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Renseignements : POUR PLUS DE RENSEIGNEMENTS SUR VEUILLEZ VOUS ADRESSER À : la reproduction du contenu Services de publication du MDNM l'achat des publications du MDNM Vente de publications du MDNM les droits d'auteurs de la Couronne Imprimeur de la Reine PAR TÉLÉPHONE : Local : (705) 670-5691 Numéro sans frais : 1 888 415-9845, poste 5691 (au Canada et aux États-Unis) Local : (705) 670-5691 Numéro sans frais : 1 888 415-9845, poste 5691 (au Canada et aux États-Unis) Local : 416 326-2678 Numéro sans frais : 1 800 668-9938 (au Canada et aux États-Unis) PAR COURRIEL : [email protected] [email protected] [email protected] A STRUCTURAL ANALYSIS OF THE CENTRAL PART OF THE SHEBANDOWAN METAVOLCANIC - METASEDIMENTARY BELT Final Report to the Ontario Geoscience Research Grant Program G.M. Stott W.M. Schwerdtner Department of Geology University of Toronto TABLE O F CONTENTS Abstract Introduction Methods Results 1 2 3 A. D^ Phase 3 3 5 D2 Phase 8 Strain Domains 9 D- Phase 10 Plutons Contact Strain Aureoles 10 11 Field Analysis General Overview Tectonic. Sequence B. Magnetic Susceptibility Anisotropy Analysis 11 C. Strain Domain Boundaries Discussion Coherent and Incoherent Boundaries 13 13 D. 13 The Greenwater Pluton and Other Late Felsic Intrusions 16 Introduction 16 Late to Posttectonic Plutons IQ The Greenwater Pluton 19 Discussion 21 Summary of Conclusions 23 References 27 ABSTRACT The central part of the Shebandowan Greenstone belt is found to comprise mappable domains of tectonic strain. These domains are a consequence of two successive phases of regional deformation with the second phase, D2 , superimposed upon the first only within megascopically - discrete zones. D, domains possess strain fabrics characterized by westerly-plunging stretching directions and a somewhat less oblateness of strain than the easterly-plunging D- domains. The boundaries between these contrasting domains of strain appear to be generally coherent (not dislocated) but some faulting along these boundaries may have occurred. Two models are proposed that apply to different settings. The concomitant development of strain domains appears to be typified by the Larder Lake "break" (Downes 1980). The sequential development of strain domains is represented in the Shebandowan belt. The variations in the strain pattern across the belt have been confirmed using magnetic susceptibility anisotropy. The results from this method also suggest that an increase in the oblateness of strain in D, strained rocks occurs close to the strain domaxn boundaries; this probably serves to lower the contrast in strain across the boundaries and avoid sharp dislocations in most areas. Dislocations along domain boundaries may have concentrated precious metals where such boundaries juxtapose lithostratigraphic sources of these metals. is suggested that discontinuities between tectonic strain domains should be considered when investigating exploration targets. A detailed study of the crescent-shaped Greenwater Pluton is outlined. The intrusion, by comparison with idealized strain models, appears to possess a primary strain fabric consistent with an antiformal sheet emplacement. i l It jntreduction So little is known of the pattern of cumulative tectonic strain within greenstone belts or whether such strain patterns can be correlated with those in adjacent subprovinces or gneissic terrains. This study documents the tectonic sequence of events and the pattern of strain within the central part of the Shebandowan greenstone belt. The pattern of strain domains is confirmed by magnetic susceptibility anisotropy. A detailed study of a crescent-shaped pluton is also outlined to demonstrate the close correspondence between an idealized emplacement model and the strain pattern within an actual pluton. The presence of strain domain boundaries and their bearing upon gold exploration is discussed. -lethods The magnetic susceptibility anisotropy (MSA) method has been used to 1) verify the general orientation of mineral lineations observed in the field and 2) estimate the range of variation of the tectonic fabric between the regional strain domains shown in Figure l and Maps A and B. The method is also being used at present to test the penetrativeness of mineral lineations in handspecimen. For example, oppositely plunging lineations locally prevail on separate foliation planes within handspecimens in areas particularly close to strain domain boundaries. The non-penetrativeness of lineations would imply a locally non-homogeneous superimposition of a later deformation upon a pre-existing tectonic fabric. Such observations have an important bearing on the nature of strain domain boundaries. The mafic to intermediate volcanic rocks of the Shebandowan belt were found to possess a very low magnetic susceptibility. As a consequence, the increased time factor required on a spinner magnetometer for acceptable precision was prohibitive for suitable time-sharing of the equipment. Instead, a more readily available low-field torque meter (King and Rees 1962) was used. This method is much slower but may be somewhat more precise than the spinner magnetometer (Ellwood 1978). Analysis in this study has been limited to the prolateness factor and orientation of the principal directions of the MSA ellipsoid (Stone 1963). Successful application elsewhere of MSA as an estimate of strain (e.g. Rathore, 1979) encourages us to use the approach to estimate strain variations in the belt. This is especially valuable in volcanic terrains where suitable primary strain gauges are sparsely preserved. The field examination has concentrated on measuring the orientations of mineral lineations and estimating the relative strength of mineral liireations and foliations following a procedure outlined in Schwerdtner et al (1977) . Results A. Field Analysis General Overview The regional fabric in the central part of the Shebandowan belt is characterized by a steeply dipping mineral foliation consistently parallel to bedding. This is also observed in other relatively narrow linear greenstone belts and in the continuation of the Shebandowan belt into Minnesota (D. Davidson, pers.comm.). Mesoscopic (outcrop-scale) fold hinges are not widely observed except in the area just south of Lower Shebandowan Lake and in a thick zone of mafic tuff west of Squeers Lake, approximately 8kn southwest of Greenwater Lake. A major westerly-plunging fold hinge lies in the vicinity of Horseshoe Lake just east of Greenwater Lake. Folds are generally tight to isoclinal with some exceptions immediately south of Lower Shebandowan Lake where the intensity of deformation is so weak as to preserve angular hyaloclastite