Transcript Document

Radiocarbon
9/18/12
Lecture outline:
1) radiocarbon dating principles
2)
Atmospheric & ocean radiocarbon variability
3)
The Calibration Curve
4)
Radiocarbon as biogeochemical tracer
What makes 14C the
“emperor” of isotopes?
The Shroud of Turin
Radiocarbon (14C) formation and decay
-formed by interaction of cosmic ray spallation products with stable N gas
1
0
n 147 N  146 C  11H
-radiocarbon subsequently decays by β- decay back to 14N with a half-life of 5730y
C  147 N      Q
14
6
Radiocarbon dating was first explored by W.R. Libby (1946), who later won the Nobel Prize.
Most published dates still use the “Libby” half-life of 5568y to enable comparison of 14C dates.
The activity of radiocarbon in the atmosphere represents a balance of its production, its decay,
and its uptake by the biosphere, weathering, etc.
Which of these three
things might change
through time,
and why?
Radiocarbon Dating
1) As plants uptake C through photosynthesis, they take on the 14C activity of the atmosphere.
2) Anything that derives from this C will also have atmospheric 14C activity (including you and I).
3) If something stops actively exchanging C (it dies, is buried, etc), that 14C begins to decay.
A  A0et
where present-day, pre-bomb,
14C activity = 13.56dpm/g C
So all you need to know to calculate
an age is A0, which to first order
is 13.56dpm/g, BUT
*small variations (several percent)
in atmospheric 14C in the past
lead to dating errors of up to 20%!
Sources of variability:
1)
geomagnetic field strength
2)
solar activity
3)
carbon cycle changes
Radiocarbon Measurements and Reporting
1) Radiocarbon dates are determined by measuring the ratio of 14C to 12C in a sample,
relative to a standard, usually in an accelerator mass spectrometer.
standard = oxalic acid that represents activity of 1890 wood
14C
ages are reported as “14C years BP”, where BP is 1950
2) Fact: Most living things do not uptake C in atmospheric ratios – i.e. they fractionate carbon,
(lighter 12C preferentially used), must correct for this fractionation because it affects the 14C/12C ratio
Researchers collect the 13C/12C ratio, use it to
correct for “missing” 14C
So the less 13C a sample has, the less 14C it has,
and so the uncorrected 14C age will be _______
than the calendar age?
Samples are “normalized” to a
13CPDB
value of -25‰
  13C / 12C    13C / 12C 

spl
std
13
 C
 1 *1000
13
12


 C / C std


Acorr
 2(25   13CPDB ) 
 Ameas 1 
 dpm / g
1000


3) The final step is to obtain a “calibrated 14C age” using the atmospheric radiocarbon content
when the sample grew.
Atmospheric radiocarbon variability through time
Convention:
The atmospheric
radiocarbon
anomaly with
respect to a standard
is defined as D14C
  14C / 12C 

