158 (1989) 191-207
Tectonophysics,
191
Elsevier Science Publishers B.V., Amsterdam - Printed in The Netherlands
Vein geometry in the Hilton area, Mount Isa, Queensland: implications for fluid behaviour during deformation R.K. VALENTA Monash University, Department
of Earth Sciences. Clayton, Vie. 3168 (Australia)
(Received May 5, 1987; accepted August 3, 1987)
Abstract Valenta, R.K., 1989. Vein geometry in the Hilton area, Mount Isa, Queensland: implications for fluid behaviour during deformation.
In: A. Ord (Editor), Deformation
of Crustal Rocks. Tectonophysics,
158:191-207.
Folding and shear zone movement occurred synchronously in rocks of the Mid-Proterozoic Hilton area, Northwest Queensland. Syndeformational with shear zone intersections. (1)Fibrous
Mount Isa Group in the
veins developed in shear zones and in sets spatially associated
Veins can be divided into the following two types:
and non-fibrous quartz-dolomite
veins which formed in orientations consistent with the regional E-W
subhorizontal shortening direction. (2)Fibrous and non-fibrous quartz-dolomite indicating local syndeformational
veins which formed parallel to shear planes, S, cleavage, and bedding,
extension parallel
to the regional shortening direction.
The complex geometry of the shear zones suggests that shear parallel veins formed as a result of movement over asperities during shear zone movement. &-parallel
veins, on the other hand, appear to have formed during restricted
episodes of fluid overpressuring during post-failure stress drops. Shear zones are divisible into highly graphitic and weakly graphitic end member types. Highly graphitic shear zones show abundant dissolution
and little veining, while weakly graphitic shear zones show abundant veining and little
dissolution.
that highly graphitic
This indicates
graphitic shear zones were syndeformational
shear zones were syndeformational
Introduction
1983). The style and geometry during
The interaction
between
veining and deforma-
tion has been a subject of interest (Hancock, Beach,
1972;
1975,
Durney
1977;
and
Ramsay,
for many years Ramsay,
1980).
inconsistent
with regional
inconsistencies
changes
in stress
during
deformation
Swager, during
1983) shear
are
and
usually
the
asso-
geometry,
(Kerrich
0040-1951/89/$03.50
movement
(e.g.
by
conditions
and Allison,
or by the influence zone
directions.
explained
fluid pressure
and vein characteristics
com-
in orientations
1978;
from
brittle-plastic
transition.
internal
veins relative
re-
cators of the interaction
interaction
Factors
characteristics,
to deformation
as
and timing
of
are sensitive
rocks
of folds located
indi-
between stress, fluid pres-
This study relates geometry to the framework
at
such
sure, and strain rate in the brittle-plastic
low-grade
Guha
gional fault zone. An attempt
0 1989 Elsevier Science Publishers B.V.
to plastic
can give vital information
aspects of fluid-rock
of asperities et al.,
of veining changes
brittle
gimes (e.g. Murphy, 1984; Gibson and Gray, 1985) on mechanical
Veins
compression
the transition
1973;
monly develop within and are systematically ciated with shear zones, sometimes These
fluid pathways, while weakly
fluid sinks.
next
regime.
and timing of veins and
shear
zones
to a long-lived
in re-
is made to explain
192
syndeformational tening direction
extension
to the shor-
Regional geology
in terms of fluid pressure (P,)
and stress conditions Classification
parallel
during brittle deformation.
of shear zones based on composi-
tion has made it possible to correlate mechanical behaviour and fluid behaviour.
Shear zone char-
acteristics are used to distinguish between regimes of continuous rock-water
interaction and regimes
of episodic
rock-water
interaction.
This paper
concentrates
on features developed in unmineral-
The Hilton deposit is located within the MidProterozoic
Mount
Queensland.
It is a stratiform
Isa
Inlier
in
Northwest
Pb-Zn
deposit
hosted by impure dolomitic sediments of the Mt. Isa Group (Mathias and Clarke, 1975). The Hilton area occurs immediately to the east of a major (100 km ) N-S
trending high strain
zone which includes the Paroo Fault Zone (PFZ)
ized rock. Structures within the mineralized zones
(Fig. l), the Mount Isa Fault Zone(MIFZ)
are similar in many ways, and have been dealt with in Valenta (1988).
l), and other N-S faults further to the west (Wilson, 1975). Rocks in the mine strike N-S and are
(Fig.
BARKLY SHEAR ZONE
EASTERN CK.
2’
BEDDING
Fig. 1. Map of the Hilton
area, with a cross section through
the Hilton mine.
