TP-EB rtt r-l
CHAPTER 7. CHAPTER 7. MACROSCOPrc STRUCTURES 99
Geologically,
the ISZ
coincidesto a large
degreewith the migmatite
zone(Figure
1'3).The
metamorphic grade boundariestrend
approximatelyNNW
andthis is highly
signiflcant.Almost the entire outcrop
withil
the ISZ has been ascribed to the Backstairs Passage Formation.Gra¡ites
(e.g. Palmer Granite) and granite gneisses (e.g. Rathjen Gneiss) and migmatized rock outcrop togetherwith
the meta-arkoses which aretypical
of the Backstairs Passage Formation.Calc-silicates occasionally occur, as do amphibolite and meta-dolerite dykes.
Unlike the KNSZ and KRSZ, no simple major structure has been mapped by previous workers and
the
relations ofthe
structuresin the
ISZto
structures outsidethe
Subzone aredifficult
to analyze.While a
numberof folds
have been delineatedfrom
magneticinterpretation, it
hasrarely
been possibleto
classifythem
as being synclinesor anticlines. This is
because facings arenot
available and directionsof
younging are oftenunknown. Additionally,
magnetic dips indicatethat
most folds are overturned. Fold closures are only rarely seen.Structures in this area appear to be discordant
with
structures elsewhere in the KNSZ and theKRSZ. This
may be dueto the overprintingof
F^o¿n folds bylater
folds because temperatures werestill
high in the ISZ which iswithin
the highest grade metamorphic zone. The open, upright folds comrnonto the
KNSZ andthe I{RSZ
are less commonin the ISZ. The
contact between the ISZ and theI{NSZ
and KRSZ appeaïsto
be discordant. Anomalies of theTruro
Anticlinal structures are truncated by the ISZ and the relationship between the ISZ and KRSZ is complex.7.4.L Subareas in the ISZ
KNSZ and KRSZ
were discussedin terms of the major
structuresin
those subzones. The relatively complex magnetic signatures and the factthat
the structure is poorly understood has madeit
more practicalto
consider the ISZin
terms of subareas of differing magnetic character.Based
on the
magnetic characteristics,the ISZ
can be dividedinto
a numberof
subareas which are shownin
Figure 7.18 (comparewith
Plate 3).Subarea type A
Multiple,
closely spaced, linear anomalies (dominant trendNNW),
are caused by migmatites and meta-arenites ofthe
Backstairs Passage Formation. Thestructural pattern within
subareas A1to
A.4 is largely unknown. These areas show evidence of previous deformation which could have beenisoclinal.
The rocks have been mapped as belongingto
the Backstairs Passage Formation probablyfor
want of evidence proving otherwise (see Mancktelow, 1979). The structure within these subareasis important, particularly if
early macroscopic isoclinal folds interpreted from magnetic data are provedto
exist.The meta-arenites of the Rockleigli region, subarea
41,
have been mappedin part
by White (1956),Malcktelow
(1979)and
Lawrence(1980).
Structuresinferred by
Mancktelow (1979) aretoo
simpleto
explain the magnetic signatures. Magneticunits, TC-MNS
and TP-MNS areboth
foldedinto the Monarto Sylclile.
AboveTC-MNS, the
magneticunits, BP-41,
do not close aroundthe Monarto
Syncline. Instead,BP-41
has been usedto
delineate afold
closure whichmust be
pre-F^o¡n(Figure 7.19). The Monarto
Synclineis
thereforenot
an F1fold
as interpretedby
Mancktelow(1979).
The rnagnetic anomaly associatedwith the
pre-F*o¿nlold
closure suggeststhe fold
wassynformal. Part of an
aeromagneticprofiie
over subareaA1
is shownin
Figure 7.17.LINE: 1160 EASTING: 313085 332747 NORTHING: 6141 183 200 0
0 000
50.00
0.@
.5000
.0000
Êc 00
!o iT
t-
-200 0
1.000
Ë FS
(5
E co
o
ÈEc (5
EÀ
ôo, 0 500
Figure 7.20: Magnetic model of the migmatite
belt
nearPalmer.
Anomalies:BP-42
between 13000 and 17000, Paimer Granite: betùeen 17500 and 18000.MIGMATITE BAND: CROSS-SECTION
\
\¡
,I I I I I I
\ /t
\/ t
\ I
¡l1l
¡l1l
¡l¡l
I I I I I I I I
ÊE
!
lr0,
, i'\ i''\ i"\ ,' \
ìi \i \l .'i ì ; I | ,.,'
r, t"' il '., li
\ ,,'
t, t, t,
\/
|-.5000
00 200.0 400 0 600.0 800 0
Figure 7.21: Magnetic model of simulated cross section of migmatite belt
CHAPTER 7.
MACROSCOPrc STRUCTURES 100Lawrence (1980) mapped the arkoses as belonging
to
the middle member ofthe
Backstairs PassageFormation.
