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The Slate Islands: A probable complex meteorite impact structure in Lake Superior

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Canadian Journal of Earth Sciences
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Abstract

Shock metamorphic effects in samples from the Slate Islands, Lake Superior (48°40' N, 87°00' W) suggest that the islands are part of a meteorite impact structure. The islands form the central uplift of a complex crater and are ringed by a submerged trough and annular ridge with a diameter of 30 km. Precambrian bedrock units are locally brecciated and cut by allochthonous breccia dikes. These dikes contain clasts of identifiable country rock and also fragments of a sedimentary unit, possibly Upper Keweenawan in age, which is no longer present in outcrop. The orienta tions of shatter-cones present in the breccia host-rocks indicate the interior of the islands as the approximate shock centre. Microscopic planar features, equivalent to those described from other impact sites, occur in quartz and plagioclase and the level of shock deformation increases towards the interior of the islands. The shock event postdates Keweenawan igneous activity (about 1.1 b.y. old) and, on the basis of the erosion level, may be early Paleozoic in age.
The Slate Islands: a probable complex meteorite impact
structure in Lake Superior1
H.
C.
HALLS
Department of Geology, Erindale College, Universiry of Toronto, Mississauga, Ont., Canada
L5L
1C6
AND
R.
A.
F.
GRIEVE
Gravity and Geodynamics Division, Earth Physics Branch, Department of Energy, Mines and Resources, Otlawa, Ont.,
Canada
KIA
OY3
Received
2
March 1976
Revision accepted for publication 3 June 1976
Shock metamorphic effects in samples from the Slate Islands, Lake Superior (48"40' N, 87"OO'
W)
suggest that the islands are part of a meteorite impact structure. The islands form the central
uplift of a complex crater and are ringed by a submerged trough and annular ridge with a diameter
of 30 km. Precambrian bedrock units are locally brecciated and cut by allochthonous breccia
dikes. These dikes contain clasts of identifiable country rock and also fragments of a sedimentary
unit, possibly Upper Keweenawan in age, which is no longer present in outcrop. The orienta-
tions of shatter-cones present in the breccia host-rocks indicate the interior of the islands as the
approximate shock centre. Microscopic planar features, equivalent to those described from other
impact sites, occur in quartz and plagioclase and the level of shock deformation increases towards
the interior of the islands. The shock event postdates Keweenawan igneous activity (about
1.1
b.y. old) and, on the basis of the erosion level, may be early Paleozoic in age.
Les effets de mttamorphisme de choc dans des echantillons de Slate Islands, Lac Superieur
(48"40' N, 8T00'
0)
suggerent que les iles font partie d'une structure d'impact meteoritique. Les
iles forment le point eleve d'un cratere complexe et sont entourees par une fosse submergee et
'
une crkte en forme d'anneau d'un diametre de 30 km. Les roches du Precambrien contiennent par
endroits des zones de breche et sont recoupees par des dykes allochtones de breche. Ces dykes
contiennent des fragments identifiables des roches encaissantes et aussi des fragments d'une
unite sedimentaire, possiblement d'ige Keweenawien superieur qui n'existe plus
a
l'ttat
d'affleurement. Les orientations des c6nes de choc presents dans les breches encaissantes
indiquent I'inttrieur des iles comme point d'impact approximatif. Des petites structures, micro-
scopiques planes semblables
a
celles decrites pour d'autres sites d'impact, se rencontrent dans le
quartz et le plagioclase et le degre de deformation par choc augmente vers I'interieur des iles.
L'impact est posterieur la phase d'activite ignee du Keweenawien (environ
1.1
Ga) et en se
basant sur le niveau d'erosion, il a pu se produire au debut du Paltozoi'que.
[Traduit par le journal]
Can. J.
Earth
Sci.
13,
1301-1309(1976)
Introduction
In this paver we revort additional shatter-cone
A
A
slate ~~l~~d~
are
a coherent, roughly cir- observations and describe other characteristic
cular group
of
two
major and several smaller shock features that provide further evidence that
islands in Lake Superior, 10 km south of Terrace the Slate Islands may have foIXIed as a result of
Bay, Ontario (Fig. 1). The form of the islands
meteorite
impact.
and the surrounding lake bottom, and the report
of "shatter-cone-like" features and breccias by
Sage (1974) prompted the inclusion of the Slate
Islands in a list of possible impact structures in
Canada (Robertson and Grieve 1975). A similar
conclusion was also reached by Halls (1975)
from geological and paleomagnetic studies car-
ried out on the islands since 1973.
I
'Contribution from the Earth Physics Branch No.
606.
Form and General Geology of the Slate Islands
As a group, the Slate Islands have a diameter
of approximately 7 km and rise to elevations of
about 120 m above lake level. Hydrographic
data indicate a submerged trough with water
depths of 200-260 m at a radial distance of 7-8
km (Fig. 1). Between the islands and the main-
land to the north, the trough is partially ob-
scured, presumably due to glacial till or more
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FIG.
1.
Map of the Slate Islands showing surrounding lake bathymetry. The islands form a central
peak with a submerged peripheral trough (water depth
>
200
m) and annular ridge
(.=
100 m depth).
The topographic expression is similar to that of an eroded compkx meteorite crater.
A
and
B
are loca-
tions referred to in text. A
:
Archean diorite intrusion in Lawrence Bay;
B
:
breccia locality on mainland,
1 km north of McKellar Harbour.
recent sedimentation, although local water
depths of 180 m are still recorded.
