Accepted Manuscript Anatomy of the Archean Anshan iron ore belt in the North China Craton: A geophysical approach Lin-Fu Xue, Chuan-Qi Dai, Ming Zhu, M. Santosh, Ze-Yu Liu PII: DOI: Reference:
S0301-9268(17)30096-7 http://dx.doi.org/10.1016/j.precamres.2017.04.004 PRECAM 4721
To appear in:
Precambrian Research
Received Date: Revised Date: Accepted Date:
23 February 2017 21 March 2017 2 April 2017
Please cite this article as: L-F. Xue, C-Q. Dai, M. Zhu, M. Santosh, Z-Y. Liu, Anatomy of the Archean Anshan iron ore belt in the North China Craton: A geophysical approach, Precambrian Research (2017), doi: http://dx.doi.org/ 10.1016/j.precamres.2017.04.004
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1
Anatomy of the Archean Anshan iron ore belt in the
2
North China Craton: A geophysical approach
3
Lin-Fu Xuea, Chuan-Qi Daia, Ming Zhua, M. Santoshb,c, Ze-Yu Liua
4 a
College of Earth Sciences, Jilin University, Changchun 130061, P.R. China
5
6
7 8
b
Department of Earth Sciences, University of Adelaide, SA 5005, Australia
c
School of Earth Sciences and Resources, China University of Geosciences Beijing, 29 Xueyuan Road, Beijing 100083, China
9 10 11
* Corresponding author e-mail:
[email protected]
12
Abstract
13
The Anshan region of the North China Craton hosts significant iron ore
14
reserves in the form of Archean banded iron formations (BIF). This study
15
focuses on NW–SE trending layered iron ore bodies identified using
16
aeromagnetic data with a 500 m point spacing and a new method that
17
combines structural analysis with the 3D inversion of magnetic susceptibility.
18
This approach has identified two prominent parallel magnetic anomalies within
19
the study area, with the bottom boundary of BIF body I estimated to be at a
20
depth of ~ 5600 m and the bottom boundary of BIF body II at ~ 5200 m. The
21
two BIF iron ore bodies are separated by granitoids associated with the
22
Archean Anshan micro-continental nucleus. The area close to this
23
micro-continental nucleus has undergone significant tectonic deformation,
24
including ductile shearing. This shearing is the main control on the distribution
25
of BIF iron ore belts in the Anshan area, in contrast to the previous view which
26
folding was thought to control the distribution of BIF. Combining our new data
27
with regional tectonic information yields a model where both folding and ductile
28
shearing controlled the distribution of the main BIF ore bodies in the study area.
29
This model provides insights into the distribution of iron ores in the Anshan
30
area as well as a guide for future deep exploration in this region.
31 32
Keyword: Banded iron formation; Geophysical imaging; 3D inversion of
33
magnetic susceptibility; Fold-ductile shear deformation; Anshan area.
34
1. Introduction
35 36
Precambrian banded iron formations (BIFs) are of considerable economic
37
importance and are the source of 90% of global iron production. Research into
38
Chinese BIF from the 1950s onwards has revealed that the majority of BIF in
39
China are located along the edges of the North China Craton (NCC), 80% of
40
which formed during the Neoarchean. These BIF are associated with
41
metamorphosed volcanic rocks and minor amounts of metamorphosed
42
sedimentary rocks. The majority of the BIF iron deposits in China are Algoma
43
type
44
metamorphism and deformation (Zhai and Windley, 1990; Zhai et al., 1990;
45
Shen et al., 1994, 2006; Zhang et al., 2011). In particular, the Anshan and
46
Benxi areas have become the focus of an increasing amount of research, as
47
these areas host more than 60% of Chinese iron reserves (Zhou, 1994; Li et al.,
48
2014). The effect of tectonic deformation on the spatial distribution of iron ore
49
and the three-dimensional geometry of belts of iron ore mineralization are key
50
research topics in these regions.
and
have
undergone
significant
and
complex
post-formation
51
It has been recognized that the spatial distribution and three-dimensional
52
geometry of Archean BIF type iron ore belts over the world are the result of
53
complex tectonic processes. Tectonic analysis indicates that folding and
54
shearing-related deformation, and the rheology of individual rock units exerted
55
important influence on the distribution of the BIF type iron deposits of the
56
Hamersley Basin of Western Australia (Campana, 1966; Powell et al., 1999;
57
Barley et al., 1999; Brown et al., 2004; Lascelles, 2006). Investigations of the
58
role of rock rheology and deformation during the formation of high-grade
59
BIF-type iron ore in the Quadrilátero Ferrífero region of Brazil have identified
60
significant rock flows or fluid activity associated with ductile shearing (Lagoeiro,
61
1998; Rosière et al., 2001; Hippertt and Davis, 2000; Siemes et al., 2003,
62
2008). The BIF within the Anshan and Benxi areas has been subjected to
63
intense deformation and the effects of large-scale magmatism, meaning that
64
these units are dismembered and dispersed throughout the surrounding
65
tonalite–trondhjemite–granodiorite (TTG) gneisses. This in turn means that
66
assessing the spatial distribution of this mineralization during mineral
67
exploration has proven difficult. The factors controlling the spatial distribution
68
of BIF-related iron ore bodies remain controversial, and include: (1) the
69
presence of a dome or anticline in the Anshan area dominated by Neoarchean
70
supracrustal rocks with a core represented by the Tiejiashan granite and limbs
71
that host iron ore belts (Li, 1977); (2) the presence of a NW-plunging
72
anticlinorium within the ancient basement of the Anshan area with an axis
73
located near Tiejiashan (Zhou, 1987); (3) the presence of ductile shear zones
74
that control the spatial distribution of BIF and associated iron deposits (Xu,
75
1991; Zhang and Wang, 1994); and (4) a new tectonic model outlined by Li et
76
al., who suggested that this region records a sagduction. The complexity and
77
multiple phases of formation of the BIF in the Anshan area have been outlined
78
previously (Liu, 1987). This research also determined that the spatial
79
distribution of BIF in the Anshan area is controlled by folding, where thicker
80
orebodies are located proximal to fold hinges. However, few studies have
81
examined the role of widespread ductile shear zones on the concentration of
82
iron ore during the structural transposition of the original sedimentary units in
83
this area. Some of the banded structures within magnetite quartzites in this
84
area may have formed by this type of structural transposition. In addition, the
85
discontinuous iron ore belts within the Anshan and Benxi areas are hosted by
86
three giant ductile shear zones that control the thickening, attenuation, and
87
breaking or pinching out of the ore bodies (Xu, 1991; Zhang and Wang, 1994).