193
a
Fig. 2. Hilton orientation data. a. F, and 4
folding: squares indicate fold axes; dots indicate F, axial surfaces, crosses indicate F3
axial surfaces. b Shear zones: stars indicate shear zones with predominantly sinistral strike-slip movement: crosses indicate shear zones with predominantly dextral strike-slip movement; and triangles indicate shear zones with predominantly high-angle reverse movement.
bounded on the west by the Paroo Fault Zone (Fig. l), across which rocks gradually increase
zones are common, both types intensifying toward the PFZ.
from very low metamorphic
The PFZ and MIFZ are large scale features which are traceable over distances of over 50 km.
grade (Saxby et al.,
1978) up to amphibolite facies (Wilson, 1975). Recent structural work (Winsor, 1983, 1985, 1986; Swager, 1983; Perkins, 1984) has shown that there are three deformation episodes in the Mt. Isa area. D, produced E-W folds and slaty cleavage, with associated late-D,, pre-D,, E-W faults (Winsor, 1986). D, produced open regional N-S folds and cleavage, dilation on pre-existing faults
(Winsor,
1986),
and late D,
E-W
to post-D,
faults in various orientations (Winsor, 1986). D, resulted in the local development of NNW-SSE cleavage and minor folds, with late faults at a low angle to S, (Winsor, 1986). S, and S, occur together in the Lake Moondara area (Winsor, 1983) and underground at Mt. Isa (Swager, 1983). The timing relationship between S, and S, in the Mt. Isa area is based largely on orientations and overprinting relationships of syntectonic veins (Winsor, 1983). Most small-scale features in the Hilton mine show orientations consistent with the D, and D, deformation episodes (Fig. 2). The mine area lies on the west limb of a large-scale anticline, interpreted by Winsor (1986) as a compound F,/F, anticline. Bedding parallel and cross-cutting shear
Structural relationships with D, and D, features in the Hilton and Mt. Isa (Perkins, 1984) would indicate that movement on the combined MIFZ-PFZ began before D, and continued well into post-D, time. Structural features Shear zones Shear zones occur in three main orientations: bedding parallel, NE-SW, and NW-SE (Fig. 2b). The first two types are most common in the mine area. Bedding parallel shear zones occur throughout the mine area, and all shear zone types become thicker and more closely spaced toward the PFZ. Slickenside data are summarized in Fig. 2b. NE trending shear zones show predominantly strike-slip movement, while both subhorizontal and subvertical movements are indicated by striae on NW trending and bedding parallel shear zones. Shear zone orientations and block movements are summarized in Fig. 3. Movement sense has been determined by the following methods: (1) offset on bedding, (2) fold asymmetry, (3) minor offsets
on earlier veins, and (4) rotation and offset of S, and S, cleavage planes. These methods confirm an EARING
overall west-block-up movement for bedding parallel shear zones, north block west and down for NE-SW shear zones, and north block east and up for NW-SE shear zones. This movement geometry
suggests E-W
subhorizontal
compres-
sion during shear zone movement. Figure 4 summarizes variations characteristics Shear
in shear zone
as a function of graphite content.
zones have been
subdivided
into
highly
graphitic and weakly graphitic end member types Fig. 3. Schematic block diagram showing relative movements of shear zones. Shaded area represents the zone of intense shear zone deformation and vein system development. Broken lines indicate movement direction on high-angle reverse faults.
(Valenta, 1988). Weakly graphitic shear zones are large areas of polyclinal and disharmonic folds separated by discrete, commonly curved, shear planes (Fig. 4b). Highly graphitic shear zones are
a
d
Fig. 4. Shear zone internal structures and vein orientations. a. Vein orientations: crosses indicate shear parallel veins; diamonds indicate minor shear parallel veins; circles and triangles indicate bedding perpendicular
and fold axis perpendicular
veins
respectively. b. Structures developed in weakly graphitic shear zones. c. Structures developed in moderately graphitic shear zones. d. Structures developed in highly graphitic shear zones. Veins are shown in black.
195
narrow
areas
which
veining
common
containing and
up to 10% graphite
disharmonic
folding
in
are less
angles show a large variation in orientation (Fig. 4b, d), and curved axial surfaces and fold axes are common
(Fig. 4d).
(Fig. 4b). Folds
within
shear
zones
are
The three shear zone types shown in Fig. 4 commonly occur together within large shear zones. This suggests that the change in graphite content
roughly coaxial with folds outside shear zones, and are east verging. S, is variably developed in folds of this type. In some cases, S, is parallel to
occurs during
the axial plane
progressive
deformation
within large
of shear-associated
other cases it is clearly
shear zones.
associated Folds
Folding Deformation accommodated
in
the
Hilton
mine
largely by mesoscopic
shear zone movement. has had a strong
The presence
has
been
folding
and
of shear zones
effect on the style of folding
and
by later shear-
folding. within
shear
complex
interaction
of open
folds
zones
commonly
vertical,
minor
offset in a vertical within
show
a
with minor shear zones. Limbs
are cut by shallow
more commonly extensional Bedding
folds, while in
overprinted
fold
zones
W-dipping,
or
shear zones with direction
generally
(Fig. 4~). shows
en-
intensity of deformation. The description of folding will therefore deal separately with folds devel-
hanced fissility with striations on bedding planes, indicating slip on bedding planes during folding.
oped within
East-dipping veins, bedding parallel veins, and shear parallel veins all develop, and will be discussed in more detail later.
and outside
shear zones.
