Paleozoic terranes of eastern Australia and the drift history of Gondwana Michael W. McElhinny * , Chris McA. Powell, Sergei A. Pisarevsky Tectonics Special Research Centre, The University of Western Australia, Crawley, Western Australia 6009, Australia Received 16 November 2000; received in revised form 7 July 2001; accepted 10 July 2001 Abstract Critical assessment of Paleozoic paleomagnetic results from Australia shows that paleopoles from locations on the main craton and in the various terranes of the Tasman Fold Belt of eastern Australia follow the same path since 400 Ma for the Lachlan and Thomson superterranes, but not until 250 Ma or younger for the New England superterrane. Most of the paleopoles from the Tasman Fold Belt are derived from the Lolworth-Ravenswood terrane of the Thomson superterrane and the Molong- Monaro terrane of the Lachlan superterrane. Consideration of the paleomagnetic data and geological constraints suggests that these terranes were amalgamated with cratonic Australia by the late Early Devonian. The Lolworth-Ravenswood terrane is interpreted to have undergone a 90j clockwise rotation between 425 and 380 Ma. Although the Tamworth terrane of the western New England superterrane is thought to have amalgamated with the Lachlan superterrane by the Late Carboniferous, geological syntheses suggest that movements between these regions may have persisted until the Middle Triassic. This view is supported by the available paleomagnetic data. With these constraints, an apparent polar wander path for Gondwana during the Paleozoic has been constructed after review of the Gondwana paleomagnetic data. The drift history of Gondwana with respect to Laurentia and Baltica during the Paleozoic is shown in a series of paleogeographic maps. D 2002 Elsevier Science B.V. All rights reserved. Keywords: Paleozoic; Paleomagnetism; Australia; Gondwana; Tasman Fold Belt 1. Introduction The apparent polar wander path (APWP) for Gondwana during the Paleozoic has been the subject of much debate for more than 25 years because many of the paleomagnetic poles for the Silurian and Devonian are derived from the Tasman Fold Belt of eastern Australia. It has been argued (e.g. Van der Voo, 1993) that some of the crucial data are derived from suspect terranes and therefore cannot be used with any certainty in deriving the APWP for cratonic Australia. Fig. 1 provides a brief history of the development of the Paleozoic APWP for Gondwana. The APWP in each case is plotted in NW Africa coordinates. It was originally believed that the Cam- brian and Ordovician (south) poles plotted in the region of northwest Africa and that the pole path moved rapidly to southern Africa by the Early Devon- ian (e.g. McElhinny, 1973). With the advent of plate tectonics, the interpretation of the geology of the 0040-1951/02/$ - see front matter D 2002 Elsevier Science B.V. All rights reserved. doi:10.1016/S0040-1951(02)00630-3 * Corresponding author. Permanent address: Gondwana Con- sultants, 31 Laguna Place, Port Macquarie, New South Wales 2444, Australia. Fax: +61-2-6584-6483. E-mail address: [email protected](M.W. McElhinny). www.elsevier.com/locate/tecto Tectonophysics 362 (2003) 41– 65
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Paleozoic terranes of eastern Australia and
the drift history of Gondwana
Michael W. McElhinny*, Chris McA. Powell, Sergei A. Pisarevsky
Tectonics Special Research Centre, The University of Western Australia, Crawley, Western Australia 6009, Australia
Received 16 November 2000; received in revised form 7 July 2001; accepted 10 July 2001
Abstract
Critical assessment of Paleozoic paleomagnetic results from Australia shows that paleopoles from locations on the main
craton and in the various terranes of the Tasman Fold Belt of eastern Australia follow the same path since 400 Ma for the
Lachlan and Thomson superterranes, but not until 250 Ma or younger for the New England superterrane. Most of the paleopoles
from the Tasman Fold Belt are derived from the Lolworth-Ravenswood terrane of the Thomson superterrane and the Molong-
Monaro terrane of the Lachlan superterrane. Consideration of the paleomagnetic data and geological constraints suggests that
these terranes were amalgamated with cratonic Australia by the late Early Devonian. The Lolworth-Ravenswood terrane is
interpreted to have undergone a 90j clockwise rotation between 425 and 380 Ma. Although the Tamworth terrane of the
western New England superterrane is thought to have amalgamated with the Lachlan superterrane by the Late Carboniferous,
geological syntheses suggest that movements between these regions may have persisted until the Middle Triassic. This view is
supported by the available paleomagnetic data. With these constraints, an apparent polar wander path for Gondwana during the
Paleozoic has been constructed after review of the Gondwana paleomagnetic data. The drift history of Gondwana with respect
to Laurentia and Baltica during the Paleozoic is shown in a series of paleogeographic maps.