88
Several of the ore bodies contain dark magnetite quartzite units with mylonitic
89
textures that have undergone grainsize reduction as a result of ductile
90
shearing. Optical microscopy indicates that iron-bearing minerals and quartz in
91
these units have undergone intense deformation during ductile shearing and
92
show features that are indicative of recrystallization (Xu, 1987; Qu, 1988). The
93
surrounding rocks have also been converted to schists and mylonites as a
94
result of tectonic deformation. This indicates that although folding and ductile
95
shearing played important roles in the formation and spatial distribution of the
96
Anshan BIF iron ore bodies, the exact distribution and extent of the ore bodies
97
in this region remains unclear. Several previous studies have explored the
98
characteristics of the iron deposits in the Anshan area, including their
99
exploration potential. For example, Fan et al. (2014) inverted interactively
100
gravity and magnetic anomalies to identify several synformal iron ore bodies.
101
This study also analyzed aeromagnetic and gravity anomalies along a profile
102
through a proven iron deposit within the Dong’anshan–Qidashan district and
103
predicted the presence of large iron ore bodies at depth beneath the Anshan
104
area.
105
Combining the three-dimensional geophysical imaging of BIF iron ore
106
belts with structural analysis could be a powerful approach to determining the
107
processes that formed these belts as well as providing useful guidance for
108
mineral exploration. This study focuses on dissecting the deep geological
109
structure of BIF iron ore belts in the Anshan area, including determining the 3D
110
geometry of these belts, the tectonic processes that formed these deposits,
111
and the prospectivity of this area for deep-seated iron ore mineralization. This
112
approach uses a three-dimensional susceptibility inversion method that
113
employs high-resolution aeromagnetic data in combination with structural
114
analysis. Our results confirm the role of folding and ductile shearing in the
115
development of iron ore bodies, with the distribution of iron ore in highly
116
deformed areas (e.g., the Anshan area) being controlled by ductile shearing,
117
whereas the distribution of iron ore in moderately deformed areas is controlled
118
by both folding and ductile shearing. Finally, the distribution of iron ore in
119
weakly deformed areas is controlled mainly by folding. This study outlines a
120
formation model of BIF iron ore belts that provides a basis for further
121
investigations into the BIF-related iron ore belts in the Anshan area and similar
122
ore belts in other areas, particularly with respect to the exploration for and
123
evaluation of deep-seated iron ore.
124 125
2. Geological background
126 127
The Anshan area is located in the eastern NCC and has a double-layered
128
crustal structure that consists of Archean crystalline basement and a
129
Neoproterozoic–Paleozoic
130
crystalline basement or micro-continental nucleus is dominated by the
131
Neoarchean Anshan Group (2.5 – 2.6 Ga), including the Yingtaoyuan (2530 –
132
2551 Ma), Cigou (2523 – 2571 Ma), and Dayugou formations, and a series of
133
tonalite–trondhjemite–granodiorite gneisses. The basement is overlain by
134
Paleoproterozoic greenschist facies (2469 ± 23 Ma) metamorphic rocks of the
135
Liaohe Group (Dai et al., 2013) that are different from the traditional
136
designation of this group (Li SZ et al., 2005, 2007, 2012). The majority of the
137
iron ore in this area is hosted by BIF within the Yingtaoyuan Formation of the
138
Anshan Group (Zhang, 1988; Zhou, 1994). The upper units within this
139
formation consist of sericite, chlorite, and biotite–quartz phyllites that are
140
unconformably overlain by units of the Neoproterozoic Qingbaikou System.
141
The lower part of the Yingtaoyuan Formation is dominated by chlorite, iron
142
ore–chlorite, sericite–chlorite, and biotite phyllites as well as sericite–quartz
143
schists. The Dayugou Formation contains felsic granulite and amphibolite units,
sedimentary cover
sequence. The Archean
144
lenses
of
magnetite-bearing
quartzite,
145
tremolite–epidote–diopside
146
unconformably underlain by the Tiejiashan granite (2.9Ga) that in turn is
147
cross-cut by the later Qidashan granite (2.5 Ga) (Fig. 1).
granulite
and
units.
layers The
of
Anshan
marble Group
and is
148
Two iron ore belts, the northern iron ore belt (ore belt I), The southern ore
149
belt (ore belt II), have been identified in the Anshan area (Fig.2), with the
150
northern iron ore belt (ore belt I) trending NW–SE (330°-340°) and dipping
151
near vertically (60°-85°). This belt contains (from north to south) the Qidashan,
152
Chentaigou, Wangjiapuzi, Hujiamiaozi, and Yanqianshan iron ores. Ore belt I
153
extends more than 14.5 km and contains main ore bodies with thicknesses of
154
100–300 m. The tops of these main ore bodies are characterized by an
155
oxidized hematite quartzite layer that has a thickness of a few hundreds of
156
meters. The main ore bodies beneath the oxidized ore belt are dominated by
157
magnetite and chlorite–magnetite quartzite units.
