EVALUATION OF GEOTHERMAL RESERVOIR STRUCTURES BY A NEW DOWNHOLE SEISMIC TECHNIQUE. Hiroaki Niitsuma, Motoyuki Sato, Hiroshi Asanuma, and

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Niitsuma, et EVALUATON OF GEOTHERMAL RESERVOR STRUCTURES BY A NE DONHOLE SESMC TECHNQUE Hiroaki Niitsuma, Motoyuki Sato, Hiroshi Asanuma, and Monya Faculty of Engineering, Tohoku University, Sendai Japan Key words: borehole seisinics, seismic mapping, geothermal reservoir, multicomponent measurement ABSTRACT Downhole seismic measurement is one of the most promising techniques for evaluation of reservoir structures, especially for deep geothermal development. e have developed new multicomponent seismic techniques which can derive useful information from three-component seismic signals. A combined technique of three-component signal processing and frequency-time distribution analysis enables the precise detection of wave onset even for the signal which has very low signal to noise ratio. Another technique termed as "triaxial doublet analysis" reveals a geothermal reservoir structure in a "cloud" of mapped seismic sources. t is feasible to use these techniques in seismic measurements with a sparse downhole network for the deep geothermal development. 1. NTRODUCTON Recently, considerable significance has been attached to the geotherinal potential of deeper reservoirs (2-5 and a new for the development of a deep reservoir has been started hy in the Kakkonda field, Japan. Additionally, the technique of utilizing subsurface artificial fractures in order to enhance production has been widely introduced in modern geothermal developrncnts. Acoustic emission (AE) and microseismic (MS) techniques are sole techniques available for mapping of natural and artificial and they are uscd in almost the geothermal developments. However, for the development of deeper reservoirs, the use of seismic networks is considerably restricted because of the effects of the weathering layer, propagation loss, and of surlace noise. One solution to this problem would be to measure a seismic wave in a borehole, where wide-band and high sensitivity detection can be achieved with less effect due to the ground surface and propagation loss. However, it is difficult to prepare many observation points in a downhole measurement because of the cost of drilling of observation wells and the cost of instrumentation. Therefore. it is very important to derive as much information as possible from the observed waveform in seismic measurements from a "sparse network." The downhole multicomponent seismic technique has the great advantage of allowing the derivation of the various types of contained a seismic waveform. ide-band and high measurement of a multicoinponent waveform allows detection of not only wave arrivals in each component, but also the three-dimensional particle motion associated with the seismic wave. Analysis of the three-dimensional hodograrn in hoth the time and frequency domains provides valuable information that cannot be obtained by a simple combination of single-component measurements. The present paper describes the multicomponent seismic techniques recently developed by the authors, and discusses their feasibility for the evaluation of deep geothermal reservoir structures. 2. DONHOLE SESMC MEASJREMENT SYSTEM t is essential to develop a wide-band and high-sensitive seismic for the multicomponent seismic technique A wide-band nhole triaxial measurement system was developed at Tohoku University (Niitsurna et al. 1982; The downhole detector consists of three-component piczoelcctric accelerometers. an electronic circuit, an electronic and clamping arms. The and equivalent input noisc are and, respectively. n-situ detectability the detector was calihrated by a spectral matrix analysis method (Moriya et and it was shown that three-dimensional particle motion up to can be precisely detected with the detector (Niitsuma et. 191) 3. DETECTON ARRVNG AVES BY SESMC TECHNQUE use of the three-component seismic signals provides on the in each also dimensional hodogram. c can derive valuable information on wave from analysis of the hodogram in both the time and frequency domains. The P-wave arrival direction. and the coherency of the wave can be precisely detected hy a method that uses the spectral matrix (Moriya et., Thew parameters can used for the detection of the wave source, focal mechanism analysis and so on The S-wave polarization direction is also a useful parameter for the analysis of focal mechanism and for the evaluation of subsurface anisotropy, shear wave splitting analysis. The wavelet transform of multicomponent is effective for the detection of successively arriving split shear waves (Niitsurna, 1993). e recently extended the three-component signal into hoth the time and domains, where the time-frequency distributions are used to analyze the non-stationary seismic signal. Using this spectral matrix composed of the time-frequency distributions. the linearity and the principal direction of wave polarization be quantitatively evaluated a function of time and frequency. t is known that a hodograrn is linearly polarized at an onset of wave and is after arriving reflected or refracted waves. Therefore, the evaluation of linearity is useful for the detection of wave arrivals Figures and 2 show the result of P-wave arrival-time detection for a signal detected at Kakkonda geothermal field, Japan. by using the time-frequency distributions and test of hypothesis (Moriya and Niitsuma. 1994, submitted). The P-wave arrival in low SNK (signal to noise ratio) be detected as a function of frequency. Figure 3 193