Folds outside shear zones occur in barren dolomitic siltstones, and to a lesser extent within ore zones. Mesoscopic folds are tight to open, and occasionally isoclinal within ore zones. Folds generally display east vergences, and there is a large variation in axial surface dip. Curved axial surfaces are common. Two coaxial phases of folding are recognized. The first phase produced upright E-
Relationship
between folds/shear
zones und timing
There is a strong spatial relationship between folding, cleavage, and shear zones in the Hilton mine
(Fig. 4b, d). S, cleavage
intensifies
toward
verging folds (regional F,) with variably developed axial plane cleavage (S,). These are locally
the contact with shear zones, although the latest shear zone movement generally overprints S,. Al-
overprinted
bitized
by rare neutral
folds ( F3) with gently
to E-verging
E-dipping
reclined
axial plane cleav-
age (S,). Polyclinal and disharmonic occur near the contacts with major
folds usually shear zones.
Fold axes in the mine plunge shallow NNW or SSE (Fig. 2a), and commonly show a large variation within small distances. Cleavages defined by dark seams of opaque material commonly develop in hinges and next to shear zones. Long limbs display boudinage or sets of inclined faults subparallel to S, with extension in a vertical direction. Early bedding parallel veins are folded by Fz and F3, and bedding perpendicular and saddle reef veins develop in hinge zones. All F, folds face upward as indicated by younging structures such as graded bedding, sole marks, and cross bedding. Mesoscopic folds within shear zones are closely associated with minor shear planes in variable orientations, and are strongly polyclinal and disharmonic (Fig. 4b). Axial surfaces and interlimb
dykes
intrude
commonly contain quently deformed. coincident
NE-SW
shear
zones
and
an S, cleavage which is subseZones of intense folding are
with shear zones,
and bedding
parallel
shear zones commonly act as detachments for F, and F3 folds. In general, however, the latest shear zone movement appears to cross-cut D, and D, features, suggesting that shear zones continued to form subsequent to D,. Veining
Syntectonic veins occur in a number of settings in the Hilton mine. In general, veins occur within shear zones (Fig. 4) in structural positions controlled by shear zone geometry (Fig. 6), and to a lesser extent elsewhere in the mine (Fig. 5). Vein characteristics are summarized in Table 1. For the purpose of description, vein occurrences have been divided into the following types (p. 197ff).
Fig. 5. General
vein sets. Veins shown in black. Vein orientations: bedding
parallel
veins; crosses indicate
dots indicate
S’, parallel
fold axis perpendicular
veins; diamonds
indicate
veins; triangles
perpendicular
indicate
early
veins.
W . BEDDING r s*
DYKE TRACi FAULT ZONE
\
f--J
EVl
a
BVl
m
EVZ
fe3
BV2
a
BV3
1 M \
Fig. 6. Vein orientations
and cross-cutting
relationships
(BP’ 1, 2, and 3 on drawing);
within
circles indicate
vein systems: NE-dipping
crosses
indicate
&-parallel
and bedding-parallel
vein sets (EV I and 2 on drawing).
veins
197
as simple veins or groups of variable density (Fig.
General vein sets
5). They are commonly confined to one layer or a Figure 5 summarizes the orientations of various extension veins occurring away from shear zones. A
typical example of veining within a fold hinge is
shown in Fig. 7b. Four major sets are recognized:
group
of
layers,
with
vein
ends
terminating
abruptly on bedding planes (Fig. 5). En echelon veins are rare, and occur in both NW-SE NE-SW
arrays. Occasionally
from narrow
fibrous
fringes
and
there is a gradation to equant
centres
(Fig. 8a), in which linkage of en echelon cracks is Fold axis perpendicular
indicated
Veins of this type develop as simple planar
consistent small angle to the main vein (Fig. 8a,b).
by the presence of minor cracks at a
features or enechelon arrays (Fig. 5). They occur
Larger veins of this type commonly contain rotated
Fig. 7. a. Late bedding parallel veins, forming due to mechanical effects. b. Veins developed in fold hinges. Bedding perpendicular veins are well developed in pyritic layers and poorly developed in shale layers. A saddle reef is developed in the hinge. c. Typical breccia vein occurring in vein systems.