The trough is surrounded by a discontinuous
annular ridge with relatively shallow water
depths of 60-120 m at a radial distance of 15-16
km. Beyond the ridge, water depths increase to
about 200 m, the average for this part of Lake
Superior. The form of the topography-a central
peak formed by the islands, peripheral trough,
and annular ridge-is that of a complex hyper-
velocity impact crater (Dence 1972) and is similar
to that of several other large impact structures in
Canada (Robertson and Grieve 1975).
The islands are geologically complex. The
principal rock units are Archean felsic to mafic
meta-volcanics and pyroclastics with dioritic
and felsic intrusives (Sage 1974). On the western
shore of Patterson Island (Fig.
I),
these early
units are unconformably overlain by approxi-
mately 20 m of Aphebian black argillite and
taconite of the Animikie Group. The Animikie
in turn appears to be overlain with little dis-
cordance by about 120 m of reversely magnet-
ized, Lower Keweenawan basalt flows and minor
sandstone, which are correlative with the Osler
Volcanic Group exposed on the mainland to the
west (Halls 1975). On the Slate Islands, the vol-
canic~ have a general dip of 30-40"
W
into the
lake, although dips of up to 70' occur locally
toward the base of the sequence. Numerous east-
trending diabase dikes, presumably feeders for
the Keweenawan flows, cut across the islands,
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HALLS
AND
GRIEVE
1303
but appear to be thicker and more abundant
toward the south.
In places, the bedrock units are highly frac-
tured and locally form autochthonous breccias.
The most striking breccia development is, how-
ever, in the form of cross-cutting polymict alloch-
thonous breccia dikes, which range in width
from a few cm to 50-60 m. They are well dis-
played in shoreline outcrops, particularly around
Patterson Island, and are stratigraphically the
youngest rocks exposed on the islands.
I
Shock Deformation Features: General Aspects
Twenty-two circular structures exhibiting a
class of deformation known as shock metamor-
phism have previously been identified in Canada
(Robertson and Grieve 1975; Caty
et al.
1976).
Shock deformation features are distinct from
those formed in normal tectonic or volcanic en-
vironments and in static loading experiments
(Carter 1971). They have been reproduced in
nuclear explosions and in numerous dynamic
loading experiments, and apparently require
transient pressures of 2-60 GPa (1 GPa
=
10
kbar), with accompanying strain rates of the
order of 1x per microsecond for their formation
(Borg 1972; Stoffler 1972). Shock-metamorphic
effects have not been observed in rocks known
to be genetically linked to explosive volcanism,
but are displayed in many meteorites and lunar
samples, and in the ejecta of young terrestrial
hypervelocity impact sites that contain meteorite
fragments or Fe-Ni spherules. This evidence has
led to the general acceptance of shock-metamor-
phic features in association with a circular struc-
ture as indicating the site of a hypervelocity col-
lision of a large cosmic body with the earth's
surface. Reviews of shock metamorphism and
its implications are given by French and Short
(1968), Horz (1971), and Stoffler (1972, 1974).
On the Slate Islands, various shock metamorphic
features have been recognized and are described
below.
Megascopic Deformation Features
Shatter-Cones
Shatter-cones have been produced in nuclear
explosions (Bunch and Quaide 1968) and in
laboratory shock experiments (Shoemaker
et al.
1961). They are formed by the interaction of a
shock wave with inhomogeneities in the rock at
pressures in excess of the Hugoniot elastic limit
(Johnson and Talbot 1964), which in the case of
non-porous silicate rocks is of the order of 4.0-
9.0 GPa (Ahrens and Gregson 1964). Accord-
ingly, shatter-cones, which have been identified
at approximately 30 terrestrial impact structures,
are generally regarded as an indicator of rela-
tively low-grade shock metamorphism (Dietz
1968; Short and Bunch 1968; Robertson and
Mason 1975).
On the Slate Islands, shatter-cones are present
in the autochthonous bedrock units and in clasts,
but not the matrix, of the allochthonous brec-
cias. Cone segments up to 30 cm in axial length
are common in the Keweenawan volcanics (Figs.
2a,b) and have a preferred eastward apical direc-
tion (Sage 1974). Similar-sized cones are ob-
served occasionally in the interiors of Keweena-
wan diabase dikes and also in an Archean diorite
intrusion exposed along Lawrence Bay on the
north side of Patterson Island (location A in Fig.
1). Smaller shatter-cones (less than 10 cm in
length) occur abundantly in Animikie argillite.
They show finer detail than in the coarser-
grained basalts and diorites, and have well devel-
oped parasitic cones, with splitting of individual
striations to form distinct horsetails (Fig. 2c).
Similar cones are found in comparatively fine
grained rocks elsewhere on the islands: in
Archean tuffaceom(?) units along the east coast
of Patterson Island, in Archean greenstones on
the south side of Mortimer Island, and in chilled
margins of the Keweenawan dikes.
In many of the more strongly cleaved and
fractured Archean rocks, cones are relatively
rare and occur as apparently isolated fractures
with curved striations (Fig. 2d), or as a her-
ringbone pattern formed on roughly planar inter-
faces by juxtaposed cone segments with common
orientation. These features result from pre-im-
pact structures within the rocks, which behaved
as open interfaces during passage of the shock
wave. Shatter-coning was initiated along these
interfaces and the formation of symmetrical,
fully developed cones, retarded. As a result,
along the south and east shores of Patterson
Island, where the Archean rocks
are
strongly
ma-
foliated and thus not conducive to cone
h-..
tion, Keweenawan diabase dikes often provided
the only source of well developed partial cones.
