© 2008 Nature Publishing Group
LETTERS
Evidence for a very-long-term trend in
geomagnetic secular variation
ANDREW J. BIGGIN*, GEERT H. M. A. STRIK AND COR G. LANGEREIS
Palaeomagnetic Laboratory Fort Hoofddijk, Budapestlaan 17, Universiteit Utrecht, Utrecht 3584 CD, Netherlands
*e-mail: biggin@geo.uu.nl
Published online: 4 May 2008; doi:10.1038/ngeo181
The Earth’s inner core is believed to inhibit rapid fluctuations
in the geomagnetic field from developing into full polarity
reversals
1,2
. Consequently, during the Precambrian, the smaller
size of the inner core might suggest that polarity reversals
could occur more readily. It is therefore surprising that there
are indications that reversals were rare during this period
3,4
.
Here we use new and existing palaeomagnetic data from three
continents to examine the stability of the Earth’s magnetic field
from 2.82 to 2.45 billion years ago. We show that, on average,
geomagnetic secular variation (the field variations produced by
normal geodynamo action) during the late Archaean and early
Proterozoic was different from that of the past 200 million years;
specifically, the apparent variability of the geomagnetic pole as
viewed at low and mid-latitudes was reduced relative to the past
200 million years. According to both dynamo simulations
4
and
more recent palaeomagnetic field observations
5
, the observed
pattern of secular variation suggests a lower frequency of
polarity reversals 2.5 billion years ago. This may imply that
the geodynamo is becoming progressively less stable over
long timescales, consistent with some numerical simulations
6,7
,
possibly as a result of changing outer-core geometry that has
accompanied inner-core growth.
Our confidence in claims
3,4
that the geomagnetic field reversed
its polarity less frequently in the Precambrian period (>542 Myr)
than in the Phanerozoic is limited by the lack of long continuous
Precambrian magnetostratigraphic sections. Fortunately, analyses
of geomagnetic palaeosecular variation (PSV)—the record of
ancient secular variation—provide an independent means of
assessing the stability of the geomagnetic field and have the added
advantage that they do not require rocks to form continuous time
series as do magnetostratigraphic studies.
A recent study analysed PSV (ref. 8) in the late Archaean
to earliest Proterozoic and concluded that it was similar to that
of the past 5Myr. The present study focuses on approximately
the same time period (about 2.45–2.82 Gyr), as it is the oldest
for which there is a sufficient (albeit limited) number of suitable
data available. However, our dataset is 3.5 times larger than that
used previously and is more strictly filtered. A detailed discussion
of the differences between the two analyses is given in the
Supplementary Information.
The new and published palaeomagnetic data (87 and 109
site mean directions respectively; see Table 1) we used for this
study were produced from fast-cooled igneous rock units from
three continents that met strict criteria of suitability (see the
Supplementary Information). We are confident that the magnetic
directions used in this study represent the geomagnetic field close
to the time the rocks recording them were formed because they are
associated with positive fold, conglomerate and/or baked contact
tests. Reversal tests were also positive, which suggests that secular
variation was adequately sampled. The PSV analysis was kept
consistent as far as possible with a previous analysis of PSV in the
period 0–5 Myr (ref. 9) (see the Supplementary Information).
Figure 1 plots the angular dispersion of the 2.45–2.82 Gyr
virtual geomagnetic poles (VGPs) against palaeolatitude, calculated
from the inclination of the mean direction assuming that the field
was a geocentric axial dipole. Despite the relatively small numbers
of site mean data (relative to studies focusing on more recent
times), the plotted dispersions are evidently accurate enough to
show a clear relationship with palaeolatitude. Furthermore, Fig. 1
shows that the basic shape of the VGP dispersion curves is extremely
robust with respect to the specific details of how we carried out
our analysis. Figure 1d shows our preferred dataset, which we
consider to be a reliable first-order description of PSV in the late
Archaean–early Proterozoic. This VGP dispersion curve is markedly
different from that produced by the 0–5 Myr dataset (also shown in
Fig. 1), suggesting that the nature of PSV was different in these two
time periods. Specifically, the angular dispersion of VGPs from the
2.45–2.82 Gyr sites at low to mid-palaeolatitudes is lower whereas
the rate of increase in VGP dispersion with palaeolatitude is slightly
higher. The data used to produce the 0–5Myr curve shown in
Fig. 1 are currently being superseded by the Time Averaged Field
Initiative (TAFI) project. These and other recent studies of PSV act
to strengthen the conclusions of the present study, as is discussed in
the Supplementary Information.
The shape of a VGP dispersion curve is dictated by several
factors and is consequently difficult to interpret directly in terms of
physical processes
10
. Nonetheless, although its physical significance
is disputed, Model G (ref. 11) (see the Methods section) has
proved effective at fitting the observed variations in the shapes of
curves for time windows from the past 195 Myr (ref. 5) (Fig. 2a).
Furthermore, the evolution of its shape parameters has been
shown
5
to correspond well to the average geomagnetic polarity
reversal frequency in the particular time window for which the
PSV analysis was carried out (Fig. 2), which suggests a link between
mean PSV and reversal frequency. Therefore, Model G may be
safely used here to describe the shapes of VGP dispersion curves,
regardless of whether interpretations
11
of the physical significance
of these shapes are correct.
The late Archaean–early Proterozoic model has both shape
parameters within errors of the model fit to the Cretaceous
Normal Superchron time window (point 5 in Fig. 2). Consequently,
the empirical relationship shown in Fig. 2b predicts that the
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