breccia fragments for example and open folds in hematized volcanic breccia and lahar units. All observed fold axes closely parallel the orientation of the local mineral lineation. Interpreted megascopic fold axes are shown in Figure 1. The structural evidence does not support the contention of Beakhouse (1974) that the greenstone belt is a large homocline facing consistently to the north. His suggestion is probably induced in part by the observation that the stratigraphic north-south section east of Greenwater Lake shows a general asymmetry with tholeiites and komatiites in the southern half of the belt and a more differentiated suite of andesites, dacites and rhyolites to the north. However, it appears that this asymmetry is a primary feature of this and other belts (Trowell etal 1980). The pillow lavas along the north edge of the Shebandowan belt north of Burchell Lake stratigraphically underlie the turbidite sediments of the Quetico subprovince (Giblin 1964 and Bau 1975). Structural interlayering of mafic volcanics with the consistently N.W.-facing Quetico sediments close to the belt margin appears to reflect contemporaneity of the units. The evidence is less clear in the area of Kashabowie Lake and eastwards where the Postans Fault defines the northern belt margin. North of Middle Shebandowan Lake the younging directions in the mafic tuffs south of the fault and Quetico sediments north of the fault suggest the Postans Fault locally represents the "broken" hinge line of a syncline along the belt margin. ~~ South of Lower Shebandowan Lake Morton (1979) has conducted detailed mapping and logging of core on the Shebandowan Mine property. The petrologic results plus chromite analysis in ultramafic sills and flows support the structural interpretations in the present study: the Shebandowan mine section is on the north limb of an anticline that lies about 300 metres south of the mine shaft. The syncline to the north was partly truncated by the intrusion of the Shebandowan pluton. The megascopic fold axes east of Greenwater Lake (Figure 1) are based on few pillow top directions and their locations are tentative. It should be noted that the fold locations are consistent with a stratigraphic feature observed by Morton (ibid) and in the present study. some coarse Ultramafic flows and sills (?) and grained mafic flows typically have magnetite - chert iron formation deposited on or close to their upper surfaces as determined by independent younging criteria elsewhere. This feature may be fortuitous. Mineral lineations are observed in this study throughout the region. Indeed with sufficient core they may be observed in virtually every outcrop in the region including the very weakly deformed rocks south of Lower Shebandowan Lake which Morin (1973) has described as "massive, with no megascopic penetrative (tectonic) fabric" p!6. The ubiquitous presence of visible mineral lineations encourages us to suggest that such structural elements can and should be more widely measured and recorded by field geologists and used effectively for structural interpretation. The sparse presence of bedding/cleavage relations, mesoscopic folds, polyphase folding, younging direction indicators, boudins, and suitable primary strain gauges in mafic volcanic rocks has forced us to concentrate on lineation orientations and variations in the nature of the tectonic strain fabric. The following is based mainly on the results of these measurements. Tectonic Sequence Three generations of regional structures are distinguished within the Shebandowan belt. These structures are attributed to successive phases of regional deformation. In addition, there is a generation of structures related to contact strain aureoles around individual late to posttectonic plutons. The first two deformation phases constitute the dominant tectonic stages in the Shebandowan belt. The sequence of structures is shown in Table l and the interpreted sequence of tectonic events is summarized in Table 2. Stereograms of D-, and D~ - domain structural elements are shown in Figures 2 and 3. D. Phase The first recognizable deformation phase, D., is characterized by consistent west - to southwest-plunging Table l MESOSCOPIC STRUCTURAL ELEMENTS AND THEIR CHARACTERISTICS Deformation Phase Associated Structural Elements D l D z Dj Fl F2 F3 s, So S, Fold Profile tight to isoclinal Fold Orientation plunging upright folds with near verticle axial surfaces and moderate to steep rake of fold axes; axes plunge W. to S.W. - Fold Distribution Surface Folded tight to isoclinal to open in sediments and "Timiskaming" volcanics plunging upright folds with near vertical axial surfaces and gentle to steep rake of fold axes; axes plunge E. to N.E. plunging upright folds with near vertical axial surfaces and generally steep rake of fold axes; axes plunge variably from W., N. to E. Characterizes D, Characterizes D2 widely observed in strain domains but sparsely observed; best seen in mafic tuffs S.W. of Geenwater Pluton. Probably occur in D domains, but not observed in outcrop domains but sparsely observed except in sediments, tuffs and "Timiskaming" volcanics. north half of belt and in Quetico metasediments; most prominent in thinly bedded units. SQ bedding S S bedding and S, S foliations S.. almost Axial Surface Foliation always parallel bedding S2 parallel to S. weak and S .j and bedding; confined to narrow hinge of F3 bedding/cleavage to bedding; bedding/ cleavage intersections intersection locally rarely observed. observed in sediments, tuffs. Axial Lineations kink folds; dominantly Z folds L- mineral lineations "L mineral lineations parallel to fold axes and plunging W. to S.W. parallel to fold axes and plunging E. to N.E. folds; commonly a fracture cleavage. L^ only locally observed, confined to F^ fold hinges as Granulations and mineral alignment. Table 2 Tectonic Sequence of Events STRUCTURAL INTRUSIVE D,, kink folding CRITERIA D^ superimposed on /^concentrated in N. half of belt and in Quetico sediments; related to late E.-W. compression parallel to foliation the late trachytic dykes Late felsic plutons and dykes D~ heterogeneously concentrated D2 predominent in zones (domains) across the belt; predominent in less competent sediments and areas of lithologically complex stratigraphy, typical of N. half of belt. D2 is superimposed in less competent units that are expected to be affected by last major deformation. upon D. and strain elements are composite of D., plus D2 deformations. D, westerly-plunging folding of supracrust across Shebandowan belt and southern Quetico sediments. Shebandowan pluton possesses steep W.