A full analysis of the shatter-cone orientations
such as that described by Manton (1965) for the
Vredefort Dome is yet to be completed. How-
ever, the azimuth of the 'direction of point' was
measured for a number of partial cone segments
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at three localities where they are exposed on ap-
proximately horizontal surfaces. These cones
exhibit horsetail striations and occurred either as
joint-controlled corrugated sheets or formed
surfaces that were not obviously part of a pre-
existing joint pattern. These data, together with
the determination of Sage (1974), show that the
shatter-cones point radially inwards and have a
reasonably coherent intersection (Fig.
3).
The
geological complexity of the Slate Islands largely
pre-empts any attempt to restore the rocks to
their possible pre-impact attitude. However, the
upward sequence Archean, Animikie, Keweena-
wan observed on the west side of Patterson
Island, and the uniform sub-vertical attitude of
diabase dikes throughout the islands, suggest
that no overturning of the rocks as a result of
impact has occurred. Therefore, since shatter-
cone axes are parallel to the local path of the
shock wave (Johnson and Talbot 1964) the
azimuth data indicate the middle of Patterson
Island as lying on the vertical projection of the
shock wave origin.
Breccias
Both the allochthonous and autochthonous
breccias are clastic down to the limit of optical
resolution. Clastic breccias, although extremely
common at impact sites (Short and Bunch 1968),
can be produced by a number of geological
processes and they are not, in themselves, defin-
itive of meteorite impact. However, as described
later, quartz grains in the Slate Island breccias
have microscopic planar dislocation lamellae
characteristic of shock metamorphism, which
suggest that the brecciation is related to a shock
event.
The allochthonous breccias were formed by
injection; they have sharp contacts with the
country rock and many have an obvious dike-
like form (Fig. 2e).
In
places, they form an in-
tersecting network and constitute the matrix of a
country rock megabreccia. They have a highly
variable clast population and their matrix ranges
in colour from brick-red to pale green or buff.
Red-matrix breccias owe their colour to exten-
sive development of hematite and are well ex-
posed along the western shore of Patterson
Island. Individual dike-like bodies contain angu-
lar lithic clasts, ranging up to 5 m in size, of
Archean, Animikie, and Keweenawan rock types
(Fig.
2f).
Many of the smaller, millimetre-sized
clasts are partially recrystallized and planar
shock features in quartz are partially healed.
Several clasts that lack planar features have ir-
regular contorted outlines with devitrification
textures. or are converted to sheet silicate. These
clasts may represent diaplectic mineral or rock
glasses produced during the shock event, which
have subsequently altered and/or devitrified.
Pale green to buff breccias are well developed
on the southern and eastern shores of Patterson
Island. Besides fragments of Keweenawan igne-
ous rocks and assorted Archean lithologies,
breccias on the south shore carry numerous
clasts of a pale green, buff, or purple, well bedded
siltstone and brown or purple arkosic sand-
stone. These clasts are lithologically unlike ex-
posed Animikie and Keweenawan interflow
sedimentary units, but resemble the Upper
Keweenawan Freda Formation. The nearest
exposures of this formation are in northern
Michigan, about 150-200 km to the southwest.
There is, however, good geological and geophys-
ical evidence that Upper Keweenawan sedimen-
tary rocks underlie most of Lake Superior,
including that part in the vicinity of the Slate
Islands (Halls 1966, 1972; Hinze
et
al.
1966;
Halls and West 1971; Dell 1975). If these rocks
once covered the area presently occupied by the
islands, the existence of Freda fragments at a
lower erosional level than the parent formation
could indicate that the breccia was injected in a
downward direction.
A small breccia outcrop containing meta-vol-
canic, quartzite and arkosic sandstone clasts oc-
curs on the mainland east of Jackfish Bay (loca-
tion B in
Fig.
l).
Examination of several samples
FIG.
2.
Megascopic deformation features found on the Slate Islands. (a) Shatter-cone in Keweena-
wan basalt flow.
(b)
Typical shatter-coned outcrop of Keweenawan basalt, showing horsetail features.
(c) Well developed shatter-coned surface in clast of Animikie argillite from allochthonous breccia.
Width of field of view is
5
cm. (d) Shatter-coned surface of Archean felsic metavolcanic. Cones are
poorly developed and appear only as curved striations. Width of field of view is
10
cm. (e) Dike-like,
allochthonous, red-matrix breccia with few clasts, cutting Archean country rock. (f) Allochthonous
red-matrix breccia with numerous angular country rock fragments. Largest clast is approximately
2
m
in maximum dimension.
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1305
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O
I2
Jim
FIG.
3.
'Direction of point' of shatter cones in the
field. Their intersection approximates present location
of the shock centre. Data from the western shore of Pat-
terson Island taken from Sage
(1974).
Remaining data are
averages and ranges of at least
10
separate cone measure-
ments per site. Solid dots show other shatter cone local-
ities where adequate directional data could not be ob-
tained, owing to poor preservation and infrequency of
shatter cone occurrence.
failed to yield evidence of shock deformation.
The outcrop is 30 km from the Slate Islands and
is beyond the limits of the complex crater de-
fined on bathymetric data. Thus, its relationship,
if any, with the Slate Islands event remains an
open question.
Microscopic Deformation Features
Quartz
Planar features, multiple sets of microscopic
lamellae, form in quartz at low to moderate shock
pressures of 7.5-30 GPa and are widely recog-
nized as a microscopic shock metamorphic de-
formation effect (Carter 1968; Robertson et al.
1968
;
Engelhardt and Bertsch 1969; Stoffler
1972). Planar features, or shock lamellae, ident-
ical in form and Orientation to those described
from other impact sites were recognized in all but
two quartz-bearing samples collected from Slate
Islands breccias and host rocks. In general the
planar features are 'decorated' with minute in-
clusions. At their weakest development, on the
western shore of Patterson Island, they occur
only in some grains, and no grain has more than
one set (Fig. 4a). Inland, virtually all quartz
grains have lamellae, with some having as many
as
6
or
7
distinct sets (Fig. 4b).