158
The southern ore belt (ore belt II) trends nearly E–W, although the iron
159
ores in this area trend NW–SE (330°-340°) and show significant variations in
160
dip (30°-80°). This belt contains (from east to west) the Dagushan, Heishilazi,
161
Dong’anshan, and Xi’anshan iron ores, with an overall extent of >2.5 km.
162
Single ore bodies within this belt have thicknesses of 90–300 m and a thin ore
163
body is also present within the units above the main Dagushan iron ore. The
164
belt is surrounded by phyllite and schist units with minor amounts of granulites
165
and amphibolites. The area contains a buried hematite–quartzite layer with a
166
thickness of 300 – 500 m as well as non-exposed magnetite quartzite and
167
amphibole–magnetite quartzite units, and minor amounts of chlorite–magnetite
168
quartzite.
169
This region also records widespread Neoarchean magmatic intrusive
170
activity, including the successive emplacement of the Lishan trondhjemite and
171
Tiejiashan monzonitic granites. These intrusions define a TTG rock series that
172
includes quartz diorite, tonalite, granodiorite, and trondhjemite units, together
173
with calc-alkaline monzonitic granites. These intrusions disrupted and
174
fragmented the Neoarchean Anshan group rocks that are preserved as islands
175
within the intrusive complex.
176
Three phases of Archean deformation have been identified in the study
177
area (Guo, 1994): (1) an initial phase of tectonic deformation during
178
2900–2800 Ma, including the generation of a NE–SW trending gneissosity
179
within granites as well as closed isoclinal folds with prominent axial planar
180
schistosity within supracrustal rocks; (2) a second phase at 2500 Ma that
181
generated NNW–SSE and E–W trending ductile shear zones and imparting
182
schistosity to the iron-bearing units along the ductile shear zones; and (3) a
183
third phase at 2000 Ma involving shallow ductile shearing and overprinting
184
deformation. The unique tectonic history of this area means that the BIF
185
records several superimposed tectonic events that generated significant
186
internal deformation (Yang et al., 1983; Zhang et al., 1986; Xu, 1991; Zhang
187
and Wang, 1994). These three stages of deformation are consistent with the
188
known major tectonic events in the NCC that were associated with Archean
189
microcontinental amalgamation, Paleoproterozoic subduction and collision (Li
190
et al., 2007, 2012), and Mesozoic reactivation (Zhai and Santosh, 2011; Zhao
191
and Zhai, 2013; Yang et al., 2016; Yang and Santosh, 2015; 2017).
192 193
3. Data and processing
194
3.1 Aeromagnetic data
195 196
Two aeromagnetic surveys were undertaken in the Anshan region, the first
197
of which involved a survey with a distance between measuring points of ~2 km
198
whereas the second survey had a distance between measuring points of 0.5
199
km. Both surveys involved a slowly rising and falling terrain flight method with
200
an average altitude of 200 m in order to obtain high-resolution data, with the
201
altitude fixed using an equivalent source filtering noise-reduction approach
202
(Zeng, 2005).
203
Typically the data obtained from a magnetic survey are a set of magnetic
204
field measurements acquired within an above-surface 2D grid within the
205
volume of interest. These data are first processed to yield an estimate of the
206
anomalous magnetic field that is the result of the magnetically susceptible
207
material in the area. This is followed by inversion, an approach that aims to
208
derive quantitative information about the distribution of magnetically
209
susceptible material in the ground from the extracted anomaly data, meaning
210
that the extracted residual anomaly data are the main input for the inversion
211
program used. Buried magnetically susceptible material has a certain amount
212
of natural remanent magnetization, and the data used for the inversion indicate
213
the strength of the local magnetic field overprinted on the regional magnetic
214
field. Here, we assume that no remanent magnetization is present in the study
215
area and as such restrict our attention to the presence of induced
216
magnetization.
217
218
3.2 Physical properties of rocks
219
220
The magnetite quartzite units within the Yingtaoyuan Formation have
221
magnetic susceptibility values as high as 552,600 × 10−6 CGSM with remanent
222
magnetism values up to 3,052,800 × 10−6 CGSM. These values are much
223
higher than the values for the plagioclase amphibolite-hosted Fe-poor
224
quartzites of the Cigou Formation, primarily as the phyllitic rocks and
225
plagioclase amphibolites are either non-magnetic or are only weakly magnetic.
226
In addition, the banded magnetic quartzite within the Anshan Group has
227
magnetic susceptibility values of 3000–100,000 × 4π× 10−6 SI, whereas the
228
sedimentary cover is non-magnetic.
229
230
4. Aeromagnetic anomaly features
231 232
The Anshan region shows a clear high aeromagnetic anomaly zone,
233
although closer examination using a 1:50,000-scale aeromagnetic anomaly
234
map reveals that this anomaly is actually composed of the parallel NW–SE
235
trending high magnetic anomaly belts I and II (Fig.2). The relationships
236
between aeromagnetic anomalies and geological formations (Fig. 1) in the
237
study area indicate that magnetic anomaly belt I is delineated by the 0
238
aeromagnetic anomaly isoline and is closely related to areas with known iron
239
ore belts or BIF. In comparison, the region containing magnetic anomaly belt II
240
is covered by Quaternary formations. The Tiejiashan intrusions are located
241
between the two high magnetic anomaly belts, are associated with a region
242
with a low magnetic anomaly, and form the basement of the BIF in this area.