Niitsurna, et 1 Figure- : Three-component seismic signal detected at Kakkonda geothermal field P-wave Arrival 5, 4 3 2 1 5 1 15 2 25 3 35 4 Time Figure-2: Detection of P-wave time and frequency domains. by the distributions of likelihood ratio in the 794

Niitsuma, et al. n Damped Sinusoidal ave Sampling frequency 1 ms = -2' -1-5 5 1 15 2 25 2 D P Damped Sinusoidal ave Sampling frequency. L O -1............... -2-1 -5 5 1 15 2 25 Figure-3: Estimation error in P-wave arrival time detection. (a) by the timefrequency distributions. (b) by the local stationary AR model. shows a relationship between estimation error and SNR for a synthetic signal. Figure is for the present method, and Figure for the conventional method using AR model. As shown in this figure, our method using the time-frequency distributions is capable of detecting P-wave arrival time even when the signal to noise ratio is less than -5dB. 4. EVALUATON OF RESERVOR STRUCTURE BY TRAXAL DOUBLET ANALYSS A seismic doublet is a pair, or a group, of seismic events having very similar waveforms, and is considered to be the expression of stress release on the same part of an active subsurface crack or crack system. Therefore, the precise source location of the doublet allows us to determine the orientation of the structural plane in a subsurface crack system, such as a geothermal reservoir. The authors have developed the triaxial doublet analysis method to estimate precise relative source location of doublets. Utilizing the similarity of waveforms within doublet, the location relative to a reference event is very precisely determined through a multicomponent signal analysis the cross-spectrum analysis and the spectral matrix analysis (Moriya et. 1994). Figure 4 shows an example of this analysis for seismic events induced by a lost circulation of drilling mud during drilling of a production well at Kakkonda geothermal field, Japan. The events were detected at a single downhole observatory with the triaxial detector. Figure shows a result of conventional mapping (absolute source location), and Figure shows a result of the doublet analysis (precise relative location). e can clearly estimate the orientation of fractures created by the lost circulation by using this method (Moriya et. 1994). Figure shows mapped seismic events observed during a prehydraulic fracturing experiment in the Ogachi Hot Dry Rock (HDR) field of CREP, Japan. The events were detected by the downhole triaxial detector which was clamped at a depth of 38 m in an observation well, Thirty doublet events were discriminated total which we could estimate the source location. Figure shows the relative source location of doublet (Moriya and Niitsuma, 1994, accepted). The result of the doublet analysis reveals that the vertical fractures have extended dominantly, whereas the cloud of source locations in the conventional map (shown in Figure does not allow these structures to be discerned as easily 795

Niitsuma, et Tnaxial Detector Detector Production ell 4 1-52 3 1 7 Lost Circulation Point Lost Circulation Point Figure-4: Estimated source locations: (a) Absolute source location and (b) relative source location (triaxial doublet analysis) The indicated numbers designate the sequence of the events. Reference source in the relative source location in denoted by No. and sources of are the locations relative to first event No. Fracturing ell N E Triaxial (depth of Sonde. 1 Figure-5: Estimated source locations: (a) Absolute source location and (b) relative source location (triaxial doublet analysis), where the reference sources are denoted by closed circles and closed triangles. The circle and closed circle denote the events observed in the first experiment, and triangles and closed triangles represent the events in the second experiment. 796