The initial development and abundance of
planar features with specific crystallographic
orientations characterize different levels of shock
deformation. Orientations of the planar features
were measured on the universal stage, and fol-
lowing the classification of Robertson et al.
(1968), four levels of shock deformation were
recognized in quartz grains in samples from the
Slate Islands. In terms of increasing shock de-
formation, they are: type A, with one set of
planar features parallel to c {0001)
;
type B, with
sets parallel to
o
(1013) and usually c; type C,
with sets parallel to
o,
(22411, and usually
c;
and Type D, with sets parallel to
o,
n{lOi2), and
usually (2231). Additional orientations, for
example {1011), were observed and occurred in
quartz with C or D type deformation. Figure
5
shows frequency plots of the angle between the
c-axis and the pole to plane of the shock lamellae
typical of the various deformation levels re-
corded in quartz from two Slate Island samples.
Orientations and the number of sets of planar
features per grain have been measured in 20
grains in each of 14 country rock samples, and
an average recorded shock pressure for each
sample has been estimated (see Grieve and
Robertson 1976 for details). Recorded shock
pressures range from about 6 to 15 GPa (60-1 50
kbar), and generally increase toward the shock
centre deduced from the shatter-cone orienta-
tions in Fig. 3.
Plagioclase
As with quartz, low to moderate shock pres-
sures produce multiple sets of deformation
lamellae in plagioclase, parallel to low-index
crystallographic planes (Stoffler 1967; Robertson
et
al. 1968; Dworak 1969). The lamellae form at
pressures above approximately 15 GPa (Stoffler
1972, fig. 16). Although their orientation does
not seem to characterize different shock levels,
lamellae formed at higher pressures (>20 GPa)
are twin-like and have measurable widths. On
the Slate Islands, shock lamellae in plagioclase
were only observed in samples with quartz planar
features indicative of the higher (C-D) levels.
They were weak, had no measurable width, and
were present in only some grains (Fig.
4c).
Maskelynite, a dense diaplectic plagioclase
glass, the transformation to which is complete at
shock pressures above 30 GPa (Stoffler and
Hornemann 1972; Gibbons
et
al. 1975), was
identified in a diabase clast from a buff breccia
on the southern shore of Patterson Island. Other
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HALLS
AND
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1307
FIG.
4.
Microscopic deformation features found on the Slate Islands. (a) Type A quartz from western
shore of Patterson Island, with few basal planar features. (b) Type
D
quartz,
1.5
km inland from type
A, with numerous planar features belonging to several sets. (c) Shock lamellae in altered plagioclase
phenocryst from an Archean felsic metavolcanic. (d) Intense microtwinning in calcite from an amyg-
dule in a Keweenawan basalt flow. Quartz from approximately the same location shows only type A
or no obvious shock deformation.
clasts, believed to have been shock-deformed to
maskelynite, are either devitrified or altered to
microcrystalline sheet silicates.
Calcite
A unique style of shock deformation has yet to
be identified in calcite. However, twinning along
e
(0112) and
r
{lOTl), common in statically
deformed calcite, is intensely developed under
shock-deformation conditions (Roddy 1968;
Robertson and Mason 1975). In the Slate Islands
samples, universal stage measurements revealed
up to 9 sets of polysynthetic twins, with predomi-
nant
e
and
r
orientations, within single calcite
grains (Fig. 4d). Microtwinning is common along
{0221), and several unindexed orientations at
high angles to the basal plane were also observed.
Intense calcite microtwinning is present in rocks
which lack obvious shock features in quartz, and
it is, therefore, regarded as a lower-grade de-
formational feature than planar features in tecto-
silicates. This is in keeping with the lower
Hugoniot elastic limit of calcite with respect to
quartz and feldspar (Ahrens and Gregson 1964).
Summary and Conclusions
The occurrence of shatter-cones, characteristic
mineral deformation features, and maskelynite
indicates that rocks on the Slate Islands have
been subjected to a shock event. Shatter-cone
orientation data further suggest that the shock-
wave origin is centrally located within the Slate
Islands, an observation that is consistent with
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J. EARTH
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0
3
C
4
+
4
C
+
SL-75-28:
20
grains
37
sets
L
10
20 30 40 50
60
70 80
90
c
-
axis
Al
planes ,degrees
63
sets
c
-
axis
A1
planes ,degrees
FIG.
5.
Frequency plot of planar feature orientations
in
20
quartz grains from two Slate Islands samples. Sam-
ple
SL-75-28
exhibits basal
{OW1
}
features (type A), and
o
{10i3}
features (type
B).
Sample
SL-75-24
has more
sets of planar features and has a generaIly higher recorded
shock level with development of
o
features,
{2241}
fea-
tures (type
C),
and
n
{10i2}
features (type
D);
other
orientations were recorded, for example
{I071
},
but no
grains have basal
(0001
} features.
the spatial variation of shock deformation esti-
mated from the development of planar features
in quartz.
The shock effects, particularly the microscopic
deformation features in quartz and feldspar, are
equivalent to those described from terrestrial
meteorite craters, nuclear explosion events, and
hypervelocity impact experiments. The estimated
recorded shock pressures range from 4 to greater
than
15
GPa (40 to
>
150 kbar) and are con-
siderably higher than peak values of 0.15-0.3
GPa (1.5-3 kbar) calculated for pressures im-
mediately prior to the most energetic volcanic
explosions (Gorshkov 1959). It is concluded,
therefore, that the shock event is due to meteorite
impact and the Slate Islands represent the central
uplift of a complex hypervelocity crater. The
chaotic geology of the islands, with intense brec-
cia development, together with an associated,
rapidly acquired remanent magnetization (Halls
1975, 1976), is further evidence of a sudden cata-
strophic event, although these features are not in
themselves definitive of meteorite impact.
