Tensor time domain electromagnetic resistivity measurements at Ngatamariki geothermal field, New Zealand

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Abstract

Experimental measurements in the Ngatamariki geothermal field, North Island, New Zealand were made to test the applicability of the time domain electromagnetic method for detailed investigation of the resistivity structure within a geothermal field. Low-frequency square wave signals were transmitted through three grounded bipole current sources sited about 8 km from the measurement lines. Despite high levels of electrical noise, transient electric field vectors could be determined reliably for times between 0.02 and 3.3 s after each step in the source current. Instantaneous apparent resistivity tensors were then calculated. Apparent resistivity pseudosections along the two measurement lines show smooth variations of resistivity from site to site. Over most of the field the images consistently show a three-layer resistivity structure with a conductive middle layer (3–10 Ωm) representing the conductive upper part of the thermal reservoir. A deep-seated region of low resistivity in the northwest of the field may indicate a conductive structure at about 1 km associated with a deeper diorite intrusion. Measurements sited closer than about 100 m to drillholes appear to have been disturbed by metallic casing in the holes. A change in resistivity structure in the east of the field may indicate a major geological or hydrothermal boundary.

Introduction

Since its introduction in the 1960s resistivity surveying has proved very useful for delineating the geothermal fields in the Taupo Volcanic Zone (TVZ) of New Zealand. The highly conductive nature of the hot water and minerals that comprise the shallower parts of the geothermal reservoirs has proved a suitable target for shallow resistivity surveying (DC resistivity), allowing the conductive reservoirs to be delineated against high-resistivity surroundings (Bibby, 1988).

However use of geophysical methods for determining details of geological structure within the fields has proved more elusive. Traditional DC resistivity methods as well as gravity and magnetic surveying can at best determine only broad-scale features within a geothermal field. Seismic reflection surveys have also proved of limited use due to strong attenuation and strong reverberation effects in the near-surface layers of unconsolidated volcaniclastics (Bannister and Melhuish, 1997). Such short-comings of geophysical methods in detailed exploration of geothermal fields contrast with the record of the oil industry in exploring petroleum prospects. Determination of structure in the deeper parts (>1 km) of most oil fields relies heavily on obtaining good quality images from seismic reflection surveys.

While DC methods are best used to provide a map view of the prospect, information on the variation of resistivity with depth beneath each measurement site can also be derived from the transient behaviour of the measured electric fields. Here, we will derive apparent resistivity tensors from these transients using the time domain electromagnetic (TDEM) method, which is sometimes referred to as the LOTEM method (long offset transient electromagnetic; Strack, 1992). This is an extension of the multiple-source bipole–dipole method used for DC resistivity surveys. Application of apparent resistivity tensor analysis to the transient EM data (Caldwell and Bibby, 1998) facilitates the visualisation of transient data using distance–time resistivity sections (‘pseudosections’) analogous to seismic reflection sections. These provide representations of the subsurface in more detail than can be done with DC resistivity surveying.

An earlier experiment with the TDEM technique made at Wairakei geothermal field (Caldwell et al., 1999) was able to delineate the northern boundary of the field and deduce some details of its internal structure. This paper discusses further experiments made in March 2000 with the TDEM method in the Ngatamariki geothermal field (Fig. 1). The intention in this work is to adopt some of the attributes of seismic reflection surveying by making close-spaced measurements along lines across the field and to test the practicality of obtaining images that are coherent from site to site and can be better correlated to the underlying hydrothermal structures than has been achieved with traditional DC resistivity methods. The emphasis is on investigating the internal structure of the field rather than on locating its boundaries, as was the intent of most earlier DC resistivity surveys.

Section snippets

Ngatamariki geothermal field

The Ngatamariki geothermal field (Fig. 1) lies about 20 km north of Lake Taupo and is one of about 20 principal geothermal fields in the TVZ. A government-sponsored investigation of the energy potential of the Ngatamariki geothermal field, made in the 1980s, included geophysical, geological and geochemical surveys. In 1985 four exploratory drillholes were sunk to provide information on subsurface temperatures, pressures and the nature of the thermal fluids and rocks. Details of this work and of

Overview of TDEM

Fig. 6 shows the general field layout used in the TDEM resistivity surveying method. Three transmitting bipoles (AB, BC and CA) are used sequentially to inject low-frequency square waves of current into the ground in a source region that is remote from the target zone being surveyed. Provided the frequency is small enough, these square waves can be approximated as a series of independent step functions. At a typical measurement point P (Fig. 6) in the target zone, the receiver instruments

Transients

Fig. 9 shows the variation with time of the apparent resistivity tensors for two typical measurement sites, #113 and #217 (locations in Fig. 2). The plots in Fig. 9a and c show how P2, ρmax and ρmin vary with time, while those in Fig. 9b and d show the evolution of the apparent resistivity ellipses. At both sites the early-time part of the P2 curve drops with time to reach a minimum at about 100 ms after which it rises to level off at the DC value after about 2 s. The ellipses correspondingly

Interpretation

From the corrected resistivity pseudosections in Fig. 12, Fig. 13 several distinct zones (A, B, C and D) can be identified. Zone A is characterised by having lower apparent resistivities than the other zones, particularly at times greater than about 200 ms. Zones B and C both show layered resistivity structures in which the lowest apparent resistivities occur at about 100 ms after the step. Resistivities are significantly higher in zone C than in zone B. A fourth signature is exhibited in zone

Conclusions

The inability of seismic methods to image the internal structure of the geothermal reservoirs in the TVZ is a significant impediment to geothermal development. Even relatively low-resolution images produced by electromagnetic surveying techniques, if available at an early enough stage in a drilling programme, would be of considerable value. However, it must be stressed that measurement densities more typical of a seismic reflection survey for the oil industry will be required. Without high

Acknowledgements

We are grateful for skilled assistance with the field measurements from D.E. Keen, S.L. Bennie and D.J. Graham. The helpful reviews of Dr S. Soengkono and an anonymous reviewer have improved the quality of the paper. The New Zealand Foundation for Science, Research and Technology supported this work through contract C05X0004. This research is IGNS contribution No. 2405.

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