D 2002 Elsevier Science B.V. All rights reserved.
Keywords: Paleozoic; Paleomagnetism; Australia; Gondwana; Tasman Fold Belt
1. Introduction
The apparent polar wander path (APWP) for
Gondwana during the Paleozoic has been the subject
of much debate for more than 25 years because many
of the paleomagnetic poles for the Silurian and
Devonian are derived from the Tasman Fold Belt of
eastern Australia. It has been argued (e.g. Van der
Voo, 1993) that some of the crucial data are derived
from suspect terranes and therefore cannot be used
with any certainty in deriving the APWP for cratonic
Australia. Fig. 1 provides a brief history of the
development of the Paleozoic APWP for Gondwana.
The APWP in each case is plotted in NW Africa
coordinates. It was originally believed that the Cam-
brian and Ordovician (south) poles plotted in the
region of northwest Africa and that the pole path
moved rapidly to southern Africa by the Early Devon-
ian (e.g. McElhinny, 1973). With the advent of plate
tectonics, the interpretation of the geology of the
0040-1951/02/$ - see front matter D 2002 Elsevier Science B.V. All rights reserved.
N is the number of sites in each study. The Q index follows Van der Voo (1990). Refno and Resultno are the Reference number and Result
number in the Global Paleomagnetic Database (GPMDB) Ver. 4.1 (May 2001) following McElhinny and Lock (1996). Ages follow the
timescale given in the GPMDB—Harland et al. (1990) as modified by Tucker and McKerrow (1995) for the Early Paleozoic.a Rotated from 19.4jN, 208.9jE as explained in the text.b Counterclockwise vertical axis rotation of 90j applied as discussed in the text.
M.W. McElhinny et al. / Tectonophysics 362 (2003) 41–65 49
The paleomagnetic south poles plotted in Fig. 3
cover the time interval from Cambrian to Early
Devonian (545–400 Ma). Groups of poles have been
ringed and a mean age for each group is indicated.
The pole for the Antrim Plateau Basalts (APB) plots
off the diagram to the west, but its age is probably
Early Cambrian (535 Ma group). The age of the
Tumblagooda Sandstone (TS) of Western Australia
is known only within rather broad limits and is
generally regarded as being of Ordovician age,
although stratigraphically the range could include
the Middle Cambrian and Early Silurian. The TS pole
plots with other Ordovician poles in Fig. 3. The pole
(CNF) from the Chatswood Limestone and Ninmaroo
Formation of the Georgina Basin (Ripperdan and
Kirschvink, 1992) does not plot near other poles
corresponding to the Cambrian/Ordovician boundary.
Either these rocks have been remagnetized, in which
case the magnetostratigraphy deduced is incorrect, or
this region has been subjected to some unknown
tectonic effects.
When assigning a Quality Index to results from the
Adelaide Fold Belt of South Australia, we have fol-
lowed the rather conservative view taken by Van der
Voo (1993) that coherence with the main craton is not
necessarily guaranteed during the early Paleozoic. In
Fig. 3, the results from South Australia have been
separately identified from those from the craton and the
agreement of these results within the 510 and 485 Ma
groups confirms that this region has been firmly
attached to the craton at least since the Early Cambrian.