797 Niitsuma, et EXPLORATON ELL [2] DRLL OF GEOTHERMAL ELL MAPPNG OF NATURAL FRACTURES [3] HYDRAULC FRACTURNG [4] PRODUCTON MAPPNG OF CREATNG FRACTURES MONTORNG OF RESERVOR STABLTY Figure-6: Sparse network of downhole multicomponent measurement in deeper geothermal development. As shown in the above mentioned examples, the triaxial doublet analysis is effective in evaluation of the dynamic behavior of subsurface crack extensions in lost circulation and hydraulic fracturing, and provides a greater understanding of the structure of geothermal reservoir systems. 5. APPLCATON OF THE DONHOLE MULTCOMPONENT SESMC TECHNQUE FOR DEEP GEOTHERMAL DEVELOPMENT t is preferable to detect seismic signals in boreholes for the deep developments. However, it is difficult to prepare many observation points because of the cost of drilling of observation wells and the cost of instrumentation. Therefore, it is important to derive as much information as possible from a signal which is detected with a "sparse network." As described in the previous chapters, the multicomponent seismic measurement is effective for the precise detection of wave source location and for the derivation of the other information included in the signals. Figure 6 shows an example of initialization of a multicomponent sparse network system in a deep geothermal development. At the first stage of development, downhole multicomponent seismic detectors are set in exploration wells or observation wells (Figure 6 This system utilizes the drilling noise to monitor the drilling of geothermal wells, and for the of the drilling target (Figure 6 1988, 199; Asanuma and Niitsuma, 1992). This measurement system is also effectively used for mapping of created fractures in the hydraulic fracturing of geothermal wells (Figure 6 Niitsuma et. 1989). During production, seismic activity is utilized to map and control the geothermal reservoir (Figure Niitsuma et 1985, 1987). 6. CONCLUSON Downhole multicomponent seismic measurement provides valuable information which cannot be obtained by a simple combination of single-component measurements. A sparse network of the downhole multicomponent detector can be effectively used for drilling monitoring, target imaging, fracture mapping, and reservoir control in deep geothermal development.

Niitsuma. et REFERENCES Asanuma, H., Niitsuma, H., Sato, M., and Chubachi, Characterization of rock formation by means of AE monitoring during well drilling. n: Progress in Acoustic Emission Yamaguchi, K., Aoki, K. and Kishi, T. (Eds)., JSND, Tokyo, Asanuma, H., Niitsuma, H., and Chubachi, N. (199). An analysis of three dimensional Lissajou pattern during well-drilling and estimation of source direction. n: Progress in Acoustic Emission Yamaguchi, K., Takahashi, H. and Niitsuma, H. JSND, Tokyo, Asanuma, H., Niitsuma, H. (1992). VSP uses drill-bits as a downhole seismic source. SEG expanded abstracts, Moriya, H., Nagano, K. and Niitsuma, H. (199). Precise estimation of AE source direction by spectral matrix analysis. n: Progress in Acoustic Emission Yamaguchi, K., Takahashi, H. and Niitsuma, H. (Eds)., JSND, Tokyo, pp.244-251. Moriya, H., Nagano, K. and Niitsuma, H. (1994). Precise source location of AE doublets by spectral matrix analysis of triaxial hodogram. Geophysics, 59, pp.36-45. Moriya, H. and Niitsuma, H. (1994). Precise detection of P-wave in low SNR signal by using time-frequency representations of triaxial hodogram. Geophysics (submitted). Moriya, H. and Niitsuma, H. (1994). Characterization of subsurface crack systems by combining triaxial doublet analysis and focal mechanism analysis. Geothermal Science and Technology (accepted). Niitsuma. H., Chubachi, N., H., Yokoyama, Sato, R. (1982). n-situ AE measurement of hydraulic fracturing at geothermal fields. Proceeding of first Japan-US Joint Seminar on Hydraulic Fracturing and Geothermal Energy, Nijhoff Publishers, The Hauge, Tokyo, pp.227-241. Niitsuma, H., Nakatsuka, K., Takahashi, H., Chubachi, N., Yokoyama, Sato, K. Acoustic emission measurement of geothermal reservoir crack in field, Japan. Geothermics, Vol. 14, pp.525-538. Niitsuma, H., Chubachi, N., and Takanohashi, M. (1987). Acoustic emission analysis of geothermal reservoir and its application to reservoir control. Geothermics, Vol. 16, pp.47-6. Niitsuma, H. (1989). Downhole AE measurement technique and its application to geothermal field. Journal of Acoustic Emission, Vol. Niitsuma, H. and Nagano, (1991). Calibration method using the spectral matrix for downhole triaxial seismic detectors. Proc. 5th Conf. on Activity in Geological Structures and Materials, (in press). Niitsuma, H., Tsuyuki, K. and Asanuma, H. (1993). Discrimination of split shear waves by wavelet transform. Canadian Journal of Exploration Geophysics, 29( 13. 798