198
199
TABLE
1
Vein characteristics Max width
Max. length
(cm)
(m)
General veins
Mineralogy
Timing
Internal textures
(rel. to D2)
F perpendicular
10
0.3
qtz-dol-cal
fib-blocky
pre-post
S, perpendicular
5
0.5
qtz-dol-cal
fib-blocky
pre-post
Early S, parallel
5
qtz-dol-ank
fib
pre-
Late S, parallel
5
0.3
qtz-dol-cal
blocky
pre-post
10
2
qtz-dol-cal
fib-blocky
syn-post
15
4
qtz-dol-cat
blocky
pre-post
0.3
qtz-dol-cal
blocky
pre-post
.S, parallel
10
Shear zones
Shear parallel
5
Other orientations Vein system
NE-dipping set
15
3
qtz-dol-py
fib-blocky
pre-post
S, and S,, parallel
50
2
qtz-dol-py
fib-blocky
syn-post
breccia fragments which retain the early fibrous fringes (Fig. 8~). Bedding perpendicular east dipping Veins of this type are abundant throughout the
(Table 1). throughout
Early bedding . parallel veins occur the Hilton area, mainly within the
Upper Mount Isa Group. Cu and Pb-Zn Sulphides and their alteration minerals occasionally replace original
quartz-dolomite
vein assemblages.
The
mine. En echelon arrays in this orientation can be up to 5 m in length, and their asymmetry indicates
veins occur in anastomosing
west-block-up slip under subhorizontal E-W com-
Fibres are usually oriented subperpendicular to the vein walls, though oblique and curved fibres
pression (Fig. 5). Groups of veins are often concentrated in individual beds or groups of beds bounded by minor shear planes (Fig. 5). Veins terminate abruptly on shear planes or seemingly undeformed bedding planes (Fig. 7b). Vein groups of this nature are internally deformed during later folding and shear zone movement. Veins are generally fibrous, though in some cases they consist of an early fine grained fringe and a later equant undeformed fill (Fig. 8a,c). Later recrystallization and dissolution
groups separated by
thin laminae of country rock.
can occur. In larger veins it is possible to see variations in composition subparallel to the vein walls. Curved fibres with undulose extinction are common, and recrystallization to equant habits occurs in fold hinges. In some cases veins of this type occur as saddle reefs in gentle F, and F3 folds, indicating that they are syn- to post-folding. The general case, however, is that veins of this type are recrystallized and partially dissolved in
is common.
zones of F, folding, indicating folding.
that they predate
Bedding parallel Bedding parallel veins show a wide variation in composition, occurrence, and internal textures
Late bedding parallel veins are distinguishable from early bedding parallel veins in a number of ways. They contain large amounts of calcite in addition to quartz and dolomite, and grains are
Fig. 8. a. Fold axis perpendicular vein showing early fibrous quartz fringe (white) and later blocky dolomite fiil (gray). Asymmetrical cracks visible at vein margins. b. Separated intercrack counter rock segments. c. Rotated breccia fragments with fine-grained fibrous quartz fringes in blocky dolomite. d. S, parallel veins (horizontal) parallel vein with internal quartz-dolomite
S,
seams and preferred dimensional
veins. g. Multistage
with intensification orientation
of S, (horizontal)
of dolomite.
veining within vein systems. h. Undeformed
f. Fibrous
at vein margins. e. S,
quartz vein cutting earlier
blocky dolomite vein cross-cutting
&-parallel vein. Scale bar in each case is 1 mm.
deformed
200
commonly coarse and equant (Fig. 7a), with varying amounts of later deformation. type occur almost exclusively
Veins of this
in areas of small
scale F, and F3 folding, as saddle reefs (Fig. 7b) or discontinuous angular veins which are roughly bedding parallel
cross-cutting relationships (Fig. 7b). However, early bedding parallel veins are clearly cross cut by bedding perpendicular, fold axis perpendicular, and early bedding parallel veins.
but cut up and down through
layers. Where they occur together with bedding
S, parallel
veins,
Veins of this type develop mainly in zones of intense S, cleavage. Narrow planar S, parallel
the three vein types appear to show ambiguous
veins tend to show fibrous textures, with fibres
perpendicular
and fold axis perpendicular
(a)
(b)
B
(d)
-
cI----l
Fig. 9. Vein-S, relationships. a. Pre-S, vein, recrystallized with S, intensification (vertical) at vein margins. b. Post-S, vein opening parallel to S,. c. Syn-S, vein, opening parallel to S, (vertical) and showing intensification of S, at vein margins. d. Syn-S, vein, opening parallel to S, and showing internal development of S, in the form of seams and preferred dimensional orientation of dolomite.
oriented subperpendicular
to the vein walls (Fig.
veins, longer veins with asymmetric breccia frag-
Sf). Larger S, parallel breccia veins generally show
ments,
either coarse-grained
slivers and anastomosing
or compositional
subhedral internal textures,
lamination
of
equant
grains
or compound
arrays with shear-parallel layers of country rock
(Fig. 4b, c, d).
are angular (Fig. 7c), and vary in size from less
Pre-existing structures within shear zones have clearly controlled the geometry of the veins. Thin
than 1 mm up to 30 cm. Breccia
graphitic partings are observed within some veins,
sub-parallel
to the vein walls. Breccia
fragments
fragments are
generally unaltered, though minor silicification and
and the margins are commonly
dolomitization
complex cross-cutting
occur in some cases. Large frag-
ments show little or no rotation,
while smaller
narrow zones of
breccia veining.