Two results (RB and MLS) from the Silurian (425
Ma) of the Lolworth-Ravenswood terrane (Clark,
1996) plot off north Arabia and lie close to the pole
from the Mereenie Sandstone (MS) of central Aus-
tralia (Li et al., 1991). The age of the Mereenie
Sandstone is only constrained to lie between Late
Ordovician and Early Devonian and is therefore
usually regarded as being of Silurian age. The close
proximity of the MS pole to the Silurian poles (RB
and MLS) from the Lolworth-Ravenswood terrane
would appear to confirm the Silurian age of the
Mereenie Sandstone. However, the Early Devonian
pole (MLD) from the Lolworth-Ravenswood terrane
lies to the south of Africa and South America in close
agreement with that from the Snowy River Volcanics
(SRV) from the Molong-Monaro terrane. This agree-
ment is either coincidental or else strongly suggests
that the Molong-Monaro and Lolworth-Ravenswood
terranes were coherent in Early Devonian times and
hence also coherent with the main craton at that time.
This implies a polar shift of 120j for the Lolworth-
Ravenswood terrane between 425 and 400 Ma, similar
to that shown for Gondwana in Fig. 1d. Generally
speaking, large polar shifts for small terranes are
usually associated with rotations. Switching the polar-
ity of the older age poles would reduce this to 60j as
in Fig. 1e. However, the paleogeographic consequen-
ces of switching the polarity of the Cambrian and
Ordovician poles are unacceptable. We note that the
results from the Mereenie Sandstone of Li et al.
(1991) are not well grouped with the Fisher precision
k = 7.8 after structural correction. Indeed, the six site
mean declinations range from 252j to 322j, stronglysuggesting local rotations or poorly determined mag-
netic directions may be involved. The authors show
that the six sites means could well be divided into two
significantly separate groups each with three sites
stratigraphically separated from one another. There-
fore, we are not confident that the pole from the
Mereenie Sandstone is truly representative of the
Silurian of Australia.
The most reasonable explanation of the observed
120j polar shift is that the Lolworth-Ravenswood
terrane was not attached to the main craton in its
present orientation at 425 Ma as was discussed
previously. In the Lolworth-Ravenswood terrane
(location 20.1jS, 146.4jE), the combined Silurian
(425 Ma) observed direction of magnetization for
the Ravenswood Batholith and the Mt. Leyshon
Silurian dykes is D = 286.5j, I=� 19.1j with a95 =4.1j. Correcting for the 90j local clockwise rotation
that is proposed to have occurred between f 425 and
380 Ma gives an in situ direction of magnetization of
D = 196.5j, I =� 19.1j. The corresponding pole posi-
tion then lies at 56.0jN, 176.4jE. At the present time
we believe this represents the best estimate of the
Silurian (425 Ma) pole for Australia. Since the Early
Devonian (400 Ma) pole from the Lolworth-Ravens-
wood terrane agrees with that from the Snowy River
Volcanics of the Molong-Monaro terrane 2000 km to
the south, it appears that the 90j clockwise rotation of
the Lolworth-Ravenswood terrane could have taken
place between 425 and 400 Ma.
We now consider the pre-400 Ma results from the
Molong-Monaro terrane, which are plotted in Fig. 3.
M.W. McElhinny et al. / Tectonophysics 362 (2003) 41–6550
These results are mainly based upon those reported by
Goleby (1980) and have been critically assessed by
Schmidt and Embleton (1987) as being unsuitable for
paleogeographic analysis. However, we have assigned
Q indices to these results and they all give Qz 3, so
until further work is carried out on these rocks, we
feel it is unreasonable to reject them arbitrarily. Bear-
ing these comments in mind, we make the following
general observations. The Early (WMP-482 Ma)
Ordovician result does not agree with the correspond-
ing group of poles from the craton. However, the
proximity of this pole position to the equivalents from
the craton suggests that the Molong-Monaro terrane
was located close to the Gondwanan cratonic margin
during the Ordovician and subsequently rotated into
its present position on amalgamation. The Silurian
results are strung out between the Ordovician (485
Ma) and the Early Devonian (400 Ma) results.