The age of the shock event is presently un-
known. However, radiometric age-dating of the
most highly shocked samples is currently under-
way. The event must be younger than about 1.1
b.y. because the breccia dikes cut Keweenawan
igneous rocks. The paleomagnetic pole position
given by the shock-induced remanence
(24"
S,
166"
E)
is chronologically not diagnostic (Halls
1975), as it occurs in a region where Grenville and
Lower Paleozoic poles also lie (Irving
et
al.
1974;
Beales
et
al.
1974). However, the distribution of
shock effects with respect to present topography
is similar to that observed at the Charlevoix
impact structure, Quebec (Robertson 1968), and
suggests a similar level of erosion. The Charlevoix
impact event occurred 360
f
25
m.y. ago
(Rondot 1971), and it may be that the Slate
Islands event has a comparable age.
Acknowledgements
The financial support of the National Research
Council of Canada to H. C. Halls is gratefully
acknowledged. The assistance of
P.
B.
Robertson
to
R.
A.
F.
Grieve in the field, in the measure-
ment of planar features, and in general discus-
sion of the structure is greatly appreciated.
AHRENS,
T.
J.
and GREGSON,
V.
G., JR.
1964.
Shock com-
pression of crustal rocks: data for quartz, calcite and
plagioclase rocks.
J.
Geophys. Res.
69,
pp.
4839-4874.
BEALES, F.
W.,
CARRACEDO, J. C., and STRANGWAY,
D.
W.
1974.
Paleornagnetism and the origin of Mississippi
Valley-type ore deposits. Can.
J.
Earth Sci.
11,
pp.
21 1-223.
BORG,
I.
Y.
1972.
Some shock effects ingranodiorite to
270
kilobars at the Piledriver site.
In:
Flow and fracture of
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... The islands have been mapped geologically over the last 100 years (Coleman, 1901;Parsons, 1918;Sage, 1974Sage, , 1991Stesky & Halls, 1983; Figure 2). Most people who have studied them interpret them as the eroded remnants of the central uplift peak of an ancient meteorite crater (Dressler et al., 1995(Dressler et al., , 1998(Dressler et al., , 1999Grieve, 2006;Halls, 1975Halls, , 1979Halls & Grieve, 1976). Although Sage (1991Sage ( , 1999 attributed their characteristics to a 'crypto explosion' at the intersection of two fault zones, this interpretation cannot explain numerous shatter cones ( Figure 2) and documented planar deformation features (PDFs) in quartz (Dressler et al., 1998;Goltrant et al., 1992;Hodge, 1994). ...
... Bathymetry surveys show a submerged trough and ring structure 30-32 km in diameter, interpreted as the surrounding crater floor and rim, from which the impactor was calculated as~1.5 km in diameter (Dressler et al., 1995;Halls & Grieve, 1976;Mariano & Hinze, 1994). Conclusive evidence for impact comes from numerous shatter cones in the basement, pseudotachylites, polymict allogenic breccias (including glass-bearing suevite), and monomictic autoclastic breccias . ...
... A letter follows the sample number if the exact grain was dated using both approaches. Plagioclase grains from sample S2 were also subjected to 40 Ar/ 39 Ar laser (35) Buchner et al. (2010), Grieve et al. (1995), Halls and Grieve (1976) Absence of Ordovician/Devonian rock fragments in impact breccia >350 Norris and Sanford (1969), Sharpton et al. (1996), Hodge (1994) K-Ar (antigorite, phlogopite) from shock-deformed and brecciated lamprophyre <282 to 310 Sage (1991) step-heating at the Oregon State University Argon Geochronology Lab. For LA-ICP-MS analyses, an Element2 High Resolution (HR)-ICP-MS with an Excimer (192 nm) laser ablation system instrumentation was employed in the UTChron Laboratory at the University of Texas at Austin. ...
Article
The Slate Islands (Ontario) is one of Canada's larger impact structures at 32 km in diameter and has been linked to the Ordovician meteorite event (OME). We report zircon U–Pb dates from two suevite and two syenite samples collected from the Slate Islands. Plagioclase ⁴⁰ Ar/ ³⁹ Ar dates were also obtained from one of the samples. The plagioclase and most zircon dates record pre‐impact ages with links to known tectonic events, including those associated with the assembly of the Superior Craton at approximately 2700 Ma. However, Neoarchean zircon grains appear to be reset at 456.1 ± 6.9 Ma (±2 σ ) based on the lower intercept of discordia for all dated samples. The date overlaps its previously accepted age of 450 Ma and would be 2–19 million years following the parent asteroid breakup if related to the OME.
... parautochthonous target rocks of the crater fl oor have been identifi ed in breccia dikes, indicating the downward sense of transportation (e.g. Halls and Grieve, 1976 ). ...
... Their early formation is also attested to by the occurrence of shatter cone fragments in breccia deposits, including dyke breccias in the floor of some impact structures (e.g. Halls & Grieve 1976). ...
