DEEP RESISTIVITY PROBES IN THE SOUTHWESTERN UNITED STATES

Geophysics ◽  
1966 ◽  
Vol 31 (6) ◽  
pp. 1123-1144 ◽  
Author(s):  
D. B. Jackson

Eight deep resistivity probes have been made along a traverse extending from southwest Colorado to southern California to determine the electrical properties of the deep crust. The dipole method for measuring resistivity was used, and dipole spacings as great as 50 to 100 km were obtained at each survey location. In the Colorado Plateaus province, the electrical basement usually does not coincide with the top of the Precambrian crystalline basement, but rather, corresponds with the top of the carbonate rocks of Paleozoic age. Because of the large electrical conductance in the sedimentary column, resistant basement rock was detected at only three of the five sounding locations in the Colorado Plateaus province. At these three locations, the minimum possible basement resistivity was 2000 to 6000 ohm‐m. Electrical basement was detected at the survey locations in the Basin and Range province. The minimum possible basement resistivity was 600 to 1000 ohm‐m. A survey near Barstow, California, indicates that the resistant portion of the crust may be 9 to 10 km thick and may have a resistivity of 600 to 700 ohm‐m. A conductive zone underlies the resistant portion of the crust.

1997 ◽  
Vol 87 (3) ◽  
pp. 606-619 ◽  
Author(s):  
Harley M. Benz ◽  
Arthur Frankel ◽  
David M. Boore

Abstract Measurements of the Fourier amplitude spectra of Lg phases recorded at high frequency (0.5 to 14.0 Hz) by broadband seismic stations are used to determine regional attenuation relationships for southern California, the Basin and Range Province, the central United States, and the northeastern United States and southeastern Canada. Fourier spectral amplitudes were measured every quarter octave from Lg phases windowed between 3.0 and 3.7 km sec−1 and recorded in the distance range of 150 to 1000 km. Attenuation at each frequency is determined by assuming a geometrical spreading exponent of 0.5 and inverting for Q and source and receiver terms. Both southern California and the Basin and Range Province are well described by low Lg Q and frequency-dependent attenuation. Lg spectral amplitudes in southern California are fit at low frequencies (0.625 to 0.875 Hz) by a constant Lg Q of 224 and by a frequency-dependent Lg Q function Q = 187−7+7f0.55(±0.03) in the frequency band 1.0 to 7.0 Hz. The Basin and Range Province is characterized by a constant Lg Q of 192 for frequencies of 0.5 to 0.875 Hz and by the frequency-dependent Lg Q function Q = 235−11+11f0.56(±0.04) in the frequency band 1.0 to 5.0 Hz. A change in frequency dependence above 5.0 Hz is possible due to contamination of the Lg window by Pn and Sn phases. Lg spectral amplitudes in the central United States are fit by a mean frequency-independent Lg Q of 1291 for frequencies of 1.5 to 7.0 Hz, while a frequency-dependent Lg Q of Q = 1052−83+91(f/1.5)0.22(±0.06) fits the Lg spectral amplitudes for the northeastern United States and southeastern Canada over the passband 1.5 to 14.0 Hz. Attenuation measurements for these areas were restricted to frequencies >1.5 Hz due to larger microseismic noise levels at the lower frequencies.


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