Internal deformation is highly variable. In some
fragments can show rotations of greater than 90 O.
cases, veins consist
In some cases individual veins show clearly defined breccia fragment-rich and breccia fragment-
subhedral grains, while elsewhere veins show strong internal recrystallization and dissolution. A
poor areas (Fig. 7~). Larger breccia fragments often contain smaller, slightly rotated, breccia
number of features indicate that shear parallel veins formed at various stages during the shearing
veins at a small angle to the main vein. Clasts
history.
appear to show a perfect fit in cases where there
(1) The occurrence of compound veins with sharply defined zones of high and low internal
has been minor brecciation
and rotation. The rare
of very coarse
occurrence of altered fragments suggests, however,
deformation,
that dissolution and replacement make it difficult to reconstruct zones of more intense brecciation and rotation. Breccia fragments show transport of up to 5 cm within veins (Fig. 7~). These features indicate a complex history of veining in which opening on planar features occurred simultaneously with brecciation. Figure 9 summarizes the various relationships observed between S, and S, parallel veins. A large proportion
cated by minor compositional zones.
of S, parallel veins appear to have had some effect on S,. This may take the form of intensification
of S,
at vein walls (darker
areas which
displace veins in Fig. 8d) in which cleavage intensity is strongly controlled by vein margin irregularities, S, parallel dissolution zones within veins (Fig. 8e,h), or breccia veins with rotated S, in the fragments. Similar textures occur in breccia veins in copper areas of the Mt. Isa mine (Swager, 1983). This indicates that opening occurred on S, planes prior to the end of S, cleavage formation. Veins within shear zones Veins in this setting develop in four main orientations (Fig. 4a), though each set shows considerable spread due to the complex nature of shear zone internal structures. Shear parallel veins Veins in this orientation are found in most shear zones. They occur variously as single lens-like
undeformed
in which repeated opening is indichanges in different
(2) Shear parallel veins which are deformed and cross-cut by minor shear planes (Fig. 4b). (3) The common occurrence of relatively undeformed shear parallel veins at shear zone margins, grading into strongly dissolved, folded, and boudinaged veins in the internal portions of shear zones (Fig. 4d). Other veins East dipping and subhorizontal veins form parallel to the common minor shear plane orientations (Fig. 4b, c), while E-W veins occur bounded groups which are perpendicular shear planes (Fig. 4b, c). They are similar shear parallel veins in composition and
as shear to major to major internal
textures, but are generally smaller (Table 1). In most cases, veins of this type occur as layer bounded groups, in a manner similar to bedding perpendicular and fold axis perpendicular veins (Fig. 4b, c). Vein systems Zones of intense veining occur where large scale shear zones intersect (Figs. 1 and 3). In these zones, vein sets of different orientations can occur over large areas in spacings as small as 10 cm.
202
from one such zone are sum-
Vein orientations
Summaty
of vein timing
marized in Fig. 6. Veins in this zone occur in two and
Table 1 summarizes the timing of veins in the
shallow NE dipping (Fig. 6a). However,
Hilton area. In the general case, all veins except
major orientation NW-SE
composition,
groups;
N-S
subvertical,
internal texture, and vein timing are
for the early bedding parallel systematically
variable within each group.
framework.
related S,
to
the
set appear to be D,
deformation
parallel veins show the most re-
stricted timing, occurring late syn- to post-S,. N W-SE
the other hand, fold axis perpendicular,
veins
These are the most common veins within vein
perpendicular,
and NE-dipping
On
bedding
veins show the
systems. They occur as single veins or anastomos-
widest spread in timing relative to D,. Veins within
ing groups spaced at intervals of 1 cm or more, and are equivalent in timing and composition to the previously described bedding perpendicular
shear zones are difficult to fit into this framework. They appear to have formed throughout the defor-
veins. In the core of the vein system they occur as dense arrays in which veins are interconnected. There is commonly a large variation in degree of
mation history of the shear zones, which themselves have been shown to span a time from pre-D, to post-D,.
vein deformation within the core (Fig. 8g). Early veins in this orientation consist dominantly of
Discussion
equant
coarse-grained
Origin of early veins
consist
mainly
quartz,
of fibrous
while later veins
quartz
and dolomite
(Fig. 8f). In some cases, vein fill consists of a fine grained fibrous quartz fringe with a coarser grained fibrous dolomite centre.