243
Reducing the magnetic anomaly data to a pole figure (Fig. 2) using areas
244
with known iron mineralization (Table 2) indicates that all of the known iron
245
mineralization in the study area is located in the region with a high magnetic
246
anomaly. The aeromagnetic anomalies associated with the southern ore belt
247
slightly overlap with the high magnetic anomaly belt II and are also associated
248
with known areas of mineralization that define an overall E–W trending belt,
249
despite the fact that the long axes of individual aeromagnetic anomalies
250
extend NW–SE to NNW–SSE. In addition, the eastern Tiejiashan granites are
251
associated with relatively closely spaced aeromagnetic anomaly contours,
252
whereas the western and northern parts of these intrusions are associated with
253
relatively widely spaced anomaly contours.
254
Reduced-to-pole aeromagnetic anomaly data for the study area yield
255
different upward continuation (Fig. 3) heights that highlight the northeastern
256
negative magnetic anomaly. This anomaly is associated with magnetic body I
257
and suggests that this orebody dips to the NE. All of the mineralization within
258
the Qidashan (32), Hujiamiaozi (35), Wangjiapuzi (33), Zhangjiawan (27),
259
Lazishan (26), Guanmenshan (36), and Yanqianshan (2) iron ores (Table 2) in
260
magnetic body I dip steeply to the NE or to the ENE. The 3D magnetic
261
susceptibility inversion model contains the same NE dip that is present in
262
magnetic body I. In addition, the high magnetic anomaly values associated
263
with magnetic bodies I and II disappear with increasing height, whereas the
264
northern magnetic anomaly remains consistently high, indicating that the
265
southern magnetic body I is located at a shallow depth whereas the northern
266
magnetic bodies are located at a deep depth. The northern magnetic bodies I
267
and II coalesce at a height of 3000 m, suggesting they may be connected at
268
depth. These bodies form a circular magnetic high at a height of 9000 m and
269
do not close at a height of 20,000 m, suggesting that this reflects the regional
270
background magnetic field. The basement slopes and extends towards the NE,
271
with a low magnetic anomaly region in the northeastern and southwestern
272
parts of the study area (Fig. 3).
273
274
5. 3D inversion of magnetic susceptibility
275
5.1 3D inversion method of magnetic susceptibility
276 277
The geometry of BIF bands obtained using a 3D inversion of the magnetic
278
susceptibility data yields a 3D image that provides important information on the
279
evolution and distribution of iron ore in this region. The regional aeromagnetic
280
anomalies suggest that the 3D inversion of magnetic susceptibility reflects the
281
presence of an underground magnetic body. The 3D inversion program
282
operates by simultaneously minimizing the model objective function while
283
generating a synthetic dataset that adequately fits the collected data (Li and
284
Oldenburg, 1998). The model is then specified using a mesh of rectangular
285
cells, each with a constant susceptibility value, with magnetic responses
286
calculated for any location within the model volume. The airborne magnetic
287
data were also inverted in order to construct 3D susceptibility contrast models.
288
These data were reduced using standard regional–residual separation
289
techniques such as wavelength filtering (Li and Oldenburg, 1998), with
290
inversions performed until the synthetic data agree with the collected data
291
within a degree of misfit calculated using the statistical attributes of the data.
292
The model objective function is minimized by generating a magnetic anomaly
293
that is close to the reference model and is smooth in all three spatial
294
directions. We used the UBC-GIF inversion code, which incorporates a depth
295
weighting function that counteracts natural kernel decay (Li and Oldenburg,
296
1998). These data are first processed to yield an estimate of the anomalous
297
field generated by the magnetically susceptible material in the area. The goal
298
of the magnetic inversion is to obtain quantitative information about the
299
distribution of magnetic susceptibilities in the ground from the extracted
300
anomaly data, indicating that the input for the inversion program is assumed to
301
be the extracted residual anomaly data.
302 303
5.2 3D magnetic susceptibility inversion in Anshan
304 305
Buried magnetically susceptible material contains a given amount of
306
natural remanent magnetization. Our inversion incorporates the local magnetic
307
field separately to the regional magnetic field, allowing us to assume that no
308
remanent magnetization is present and enabling this modeling to focus on
309
induced magnetization. An upward continuation of 25,000 m is used as the
310
background of local field extraction with 1:50,000 local field magnetic anomaly
311
data inverted using the UBC Mag3D software package. This inversion used a
312
horizontal mesh subdivision value of 350 × 350 m with E–W profiles divided
313
into 162 grid cells and N–S profiles divided into 112 grid cells. Three of these
314
grids were extended with widths of 350, 700, and 1400 m, with an internal
315
depth subdivision of 175 m divided into 85 grid cells. The total number of grid
316
subdivisions is 1,685,040, including 168 E–W nodes, 118 N–S nodes, and 85
317
depth nodes.
318
The 3D magnetic susceptibility model for the Anshan area was obtained
319
after 60 iterations, yielding a 3D inversion map of magnetic susceptibility in the
320
Anshan area and an E–W cross-section. The map indicates that the Tiejiashan
321
granites are surrounded by high magnetic anomalies associated with magnetic
322
bodies I and II, and the 3D inversion model should conform to this. We
323
combined geophysical and geological data and selected a value of 0.14 as a
324
cut-off, with this value used during the 3D geological inversion of the magnetic
325
material within the study area (Fig. 4).