-plunging primary lineation in N. half of pluton but D2 - deformed in south half; no contact strain aureole. D. folds and lineations locally preserved in Quetico sediments (E. Sawyer, personal communication); Inliers of D, in D2 domain of belt. mineral lineations end mesoscopic fold axes. The lineations are typically moderately - well developed, at least within the major D, domain in the southern half of the belt and are more pronounced than lineations observed in Dj domains. the bedding. The tectonic foliation, S-,, is almost invariably parallel to Megascopic F., folds are defined from lithologic patterns and facing directions notably east and north of Greenwater Lake. D, synclines and anticlines possess plunging fold axes with upright to steeply northward dipping axial planes. Just east of Greenwater Lake they are deflected around a crescent-shaped pluton and tonalitic gneiss dome. L^ mineral lineations are typically prominent and plunge generally 50 to 65 degrees westward. This degree of plunge is consistent throughout the D. strain domains (Figure l and Map A) except close to the late to posttectonic plutons where they steepen within the contact strain aureoles, and except close to the boundary of D~ strain domains (Figure 1) where the lineations in places become either shallower along some boundaries or steeper. This is discussed later. D0 Phase The second deformation phase, D2 is characterized by weakly developed east-plunging mineral lineations. The tectonic foliation is generally more prominently developed and mineral lineation more weakly developed than in areas affected exclusively by D, . The plunge of mineral lineations within the northern half of the belt changes from relatively shallow, 10 to 30 degrees, in the Burchell Lake - Kashabowie Lake area to 55 to 65 degrees further east in the area north of Middle Shebandowan Lake. The plunge of lineations within the Quetico metasediments is consistently shallow. Within the core of the belt, 1,2 lineations range from 35 to 70 degrees in plunge with the steeper lineations typically found close to strain domain boundaries. Strain Domains The greenstone hele has been subdivided into domains of tectonic strain. These are separately characterized by either predominance of D, ~ induced structures (D., domains) with westerly-plunging lineations and folds or by the predominance of easterly-plunging D2 -induced structures (D ? domains) These domains are separated by rather sharp boundaries or discontinuities (Maps A, B) across which the mineral lineation changes orientation. This change may occur sharply or at least within 60 metres (200 feet) as seen along the ramp section of the Shebandowan Mine (Figure 8). Steep mineral lineations are widely observed in the vicinity of such boundaries. Or the lineation orientation may change progressively through shallow plunges as seen along the south shore of Upper Shebandowan Lake, northwest of Greenwater Lake (Figure l, Map A). The discontinuities tend to follow the stratigraphy closely but have been observed to obliquely cross-cut mappable units. For example, Figure 4 shows a volcanic breccia unit, south of lower Shebandowan Lake, transected by the strain boundary. Faulting has not been observed to follow these strain discontinuities. Instead, a relative increase in oblateness of strain is observed within the larger D, domain in the south close to the adjacent discontinuities. Narrow domains occur within the northern part of the belt especially around Upper Shebandowan Lake ( see Maps A and B). Both D- and D2 domains are generally characterized there by oblateness of strain with relatively weak mineral lineations. (See also-results of MSA analyses). These naxrower D^ domains appear to be tectonic "inliers" within the major D2 strain domain. Although the bulk of D2 deformation is confined to clearly mappable D ? strain domains, narrow, probably discontinuous D. zones typically less than \o 300m wide, occur within the najor D., domain close to the mutual boundary. These are most prominent between Greenwater and Upper Shebandowan Lakes. Within such narrow zones, both L, and L9 lineations are observed within handspecimens. The regional strain pattern is not restricted to the Shebandowan belt but extends across the Quetico subprovince(an easterly-plunging D2 domain) to the north and there is evidence that at least the margin of the tonaliticgranodioritic gneiss terrain to the south is also affected. However, posttectonic plutons have intruded the belt's southern margin and distorted the original strain field so that correlation of the D2 strain donain into the gneiss terrain is limited. D- Phase A third phase of deformation, D~, appears confined to the northern half of the Shebandowan belt and at least the southern subprovince. part of the Quetico It is identified by steeply, almost vertically-plunging kink folds within well foliated supracrustal units, especially pryroclastic deposits and sediments. This phase is locally imposed upon, and thus postdates, the otherwise posttectonic syenitic-trachytic dykes that transect the stratigraphy. The kink folding appears to have been generated by a late east-west compression and post-dates all other deformation and intrusive events. Plutons Discussion of the plutons is presented later. These bodies are late to posttectonic and each possesses primary stretching lineations which appear related to the pluton's internal strain during its emplacement. Pluton is given as an example in detail. The Greenwater \\ Contact Strain Aureoles Subsequent Co the D^ deformation phase, the rise c;f late to posttectonic plutons deflected the stratigraphy and imposed contact strain aureoles upon the supracrustal rocks typically less than 600m in width. The most prominent contact strain envelopes enclose the Greenwater and Kekekuab Plutons. The regional pattern of stretching lineations in the belt is deviated in proximity to these late intrusions. The width of contact strain around a pluton is taken to begin where the regional lineation trend begins to deviate and plunges steeply toward the pluton. Such changes in lineation orientation are revealed by changes in lineation pitch relative to the strike of the foliation. No separate lineation is superimposed upon the regional fabric indicating that, as expected, sufficiently high pressure-temperature conditions prevailed to cause a simple re-orientation of the pre-existing stretching direction. Outside the contact strain aureoles, the plutons (e.g. Greenwater and Peewatai) also mechanically rotated the stratigraphy and its regional stretching lineations. The width of such effects appears to show a direct correspondence with the horizontal width of the pluton involved. B. Magnetic Susceptibility Anisotropy Analysis Oriented cores one inch in diameter and 0.85 inch long