Although it is unlikely that the Molong-Monaro
terrane was amalgamated with the craton during this
time interval and, considering the uncertainties sug-
gested for the pre-400 Ma data, there is general
support for the view that the terrane lay close to the
craton as suggested by the geological observations
discussed previously. In all cases the deviations from
the cratonic poles can be explained by local rotations.
4. Late Paleozoic paleomagnetic data from
Australia
Results from the Devonian and Carboniferous of
the main craton and the Tasman Fold Belt are shown in
Fig. 4. The pole positions are plotted on a Gondwana
reconstruction but in Australian coordinates so that the
poles listed in Table 1 are more easily identified. The
oldest poles from central Australia (main craton), as
shown in Fig. 4a, are derived from a stratigraphic
succession in the Amadeus Basin and in sequence
from oldest to youngest are Parke Siltstone (PS—early
Middle Devonian), Hermannsburg Sandstone (HS—
late Middle to early Late Devonian) and the Brewer
Conglomerate (BCG—Famennian). This sequence
produces a series of poles that runs from the region
of southern Africa to central Africa. Placed within
this sequence in the appropriate place are poles from
the Canning Basin Reef Complexes in Western Aus-
tralia (CB1 and CB2—Late Frasnian to Early Famen-
nian). This sequence of poles from the craton ends
with the Early Carboniferous Mount Eclipse Sand-
stone (MES—Early to mid-Visean). This succession
of poles must be compared with a similar succession
derived from the Molong-Monaro terrane, including
the Comerong Volcanics (CV—Givetian/Frasnian
boundary), Worange Point Formation (WP—Famen-
nian) and the Hervey Group (HG—Famennian) that
form a similar sequence.
For the Early Devonian the pole from the Snowy
River Volcanics agrees with that from the Mt. Ley-
shon Devonian dykes of the Lolworth-Ravenswood
terrane in northeast Queensland. Therefore the evi-
dence is overwhelming that the paths for the main
craton and the Molong-Monaro terrane coincide since
at least Early Devonian times. This is entirely con-
sistent with the geological evidence presented earlier.
For times earlier than the Early Devonian, the poles
from the Molong-Monaro terrane are different from
the main craton in the Ordovician, and there is no
reliable data for the craton in the Silurian with which
they can be compared (Fig. 3). The implied pole path
for the Molong-Monaro terrane, however, does follow
the likely APWP for Gondwana, implying that during
the Late Ordovician to Early Devonian, the terrane
was near the Australian Gondwanan margin (Fig. 4b).
The poles from the Tamworth terrane of the New
England Fold Belt (Table 1) tend to support the
overall geological view that extensive movements
between the Tamworth terrane and the Lachlan Fold
Belt may have persisted at least until the end of the
Permian. Recent paleomagnetic results confirm this
view (Geeve et al., 2002). The Tamworth terrane is
currently the subject of substantial paleomagnetic
investigation, so we will not discuss these results in
detail here. However, of particular interest is the major
study of the basal sequence of the Kiaman Superchron
published by Opdyke et al. (2000) from the Rocky
Creek and Werrie synclines as listed in Table 1. Poles
from the Rocky Creek syncline (LHF, RCC, CLF) lie
to the east of poles of corresponding age shown in
Fig. 4b. However, the pole from the Werrie syncline
(CUF) is more westerly. This difference becomes
more apparent when compared with poles of similar
age from Gondwana (see Table 3 below). The best
estimate of the Gondwana pole for 310 Ma can be
found by interpolating between the mean poles listed
for 300 and 320 Ma. This gives a Gondwana pole
M.W. McElhinny et al. / Tectonophysics 362 (2003) 41–65 51
Fig. 4. Paleozoic paleomagnetic (south) poles for Australia plotted on a reconstruction of Gondwana in Australian coordinates. (a) Poles ranging
from 400 to 300 Ma. The solid line is the derived APWP. (b) Derived APWP from (a) compared with pre-400 Ma poles from the Molong-
Monaro terrane.