Article
Full-text available
This paper is part of the special publication Meteorites: flux with time and impact effects (eds M.M. Grady, R. Hutchinson, G.J.H. McCall and D.A. Rothery). The terrestrial record of impact events is incomplete and evolving. There are inherent biases in ages, distribution and sizes of known impact events that result from the high levels of endogenic activity on the Earth. Nevertheless, an estimated terrestrial cratering rate of (5.6±2.8) x 10 15 km -2a -1 for impact structures with diameters >20km and younger than 120 Ma can be calculated and is compatible with astronomical observations. The most obvious evidence of impact is the occurrence of 156 impact structures known as of the end of 1996. Few impact structures, however, are sufficiently pristine to provide great detail concerning their original morphology. Some basic morphometric parameters, however, can be estimated. Confirmation of an impact origin for particularly terrestrial structures comes generally from the recognition of diagnostic shock metamorphic effects in the target rocks. Some 16 impact events are currently recognized in the stratigraphic column but it would appear that many others await discovery. The best documented and only global example of such events is at the Cretaceous-Tertiary (K-T) boundary. Although a number of killing mechanisms have been proposed for the attendant mass extinction, the nature of the target, in this case containing sulphates, may be the reason for the devastating effect of this event on the biosphere. In early Earth history, the high impact flux was probably a significant factor in the modification of the atmosphere, biosphere and hydrosphere and the collision of a Mars-sized object with the proto-Earth may have been responsible for the formation of the Earth's Moon. Prompted by the association of the K-T event with a global mass extinction, it has been proposed that other mass extinctions and geological phenomena in the Phanerozoic are impact related, possibly through periodic cometary showers. At this time, there is little or no evidence for this association, although model calculations and the terrestrial cratering rate suggest that impact cannot be ignored as a forcing function for transient changes in the Earth's atmosphere and climate. Although unequivocal evidence linking impact to climatic changes remains to be discovered, it is a statistical certainty that if human civilization exists for time-scales of hundreds of thousands of years it will be severely affected or possibly destroyed by an impact event. Given the stochastic nature of impact events, however, this could happen sooner rather than later.
... Transverse faults and accommodation zones separate grabens with different senses of asymmetry and thus were active when the grabens were evolving (Cannon et al. 1989). One of the faults, the Thiel fault (Fig. I), forms part of the Trans-Superior Tectonic Zone (Klasner et al. 1982), which is also defined by the trend of potential field anomalies and by the alignment of Superior Shoal, the Slate Islands cryptoexplosion structure (Halls and Grieve 1976), and alkaline igneous complexes and diatremes. ...
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A Johnson-Sea-Link submersible was used to examine the geology of Superior Shoal in central Lake Superior. Here, glacially scoured, vertical cliffs, some more than 100 m high, are formed of 1.1 Ga middle Keweenawan basaltic lava flows displaying ophitic interiors and red amygdaloidal tops. Flat-lying sandstones, lithologically similar to the upper Keweenawan Bayfield–Jacobsville sequences, occur to the north of the volcanic rocks. These are inferred to have been downthrown along an eastward extension of the Isle Royale fault, a major boundary fault of the Midcontinent rift. The volcanic rocks are normally magnetized, supporting lithological evidence that they correlate with the middle Keweenawan sequence on Isle Royale. Paleomagnetic data suggest that the volcanics have a complex structure, possibly involving drag folding along the Isle Royale fault.
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The number of newly discovered and confirmed impact structures on earth is growing continuously. In this review paper, the main attributes of 198 confirmed impact structures and 10 further structures, for which final confirmation based on the identification of shock features is not yet entirely satisfying, are presented. The impact craters are compared statistically, with regard to their morphology, structure, and status of erosion or burial. The size– and age–frequency distributions of terrestrial impact structures are presented. Additional aspects concern target petrography and shock effects found in the craters. Based on the discovery statistics of presently known crater structures, an estimate can be made of the number of craters that await discovery. The paper is complementary to the recently published atlas of terrestrial impact structures by Gottwald et al. (2020).
Article
Hypervelocity impacts within the solar system affect both the magnetic remanence and bulk magnetic properties of planetary materials. Spherical shock experiments are a novel way to simulate shock events that enable materials to reach high shock pressures with a variable pressure profile across a single sample (ranging between ∼10 and >160 GPa). Here we present spherical shock experiments on basaltic lava flow and diabase dike samples from the Osler Volcanic Group whose ferromagnetic mineralogy is dominated by pseudo-single-domain (titano)magnetite. Our experiments reveal shock-induced changes in rock magnetic properties including a significant increase in remanent coercivity. Electron and magnetic force microscopy support the interpretation that this coercivity increase is the result of grain fracturing and associated domain wall pinning in multidomain grains. We introduce a method to discriminate between mechanical and thermal effects of shock on magnetic properties. Our approach involves conducting vacuum-heating experiments on untreated specimens and comparing the hysteresis properties of heated and shocked specimens. First order reversal curve (FORC) experiments on untreated, heated and shocked specimens demonstrate that shock and heating effects are fundamentally different for these samples: shock has a magnetic hardening effect that does not alter the intrinsic shape of FORC distributions, while heating alters the magnetic mineralogy as evident from significant changes in the shape of FORC contours. These experiments contextualize paleomagnetic and rock magnetic data of naturally shocked materials from terrestrial and extraterrestrial impact craters. This article is protected by copyright. All rights reserved.