were cut from one hundred and thirty-one samples across the belt. Fifteen axial measurements were obtained for each of generally three cores per specimen with the low field torque meter and from these were computed the principal axial directions of susceptibility and a prolateness factor - P. P is used as an estimate of prolateness,one aspect of the shape of the susceptibility ellipsoid where P - (^ - k2 ) l (k ? - * 3 ) and k^ k^ > k^ are the principal semi-axes of the ellipsoid. The P value as a prolateness factor is strictly valid only for quasi- isotropic rocks, <:>'^ anisotropy, or highly lineated rocks (Schwerdtner 1976), but it nevertheless serves as a rapid measure to quantify regional tectonic fabric changes. The results of the MSA analysis are displayed on Map B. The maximum directions of susceptibility are consistent with the mineral extension directions measured in the field within the corresponding strain domains. The exceptions are to be found generally close to the boundaries between the strain domains particularly within the D^ domains where it is believed relict D., fabrics may be locally preserved but easily missed in the field. The orientation of the MSA for each strain domain verifies the existence of these domains and the field observations recorded on Map A. The P value for 87 stations is shown in Figure 6 corresponding to azimuth direction of plunge of the major axis of the magnetic susceptibility ellipsoid. There is a general increase in P from susceptibility ellipsoids plunging eastward in the D2 domains, to those plunging westward, characteristic of D domains. This is more clearly evident if we disregard the D,-oriented samples close to the strain domain boundaries which possess low P values and typically steep plunges in their extension directions. These are interpreted to have acquired increased flattening strain as a consequence of the D2 deformation. Figure 5 illustrates the orientations of magnetic lineations for all supracustal samples measured. Orientations within D, and D2 domains are comparable with those of mineral lineations shown in Figure 2. We m.iy consider the D., domain to be characterized by a wider variation in the prol:iteness of strain th-an is evident: in D, dor-ains. The higher P values correspond to the field observation of relatively more pronounced mineral lineations in the major D, domain. Note that unusually high P values in D2 domains are from samples of chilled pillow margins wherein a primary component of the magnetic lineation has probably been preserved. C. Strain Domain Boundaries Discussion To our knowledge, this study constitutes the first discussion of strain domains and their boundaries on a regional scale in a greenstone belt. Discontinuous interfaces between contrasting strain domains have been observed locally in other areas: in Saskatchewan (Schwerdtner 1970) and in the Larder Lake area in Ontario (Downes 1980). Both W.M. Schwerdtner and M.J. Downes have suggestad for their respective areas that rotational faulting may account for the discordance in the plunge values of the fold axes and mineral lineations between the adjacent domains. The difficulty with this is that the amount of rotation required to bring the two orientations in line can be quite considerable; the lack of major lithologic discontinuities across these boundaries in many areas suggests that two other models to explain these features should be considered. Before we discuss these models, some basic implications of these strain boundaries are considered. Coherent and Incoherent Boundaries No faulting or shearing has been observed along the strain domain boundaries in the Shebandowan belt. boundaries are said to be Ideally, if slip has not occurred, then domain coherent (Means, 1976) since the strain in all directions within the plane of the boundary is the same on both immediate sides 14 of the boundary. The failure of two strain domains to produce a mutually composite strain within the ideal boundary results in slipping along the boundary to relieve the contrast in strain. as being incoherent. Such a boundary is referred to Thus, when two contrasting strain domains develop adjacent to each other, they have a choice to resolve their differences: either come to a mutual "agreement" at the interface or create a space-problem that can only be resolved by slipping. These conditions are illustrated in Figure 7. It appears that in the Shebandowan belt, nature has attempted to retain coherency at the boundaries. The evidence from figures 6 and 8 suggest that the effects of superimposition of D2 upon D, go beyond the boundaries as shown on Maps A and B. The boundaries are defined where the visible lineation reverses plunge direction; but, the "effective boundary" appears to be a narrow zone of undetermined width wherein the oblateness of cumulative strain in D., domains is increased in proximity to the "new" D2 domain. is not severe and slippage is avoided. Thus the strain adjustment We could conceptualize the domain boundaries as "strain fronts" at the leading edge of a conversion of D, strained rocks to a new cumulative strain induced by D^. In essence, the D2 domains possess a cumulative strain (D.. 4- 02). We cannot be certain that all such boundary surfaces have avoided slippage entirely in this greenstone belt since it is conceivable that a spectrum of adjustments may have developed. Peewatai Pluton follows faults). (Note also that a boundary west and north of The implication here is that boundaries on the surface may be cryptic traces of local fracture surfaces or shear zones at depth. Thus, dislocations may have developed without any evidence of such at the surface, The distribution of fracture zones has an important bearing on the hydrothermal concentration of precious metals and the tendency for such 15 favourable zones to be developed ac planar discontinuities of strain should be considered for future investigation. An example of a boundary that has been dislocated and within which gold has been concentrated is outlined by Dovmes (1980). Along the Larder Lake "break" Downes has located a major discontinuity between strain domains that juxtaposes lithostratigraphic hosts for gold. Nevertheless, there are some basic differences between the Larder Lake area and the Shebandowan belt. Downes notes that his "structural discordance B" is characterized by simple megascopic folds of the sar:e apparent generation having contrasting plunge directions on opposite sides of the discordance. In the Shebandowan belt, different generations of folds are involved with a complex of strain domains, some merely 100 metres wide, that reflect a localized superimposition of one generation upon the older. These settings suggest two models beyond a simple rotational fault model. 