M.W. McElhinny et al. / Tectonophysics 362 (2003) 41–6552
lying at 25jN, 240jE in NWAfrica coordinates or at
45.6jN, 297.3jE in Australian coordinates. This pole
(south pole at 45.6jS, 117.3jE) lies significantly to
the west of the Rocky Creek syncline poles obtained
by Opdyke et al. (2000), as Fig. 4 shows. The pole for
the Werrie syncline lies more westerly, as might be
expected for results of this age from the main craton
and is not significantly different to that expected for
Gondwana as calculated above. Indeed, the mean
directions of magnetization listed by Opdyke et al.
(2000) for the Rocky Creek and Werrie synclines
differ by 9.6j and are significantly different at the
95% confidence level (critical angle is 6.1j). We
have no simple explanation for these differences,
except to observe that extensive movements between
the Tamworth terrane and the Lachlan Fold Belt
(Geeve et al., 2002) may have persisted up until
the Middle Triassic. Therefore, we do not consider
any of the results from the Tamworth terrane during
the Carboniferous and Permian to be representative
of cratonic Australia.
5. The Paleozoic apparent polar wander path for
Gondwana
Table 2 summarises all the Paleozoic pole positions
from the Gondwana continents with Quality Index
Qz 3. Each result is referenced by the Refno and
Resultno in the Global Paleomagnetic Database of
McElhinny and Lock (1996) using the latest version
(4.1 of May 2001). As discussed above, for Australia
pre-Devonian results from the Molong-Monaro and
Paleozoic results from the Tamworth terrane as listed
in Table 1 have been omitted. Pole positions are given
in NWAfrica coordinates according to the reconstruc-
tion parameters of Lottes and Rowley (1990). In
addition to these parameters, the Parana Basin and
southern parts of South America have been rotated
using modified rotations following Nurnberger and
Muller (1991). Tasmania has been rotated to Australia
following Powell et al. (1988). The complete set of
rotations is as follows:
1. Southern Africa to NW Africa: 9.3jN, 5.7jE,angle of � 7.8j.
2. Northeast Africa to NWAfrica: 19.2jN, 352.6jE,angle of � 6.3j.
3. Arabia to NW Africa: 26.2jN, 11.2jE, angle of
� 14.2j.4. South America (north of Parana Basin) to NW
Africa: 53jN, 325jE, angle of + 51.0j.5. Parana Basin subplate to South America: 9.6jS,
300.6jE, angle of + 4.1j.6. To NWAfrica: 48.8jN, 324.9jE, angle of + 52.8j.7. Colorado subplate to South America: 7.4jN,
299.6jE, angle of + 4.6j.8. To NWAfrica: 49.2jN, 324.2jE, angle of + 54.0j.9. India to NW Africa: 26.7jN, 37.3jE, angle of
� 69.4j.10. Australia to NW Africa: 28.1jS, 293.2jE, angle
of + 52.1j.11. Tasmania to Australia: 47.0jN, 4.0jE, angle of
+ 3.6j.12. To NWAfrica: 24.1jS, 294.3jE, angle of + 51.7
13. Antarctica to NWAfrica: 12.4jS, 326.2jE, angleof + 53.3j.
14. Madagascar to NW Africa: 14.9jS, 277.6jE,angle of + 15.7j.
It has been suggested that some counterclockwise
rotation of the Salt Range has occurred and that the
Cambrian and Permian results from this region should
not be used in Gondwana reconstructions (Opdyke et
al., 1982). The poles listed in Table 2 have been
grouped in approximately 20 my bands. Our obser-
vation is that the Middle to Late Cambrian (510 Ma)
group and the mid- to Late Permian (260 Ma) group
change very little whether results from the Salt Range
are included or not (both calculations are listed in
Table 2). This suggests that any rotations involved are
small and within the range of the reconstruction errors
in transforming the poles.
Some poles do not agree with those of similar age.