326
The 3D magnetic susceptibility inversion indicates that the top parts of
327
buried magnetic bodies I and II are located at a depth of ~300 m. The northern
328
magnetic bodies are located deeper than the southern bodies, with a bottom
329
interface burial depth of ~7000 m. Magnetic bodies I and II (Fig. 4) are
330
centered on the Tiejiashan granites, have a ring-shaped distribution, and are
331
located in the northwestern part of the study area. The 3D magnetic
332
susceptibility inversion indicates that magnetic body I dips to the NE with a dip
333
angle that is spatially variable. In comparison, the southern magnetic body
334
initially dips more gently, although this dip steepens to the north before
335
eventually becoming nearly vertical. The inversion also highlights a small
336
branch of southern magnetic body II that has a “U”-shaped connection with the
337
rest of the body before having a distorted central section with a middle domain
338
deeper than the end parts of this branch. Finally, the sections of magnetic body
339
II change from flat to elliptical with increasing distance from south to north.
340 341
6. Discussion
342
6.1 Formation mode of the BIF iron ore belt
343
6.1.1 Formation mechanism of the BIF iron ore belt
344 345
Different regions of the study area are associated with differently
346
deformed BIF, with magnetite quartzite in the Anshan area having a streaky
347
and banded structure that is defined by folded streaks and bands. The
348
deformation of quartz and magnetite within these units is also clearly visible
349
during optical microscopy. These rocks record ductile deformation and
350
recrystallization that has transformed the iron ore into a fine-grained
351
ferruginous–quartzose mylonite containing a well-developed foliation. Many of
352
the iron ore layers and over- and underlying units are also intensely deformed
353
and define ductile shear zones that impart a parallel banded structure to these
354
iron ore bodies. The bands within the ore bodies appear to be the original
355
sedimentary layers although they have been tectonically sliced. The
356
composition of this material, combined with structural and sequence
357
relationships, suggests that the original iron-bearing formation has been
358
essentially obliterated by multi-phase post-formation deformational events.
359
The Anshan area does not contain intensely developed fold structures
360
although mineralization in the Waitoushan area of the northern Anshan region
361
is associated with folds of various sizes (Yang et al., 1983). The BIF iron ore
362
belts in this area are considered to be tectonic deformation zones that record
363
strong ductile deformation in regions of compression, but have only undergone
364
folding in areas recording only weak deformation, with intermediate domains
365
that record moderate tectonic compression containing zones of folding of
366
various intensities as well as ductile shear zones.
367
The 3D magnetic susceptibility inversion has identified two NW–SE
368
trending tabular BIF bodies within the Anshan area (Figs. 4 and 5). The bottom
369
depth of these tabular bodies lies at ~7 km and these bodies have complex
370
internal structures relating to the intercalation of BIF with surrounding units.
371
These data suggest that the formation of the BIF iron ore belts is closely
372
related to both folding and ductile shearing. The location of BIF-related iron ore
373
belts is controlled by folding in areas with well-developed folds, whereas the
374
main control on the location of this type of mineralization is ductile shearing in
375
areas with more intense deformation. The BIF in the Anshan area clearly
376
records ductile shearing, suggesting that the formation of the BIF iron ore belts
377
was controlled mainly by this shearing.
378 379
6.1.2 Favorable sites for BIF iron ore belt
380 381
A composite multi-phase intrusion crops out between northern iron ore
382
belt I and the concealed northwestern iron ore belt II (Figs.1 and 2). This
383
composite intrusion includes the Chentaigou (3.3 Ga), Lishan (3.0 Ga),
384
Tiejiashan (2.9 Ga), and Dong’anshan (3.0 Ga) plutons (Wan, 2001), all of
385
which are older than the BIF in this area and are considered to be part of an
386
Archean microcontinent block. The formation of the ancient continental
387
nucleus and micro-continental blocks in this area might have occurred prior to
388
3.0 Ga, with dating of granite gneisses in the Anshan area indicating that the
389
Anshan micro-continental nucleus, one of the ancient Archean continental
390
nuclei of the NCC, formed at ~ 3.3 Ga (Wu et al., 2008). The formation of this
391
micro-continental block was followed by continental crustal accretion events at
392
2.9–2.7 Ga and tectonic deformation, metamorphic, and magmatic events at
393
2.5 Ga (e.g., the formation of the granitic Qidashan Pluton). The latter event
394
marks the splicing and cratonization of micro-continental blocks within northern
395
China during 2600 to 2500 Ma during a sequence of continent–continent,
396
continent–arc, and arc–arc collisions. Smaller arcs could also have been
397
present at this time that were not involved in the accretion and formation of this
398
micro-continental block collage, an event that is locally known as the Anshan
399
movement (Zhao et al., 1993; Bai et al., 1993; Cheng, 1994; Wu et al., 1998;
400
Zhai, 2010). The margins of the Anshan micro-continental nucleus underwent
401
intense deformation during the middle to late Neoarchean, as evidenced by the
402
presence of near-vertical schistosity within magnetite quartzite units as well as
403
broad and gentle folds, and small-scale ductile shear zones within zones of
404
weaker deformation. Areas with large-scale TTG intrusive magmatism
405
associated with significant tectonic deformation contain magnetite quartzite
406
units that also have a near-vertical schistosity. These rocks are largely
407
well-preserved despite the multiple pulses of magmatism (Fig. 6). However,
408
the BIF are more plastic and are more easily dismembered and destroyed,
409
meaning that composite fold–ductile shear zones are more widespread within
410
the northeastern and southwestern sides of the micro-continental nucleus, and
411
represent areas that were more favorable for the development of BIF ore belts.
