 1999. Ultrasensitive Isotope Trace Analyses with a Magneto‐Optical Trap. Science 286, 1139‐1141.
• Idea – Isotopically selective laser cooling and trapping– Detection of single atoms in magneto‐optical trap (MOT)
• Advantage – extremely selective (no interferences)
• Problem – achieve sufficient trapping/counting efficiency
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik36
Principle of ATTAatoms laserlight
source Laser Cooling:Slowing (cooling) of atoms by multiple photon absorption
Isotopically selective due to resonance condition and very arge number of absorbed photons
hν, ħk
7
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik37
Principle of ATTA
1) Excitation to metastable state in source.
2) Cooling in Zeeman slower.
3) Trapping in magneto‐optical trap (MOT).
4) Detection of single atoms in MOT by fluorescence.
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik38
First Application of ATTA
6 (!) groundwater samples for 81Kr, Nubian Sandstone, Egypt
Sturchio et al., 2004. Geophys. Res. Lett. 31, doi:10.1029/2003GL019234
Sampling:Several m3 of water degasssed
Sample preparation:Separation of Kr by GC system
Measurement by ATTA:12 cph from 50 µl Kr (∼ 700 l water)Efficiency ∼ 10‐4
Results:Groundwater ages 0.2 – 1 Myr
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik39
ATTA in Heidelberg: StatusEnviron. physics: Gas extraction & Ar separation under developmentAtom physics: Dedicated atom trap system for ATTA constructedTrapping and detection in MOT demonstrated with 40Ar atoms
2 atoms1 atom0 atoms
• Spectroscopy of 39Ar conducted successfully
Welte et al., 2009. Rev. Sci. Instrum. 80, 113109, doi:10.1063/1.3257691
Physics of Aquatic Systems, 13. Dating old Groundwater Universität HeidelbergInstitut für Umweltphysik40
Summary
• 14C dating requires knowledge of atmospheric 14C history• In aquatic systems: DIC‐reservoir not in equilibrium, A0 < Aatm
• Groundwater 14C dating is special:– Carbon from calcite dissolution: A0 << Aatm
– Mixing: no single exact age, no high resolution• 14C correction models (estimation of A0):
– Different models based on chemical and isotopic balances– Fontes & Garnier (1979) model: most flexible, often used
• Mixing: 14C piston flow ages underestimate true mean age• Alternative Methods: Noble gas radioisotopes 39Ar and 81Kr
– Very promising tracers in principle, but hard to measure– Atom trap trace analysis (ATTA) offers an new chance