Article
During an impact event, a crater's transient structure adjusts gravitationally. Within medium-sized complex craters, a central uplift rises and collapses resulting in large-scale rotations of the target rock. Estimated crater modification rates from numerical models indicate that complex impact craters modify to a structurally stable state within tens of seconds to several minutes after excavation. However, there is little direct geologic evidence constraining these rates. We show how paleomagnetic measurements of lithic breccia dikes emplaced during crater excavation can be used to constrain the rate of crater modification within the central uplift of the ∼34-km-diameter Slate Islands impact structure, Ontario, Canada. The uniformity and linearity of paleomagnetic directions among the clasts and matrix of breccia dikes throughout the impact structure indicate that breccia dikes were frictionally heated above the magnetite Curie temperature (580 °C) during their emplacement and subsequently cooled in situ through magnetic blocking temperatures. The tight grouping of these paleomagnetic directions implies that these breccia dikes cooled and locked in magnetic remanence over a time interval in which the impact structure was not experiencing structural rotations and had already reached a stable state. Conductive cooling of the thinnest sampled breccia dike would have led to the recording of magnetic remanence approximately six minutes after emplacement. This constraint necessitates a stable crater structure only minutes after impact and presents a rare case in which a geological process can be resolved on such a short time scale.
Article
Drill cores from the Fraser River delta and western Fraser River floodplain, British Columbia, reveal a widespread tephra marker bed within silty floodplain deposits. Isolated tephra layers have been noted in previous studies in the Fraser Lowland and have been assumed to be Mazama tephra (ca. 6800 BP). This note presents the results of the first attempt to systematically identify a number of tephra samples from this area, based on X-ray energy spectroscopic analysis of their chemical compositions and bracketing radiocarbon ages. The results confirm that the tephra bed is Mazama, a finding of considerable utility to future studies in this area.
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Full-text available
Plagioclase from fragments of crystalline basement rocks in breccias found in the area of the Nördlinger Ries crater displays characteristic plastic deformation and phase transition phenomena due to shock metamorphism at different pressures in the range of 100 to 1000 kilobars. These phenomena are discussed in the scope of a progressive impact metamorphism the degree of metamorphism reflecting a radial gradient of pressure and temperature diminishing outward from the point of meteorite impact. Within the lowest pressure range of about 100 to 300 kilobars (shock stage I) strong fracturing and plastic deformation such as bending of crystals, deformation bands and “planar features” (lamellae of lowered refractive index and of lowered or no birefringence) are to be found. The lamellae which are mostly isotropic, are interpreted as slip bands the glide planes of which are low indices planes of the plagioclase lattice such as (001), (010), (100), (1¯20), (130) and others. These slip bands are unknown from feldspar formed by normal processes within the earth's crust. Plagioclase of such a stage of deformation shows an unusual strong decrease of refraction and birefringence. Its optical properties are those of a highly disordered plagioclase. It may be called “diaplectic” plagioclase. Total isotropization of plagioclase is a typical feature of the pressure range from 300 to 500 kilobars (shock stage II). This glass which is called “diaplectic” glass differs strongly from the normal glass in physical properties and structural state. It is formed by a kind of solid state transformation without actual melting. Shock pressures in the order of 500 to 650 kilobars (shock stage III) are able to cause selective melting of plagioclase grains in a crystalline rock. Normal glasses with vesicles and streaks are formed by this process. Within the pressure range of about 650 to 1000 kilobars (shock stage IV) residual temperatures are so high that total melting of rocks occurs. Plagioclase melts are mixed inhomogenously with other silicate melts forming rock melts which can be found in suevite as flat glassy bombs. Vaporization of silicates must be expected in the upper pressure range of this shock stage. Statistical universal stage measurements on the fabric of plagioclase support theoretical considerations after which the deformation pattern of a single crystal should depend on the fabric relations to the surrounding minerals and on their physical properties. Strongly inhomogenous deformation of plagioclase minerals within the microscopic rock scale was observed because polycrystalline rocks are disorganizing a unique shock front by interaction of wave fronts at interfaces and free surfaces and perhaps by multiwave shocks. Directions of compressive and tensile stresses on a mineral are therefore changing from grain to grain.
Article
A regional aeromagnetic survey was conducted to determine the relatively unknown basement geology and tectonics of eastern Lake Superior and the eastern half of the Northern Peninsula of Michigan. During this survey approximately 6500 miles of flight lines spaced at 6-mile intervals were recorded with a digital recording proton precession magnetometer system. The results of the survey generally support the geological interpretation that the Lake Superior structural basin consists of thick basic volcanics overlain by clastic sediments. This basin extends southward into the Northern Peninsula of Michigan with the basic volcanics of the Keweenaw Peninsula curving southward through Stannard Rock and Grand Island. The Isle Royale fault parallels the general curvature of the Keweenaw Peninsula to the vicinity of Superior Shoal, where it is terminated by a cross fault striking from Ashburton Bay, Ontario, to Big Bay, Michigan. A fault on the north side of Michipicoten Island continues to the southeast toward Gargantua Point and northward, paralleling the shoreline at a distance of 10 to 15 miles. Midway between Michipicoten Island and Pic Bay, this fault turns northwest and continues south of the Slate Islands to the volcanics outcropping on the islands of Nipigon Bay. South of Michipicoten Island the basic volcanics have been uplifted by an east-west-striking fault which may be a continuation or a branch of the Keweenaw fault. On the east side of the basin, south of these basic volcanics, the volcanics appear to be discontinuous, with major volcanic rock areas extending southwest from Mamainse Point and the eastern margin of the Northern Peninsula of Michigan.