412 413
6.1.3 Influence of the later structures on the BIF distribution
414 415
The southern ore belt (ore belt II) trends E–W although the majority of the
416
iron ore bodies within ore belt II trend NW–SE as a result of activity along the
417
Mesozoic Hanling–Pianling strike-slip fault. This southern ore belt does not
418
show a significant aeromagnetic anomaly within the map produced during this
419
study, with the upward continuation of the belt nearly disappearing at a height
420
of 3000 m (Fig. 3). This suggests that the iron-bearing lithological units (i.e.,
421
magnetic bodies) within this southern ore belt are shallow and small. The
422
southern ore belt also contains the aforementioned Hanling–Pianling Fault, a
423
feature that also cross-cuts and offsets the northwestern BIF. Some of the BIF
424
fragments within the southern ore belt also trend NW–SE, and the entirety of
425
this southern ore belt was the result of post-formation strike-slip movements
426
that affected the northwestern part of the BIF iron ore belts.
427
428
6.1.4 Formation mode of the BIF ore belt
429 430
The intense folding and contemporaneous intrusion of TTG rocks during
431
the late Neoarchean, and subsequent Mesoproterozoic and Mesozoic uplift
432
events dismembered and significantly denuded the BIF within the study area.
433
This means that the only BIF present in this area is relicts within the
434
widespread TTG gneisses, making it difficult to determine the original
435
distribution of these BIF. Existing models suggests that the preserved BIF in
436
this area was originally part of the folds, forming the cores or limbs of
437
preserved synclinal folds of parts of hook-shaped folds. The northern ore belt
438
has a monoclinal structure although the counterpart to this structure has not
439
been identified. Although the prevailing view is that the spatial distribution of
440
BIF and associated iron ore bodies is controlled primarily by fold structures,
441
these models cannot effectively explain the ductile shearing that is commonly
442
found in these iron formations, the fact that a tabular BIF body with an extent of
443
nearly 12 km does not contain any macro-scale folding, and the fact that
444
lenticular ore bodies occur intermittently throughout the ore belt. Here, we
445
combine our new data with previous research to develop a composite
446
fold–ductile shearing model that provides insights into the controls on the
447
spatial distribution of BIF iron ore belts (Fig. 6).
448
Significant NE–SW compression during the middle–late Neoarchean
449
affected the BIF in the study area. These ferruginous rocks behave plastically
450
at high temperatures, meaning that increased compression caused ductile
451
shear zones to develop along fold limbs. The initial stages of shearing were
452
associated with divergent ductile shear zone and fold axial surface directions
453
that changed with increasing compression, leading to the closing of folds and
454
the movement of the ductile shear zones towards being parallel with the fold
455
axial surfaces (Fig. 6). This sagduction-related process (Li et al., 2015a, b, c, d,
456
e, 2017) of folding and ductile shearing caused the squashing and expansion
457
of BIF within fold hinge zones, a process that can explain the hook-shaped or
458
tabular bodies in the study area. The limbs of folds that underwent intense
459
ductile shearing are also preferentially enriched with iron ore, as evidenced by
460
the high grade tabular bodies. Increased compression caused fold limbs to
461
become parallel, eventually forming closed folds with near-vertical axial
462
surfaces and a series of ductile shear zones. These structures further evolved
463
to large-scale ductile shear zones. This enhanced compression occurred
464
within the
465
micro-continental nucleus, forming areas of iron-enriched ductile shear zones
466
that correspond to aeromagnetic anomaly belt I as well as the northern ore belt
467
(Fig. 6).
northeastern
and southwestern domains
of the Anshan
468 469
6.2 Spatial distribution of the BIF
470 471
The cross-section provided in this study was constructed using drill hole
472
data and provides evidence of a structural configuration comprising
473
iron-bearing units within a closed fold. The BIF in this area is interlayered with
474
schists that decrease in frequency with increasing depth and are thought to
475
represent part of the original formation. This suggests that the iron ore bodies
476
form thick tabular-shaped units that extend to significant depths, indicating in
477
turn that this region is highly prospective for deep-seated iron mineralization
478
(Fan et al., 2013).
479
The fold–ductile shearing composite model for the Anshan area indicates
480
that the BIF ore belts are a series of synclines, anticlines, and ductile shear
481
zones, with different layers of iron-bearing units repeatedly appearing within
482
fold–ductile shear zones. The different iron-bearing layers and interlayers may
483
be the result of the same unit undergoing repeated folding and ductile shearing.
484
The original iron-rich BIF layers had transformed to discontinuous ore bodies
485
by the end of the Neoarchean as a result of intense folding and ductile
486
shearing. These iron ore bodies are generally located within composite
487
structural zones, and the bottom of the iron mineralization appears to be
488
dependent on the depth of development of closed folds and ductile shears.
489
Combining the 3D magnetic susceptibility inversion with the new genetic model
490
for the formation of BIF ore belts suggests that the BIF magnetic body
491
corresponding to aeromagnetic anomaly I (i.e., ore belt I) is tabular and formed
492
as a result of folding and ductile shearing. This BIF body has characteristics
493
that are indicative of formation within a ductile shear zone, and the shallow and
494
deep parts of the body have similar features, suggesting they formed as a
495
result of the same processes. The bottom of this body is located at ~5200 m,
496
suggesting this area has significant deep exploration potential. The BIF
497
magnetic body corresponding to aeromagnetic anomaly II (i.e., ore belt II) has
498
the same characteristics as iron ore belt I, with a bottom depth (~5600 m) that
499
again is indicative of significant deep exploration potential. In comparison, the
500
bottom boundary of the magnetic body in the southern ore belt (i.e., iron ore
501
belt II) is at a depth of ~3000 m. The fact that this belt consists of fragments of
502
the main ore belt that were dismembered during the Mesozoic suggests that
503
this belt has a shallower bottom depth with only limited potential for deep
504
exploration.
