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Understanding the Glacial Cycles
J.C. Hargreaves
Paleoclimate Group,Global Warming Division,
Frontier Research System for Global Change.
23 March 2004
Outline of talk.
• An analysis of time-series data of the Glacial Cycles, concen-
tration on the Ice-age terminations.
Hargreaves, JC and Abe-Ouchi, A., Paleoceanography, 18(2): 1035, 2003
• Combining data and models in paleo-climate studies.
Hargreaves, JC and Annan, JD, Climate Dynamics, 19 (5-6): 371-381, 2002
Annan JD, Hargreaves, JC, Edwards, NR, Marsh, R, Ocean Modelling, in press.
• Conclusions and future work.
Data analysis using an antisymmetric wavelet
Development of objective methods for determining the timing of
terminations and analysing the variation of aperiodic and quasi-
periodic oscillation in various paleoclimatic data sets.
The last four ice-ages - [Shackleton 2000 data]
−2
−1
0
1
2
3
Air temperature
0 100 200 300 400
−2
−1
0
1
2
Atmospheric CO2
Normalised
Data
time (kyr B.P.)
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−1
0
1
2
Deep ocean temperature
Normalised
Data
0 100 200 300 400
−2
−1
0
1
2
time (kyr B.P.)
Sea level
The ice-age ‘cycles’
• Asymmetrical - slow ice growth, fast terminations.
• Non-identical
Defining a ‘termination’
• “Rapid and abrupt change from extreme glacial to extreme
inter-glacial conditions” [Broecker 1984] – but they look
more complicated than this implies.
• Defining the start of a termination is complicated by small
scale variation in the data. Here we concentrate on finding
the time at which the greatest change occured.
→ Fourier analysis is inappropriate but wavelet analysis
produces a 2-dimensional frequency-location spectrum.
The general forms of the well-known Morlet wavelet and the
less well-known antisymmetric wavelet (Lewalle et al. 1995).
−5 0 5−1
−0.5
0
0.5
1Morlet Wavelet
−5 0 5−0.8
−0.6
−0.4
−0.2
0
0.2
0.4
0.6
0.8Antisymmetric Wavelet
Estimation of the correspondence between wavelet number and
time scale
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0
1
(a) Sine wave, period = 50
20406080
100120
(b) Real part of continuous Morlet wavelet transform
wav
elet
no.
50 100 150 200 250 300 350 400 450 500 550 600
510152025
(c) Continuous antiymmetric wavelet transform
wav
elet
no.
Analysis of data with Morlet and antisymmetric wavelets
−2
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airtemp.
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CO2
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2
Normalised data
oceantemp.
0 100 200 300 400
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1
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time (kyr B.P.)
sealevel
20
40
60
wav
elet
no.
Antisymmetric wavelet
20
40
60
wav
elet
no.
0 100 200 300 400
20
40
60
wav
elet
no.
time (kyr BP)
0 100 200 300 400
20
40
60
wav
elet
no.
20406080
100120
wav
elet
no.
20406080
100120
wav
elet
no.
Morlet wavelet
20406080
100120
wav
elet
no.
0 100 200 300 400
20406080
100120
wav
elet
no.
time (kyr BP)
Summary of qualitative results
• Morlet wavelet – Variations at the higher frequency Milankovitch
time scales are evident. Saw-tooth signal of the ice-ages is
not clearly identified.
• Anti-symmetric wavelet – Terminations are precisely located.
Close-up views of the ice-age terminations in the Shackleton
data.
−2
0
2
data
Termination 1
10
20
30
ocean
temp. wav
elet
no.
10
20
30
CO2
wav
elet
no.
0 20 40
10
20
30
sea
level
time (kyr B.P.)
wav
elet
no.
10
20
30
air
temp. wav
elet
no.
−2
0
2
Termination 2
10
20
30
10
20
30
120 140 160
10
20
30
time (kyr B.P.)
10
20
30
−2
0
2
Termination 3
10
20
30
10
20
30
220 240 260
10
20
30
time (kyr B.P.)
10
20
30
−2
0
2
Termination 4
10
20
30
10
20
30
320 340 360
10
20
30
time (kyr B.P.)
10
20
30
The timings of the ice-age terminations detected in the
Shackleton data by the antisymmetric wavelet analysis.
Lags are calculated relative to the centres of the air temperature ranges. Mb
(Ma) show the average of Terminations T1,T2,T3b (T3a) and T4, assumingthe central values of the T1 and T3 ranges.