Article
Postshot exploration around the 61 ± 10 kT Piledriver underground nuclear explosion in granodiorite indicates that the cavity radius rc is 40.1 meters. The shape of the vertical chimney, which extends 277 meters above the shot level, was influenced by pre-existing joints and fractures and is asymmetric. The limit of detectable shock-induced microfracturing is 2.7 ± 0.2 rc, at which point rocks have been subjected to peak radial pressures of 6-8 kb. Extensive fracturing occurs at distances to the shot point of <1.3 ± 0.2 rc, corresponding to pressures exceeding the granodiorite Hugoniot elastic limit of 45 kb. The onset of slip and twinning in mineral constituents is correlated with measured shock pressures at estimated strain rates of ≤104-105 sec-1, ambient temperatures of 30°C, and calculated Hugoniot temperatures for granodiorite of <300°C. For quartz, planar lamellas are detectable in some grains subjected to pressures of 75-78 kb and in all grains subjected to a pressure of 205 kb. Mechanical (1¯01) twinning in hornblende and sphene <110> is evident in rock that has experienced pressures of 24-40 and 14-18 kb, respectively. Some kinking in biotite is associated with shock pressures as low as 15-16 kb; above 75 kb all biotite contains kink bands. At ≤270 kb no shock-induced twinning or planar lamellar structure was noted in either the orthoclase or the albite-oligoclase component of the granodiorite, although there was a noticeable loss of birefringence in both. Glass occurs within the chimney rubble and in distant fractures within the surrounding granodiorite where it was injected by expanding gases. No diaplectic glass was noted in rock forming the cavity walls (270 kb). Dissociation of the hydrous phases, biotite and hornblende, in wall rock surrounding the cavity is attributed to the permeation of hot gases along fractures.
Article
Hugoniot data in the 4- to 250-kb stress range were obtained for quartzite and novaculite, sandstones of varying porosity, single-crystal calcite, marble, porous and nonporous limestone, several plagioclases of varying composition, and a basalt. Conventional plane-wave, in-contact explosive assemblies were used; the shock state was computed from measured shock velocities; particle velocities are inferred from either specimen or driver plate free-surface motion. Impedence-match solutions were obtained for porous rock. High values of the Hugoniot elastic limit were observed in nonporous rocks—approximately 40 to 90 kb in quartzite and novaculite, 40 to 50 kb in the plagioclase rocks, and 15 to 25 kb in calcite and marble. Reduced values were found for porous rocks, approximately 5 kb in sandstone and limestone. Phase transitions are inferred at 30, 45, and 95 kb in calcite, and 22, 45, and 90 kb in marble and limestone. For calcite these are indicated by multiple shock fronts. Anomalously low volumes achieved by sandstone shocked to above approximately 40 kb, and high calculated shock temperatures, suggest partial conversion to coesite or stishovite. High-pressure states observed in basalt and plagioclase agree with previously reported states for gabbro [Hughes and McQueen, 1958] above 300 kb when both data are plotted in terms of relative volume. The previously observed slope-change of the gabbro Hugoniot is believed to result from an elastic wave of perhaps 50-kb amplitude which is overdriven at 300 kb.
Article
Paleomagnetic poles from the Precambrian shield of North America (Laurentia) for the interval - 1500 to -600 m.y. are reviewed. The results are best explained by assuming that the path(s) of apparent polar wander had the form of a sequence of loops with amplitudes of about 60 ø and period of 200-300 m.y. It is possible that such polar paths are the signature of the Wilson cycle, the cycle of opening and closing oceans. The presence of such loops does not imply that this cycle necessarily operated but only that their presence is consistent with its operation during the later Proterozoic. Many pole determinations are now available from medium- to high-grade metamorphic terrain of the Grenville structural province, and the poles from that part of the province (Grenvillia) not immediately adjacent to the Grenville front are statistically distinct from the poles from the remainder of Laurentia (Interior Laurentia). Three hypotheses have been invoked to explain this fact, and a fourth is added here. Only hypotheses I and 2 adequately explain the paleomagnetic data. Hypothesis 2 requires rapid drift of Laurentia at rates of 20 cm/yr for about 200 m.y. Hypothesis I requires that at -1150 m.y., Grenvillia was displaced 5000 km from Interior Laurentia and approached and became sutured to it at about -1000 m.y., the Laurentian shield as we know it today being formed. In Figure 1 the structural provinces of the Precambrian shield of North America (Laurentia) are shown. All provinces except the Grenville (labeled 1070 in Figure 1) were stabilized prior to about -1400 m.y., and there is now substantial paleomagnetic and geological evidence to show that there has been no substantial relative movement among them since that time [Donaldson et al., 1973]. The Grenville province was formed in the later half of the Proterozoic, although some older rocks may be present. In this paper we review the paleomagnetic results from this interval (about - 1450 to -600 m.y.) and discuss their possible implications for the tectonic history of the Grenville province. Paleomagnetic results based on fewer than 10 samples and with errors greater than 20 ø are not considered. The results are summarized in diagrams showing the paleomagnetic pole positions. The results from the Grenville province are also tabulated because of their special interest for this paper. The sources of the paleomagnetic information are cited in the table and in the figure legends. The sources of the age informatiofi are cited only if they are specifically mentioned in the discussion or if they cannot readily be traced through the paleomagnetic literature. Otherwise, they may be found by referring to the paleomagnetic article cited. The Grenville structural province consists largely of highly metamorphosed rocks and is bounded on the north by the Grenville front. The front cuts across the older, but generally less metamorphosed, Archean superior province and the Hudsonian, Elsonian, and Archean terrain of Labrador (Figure 2). Age determinations by the U-Pb and Rb-Sr methods range from about -1500 to -1100 m.y. and by the K-Ar method from about - 1100 to -850 m.y. In places, south of the front, there is a belt up to 100 km in width that consists of metamorphosed equivalents of rocks to the north; this is referred to as terrain B. The probable extent of terrain B is shown later (Figure 13,). This distinction is made in order to recognize the fact that the front cannot be a suture. We refer to the Grenville province without terrain B as Grenvillia. Laurentia without Grenvillia is referred to as Interior Laurentia. Paleomagnetic studies from Grenvillia have yielded