1) Theconcomitant development of two strain domains with a single major generation of folds as in the Larder Lake setting. There is no local interaction of one strain domain upon the other; the boundary between the two is sharp. The difference in the stretching direction on each side of the fault may be related to "mega-release" directions on a large scale, possibly governed by the position of batholiths. The movement on the fault itself would be the resultant of the strains on each side of the fault. In the Larder Lake case, this would presumably be dip-slip although this may not be evident in the field if subsequent strike-slip has occurred. 2) The sequential development of strain domains with a sequence of folding exemplified by the Shebandowan belt. Fault discontinuities mayor may not be present. However, it is likely that during the progressive localized development of the second strain domain (D^) the entire deforming system is more able to maintain coherency of strain domain boundaries. The absence of two "actively gener--icing" strain domains avoids the dramatic interfacing of domains that produces slip. The major distinguishing features of this model situation are: the presence of narrow zones where D2 is non-penetratively superimposed on D , close to major boundaries of strain; the presence of "relict-inliers" of smaller D, domains within a major D2 field; and the tendency for D., rock fabrics to resemble the more oblate anisotropy of strain typical of D^ as one approaches the domain boundary. The smaller D., domains in the Shebandowan belt have undergone a more uniform increase in oblateness although they still retain their signature of a westerly-plunging lineation (only preserved nonuniformly in some areas). The mechanisms for producing the deformations observed here still lie in the realm of speculation and will not be commented upon. D. The Greenwater Pluton and other Late Felsic Intrusions Introduction A set of late to posttectonic felsic intrusions is located within or marginal to the Shebandowan greenstone belt: this set extends from the Saganaga intrusion on the Minnesota border to several small intrusions northwest of Thunder Bay. Many, if not all, plutons shown in Figure l may be comagmatic. With the exception of the pluton north of Burchell Lake, all possess hornblende laths as the predominant mafic mineral, and vary compositionally from tonalite to adamellite .(granodiorite predominant) with some monzonitic to syenitic outer margins. Some of the intrusions tend to be quartz porphyritic such as the Saganaga (Davidson, Jr. 1980), Qreenwater and Shebandowan bodies with plagioclase and/or K-feldspar phenocrysts dominant towards the outer margins. Other intrusions such as the Peewatei granite and Hood syenite plutons and some smaller syenite bodies south of Burchell Lake are exclusively K-feldspar porphyritic and markedly homogeneous. Dark greenish-red to red trachyandesitic-trachytic dykes are spatially associated with the Greenwater and Shebandowan bodies and sharply transect the local stratigraphy. These dykes are most prominent north of Greenwater Lake (Hodgkinson 1968). Dykes associated with the Greenwater pluton contain steeply plunging mineral lineations that are clearly unrelated to the regional D., and D2 strain domains of Figure l, attesting to their generally late to posttectonic emplacement. The internal strain fabric of the Greenwater Pluton, described in detail below, is typical in one sense of all but the Shebandowan Pluton: it appears that these late intrusions possess primary strain fabrics related to the emplacement of the bodies and do not possess any regional tectonic overprint. It is critical to note that this holds true for the marginal phases of such intrusions and associated dykes or apophyses extending into the surrounding host rocks where any regional deformation would certainly have been recorded. The one exception is the compositionally variable Shebandowan Pluton and its associated small gold-bearing porphyry intrusions (see Morin 1973). Not only is it an elongate body, typical of syntectonic intrusions, but it appears .o straddle two regional strain domains (Figure 1). The northern half of the body displays steep westerly-plunging primary mineral lineations accentuated by quartz that appears to parallel the prevailing regional D, strain fabric. The southern half of the body shows a marked flattening strain with shearing heterogeneously concentrated in zones. Correspondingly hornblende, prominent in the north, is progressively retrograded to chlorite in the south. A contact strain aureole around each of the late to posttectonic intrusions is superimposed upon the'volcanic envelope and this contrasts with an apparent lack of such an aureole around the Shebandowan body. The separation in time of emplacement between the Shebandowan and Greenwater Plutons is further evident from the contrasting internal strain fabric of their respectively associated trachyandesite dykes. The evidence suggests that if the various intrusions are comagmatic, there is a protracted timing to the final emplacement of related felsic intrusions from at least the D, deformation phase to a post - D^, pre-D~ period. The relatively older emplacement age of the Shebandowan pluton suggests that the pluton is structurally an acceptable candidate as the sub-volcanic equivalent of the late "Timiskaming" calc-alkaline volcanic suite (Shegelski 1980) to the south and east. Petrologic confirmation of this is outside the scope of this study but, is recommended in the light of gold showings within porphyry phases of the Shebandowan Pluton (Morin 1973) and the proximity of the calc-alkaline volcanic suite that appears to be tectonically and lithologically comparable with the gold-enriched (Tihor and Crocket 1977) Timiskaming Group at Kirkland Lake. Late to Posttectonic Plutons Most other plutons postdate the bulk of the regional supracrustal deformation and preserve their primary unmetaiaorphosed fabric. Several intrusions (the Greenwacer, Pinecone and Kekekuab Flutens) are crescent-shaped and are semi-concordantly emplaced between the granitoid gneiss terrain to the south and the greenstone belt. Such intrusions have become more widely recognized in recent years with detailed mapping of the granitoid complexes (Schwerdtner et al. 1979). Because of their distinctive shape, these plutons possess internal strain patterns that are distinctive of either diapirism or a sheet intrusion mechanism. In the following section, we shall demonstrate that the internal strain pattern of the Greenwater Pluton more closely resembles a concordant intrusive sheet. The Greenwater