505 506
7. Conclusions
507 508
(1) The spatial distribution of BIF and iron ore bodies in the Anshan area is
509
controlled by folding and ductile shearing. Ductile shearing is the dominant
510
control on the distribution and geometry of BIF close to the Anshan
511
micro-continental nucleus. Both folding and ductile shearing have
512
enhanced iron ore grades. Potential iron ore bodies are generally located
513
within large-scale BIF-hosted ductile shear zones that record intense
514
deformation.
515
(2) The two tabular BIFs within the Anshan area extend NW–SE and dip to the
516
NE. The bottom of tabular body I is located at a depth of ~5200 m, whereas
517
the bottom of tabular body II is located at a depth of ~5600 m. These two
518
bodies developed separately within the northeastern and southwestern
519
sides of the Archean Anshan micro-continental nucleus. Both bodies are
520
associated with ductile shear zones and have significant deep exploration
521
potential.
522
(3) The southern ore belt consists of BIF fragments derived from the
523
northwestern ore belt and is cross-cut by strike-slip faults. These fragments
524
are generally shallow and have only limited potential for deep exploration.
525
Acknowledgments
526
We thank the editor and two referees for their valuable suggestions and
527
comments that improved our manuscript. Thanks to Prof. Sanzhong Li for his
528
kind comments on Fig. 6. This research is funded by a pilot project “Deep
529
Geological Survey of Benxi-Linjiang area” (Project No. 1212011220247), from
530
3D geological mapping and deep geological survey of China Geological
531
Survey.
532 533
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Xu, G.R., Chen, H.J., 1984. A preliminary study of komatiites in Anshan – Benxi
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Xu, Y.G., 1987. Transformation of BIF-Type iron deposit in ductile zone,
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of Geology 17(3), 283-292.
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Xu, Z.Y., 1991. The origin and evolution of the banded structure in Archaean
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Yang, X.Q., Zhang, Z.H., Duan, S.G., et al., 2015. Petrological and
841
geochemical features of the Jingtieshan banded iron formation (BIF): A
842
unique type of BIF from the Northern Qilian Orogenic Belt, NW China.
843
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844
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845
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848
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Liaoning Province. Journal of Changchun University of Earth Science 2,
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iron deposit, Liaoning, China. Contributions to Geology and Mineral
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demagnetization -–a case study at the Mussel white Mine, Ontario,
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their
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and
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Anshan area, Liaoning Province. Journal of Changchun University of
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Earth Science 2, 47-56.
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Zhang, B.H., Qu, F.X., 1996. Control of polyphase folds and structural transposition. Geology & Prospecting 32(6), 12-16. Zhang, J., 2009. Research on Typical Mineral Deposit of Xi-Anshan Iron Ore and Deep Forecast to “An-Shan-Type” Iron Ore. Jilin University.
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Metamorphism in Ural Mountain Area, North China Craton: SHRIMP
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F., 2011. Formation age and tectonic setting of the Shirengou
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BIF-iron deposits in the North China Craton: Progresses and questions.
895
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Zhang, L.C., Dai, Y. P., Wang, C. L., et al., 2014. Age, Material Sources and
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Formation Setting of Precambrian BIFs Iron Deposits in Anshan-Benxi
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Area. Journal of Earth Sciences and Environment 36(4), 1-15.
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characteristics and ore-searching guides of the iron deposits in
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Anshan-Benxi area, Liaoning Province. Geology & Resources 21(6),
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516-521.
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Zhang, Q.S., 1988. Early crust and mineral deposits of Liaodong peninsula, China. Geological Publishing House.
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Zhang, R.H., Wang, S.L., 1994. A new viewpoint about iron ore deposit:
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Controlled by ductile shear zones at Waitoushan. Contributions to
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Geology and Mineral Resources Research 9(4), 57-62.
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Zhang, Z., Liu, J.M., Yu, C.M., et al., 2013. Application of integrated
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geophysical prospecting methods in the evaluation of BIF deposits-a
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case study in Inner Mongolia AohanqiSijiazi BIF deposits. Progress in
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Geophysics 28(4), 2078-2084.
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Zhao, G.C., Zhai, M.G., 2013. Lithotectonic elements of Precambrian
913
basement in the North China Craton: review and tectonic implications.
914
Gondwana Research 23, 1207–1240.
915 916 917 918 919 920
Zhao, Y.M., 2013. Main genetic types and geological characteristics of iron-rich ore deposits in China. Mineral Deposits 32(4), 685-704. Zhao, Z.H., 2010. Banded iron formation and related great oxidation event. Earth Science Frontiers 17(2), 1-12. Zhao, Z.P., Zhai, M.G., Wang, K.Y., Yan, Y.H., et al., 1993. Precambrian crustal evolution of the Sino-Korean Paraplatform. Beijing: Science Press.
921
Zheng, J.Q., Zhang, B.H., Cai, Y.T., Cui, W.Z., Zhang, W.B., Liu, R.Q., 1986.
922
Tectonic characteristics of the Archean Anshan group and their effects
923
on iron ore deposits in area of Beitai to Waitoushan, Benxi, Liaoning
924
Province. Contributions to Geology & Mineral Resources Research 1(1),
925
20-29.