Air temp. Deep ocean temp. Carbon dioxide Sea level
time lag time lag time lag time lag timescale scale scale scale
(kyr (kyr) (kyr) (kyr) (kyr) (kyr) (kyr) (kyr) (kyr)BP)
T1 17-18 0 30-55 1.5–5.5 40-60 0.5–1.5 40–60 4.5–6.5 20–35T2 140 0 30 -6 50 0 45 7 20T3a 249-254 0 30-20 0.5 20 1.5 35 7.5 15T3b 0 15.5 55T4 342 0 25 -7 40 -1 35 6 20
Ma 0 30 -2 40 0 35 7 20Mb 0 9 30
Summary of time series analysis 1
The ice-age cycles differ greatly in character from the Milankovitch
driven 23ka and 41ka signals
• They are non-identical and asymmetrical.
• The Morlet wavelet analysis of the carbon dioxide record
showed no clear indication of signal at the 23ka and 41ka
periods, however these frequencies appear in air temp and
ice volume.
• There is a strong signal in all data sets close to 100ka fre-
quency – less significant in the sea-level data.
Summary of time series analysis 2 - results from the antisym-
metric wavelet
• The change in sea-level lags ocean temperature, carbon diox-
ide and air temperature changes by about 7 ka. Within the
accuracy of our results, the other three components are all
approximately co-incident.
• Neither T3 nor T6 fit the description of a termination, since
rather than one large, fast change they consist of a series of
smaller changes over a range of different timescales.
Data Assimilation - combining data with models
Various simple models have been used to study climate change
over the timescales of the Glacial Cycles. These models are run
for 100 ka to 1 Ma, and are typically computationally cheap.
For such models a computationally expensive method such as
the Monte Carlo Markov Chain can be implemented.
In recent years, intermediate complexity GCMs have been being
developed, which aim to run a spatial representation of the full
earth system for of the order of 100 ka. A more efficient data
assimilation technique is required, such as the ensemble Kalman
Filter.
State-of-the art high resolution GCMs are used for snap shot
experiments.
Monte Carlo Markov Chain and a simple Earth System Model
• Model - Three equation model of the sea level, ocean tem-
perature and CO2 concentration of the last 400ka
• Data - Time series data of sea level, deep ocean temperature
and atmospheric CO2 concentration over the last 400ka.
• Parameter estimation - 9 parameters estimated simultane-
ously
• The resulting ensemble spans the range of uncertainty.
• Method produces a prediction of the timing of the next ice
age.
Model Results
-500 -250 0 250Date (ka)
-1
Ocean 0
1
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CO2 0
1
-1
Ice 0
1
-1
Sun 0
1
Run with 500 ka of data assimilated. The vertical magenta line shows when assimilation was
halted. The red line at the top is the solar insolation forcing. The green dashed lines are the
results from using the untuned parameters. The black dot-dashed lines are the data. The
dark blue lines show the mean of the ensemble and the light blue lines show the one standard
deviations of the ensemble.
Ensemble Kalman Filter and an Intermediate Complexity Model
• Model - GENIE intermediate complexity AOGCM.
• Data - Spatial climatology of ocean temperature, salinity,
atmospheric temperature, humidity.
• Parameter estimation - 12 parameters estimated simultane-
ously
• The resulting ensemble spans the range of uncertainty of the
climate.
• Can be used to make probabilstic estimates of climate change.
• For this initial experiment, present day climatology was used.
THC Collapse, Recovery, Hysteresis
0
5
10
15
20
Max
. Atla
ntic
Ove
rtur
ning
(S
v)
0 2 4 6 8 10 120
500
1000
Atm
os. C
O2
Time (ka)
Conclusions and Future Work
Analysing data in a complete way is important, particularly on
paleoclimate timescales when relatively few data are available.
From this analysis we have calculated the relative leads and lags
between different components of the earth system at the ice-age
terminations. The different terminations vary somewhat, but the
changes in ice mass consistently lag the other components by
about 7ka.
For climatological estimation using models, lack of knowledge in
the parameters is a much larger cause of uncertainty than the
initial conditions. I have described some assimilation techniques,
based on variation on the parameters, which make optimal use
of the data and produce probabilistic ensembles.
In the future we plan to apply the EnKF to intermediate com-
plexity Earth System Models of paleoclimate states. Use of the
MCMC in other computationally cheap paleoclimate models is
also underway.