Early bedding parallel veins do not show a systematic spatial correlation with deformation features in the Hilton area. It is possible that these veins are features caused by periodic overpressuring during burial dewatering (Fyfe et al., 1978).
N-S vertical These veins are similar to the previously described S, parallel vein set. Breccia, and fibrous veins occur in this orientation, in spacings much closer than those observed in general S, parallel
Localization
of vein systems
Figure 1 shows the area in which a large scale vein system is developed within the Hilton mine.
veins. The only demonstrably syn-S, (Fig. 8e, h) veins are dolomite rich and recrystallized to subequant textures. They contain irregular seams
On the scale of the area, this would correspond to the zone of intense shear zone deformation shown in Fig. 3. It is important to note that the area of
which are oriented sub parallel to S, (Fig. 8e, h). Dolomites show sutured boundaries, and there is a strong preferred dimensional orientation of
vein system localization is an area where space problems would arise during continued movement
dolomite parallel to S, (Fig. 8e, h). Veins of this type are cut at oblique angles by veins (Fig. 8h) composed of equant dolomite which coarsens into the vein centre. The veins contain breccia fragments of the earlier S, parallel vein set. In these occurrences there is a strong rotated S, in the breccia fragments, but the equant vein material is virtually undeformed. Later breccia veins can be either S, parallel or NE-dipping, and individual veins often bend from one orientation to the other (Fig. 6).
on the shear zones (Fig. 3). Thus it would appear that shear zone geometry is the main control on localization of vein zones. Evidence for abnormal syndeformational
extension
The movement geometry of shear zones in the Hilton area (Figs. 2b and 3) suggests E-W subhorizontal compression during D, and D,. However, the following points suggest local syn-D, extension parallel to the regional compression direction:
203
(1) Veins which are parallel strong dissolution
to S,
and recrystallization,
and show resulting
in shape preferred orientations and solution seams
in turn cause heterogeneous fluid flow patterns and irregularities in shear-parallel veins. (2) On a small scale, shear planes commonly
parallel to S, (Fig. 8e). This indicates that the veins formed after the start of cleavage develop-
parallel a single layer for a considerable distance, and then abruptly cut across layering at a high
ment, and were internally
angle,
deformed during con-
thus
transferring
movement
to another
tinued cleavage development. Opening in a direc-
horizon. Veins are commonly thickest in the areas
tion perpendicular
where the shear planes bend.
to S, is indicated by $-per-
(3) Gentle
pendicular fibres.
folds with axial surfaces
subper-
(2) Veins which are parallel to S,, contain &-perpendicular fibres, and show an intensifica-
pendicular to shear zone walls occur in close as-
tion of S,
extensional
in the country
rock as the vein is
sociation with conjugate minor shear planes with movement.
The
former
indicates
approached (Fig. 8d). This indicates that the veins
shortening subparallel to the shear zone, while the
formed after the start of cleavage development, and vein margin irregularities caused variations in
latter indicates extension subparallel to the shear zone. These seemingly conflicting features coexist
cleavage intensity during subsequent cleavage development. (3) Individual shear-parallel veins which show distinct internal boundaries between zones of
as a result of periodic fluctuation of the shear plane between the shortening and extension fields.
varying dissolution
and recrystallization,
indicat-
Mechanical models generally consider the effect of movement over asperities (e.g. Ladanyi and Archambault, 1970; Guha et al., 1983) or the
ing periodic reactivation of pre-existing veins during continued deformation. This indicates re-
effect of movement terminations (e.g. Muraoka and Kamata, 1983). Geological asperity models in
peated opening at a high angle to the shortening direction.
effect divide the zone of movement into high-strain
Given that in normal circumstances
it is dif-
ficult to have extension parallel to the shortening direction, and assuming that the regional shortening direction now observed is similar in orientation to the maximum principal stress (a,) during D, and D,, it is obvious that during vein formation an abnormal local stress framework must have been in effect. The main factors reponsible for abnormal stress fields are mechanical irregularities and abnormal fluid pressures. The following sections will discuss the possible influence of these two variables. Mechanical
irregularities
A number of features within shear zones indicate that mechanical irregularities may have been important in the formation of shear-parallel veins: (1) Shear zones are strongly non-planar in plan and section, commonly bending into parallelism with other shear zones or bedding (Fig. 4b, c). Movement between two irregular surfaces results in variations in aperture at various scales (Guha et al., 1983; Brown, 1987). These aperture variations
and low-strain zones. The position and effectiveness of these zones is determined by factors such as height and wavelength of the asperities (Guha et al., 1983) and conditions during deformation (Knipe, 1985). In terms of observed veining at Hilton, one would expect to see shear veining in zones which have opened as a the overriding of asperities, and shear extensional features where major bends
parallel result of parallel in shear
zones have caused increased shortening perpendicular to the shear zones (e.g. Guha et al., 1983, fig. 7c). Muraoka
and Kamata
(1983)
considered
the
effect of shear zone terminations and competency contrast on strain patterns. Their results can be applied generally if the assumption is made that movement on a shear zone occurs in a finite zone at any one time, rather than assuming simultaneous movement all along the shear zone. In this way, each movement episode produces zones of compression and extension (Muraoka and Kamata, 1983, fig. 10). The theoretical strain heterogeneity produced by this method is consistent with the observed occurrence of apparently simultaneous shear parallel shortening and extension, and would
204
allow the formation of veins in anomalous orien-
and Mt. Isa (Swager, 1983), there is evidence
ton
tations.