926
Zhou, S.T., 1987. The petrochemical study of the Archean banded iron deposit
927
in Anshan-Benxi district, Liaoning Province. Bulletin of the Chinese
928
academy of Geological Sciences 16, 139-152.
929 930 931 932
Zhou, S.T., 1994. Geology of the BIF in Anshan-Benxi Area. Beijing: Geological Publishing House 1-277. Zhu, K., 2016. The formation and evolution of the Archean greenstone belt in the Anshan-Benxi area. Jilin University.
933
Figure captions
934
Fig. 1. Simplified geological map of the Anshan area. The inset shows the
935
location of the study area.
936 937
Fig. 2. A 1:50,000 scale reduced-to-pole magnetic anomaly map showing the
938
location of known iron ore deposits (triangles).
939 940
Fig. 3. Images showing the upward continuation of reduced-to-pole magnetic
941
anomaly data for the study area: (a) Location of the two main highly magnetic
942
anomalies associated with magnetic bodies I and II. (b) A 1000 m upward
943
continuation map showing a smoothing of the shapes of the main magnetic
944
bodies and the disappearance of some minor highly magnetic anomalies. (c) A
945
3000 m upward continuation map showing the coalescence of northern
946
magnetic bodies I and II, suggesting they may be connected at depth. (d) A
947
5000 m upward continuation map showing an enlargement of the coalesced
948
part of magnetic bodies I and II and the disappearance of all of the weaker
949
magnetic anomalies. (e) A 7000 m upward continuation map showing magnetic
950
bodies I and II forming a circular magnetic high. (f) A 9000 m upward
951
continuation map showing magnetic bodies I and II forming a circular magnetic
952
high. (h) A 20,000 m upward continuation map showing that the areas of
953
magnetic bodies I and II remain open.
954
955
Fig. 4. 3D magnetic susceptibility inversion for the Anshan area.
956 957
Fig. 5. E–W cross-section showing the distribution of iron formations within the
958
Anshan area.
959 960
Fig. 6. Model of the formation of BIF iron ore belts by folding and ductile
961
shearing within the Anshan area. (a) Initial formation of BIF during the
962
Neoarchean (2.6–2.5 Ga). (b) Initial folding of BIF in the Anshan area was
963
followed by significant compression near the Anshan micro-continental
964
nucleus, generating ductile shear zones (2.52–2.47 Ga). (c) Further intense
965
folding and ductile shearing led to the coalescence of several ductile shear
966
zones and the generation of wider ductile shear zones near the Anshan
967
micro-continental nucleus. This process concentrated iron mineralization
968
within the resulting ductile shear zones and formed the BIF-hosted iron ores in
969
the study area. This was followed by large-scale magmatism at the end of the
970
Neoarchean (2.5 Ga) that disrupted the BIF.
971 972
Fig. 7. Map and cross-section showing the location of iron ore in the study area.
973
The cross-section is based on drilling data from the Anshan area and shows a
974
structural configuration where iron-bearing units are hosted by a closed fold
975
that is indicative of intense deformation of the BIF in this region. Schistose
976
rocks are present as interlayers within the BIF, decreasing in number with
977 978
depth. The interlayers are generally thought to be part of the original protolith.
979 980
981 982
983 984
985 986
987 988
989 990
991 992
993
lithostratigraphic
main lithology
magnetic
remanent
susceptibility
magnetism
(4π×10−6SI)
(10−3A/m)
0–4100
0–3700
biotite–granulite
383–625
73–101
gneiss
80–57000
21–14900
magnetite
2000–61000
2900–479000
unit
Cigou formation
plagioclase amphibolite
quartzite Yingtaoyuan
phyllite
0–7360
250–3700
formation
magnetite
3000–100000
20000–50000
quartzite Table1.magnetic susceptibility of main rocks
994 995
number
iron ore
strike
dip
dip angle
32
Qidashan
305°-335°
SW,NE
70°-90°
35
Hujiamiaozi
145°-165°
NE-SW
80°-90°
33
Wangjiapuzi
310°-335°
SW,NE
70°-90°
27
Zhangjiawan
110°-290°
S-NE
65°-90°
26
Lazishan
100°-135°
NE
50°-80°
36
Gumenshan
275°-285°
NE
70°-85°
2
Yanqianshan
NNW
NEE
48°-90°
31
Dagushan
310°-315°
NE
60°-75°
38
Heishilazi
70°
NW-SE
75°-85°
37
Dong’anshanxiangqianyu
EW
S
25°-30°
24
Xi’anshan
NW-SE
NE
20°-47°
25
Dong’anshan
NW
NE
65°
996 997 998
29
Huolongzhai
30
Xiaolingzi
5
Zhanchigou
EW
NE
N
30°-80°
NW
42°-76°
NW
55°-80°
Table2. main iron mines occurrence features in Anshan
999 1000 1001 1002 1003 1004 1005 1006 1007 1008 1009 1010 1011
The 3D magnetic susceptibility model of Anshan is obtained using UBC Mag3D software. The 3D inversion results of magnetic susceptibility show that the buried depth of magnetic bodies. The model of fold-ductile shearing that controls the spatial distribution of iron formation and ore bodies is proposed, the composite fold-ductile shear zone is consequently easy to form in the northeastern or southwestern sides of the micro continental nucleus, where favorable development of the BIF ore belt occurs. Iron ore bodies are developed mainly along the composite structural zone. The bottom depth of the iron ore bodies depends mainly on the bending depth of the closed folds and the developed depth of the ductile shear zones.