Pluton The Greenwater Pluton (Figure 9) is a single intrusion grading outwards from a hornblende-biotite granodiorite with quartz megacrysts tov/ards the margins of feldspar porphyritic syenodiorite to diorite. Typically, the mafic minerals are concentrated in elongated clots or xenoliths of amphibolite or meta-hornblendite. The pluton is separated from a tonalitic gneiss dome to the south by a narrow screen of amphibolite. The intrusion and its apophyses display clear evidence of late to posttectonic emplacement. The body appears to have advantageously invaded along the curved interface between a gneiss dome and the volcanic belt. Figure 9 illustrates that the southern, concave boundary of the pluton dips away from the gneiss dome. The convex boundary to the north and east dips near vertically. Natural strain gauges in the form of quartz aggregates (l-8mm across) have been used for strain analysis using a method developed by Robin (1977). The results (Table 3, Figure 10) show a symmetric strain pattern with a zone GREENWATER PLUTON STRAIN DATA TABLE 3 1 A/ B B/C A/C k X, 1.99 1.19 2.03 1.42 1.35 1.91 2.98 2.54 1.84 1.28 1.33 3.39 1.56 1.71 1.55 1.12 1.14 1.20 1.23 3.23 2.14 3.60 2.00 2.79 2.29 3.55 2.81 2.73 1.93 2.01 3.75 2.33 2.96 2.47 17 18 19 1.62 1.80 1.77 1.40 2.06 1.20 1.19 1.10 1.48 1.51 1.51 1.11 1.49 1.72 1.60 1.61 1.17 1.75 1.59 0.6 4.2 0.7 1.0 3.0 0.2 0.1 0.07 0.6 1.8 1.5 0.05 0.9 1.0 1.1 4.9 1.2 3.7 2.6 0.96 0.65 1.05 0.56 0.86 0.71 1.12 0.93 0.82 0.54 0.57 1.20 0.69 0.88 0.74 0.51 0.23 0.63 0.56 20 21 22 23 24 25 26 27 28 29 30 31 1.67 1.61 1.07 1.26 1.36 1.50 1.59 1.28 1.73 1.17 1.10 1.21 1.10 1.12 3.35 1.65 1.22 1.41 3.62 1.56 1.18 1.21 1.95 1.85 1.84 1.79 3.61 2.14 1.47 2.11 6.15 1.99 2.05 1.43 2.14 2.25 6.7 5.2 0.03 0.4 1.6 1.2 0.2 0.5 4.0 0.8 0.1 0.2 0.53 0.50 1.17 0.63 0.35 0.61 1.51 0.57 0.61 0.29 0.68 1.40 32 1.11 1.45 1.62 0.2 0.41 SAMPLE 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 1.80 1.33 2.10 1.95 | i of constriction (extension as opposed to flattening deformation) extending along the central length of the pluton, progressing to flattening deformation near the pluton margins. The k value of Figure 10, is a measure of the prolateness of the strain ellipsoid (Flinn 1965) where: k s C(A - B) B(B - C) and A > B > C are the principal semi-axes of the strain ellipsoid. The symmetric strain pattern is inconsistent with an arcuate diapiric ridge model (Ramberg 1967, Fig. 71; Schwerdtner and Troeng 1978). This model shows, among other features, a distinct asymmetry of the total strain pattern in a radial cross-section with k < l near the concave boundary of the arcuate ridge and k > l near the convex boundary. In addition, secondary domes typically emerge within the end regions of the ridge. These tend to cause bilateral flow of the magma towards domes, producing a central region of subhorizontal prolate strain ellipsoids. Such features are not present in the Greenwater Pluton. Rather, tha structural trends (Figure 9) display steeply-plunging prolate ellipsoids that reflect longitudinal extension in the direction of material transport. This plus the symmetry of the strain pattern are consistent with the pattern of an ideal antiformal intrusive sheet. Furthermore, the trajectory of lineation trends (Figure 11) shows a steep fanning of plunge directions which approximately parallels the direction of material transport within an antiformal sheet (Figure 13). Discussion This is to our knowledge the first documented example of an arcuate antiformal sheet intrusion. Other known arcuate intrusions possess characteristics of synformal sheets or arcuate diapirs (Schwerdtner 1976, Sutcliffe 1977, Schwerdtner et al in preparation). These studies of granitoid bodies demonstrate that posttectonic plutons often retain strained mineral fabrics as a consequence of emplacement. Those bodies which appear "massive" may possess a fabric that can be confirmed only by testing the magnetic fabric (e.g. King 1966). The presence of a strain fabric implies that granitoid magmas continue to flow during consolidation. The distribution of flow during the very last stage of consolidation may be evident from a map of strain intensity across the pluton. Figure 12 shows the approximately symmetric variation in the octahedral logarithmic shear strain, a measure of strain intensity where V - 2^ /"(In A ) 2 * (In IJ ) 2 * (In C^ 2 i ^ . 0 3 'B C A - It appears that the central core of the pluton preserved a much lower strain intensity as though rising as a single arcuate "plug", transferring much of the shear strain towards the margins during at least the final stage of consolidation. Finally, the study of the Greenwater Pluton demonstrates that proposed mechanisms for generating observed strain patterns can at least be qualitatively rppraised. We anticipate similar success in greenstone belts as strain models become available, (e.g. Dixon and Summers 1980). Summary of Conclusions We have examined the structural record of the Shebandowan belt by emphasizing the orientation and relative strength of development of mineral lineations. A review of Archean literature and government survey reports demonstrates that lineations are not consistently recorded (even by structural geologists) and are otherwise generally neglected. This may in part be due to the extra time required to obtain accurate preasurements in weakly-fissile rocks. Most lineations measured within the Shebandowan belt are visually subtle and easily dismissed during rapid examination. However subtle, these features constitute an intrinsic element of the total strain fabric and have provided us, in conjunction with other types of data, with the following general results and conclusions at this time: 1. A major phase of folding, D , appears to have developed across the full width of the belt and into the Quetico subprovince. This phase is characterized by a total strain fabric with its extension direction plunging to the west. 2. This was superimposed by a second regional deformation, the strain effects of which are confined to megascopically discrete domains and dominating the structurally more ductile lithologies including the Quetico sediments, 3. A third deformation, D-, is represented by mesoscopic kink folds within the northern half of the belt. This is related to late east-west compression and one should expect to find more bedding-parallel shearing in the northern half of the belt than in the south. 4. Most felsic intrusions have invaded the belt and its southern margin following the D^ phase of deformation. Their timing is characterized by their primary internal strain fabrics and contact strain aureoles imposed upon the volcanic envelopes. The one exception is the Shebandowan Pluton, which aqprobably intruded during D . 