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Exploration for porphyry-style copper mineralisation near Llandeloy

Exploration for porphyry-style copper mineralisation near Llandeloy

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QnD (BH 7) 1<br />

Log rwceptibitity (9 uniu x 1~3)<br />

1 -0.5 0 0.5 +I +1.5<br />

L I I 1 I f<br />

T I n Y<br />

V - t<br />

mS t 8 Y<br />

QnD (BH 2) 1<br />

n -<br />

w " I<br />

QDI<br />

- I<br />

n Y<br />

w - I<br />

h u<br />

V -<br />

I<br />

0.1 0.5 1.0 2 5 10 20<br />

Figure 46 Magnetic susceptibilities of borehole samples<br />

1976). Three co m~onent populations with geometric<br />

means of 0.22, 0.6 and 17 x 10-3 SI units were defined<br />

(Fig. 47). The largest population (mean 0.6), consisting of<br />

about 75 percent of the sample, can be regarded as the<br />

'primary' background susceptibility of the rocks and<br />

probably contains unresolved populations related to<br />

different lithologies. The lower population is related to<br />

weathered rocks whilst the upper population can be<br />

ascribed to rocks containing magnetite generated during<br />

late stage propylitic alteration. Magnetic susceptibility<br />

may, there<strong>for</strong>e, be useful in detecting such rocks in<br />

boreholes. The magnetic complexity of the area as a<br />

whole, however, means that this magnetic signature is of<br />

little use on a wider scale because there are at least four<br />

modes of occurrence of magnetite here: secondary<br />

hydrothermal, primary magmatic, magnetite horizons<br />

within sedimentary rocks and detrital magnetite in<br />

lacustrine sediments.<br />

The identification of localised highly altered rock as<br />

the most magnetic is partly at odds with the<br />

interpretation of anomalies in the wider area discussed<br />

above. The model of an anticlinal core of magnetic<br />

Susceptibility (SI units X ~ O - ~ J<br />

Precambrian rock clearly cannot be adopted without<br />

qualification in the <strong>Llandeloy</strong> area, but the broad<br />

magnetic anomaly further west does extend unbroken to<br />

<strong>Llandeloy</strong>, and it is likely that these rocks underlie the<br />

area at no great depth. The <strong>for</strong>ms of some of the ground<br />

profiles (Appendix 2) certainly suggest some local, <strong>near</strong><br />

surface effects superimposed on a much deeper seated<br />

anomaly. An alternative possibility is that the broader<br />

anomaly at <strong>Llandeloy</strong> is due to a subvolcanic intrusion,<br />

perhaps representing the remains of a magma chamber<br />

underlying the hypothetical Treffynnon volcano.<br />

However, the magnetic source indicated by numerical<br />

modelling has sides sloping outwards and a base width of<br />

5 km or more at a depth of about 3 km, not a likely <strong>for</strong>m<br />

<strong>for</strong> a subvolcanic intrusion. The susceptibility used <strong>for</strong><br />

the models, about 7.5 x 10-3 SI units, is much greater<br />

than that of the unaltered intrusions at <strong>Llandeloy</strong>, but<br />

more typical of the Precambrian rocks which cause the<br />

western part of this anomaly. An anticlinal core<br />

there<strong>for</strong>e provides a more likely explanation of the broad<br />

anomaly than a subvolcanic intrusion.

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