The Talchir Series pole appears to contain an over-
print as suggested by Van der Voo (1993). The pole
from the Gilif Hills Volcanics (primary component C)
appears out of place. The tectonic situation at the
sampling location may be more complex than sup-
posed and we suggest that this result comes from a
possibly rotated block. The result from the Silurian
Lipeon Formation of northwest Argentina does not
agree with those from Australia in either their present-
day or restored position. It is derived from ferruginous
horizons assumed to be diagenetic, and, although
there is a positive fold test, the folding is Late Tertiary
M.W. McElhinny et al. / Tectonophysics 362 (2003) 41–65 53
Table 2
Gondwana (north) paleomagnetic poles in NW Africa coordinates for the Cambrian to Permian (545–250 Ma)
Age N Plat(N) Plong(E) Rockunit Q index Refno Resultno
Means are calculated using the method of McFadden and McElhinny (1995) for combining groups of poles. m is the number of poles; N is total
number of sites; k is the estimate of Fisher (1953) precision; A95 is the radius of circle of 95% confidence about the mean pole position. Ages are
based on the timescale used in the GPMDB (see Table 1).a Mean calculated omitting results from the Salt Range, Pakistan.b Lolworth-Ravenswood terrane, Australia rotated about vertical axis by 90j counterclockwise.
M.W. McElhinny et al. / Tectonophysics 362 (2003) 41–65 57
mation, a Cambro-Ordovician boundary sequence in
the Georgina Basin, Australia, do not agree with their
counterparts from the rest of Gondwana. There may
be some local tectonic effects or later remagnetization
involved.
In the Early/Middle Cambrian (520 Ma mean
pole), the results are from Australia and Antarctica
and seem to form two separate groups from each
continent. Two of the Antarctic poles come from the
Transantarctic Mountains (Grunow and Encarnacion,
2000) whereas the Mirnyy Charnokites clearly come
from the craton. These poles agree well, suggesting
the results from the Transantarctic Mountains are not
derived from exotic terranes. It is possible that the
differences between the Australian and Antarctic
results in this group may merely reflect age differ-
ences, but the Australian poles are of poor quality and
we are not confident that this mean pole at 520 Ma has
been correctly defined.
Using the groupings from Table 2, mean pole
positions have been calculated using the method of
combining groups of poles of McFadden and McEl-
hinny (1995). The method enables the mean pole
position to be calculated from m pole positions where
the poles are derived from widely different numbers
of sites (N). The advantage of the method is that one
does not have to consider whether each individual
result by itself is sufficient to average out secular
variation and even a single VGP can be included. The
mean pole positions for each group of poles using this
method are listed in Table 3 in NWAfrica coordinates.
It should be noted that the method assumes that the
precision of the site means (Fisher, 1953) for each
pole position is the same and then attempts to calcu-
Fig. 5. Paleozoic (south pole) APWP for Gondwana using the mean poles (solid circles) as listed in Table 3. Ages are given in Ma and circles of
95% confidence are drawn around each mean pole. The 425 Ma pole (open circle) is that derived from the Lolworth-Ravenswood terrane in
eastern Australia after counterclockwise rotation through 90j.
M.W. McElhinny et al. / Tectonophysics 362 (2003) 41–6558
late that precision that would best represent all the site
means from the entire group of poles. Obviously this
assumption is not strictly valid, especially when one is
dealing with a mixture of results derived from vol-
canics on the one hand and sediments on the other. As
a consequence the calculated optimum precision of
the site means in each group tends to be in the range
of 4–10. This then leads to a very conservative
estimate of the polar error based upon the total
number of sites in each group of poles. Although
the group mean poles of Table 3 have been calculated
using all those results with quality index Qz 3, the
means are changed insignificantly if only results with
Qz 4 are included. Therefore we believe that using
Q = 3 as the cut-off point for accepting data is quite
reasonable.