Trends markedby
Mancktelow (1979)follow
magnetic trendsof
BP-41 and stopjust
shortof the fold
closure.North of the fold
closure,similar
air-photo trends donot
continue:this
is consistentwith
the interpretation of an early macroscopic fold refolded by F^oin.White (1956) called subarea A2 the "zoîe of veins". Subarea A2 contains the multiple, linear,
NNW
trending, magnetic and radiometric rocks west of Palmer. Magnetic anomaly amplitudes and radiometric count increase as rocks passinto
the migmatite zone. Whilelinear
anomalies predominate on a large scale, individual trends can only be followedfor
short distances. Despitethe ptygmatic folding
associatedwith the migmatite
zone,the
overalltrend of the
magneticunits is
dominantlyNNW. The
regional structureis a
synform, interpretedby
Fleming and\Mhite (1984)
to
bel'3.
New, closely spacedgravity
data are being collectedin the Mt.
Lofty Ranges (Boyd, pers.comm.). A gravity
high has been located above subareaA2
(Middleton, 1e73).Modelling is
difficult
and magnetic prolìles show a series of peaksin
thetotal
magnetic fleld andits vertical
gradient (Figure7.20). The
closenessof the
anomalous sources increases the ambiguity of theinterpretation.
Even on the vertical magnetic gradient profile, the true negative peaks arenot seen. An
experimental model showing short-wavelength foldsis illustrated
in Figure 7.21. Such a model also gives riseto
a series of linear magnetic anomalies similar tothat
shownin
Figure 7.20. The structurewithin
such a belt isdifficult
and impossible to resolve from magnetic modelling alone.The migmatite
band eastof the Monarto
Graniteis
a,n extensionof
subarea42, with
at least two anomalous magnetic units establishing the continuity (there are gapsin
detailed aero- magnetic coverage as shownin
FigureI.2).
Closures from contour maps indicate the presence of isoclinal folds foldedby
F^o¿n.The limbs of the fold are parallel and trend NN\M. The closures can be seenin
Figure 7.1-8, Plates 1to
3 and Plate 5, andin
Figure5.4. Attempts to
model the isoclinal folds werenot
successful due to interference from neighbouring magnetic anomalies (Figure 7.22). The isoclinal folds are on the east limb of a regional synform. They may be F"o,¡uor
-t]ro¿,, folds.Subarea
A3 is
characterizedby linear
magnetic anomaliestrending NS.
SubareaA3
lies betweenthe
southern extensionof the Monarto
Syncline andthe Wellington "Granite".
Foldclosures
in
subarea A3 are probably of the same generation as the isoclinal foldsin
subarea 42.A
strong magnetic gradient separates subarea A3 from the KNSZ and may indicate a structural boundary. Anomaliesin the
KNSZ adjacentto the
contact are oflow
amplitudes (less than a few hundreds of nanoTeslas) comparedto
the high amplitude anomaüesin
subarea43.
The magnetic character of subareas A2 and A4 are similar, though they are separated by sub- area C1. The pronounced
NNW
trend characteristic of subarea A2 is again seenin
subarea 44.Granitic
rocks a,lso outcropin this
area, and geological maps (Thomson, 1969b) indicate the presence of granitized sediments (presumably meta-arenites or migmatites). The basic structure of subarea A4 may be anticlinal in keepingwith
the major syncline, the Karinya Syncline, to the east. Faultsto
the west and northwest obscure the relation between subarea A4 and the KRSZ'The
southwestern contact betweenthe Karinya
Syncline andthe
subareaA4 of the
ISZis
a problem area. Carrickalinga Head Formation rocks on the west limb of the Karinya Syncline are flanked on both the east and west by rocks of the younger Backstairs Passage Formation. In the east the younger rocks are foldedinto
a syncline. But for Backstairs Passage Formation rocks to outcrop on the west as well requiresfurther
explanation. Abbas (1975) has mapped overturned dipsin
the ISZ west of the KRSZ. The feasible alternatives include the following: the boundary between subarea A4 and the KRSZ is afault,
the combination of several deformation events hasLINE: 1250 EASTING:33'1831 341983 NORTHING: 6118502 300.0
200.0
100 0
00
-100 0
1 000
Fc Eo
iI
t-E c (,
=o ôo
-1.000 00 160 0 320.0 480 0 640.0 0.000
1.000
Figure 7 .22: Magrtetic model of the "isocünal" folds of subarea A3 of the ISZ. Anomalies: BP-42 between 2300 and 3500.
LINE: 1690 EASTING: 312s29 340504 NORTHING: 6157150 200 0
lt
00
F
c!o iE
0 000
ÈE
It
-200 0
-1.0ûD
850
Figure 7.23: Magnetic model
of the
SpringtonFault.
Thefault is
indicatedby the bold
line.Anomalies:
BP-NI(S at
4800, possible subsurface granite between 7000 and 12000, BP-Á.4 bc' tween 12000 and 16000.Tc
ôC¡