Geothermal exploration method utilizing electrical resistivity and seismic velocity

• US 3,975,674 A
• Filed: 09/29/1972
• Issued: 08/17/1976
• Est. Priority Date: 09/29/1972
• Status: Expired due to Term

• Current Assignee: Robert B. Mceuen
• Original Assignee: Robert B. Mceuen
• Inventors: McEuen, Robert B.
• Primary Examiner(s): Strecker, Gerard R.
• Application Number:
  US05/293,480
• Time in Patent Office: 1,418 Days
• Field of Search: 324/1, 324/5, 324/6, 324/10, 324/9, 340/15.5 R, 340/15.5 CC, 340/15.5 TA
• US Class Current: 324/357
• CPC Class Codes: G01V 11/00 Prospecting or detecting by methods combining techniques covered by two or more of main groups G01V1/00 - G01V9/00

Abstract

A method of geothermal exploration in which the arrival times of reflected seismic waves and voltage differences caused by subsurface current flow are detected and processed to provide useful estimates of subsurface porosity, pore-fluid resistivity and equivalent salinity as functions of position.

Claims

1. A method for locating and characterizing subterranean layers comprising the steps of:

a. detecting at several locations on the earth'"'"'s surface a first set of outputs which are proportional to the amplitudes of the reflected seismic waves generated by a combined seismic wave and electrical current source while simultaneously detecting at the same locations a second set of outputs proportional to the voltage induced in the ground by the current produced at the seismic wave and electrical current source, and while simultaneously recording the pilot voltage used to generate the seismic and electrical current pulses, at the combined source, said pilot voltage being identical in form and proportional to both the source'"'"'s seismic pulse and the source'"'"'s electrical pulse;

b. processing in a multi channel cross-correlator the pilot voltage and the first and second set of outputs using the pilot voltage as the noise free reference signal, so as to obtain accurate values for the seismic wave arrival times, the amplitudes of these seismic arrivals and accurate values of the induced voltages and the relative time delays of these voltages;

c. computer processing the outputs of the cross-correlator which contain the reflection arrival times to obtain the seismic velocity V_n for all layers by automatically solving the equation ##EQU17## in which t_n (0) and t_n-1 (0) are respectively the arrival time at x = 0 from the bottom and top of the nth layer and in which Δ

t_n and Δ

t_n-1 are respectively the difference in arrival time between x=0 and x=x for the reflection from the bottom and the top of the nth layer, the variable x in said equation being known and input to the computer;

d. computer processing of the outputs of the cross-correlator which contain the induced voltage values to obtain for all layers the value of bulk rock resistivity, ρ

_r, determined from the n-layer equivalent of the half space solution ##EQU18## in which Δ

μ

is the potential difference created by the injection of current I as measured between electrodes located at distances x_n and x_n+1 from the surface current pole, said values of ρ

_r being those which best bring into accord in the least squares sense the seismically determined sequence of layers, Σ

h_n, given by ##EQU19## where the quantities are those defined in step c, and the measured induced voltage values, this accord being brought about by the fact that there is only one sequence of ρ

_r values possible for the measured induced voltages once the sequence of thicknesses has been seismically established;

e. computer processing the values of layer resistivity, ρ

_r, in conjunction with values of layer seismic velocity, V, to determine the pore fluid resitivity, ρ

_w, through solution of the relation ##EQU20## in which a and b are constants determined for the area undergoing exploration.

2. The method of claim 1 in which step (a) comprises detecting at several locations on the earth'"'"'s surface as a first set of output functions of time the amplitudes of reflected seismic waves generated by a remote combined seismic wave and electrical current source while simultaneously detecting as a second set of output functions of time the voltage induced at various distances by an electrical current waveform which differs from the source'"'"'s seismic waveform only in terms of its time base, and while detecting and storing as a third output function of time the pilot voltage which is identical in form and proportional to the seismic pulse produced by the source and which differs from the source'"'"'s current waveform only in terms of its time base;

and in which step (6) of claim 11 comprises generating a fourth set of functions of time by altering the time base of the second set of functions of time until the frequencies present in the voltage induced by the current source are identical with those contained in the third function of time and correlating as described in step (b) of claim (11) the third function of time with the first and fourth set of functions in such a way as to obtain accurate values of the seismic wave arrival times and the amplitudes of these arrivals and accurate values of the voltages and the relative time delays of these induced voltages.

3. The method of claim 1 where in values of pore fluid resistivity are used in conjunction with values of equivalent salinity, obtained from bore hole samples, to determine by means of the equation presented in claim 5 the temperature of the fluid saturating each layer.

4. The method of claim 1 wherein values of pore fluid resistivity obtained are used in conjunction with temperature values determined from surface temperature, T_s, heat flow, Q, and seismic velocity, V_k, values using the relation ##EQU21## in which Δ

Z_k is the thickness of the layer having seismic velocity V_k, and in which K_w and K_ma are respectively the thermal conductivity of the fluid phase and rock matrix respectively, and in which Δ

t_w and Δ

t_ma are respectively the interval time for the fluid phase and rock matrix, to determine the equivalent salinity of the fluids saturating all layers through solution of the equation ##EQU22## in which M is the molecular weight of the dissociated salt, β

is its degree of dissociation, u_a.sbsb.1.sbsb.8 and u_c.sbsb.1.sbsb.8 are the ionic mobilities at 18°

C for the anions and cations respectively, α

is a coefficient which takes on the value 0.025 for most electrolytes, T is temperature in degrees Centigrade, and ρ

_w is the pore fluid resistivity in ohm-meters.

5. The method of claim 1 wherein the values of layer resistivity ρ

_r and layer pore fluid resistivity ρ

_w are used to compute the porosity, φ

, for each layer through solution of the relation

space="preserve" listing-type="equation">ρ

.sub.r = kρ

.sub.w φ

.sup..sup.-m

in which k and m are constants for the area undergoing exploration.

6. The method of claim 1 wherein the values of layer seismic velocity, V, obtained are used to compute the porosities of the individual layers or zones by use of the relation ##EQU23## in which φ

is the porosity, V_w and V_ma are respectively the seismic velocity in the fluid phase and in the solid matrix phase and in which c is a correction factor to be applied in areas of under-compaction.

7. The method of claim 1 in which the receive transducers consist of a seismometer and potential measuring electrode housed in a common container.

8. The method of claim 1 in which the seismic energy source and the electrical current source are housed in a common container.

9. The method of claim 1 in which the amplitude and sign of reflected arrivals are used to verify the distribution of velocity as a function of distance in accordance with the equation ##EQU24## where d_n-1 V_n-1 is the acoustic impedance on the side of the boundary nearest the source and d_n V_n is the acoustic impedance on the far side of the boundary and where A_r is the amplitude of the reflected seismic wave and A_i is the amplitude of the incident seismic wave.