that tensile failure occurred during deformation, with extension
in a direction
parallel
to the re-
gional direction of maximum compressive
Fluid pressure (P,) during veining
stress.
In order to produce this, the following Pf condiS, parallel veins form within vein systems in
tions are required (Fig. 10a) (Secor, 1965; Sibson
areas where the only evidence of brittle deforma-
et al., 1975; Etheridge, 1983):
tion is the presence of extension veins. It would be
(1) Pf approaches lithostatic values.
difficult, therefore, to assert that S, parallel veins
(2) Pf r + + T’.
in this setting form as a result of the influence of
(3) ul--u3 5 T.
small
scale
mechanical
irregularities.
Thus,
it
T’ in this case is the tensile strength of the rock
would appear that the important influence in this case must be fluid pressure (P,).
including the effect of planar elements such as bedding and cleavage. The differential stress com-
In order to form veins, Pf must be high enough to shift stresses at least partially into the tensile field (Etheridge et al., 1984). The expression Pf 2 u3 + T (where u3 is the minimum principal stress and T is the tensile strength of the rock) explains the general conditions required for tensile failure
monly
shows a considerable
brittle
(1977) reports a typical range in stress drops of 1 to 10 MPa for examples from Southern California, while stress drops as high as 35.5 MPa have been reported (Brune and Allen, 1967).
(Etheridge, 1983). Failure of this nature should produce veins subparallel to the direction of maximum compressive stress (Ramsay, 1980). At Hil-
Sibson et al. (1975) have outlined the stress, fluid pressure, and fluid flow conditions before
a
b ,BULK
drop after
failure on large faults (Chinnery, 1964; Brune and Allen, 1967; Hanks, 1977; Sibson 1977). Hanks
FAILURE
1
ROCK
ANISOTROPY
Pf
FLUID
FLOW
AROUND DILATANT ZONE
TIME Fig. 10. Differential stress, fluid pressure and fluid flow up to and after a failure episode. a. Mohr diagram showing conditions before (i) and after (ii) failure. Stress drop allows dilation of anisotropies oriented at a high angle to q. b. Changes in differential stress, fluid pressure and fluid flow with time (after Sibson et al., 1975). The period of time in which differential stress is low and fluid pressure is high is shaded.
and after brittle failure on a fault which contains a
of
dilatant zone (Fig. lob). As stresses build up prior
reached similar conclusions
to failure, fluid flows into the dilatant zone. Im-
volumes in a study of volume loss in calcite-rich
mediately after failure, the differential stress drops,
rocks of the Apennines.
resulting in collapse of the dilatant zone. At this
dence of fluid presence in weakly graphitic shear zones is largely mechanical, taking the form of
point, differential
stress is at a minimum, and Pr
is at its highest value (Fig. lob). If the stress drop is sufficient
to satisfy condition
will be a situation
(1) above, there
in which tensile
failure
on
the original
rock
volume.
Engelder
(1984)
with respect to fluid
On the other hand, evi-
tensile veins in various orientations. Tensile veining generally occurs in regimes of transient high P, (Etheridge et al., 1984)
suggest-
to what was initially u1 is
ing that large volumes of fluid were present within
possible (Fig. 10a) while fluid is flowing out of the
weakly graphitic shear zones only for short peri-
dilatant zone (Fig. lob).
ods up to and after failure. On the other hand, the
planes perpendicualr
In the previously described vein systems (Figs.
