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Geological Survey of Canada
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3-D Magnetic Imaging using Conjugate Gradients

Temagami anomaly

The Temagami magnetic anomaly (Figure 1) is located within the Cobalt Embayment area of the Southern Province, Ontario, Canada. With an areal extent of 50×15 km, the Temagami anomaly reaches a magnitude of ~10,000 nT making it one of the largest anomalies in North America. In the east, short wavelength linear NE-SW trending highs coincide with outcropping Archean iron formation. The central section has the greatest amplitude and an E- W strike. The western portion appears smoother in character than the eastern sections with values <2500 nT and an ENE-WSW trend. Reflection seismic data acquired along N-S lines over portions of the Temagami anomaly have imaged a 20 km-wide early Huronian rift basin bounded by north- and southerly dipping faults (Milkereit and Wu, 1996). Prominent subhorizontal reflectors exist at depths of 3-6 km, coincident with the maximum of the anomaly, and may represent lower Huronian volcanics of the Elliot Lake Group. However, modeling suggests that the limited depth extent of this unit precludes it as the source of the observed anomalies (Milkereit and Wu, 1996). The origin is more likely located within the basement.

The observed data (Figure 1) were modeled using the preconditioned CGA to solve equation (5). The data were sampled every 2 km resulting in a model subsurface of dimensions 32×32×16 blocks. Assuming only induced magnetization, the appropriate values of inclination 74°, declination -10° and magnitude 58250 nT were used. The results of the inversion are shown along east-west (Figure 2) and north-south (Figure 3) cross-sections as indicated by the white arrowheads in the magnetic field map (Figure 1). The cross-sections show a slight widening of the body with depth and an accompanying shift in the position of highest susceptibility from the center to the west. N-S cross-sections (Figure 3) indicate dips of <10° for both the shallow and deep parts of the body. These estimated dips are, however, valid only if any remanent magnetization is in the inducing field direction.


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Figure 1.
Figure 1
Figure 2.
Figure 2
Figure 3.
Figure 3

1998-09-16 Important notices