5. A regional pattern of strain domains is defined across the belt and the adjacent Quetico subprovince. This pattern features domains of D. total strain and other domains of cumulative strain arising from the superimposition of D~ upon D-. 6. The existence of these strain domains is confirmed by magnetic susceptibility anisotropy (MSA). Further, there is a general contrast in the relative prolateness of the susceptibility ellipsoid, and by inference, the rock strain ellipsoid; the major D. domain is characterized by less oblate total strain than the D2 domains. 7. The boundaries or discontinuities between domains appear, from field and MSA results, to have retained their coherency and avoided major dislocations. This seems to have been accomplished by increasing the oblateness of strain in the D. rocks close to the boundaries so as to conform more closely with the typical oblateness of strain in D2 domains. then is a zone. The effective boundary It is not as sharp as the rapid change in mineral lineation orientation would suggest. 8. Two models are suggested to accommodate different settings in which strain domains are observed: i) The concomitant development of strain domains producing a dislocation along the boundary; this is illustrated by the " M Larder Lake break along which gold is locally concentrated, ii) The sequential development of strain domains in which a deformation is locally superimposed upon an earlier regional deformation and produces strain domain patterns with coherent (non-dislocated) boundaries. 9. The Greenwater Pluton possesses a primary strain fabric that strongly suggests the body was emplaced as an antiformal crescentic sheet intrusion and not as an arcuate ridge diapir. This demonstrates a successful confirmation of an idealized strain model with a field example. As idealized models for greenstone belt strain patterns become more complex, it is hoped that similar comparisons may be applied to documented total strain patterns of actual greenstone belts. 10. The bearing of this study upon mineral exploration is as follows: a) The presence of fractures suitable for the hydrothermal concentration of precious metals may be explored in the vicinity of strain domain boundaries where they juxtapose lithostratigraphic hosts of metals. Their surface expression may not be exposed or their presence at depth may be inferred only from a coherent strain domain boundary at the surface. Such boundaries would probably not appear as lineaments and would require detailed mapping to define them. Many suitable targets may not be as pronounced in their surface expression as the Larder Lake "break". b) The stratigraphic and structural setting south of Lower Shebandowan Lake displays features that bear some limited resemblance to the Kirkland Lake area. Major strain domain boundaries lie in the proximity of the Shebandowan pluton and a Keewatin/"Timiskaming" unconformity. What is required for a viable exploration "mix" is the presence of suitable lithostratigraphic sources of gold For example, southwest of the Shebandowan Mine are found ultramafic units and associated carbonate facies iron formation (Morton 1979) that lie on or very close to a major strain discontinuity that has been locally offset by faulting. Carbonatization of stratigraphy has not been do c lament: id in this study, but the example above, nevertheless, illustrates the potential significance of juxtaposed discontinuities of regional strain. c) Ore deposits are likely to be rotated and extended in directions closely paralleling local extension directions of cumulative strain, Two examples in the Shebandowan belt appear to confirm this. The now abandoned North Coldstream Mine (Cu, Au, Ag) on Burchell Lake contained lenticular (baudinaged?) orebodies plunging eastward at about 50 (Giblin 1964) within an easterly-plunging D,, domain. The Shebandowan Ni-Cu Mine contains a long ribbon-shaped tabular orebody that plunges eastward parallel to the local extension directions of strain. Undiscovered orebodies in this belt can be predicted to have responded similarly to the local cumulative strain- This has obvious implications for geophysical exploration and drilling programs. 11. Finally, it is emphasized that this study is to our knowledge the first: to define regional pattern of strain domains for a greenstone belt; to demonstrate the value of magnetic susceptibility anisotropy for examining variations of strain on a regional scale; and (of more academic interest) to record the presence of an antiformal crescentic sheet intrusion. We are at present, continuing to examine additional aspects through support from an NSERCC Grant. REFERENCES Bau, A.F.S., 1975: Structures in the Kashabowie Upsala region, northwestern Ontario; Proceedings of the 1975 Geotraverse Workshop,Precambrian Research Group, University of Toronto, paper 14, p. 78-80. Beakhouse, G.P., 1974: Volcanic stratigraphy in the Greenwater-Upper Shebandowan Lakes Area, Northwestern Ontario; 1974 Annual Report, part 2, Centre for Precambrian Studies, University of Manitoba, p. 89-99. Ellwood, B.B., 1978: Measurement of anisotopy of magnetic susceptibility: A comparison of the precision of torque and spinner magnetometer systems for basaltic specimens; J. Phys. E. Sci. Instrum., vol. 11, p. 71-75. Davidson, D.M., Jr., 1980: Emplacement and deformation of the Archean Saganaga batholith, Vermilion District, northeastern Minnesota; Tectonophysics, v. 66, p. 179-195. Dixon, J.M., and Summers, J.M., 1980: A centrifuged model study of the tectonic development of Archean greenstone belts; Grant 68, p. 58-71. in Geoscience Research Grant Program, Summary of Research, 1979-1980, edited by E.G. Pye, Ontario Geological Survey, MP93, p. 262. Downes, M.J., 1980: Structural and stratigraphic aspects of gold mineralization in the Larder Lake area, Ontario; p. 92-103 in Roberts, R.G. (editor): Genesis cf Archean, Volcanic-Hosted Gold Deposits, Ontario Geologies.! Survey Open File Report 5293, p. 387. Flinn, D., 1965: On the symmetry principle and the deformation ellipsoid. Geological Magazine, v. 102, p. 36-45. Giblin, P.E., 1964: Rep. 19, 39 p. Burchell Lake Area; Ontario Department of Mines Geol. Hodgkinson, J.M., 1968: Geology of the Kashabowie Area; Ontario Department of Mines Geol. Rep. 35 p. King, R.T., 1966: p. 43-66i Magnetic fabric of some Irish granites; Geol. J., v.5, King, R.T., and Rees, A.I., 1962: The measurement of the anisotropy of Magnetic susceptibility of rocks by the Torque method; Jour. Geophys. Res., v. 67, p. 1565-1572. Means, W.D., 1976: Stress and Strain - Basic Concepts of Continuum Mechanics for Geologists; Springer-Verlag, New York, p. 339. - 23- Morin, J.A. 1973: Geology of the Lower Shebandowan Lake Area, District of Thunder Bay; Ontario Division of Mines Geol. Rep. 110, 45p. Morton, P., 1979: Volcanic stratigraphy in the Shebandowan Ni-Cu Mine Area, Ontario; p. 39-43 in Current Research, Part B, Geological Survey of Canada, Paper 79-1B. Ramberg, H., 1967: Gravity, deformation and the earth's crust (as studied by centrifuged models). Academic Press. London, England, .214p. Rathore, J.S., 1979: Magnetic susceptibility anisotropy in the Cambrian Slate Belt of North Wales and correlation with strain; Tectonophysics, v. 53, p. 83-97. Robin, P.