intense dissolution in highly graphitic shear zones
6, 7c, 8e-h), two general types of vein develop. The most common is the set which is shallow
would suggest the relatively constant presence of large volumes of fluid during deformation. A pos-
NE-dipping (Fig. 6, EV’s (extension veins) 1 and 2). Veins of this type appear to have formed continuously during the movement history of the shear zones. The $-parallel veins (Fig. 6, BV ‘s (breccia veins) I, 2, and 3) on the other hand, are rarer and are bracketed in time by the NE-dipping set. This would suggest that the NE-dipping veins
sible explanation
for this is the nature of permea-
bility in the two different shear zone types. Highly graphitic shear zones are roughly planar zones of penetrative microfracturing in which the permeability was probably high regardless of the surrounding stress conditions. Weakly graphitic shear zones are irregular bodies with a large proportion
in this case formed under general tensile failure conditions (Fig. lOa). They represent veins which formed perpendicular to u3 in the dilatant zone prior to failure (Fig. lob). S, parallel veins, on the
of undeformed and relatively impermeable rock. Permeability in weakly graphitic shear zones would therefore be highly variable and strongly dependent on the geometry of individual fracture
other hand, represent veins which formed under the restricted set of stress and fluid pressure conditions which were satisfied for a short period of
surfaces and the differential stress and fluid pressure conditions at a given time. The relative scarcity of veining within highly graphitic shear zones
time after failure on the shear zone (Fig. (Sibson et al., 1975).
suggests that deformation within those zones occurred by slow creep processes with only minor
lob)
dilation, Fluid behaviour acteristics
as a function
of shear zone char-
The fact that highly graphitic shear zones show dissolution and little veining, and weakly graphitic shear zones show weak dissolution and abundant veining, suggests that fluid behaviour in the two end member types is fundamentally different. Evidence for the presence of large volumes of fluid within highly graphitic shear zones is based on estimates of fluid volumes required in order to passively concentrate graphite by dissolution of carbonates. Preliminary mass balance calculations (Valenta, 1988) have shown some shear zones display volume factors as low as 0.4, requiring the circulation of enough fluid to have dissolved 60%
while brittle
deformation
process
failure was the dominant in weakly
graphitic
shear
zones. As a consequence of this, fluid pressure and permeability variations would be largest in weakly graphitic shear zones (Fig. lob), and failure episodes within this shear zone type would exert a strong influence on fluid movement during deformation (Sibson et al., 1975). Conclusions Veins in the Hilton area show a large variation in orientations and characteristics. Vein orientations are commonly influenced by small scale features such as folds, bedding, cleavage, and shear planes, indicating localized reversals in the stress field in response to deformation.
206
Vein systems developed as dilatant zones associated
with stress buildup and failure on large
scale shear zones. Large scale shear zone geometry controlled the localization
of vein systems. In the
general case, veins within these systems developed perpendicular
to u3. Veins formed perpendicular
to what was originally
u, in the restricted
time
after failure episodes in which Pf was high and differential
stress was low.
Highly graphitic shear zones deformed by slow creep processes and acted as fluid pathways, while weakly graphitic shear zones deformed by brittle processes and acted alternately as fluid sinks during stress buildups and fluid sources after failure (Sibson et al., 1975).
Engelder. T., 1984. The role of pore water circulation the deformation
during
of foreland fold and thrust belts. J. Geo-
phys. Res., 89: 4319-4325. Etheridge,
M.A., 1983. Differential
regional
deformation
stress magnitudes during
and meatmorphism:
upper bound
imposed by tensile fracturing. Geology, 11: 231-234. Etheridge, M.A., Wall, V.J. and Cox, SF.,
1984. High fluid
pressures during regional metamorphism implications
for mass transport
and deformation:
and deformation
mecha-
nisms. J. Geophys. Res., 89: 4344-4358. Fyfe, W.S., Price, N.J. and Thompson,
A.B., 1978. Fluids in
the Earth’s Crust. Elsevier, Amsterdam, 383 pp. Gibson,
R.G. and Gray, D.R.,
tion during thrust
1985. Ductile-to-brittle
sheet emplacement,
transi-
Southern
Appa-
lachian thrust belt. J. Struct. Geol., 7: 513-525. Guha, J., Archambault,
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between the evolution of mineralizing fluids and the geomechanical development of a shear zone as illustrated by the Henderson 2 mine, Quebec. Econ. Geol., 78: 1605-1618.
Acknowledgements
Hancock, P.L., 1972. The analysis of en-echelon veins. Geol.
I would like to thank Bruce Hobbs, Paul Williams, Dave Gray, and Nick Oliver for ideas,
Hanks, T.C., 1977. Earthquake stress drops, ambient tectonic
Mag., 109: 269-276.
discussions, and constructive criticism of an early draft of this paper; Vie Wall, Chris Waring, and Cees Swager for ideas and discussions; Draga Gelt for drafting assistance; and Steve Moreton for photography help. Field support from Mount Isa Mines Ltd. is gratefully acknowledged. I would like to thank Brice Mutton, Bill Perkins and Rod Johnson of MIM for useful ideas and discussions. This work was carried out during tenure of a Natural Sciences and Engineering Research Council of Canada Postgraduate Scholarship.
stresses and stresses that drive plate motions. Pure Appl. Geophys., 115: 44-458. Kerrich, R. and Allison, I., 1978. Vein geometry and hydrostatics during Yellowknife
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