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Fig. 11.25
Apparent-
resistivity curves filtered by
the North-West technique
time
t.
One-dimensional modeling shows that in the absence of sharp resistivity
contrasts the transient apparent-resistivity curves
TEM
(5
.
15t)and the undistorted
magnetotelluric apparent-resistivity curves
MT
(
T
) are almost similar. As long as
we avoid comparing the steep parts of the
MT
-curves, the transient
apparent-resistivity curves offer rather reliable reference for correcting magnetotel-
luric apparent-resistivity curves distorted by the static shift. A practical example
of such a correction is given in Fig. 11.26. Here the transient
TEM
- and
TEM
-curve offers
a resistivity-depth profile that is in line with well-log data. At the same time the
magnetotelluric
TEM
-curve, and
its inversion differs severely from well-log data. Correcting this distortion, the
MT
-curve is displaced to the left from the transient
MT
-
curve is shifted to the right so that its high-frequency branch fits the
TEM
-curve. Now
the inversion of the static-shift corrected
MT
-curve is in reasonably good agreement
with the well-log resistivities.
Another shift-correction technique involving TEM-soundings has been
suggested by Pellerin and Hohmann (1990). To improve the accuracy in com-
paring MT- and TEM-data, the apparent-resistivity
TEM
-curve is converted to
the apparent-resistivity
MT
-curve. The correction scheme is simple. The one-
dimensional TEM-inversion gives a resistivity-depth profile, from which a reference
MT
-curve is calculated. Then the distorted
MT
-curve is matched with the reference
MT
-curve. Here, contrary to Sternberg et al. (1988), we compare data of the same
kind and do not place restrictions on the resistivity contrasts. The technique is