-Y.F., 1977: Determination of geological strain using randomly oriented strain markers of any shape; Tectonophysics, v. 42, p. T7-T16. Schwerdtner, W.M., 1970: Hornblende lineations in Trout Lake area, Lac La Ronge map sheet, Saskatchewan; Can. J. Earth Sciences, vol. 7, p. 884-899. Schwerdtner, W.M., 1976: Remanent magnetization and magnetic susceptibility anisotropy measurement in Lac des Mille Lacs area of northwestern Ontario: Discussion; Can. J. Earth Sciences, v. 13, p. 493-494. Schwerdtner, W.M., Bennett, P.J., and Janes, T.W., 1977: Application of ' L-S fabric scheme to structural mapping and paleostrain analysis; Can. J. Earth Sciences, v. 14, p. 1021-1032. Schwerdtner, W.M., and Troeng, B., 1978: Strain distribution within arcuate diapiric ridges of silicone putty, Tectonophysics, v. 50, p. 13-28. Schwerdtner, W.M., Stone, D., Osadetz, K., Morgan, J., and Stott, G.M., 1979: Granitoid complexes and the Archean tectonic record in the southern part of northwestern Ontario; Can. J. Earth Sciences, v. 16, p. 1965-1977. Schwerdtner, W.M., Sutcliffe, R.H., and Stott, G.M., in preparation. Crescentic granitoid plutons in metavolcanic-metasedimentary terrains of the southern Canadian Shield. Shegelski, R.J., 1980: Archean cratonization, emergence and red bed development, Lake Shebandowan area, Canada; Precambrian Research, v. 12, p. 331-347. Stone, D.B., 1963: Anisotropic magnetic susceptibility measurements on a phonolite and on a folded metamorphic rock. Geophys. J., v. 7, p. 375-390 Sutcliffe, R.H., 1977: Geology and emplacement of the Jackfish Lake pluton, a major intrusion in the Rainy Lake dome. Proceedings of the 1977 Geotraverse Workshop, Precambrian Research Group, University of Toronto, p. 146-154. Tihor, L.A., and Crocket, J.H., 1977: Gold distribution in the Kirkland Lake - Larder Lake area, with emphasis on Kerr-Addison-type ore deposits - a progress report; p. 363-369 in Report of Activities, Part A, Geological Survey of Canada, Paper 77-1A. Trowell, N.F., Blackburn, C.E., and Edwards, G.R., 1980: Preliminary Geological Synthesis of the Savant Lake - Crow Lake Metavolcanic Metasedimentary Belt, Northwestern Ontario, and Its Bearing upon Mineral Exploration; Ontario Geological Survey, Miscellaneous Paper 89, 30p. 30 FIGURE CAPTIONS Figure l : Generalized summary of major strain domains, megascopic folds, lineation and foliation orientations. Figure 2 : Equal area stereograms showing a) D- donain lineations and b) D. domain lineations in the eastern half of the belt. Figure 3 : Equal area stereograms showing a) D 0 domain foliations and b) D domain foliations in the eastern half of the belt. Figure 4 : Sketch showing the discontinuity between strain domains obliquely transecting the stratigraphy southeast of Shebandowan Mine, (stratigraphy from Morton, 1979). Figure 5 : Equal area stereogram showing the westerly (D-,) and easterly (D.-) concentrations of MSA lineations for supracrustal samples. Steep north and south - plunging lineations tend to occur close to strain domain boundaries. Figure 6 : Variation of prolateness of the magnetic fabric with lineation plunge direction for mafic volcanic, gabbro and ultramafite samples. Note higher tendency to higher P value for rocks within the major D2 domain and decrease in P value close to strain domain boundaries. Figure 7 : Sketch illustrating the difference between coherent and incoherent strain domain boundaries. See text for description, (from Means, 1976). Figure 8 : Cross section of the Shebandowan Mine ore haulage incline showing change from westerly-plunging to easterly-plunging magnetic lineations as one crosses the boundary between strain domains from south to north. Note the greater variation in orientations within the D domain suggesting relict D., fabrics are locally preserved. P value increases for westerly-plunging lineations. The major discontinuity between strain domains probably lies close to the steep easterly-plunging lineations as shown. Figure 9 : Map showing the general geology and structural elements within and around the crescent-shaped Greenwater Pluton. -3! - Figure 10: Map of k values determined at stations within the Greenwater Pluton. Note the two zones of constriction. The smaller zone to the north is apparently due to the separate rise of magma behind a thin screen of partly assimilated volcanics along the north edge of Shelter Island., The strain pattern within the pluton is otherwise notably symmetric and contrasts with the asymmetric pattern of arcuate ridge diapirs (see text). Figure 11: Map showing the fanning pattern of steeply plunging mineral lineations within the Greenwater Pluton. This is typical of an idealized antiformal sheet intrusion. Note shallow lineations plunging away from the core of the gneiss dome which steepen towards the outer margins as shown in Figure 9. Figure 12: Map showing the distribution of strain intensity within the rock fabric of the Greenwater Pluton. Asymmetric increase in intensity towards the margins suggests that during the final stage of emplacement, the bulk of the shear strain was transferred towards the margins. Figure 13: A sketch illustrating the contrast in flow lines and resulting extension directions of the strain fabric between synformal and antiformal sheet instrusions. o 2a 141 Stations 2b 169 Stations 3a 178 Stations 3b 192 Stations D1 domain D2 domain 116 Stations coe ic to 'S O* a E SS 0 g 0) 5 i: o .2 4) Q t. ' "O'O g t 2 cf ? ? ? S o 2 i l A O w w i o O CM h. CO t- (/) CO S*\ O O o O p UJ l i O o UJ i* 5ac Points UJ o (0 O ^ 00 (O UJ ac D O iZ aoiovd d Ul X (C CC Ul ^ ft Q lu * 09 lu 2 2 S O O O 00 ffi ft: D O .E! ffi c .Eg cog E i o O) "O j* ,* O as o 2: E 2 o ~ 'S c — (Q 3 -S ** — o *-O) M-O o Of LU O O l ^ o "J z o ffi 3 9?z^- gz^ 2* ^ O u p >- i iu u-g o y gSgs:| g ia yy^ i| s| 5 il 8 e l si lil 1111 of O S DEG CSZ3 DiD CSD of "H s0|^ si A^^^o./ ^^ J *n is. < o *u s: — Q. — Q. UU C UJ o h- Q. CO O ir JD 1Z - - Q) " U *'g g W •J-f ^ 5^ O 1 o o -s H- O. CO y SYNFORMAL SHEET INTRUSION ANTIFORMAL SHEET INTRUSIO FIQUBG. 13
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