Table 3 gives the mean north paleomagnetic poles
for each time interval, even though it is common to
plot the south pole APWP as shown in Fig. 5 (see also
Fig. 1). There is some difference between this APWP
for the Paleozoic and that shown in Fig. 1d as derived
by McElhinny and McFadden (2000). For this ana-
lysis we have also included data at the Precambrian/
Cambrian boundary and this provides more detail in
the early Paleozoic path. The main difference is the
elimination of the 112j polar shift between 425 and
405 Ma. This was based on the pole position from the
Mereenie Sandstone that we have now excluded. It
should be noted that the age of the Air ring complexes
of Niger, West Africa is now determined as 407F 8
Ma from the mean of the Rb–Sr isochrons determined
from several complexes (Moreau et al., 1994). The
inferred 425 Ma pole for Gondwana is that derived by
rotating the Lolworth-Ravenswood terrane of eastern
Australia 90j back to its likely mid-Silurian position
adjacent to the Georgetown Inlier of the Gondwanan
craton (Fig. 2c). When this pole is rotated to NW
Africa coordinates in the Gondwana reconstruction, it
lies at 15.9jN, 168.4jE (north pole). The correspond-
ing south pole (15.9jS, 348.4jE) is then placed
between the Late Ordovician (455 Ma) and Early
Devonian (405 Ma) poles for Gondwana shown in
Fig. 5. This inferred 425 Ma (Silurian) pole position
places Bolivia and adjacent regions in a near polar
position (f 85j latitude). This is supported by sed-
imentological evidence for Silurian glaciation in Boli-
via at this time (Caputo and Crowell, 1985). The
questionable pole derived from the Mereenie Sand-
stone gives a low-latitude (f 5j) position for Bolivia,inconsistent with the geological information.
6. Paleogeographic implications
The consequences of this revised Gondwana
APWP for the paleogeographic relationships between
Baltica, Gondwana, Laurentia and Siberia are illus-
trated for 10 time slices between 530 and 320 Ma
(Fig. 6). The positions of Baltica and Laurentia are
derived from mean pole positions calculated by
McElhinny and McFadden (2000); Siberia’s position
has been derived from the poles listed by Smethurst et
al. (1998), updated with results from Gallet and
Pavlov (1996), Pavlov and Gallet (1998) and Pisar-
evsky et al. (1997). In constructing the maps, we have
adjusted the positions of the major continental blocks
within the 95% confidence limits of the mean paleo-
magnetic poles to fit geological constraints. The
rotation parameters used for the maps are listed in
Table 4.
The Iapetus Ocean between Laurentia and the
Amazonia margin of Gondwana opened in the latest
Neoproterozoic, between 575 and 550 Ma. The best
estimate of the rift–drift transition on the East Lau-
rentian margin is latest Precambrian (Bond et al.,
1984). Baltica had separated from its Neoproterozoic
position adjacent to East Greenland before ca. 580 Ma
(Torsvik et al., 1996), and Siberia had separated from
northern Laurentia by 530 Ma (Pelechaty, 1996). By
Early Cambrian, Laurentia lay astride the Equator
with Gondwana extending from the South Pole in
northwest Africa to the northern tropics in Australia
(Fig. 6a).
The Iapetus Ocean continued to widen until around
513 Ma, the age of the oldest inferred intra-Iapetus
subduction (Van Staal et al., 1998). Laurentia stayed
near the Equator in the Cambrian and Early Ordovi-
cian. By the Early Ordovician, the South American
margin of Gondwana was converging with Laurentia
(cf. Fig. 6b and c), and Iapetus was closing along both
its Laurentian and NW Gondwanan margins (Van
Staal et al., 1998). Baltica and Siberia remained
separated from Laurentia.
The Precordillera terrane, widely accepted as hav-
ing been derived from the Ouachita embayment in the
southeastern Laurentian continental margin in the
M.W. McElhinny et al. / Tectonophysics 362 (2003) 41–65 59
Fig. 6. Paleogeographic reconstructions at (a) 530 Ma; A=Amazonia, B =Baltica, G =Gondwana, L= Laurentia, S = Siberia, (b) 510 Ma, (c) 485