D 14C   14 12 spl  1 *1000
 C / C 

std


-solar activity changes
Note:
the D14C is 0
during 1890,
b/c that’s
the activity of the
oxalic acid standard
-addition of isotopically light
fossil fuel C to atmosphere
time
But how did somebody
construct this curve?
Reconstructing atmospheric radiocarbon variability through time
What you need:
absolute age & radiocarbon age
A  A0et
tree cut in 1999A.D.
What you get:
history of 14Catmos
1821A.D. by ring-counting
Most of the Holocene 14Catmos
variability derives from changes
in the geomagnetic field
Over longer timescales, what’s controlling atmospheric 14C?
Earth’s Carbon Reservoirs
(in Gigatons C):
atmosphere
748
terrestrial
2,000
oceanic
38,000
geologic
4,000
Climate changes perturb the E’s carbon
cycle (and therefore 14Catmos) by:
-changing the amount of C stored on land
(ex ice sheets of LGM)
-changing the ability of the deep
ocean to sequester old carbon from
atmosphere (ex increased stratification)
14C
content
highest (site of production)
high (some old organic matter)
high (surface) and low (deep)
zero (isolated from atmos. for long time)
The ocean “conveyor belt” and radiocarbon
Seawater radiocarbon measurements
set a time-scale for whole-ocean
mixing (~1500y), and identified
the locations where deep-mixing occur
The 14C ages of waters along a N-S
transect in the Atlantic.
note non-zero age at surface
the youngest
waters are
at the surface
and in the deep
North Atlantic
the “bomb”
spike
the oldest
waters are
in the mid-depth
pacifc (age~1500y)
14C
measurements from vertical
profiles taken in world’s oceans
4) If dating a marine sample, you will need to correct its calibrated 14C age with a reservoir age,
which ranges from <100yrs in the stagnant subtropical gyres to >1000yrs in the mid-depth Pacific.
Paleo-ventilation ages from 14C in marine carbonates
Atlantic
Pacific,
LGM=large symbols
GEOSECS=small dots
Broecker et al., 2004
Adkins et al., 1998
diff. in 14C ages=670y!
2. compare U-series and 14C ages
for deep-sea corals
100y of growth (study modern corals)
1. compare 14C ages
of benthic and planktonic
forams in same core horizon
The Radiocarbon Calibration Curve (atmospheric 14C history)
Principle: compare radiocarbon dates with independent dates
examples of independent dating: tree-ring counting, coral U-Th dates, varve counting,
correlation of climate signals in varves with ice core
Observation:
radiocarbon dates
are consistently
younger than calendar
ages
data from:
corals (bright red)
lake varves (green)
marine varves (blue)
speleothems (orange)
tree rings (black)
So was atmospheric
14C larger or
smaller at 20k (LGM)
than today?
time
Hughen et al., 2004
But what caused these large changes in atmospheric 14C?
Use a carbon cycle model that includes radiocarbon, play with different scenarios,
check fit with reality.
geomagnetic
field from
paleomag
studies
only
geomagnetic
field +
mag. anomaly
+ reduced
sedimentation
during glacial
stop transferring
radiocarbon
into deep ocean
red=observed 14C
black=modelled 14C
geomagnetic
field from
paleomag
+ magnetic
anomaly
at 44k
geomagnetic
field +
mag. anomaly
+ reduced
sedimentation
during glacial
+ change
in overturning
circulation
Beck et al., 2001
So what is the average geochemist to do?
Trust the experts!
INTCAL09 – established one curve to use for 14C calibration:
Reimer PJ, Baillie MGL, Bard E, Bayliss A, Beck JW, Blackwell PG,
Bronk Ramsey C, Buck CE, Burr GS, Edwards RL, Friedrich M,
Grootes PM, Guilderson TP, Hajdas I, Heaton TJ, Hogg AG, Hughen KA,
Kaiser KF, Kromer B, McCormac FG, Manning SW, Reimer RW,
Richards DA, Southon JR, Talamo S, Turney CSM, van der Plicht J,
Weyhenmeyer CE. 2009. IntCal09 and Marine09 radiocarbon age
calibration curves, 0–50,000 years cal BP. Radiocarbon 51(4):1111–50.
Use their calibration program (current version = CALIB 6.0):
http://radiocarbon.pa.qub.ac.uk/calib
M. Stuiver, P.J. Reimer, and R. Reimer
Also, avoid contamination with post-bomb/tracer carbon at all costs!
Ex: diagenesis may replace original C with post-bomb (modern) C
or
contamination with tracer (super-enriched) 14C used by biologists (done in IBB)
The timing and structure of the “bomb” spike
Bomb-produced radionuclides (in 1018 Bq (1Bq=1dps)
*
*
*
*
The radiocarbon bomb spike – atmosphere vs. other reservoirs
+1000‰ = 14C doubles
Trumbore, 2000
Source of bomb
14C:
stratosphere, Northern Hemisphere
Incorporation of bomb 14C into various C reservoirs depends on the residence time
of C in that reservoir
Ex: short residence time = quick, high-amplitude response
Why?
long residence time = delayed, low-amplitude response
Seawater radiocarbon observations
1.
GEOSECS – Geochemical Ocean
Section Study
1972-1978
transects through all major oceans
2.
WOCE – World Ocean Circulation
Experiment
1990-2002
extensive coverage of the ocean
Ocean models of bomb 14C
Can ocean general circulation models
accurately capture the spatial and temporal
evolution of the bomb radiocarbon spike?
*Our understanding of ocean mixing (esp.
vertical mixing) is extremely limited, 14C can
help.
Rodgers et al., 1999
Atmosphere-Ocean-Biosphere models of bomb 14C evolution
Atmosphere
Terrestrial biosphere
w/ three different
carbon residence times
The contributions of ocean, terrestrial
biosphere, fossil fuel combustion and bomb
testing to atmospheric D14C was
investigated with an Atmospheric General
Circulation Model (GCM) coupled to a
carbon cycle model.
Why does the terrestrial biosphere
lag the atmosphere?
The detrended atmos D14C,
showing large seasonal cycle
Randerson et al., Global Biogeochemical Cycles, 2002
Why do Southern and Northern
Hemisphere D14C values differ in 1970?
Map of mean annual Δ14C relative to South Pole. Randerson et al., 2002
Why does the Northern Hemisphere have lower Δ14C?
Model D14C-coral D14C comparisons
French Frigate
Shoals
Fiji
Rodgers et al., 1999
Why are some records “smoother”
than others (ie Galapagos vs. Fiji)?
Galapagos
Nauru
Radiocarbon in the Biosphere
Approach:
Use bomb 14C as a tracer of
carbon cycling in complex
environments.
Or use natural level 14C to
date carbon in various pools.
Gaudinski et al., 2000
Radiocarbon measurements of carbon cycling in the ocean
dissolved
organic carbon
old – highly
refractory
dissolved
inorganic carbon
contains bomb
14C at surface,
not at deep
sinking particulate
organic matter
contains bomb
carbon
Figure 1. Radiocarbon in different reservoirs of carbon at
Station M in the North Eastern Pacific Ocean. Red circles
represent values for HMW DOM (Aluwihare, 1999); blue bars at
0 m and 1500 m represent the range of values observed for
individual monosaccharides isolated from HMW sugars
(Aluwihare, 1999). DIC, total DOC, and POC data are from
Druffel et al., 1996 and Bauer et al., 1998.