| 摘要 |
<p>1,096,590. Geophysical prospecting; ultrasonic probes. SOCIETE DE PROSPECTION ELECTRIQUE SCHLUMBERGER. March 24, 1965 [April 2, 1964], No. 12528/65. Headings H4D and H4J. In an arrangement for detecting fractures in the material forming the wall of a bore-hole, the travel time and attenuation of pulses of shear waves propagated in the material are determined. In the embodiment of Figs. 1, 2, 3, piezoelectric transmitting and receiving transducers (38, 40) are respectively mounted in housings (30, 32) in a shoe (22) sprung against the wall (14) of a liquid-filled bore-hole. The housings are so angled as to promote the propagation of shear waves in a direction parallel to the wall (14), and compressional waves are prevented from reaching receiver (40), either directly or after reflection from wall (14), by absorption in shoe (22) which is made of lead shot embedded in synthetic resin. A second pair of transducers, which may operate at a different frequency from that of transducers (38) and (40), is mounted in housings (34, 36) (Fig. 3). Determination of the shear wave velocity.-A transmitted pulse (S62) (Fig. 5, waveform diagram) is initiated by a time base 60 which simultaneously keys a transmitting oscillator 62 and triggers a monostable circuit 68. The monostable circuit 68 delivers an output pulse (S66-1), whose length is controlled in a linear manner by the voltage on a storage capacitor 92. A receivd acoustic pulse is amplified by a variable-gain amplifier 72 and fed to a pulse shaping circuit 80 producing an output pulse (S80). The outputs of circuits 68 and 80 are applied to AND gates 82 and 84, the arrangement being such that gate 82 gives an output pulse (S82) when both puleses (S66-1 and S80) are present at its input terminals, and gate 84 gives an output pulse (S84) when pulse (S80) is present at, but pulse (S66-1) is absent from, its input terminals. The gate pulse (S82) closes a switch 86 to connect capacitor 92 to a negative current source 90, and gate pulse (S84) closes a switch 86 to connect capacitor 92 to a positive current source 94. In each acoustic transmission cycle, the resulting voltage change on capacitor 92 is such as to tend to bring the trailing edge of pulse (S66-1) into coincidence with the centre of pulse (S80). The mean voltage on capacitor 92, which is proportional to the length of pulse (S66-1) and hence to the shear wave velocity, is recorded by a meter 21. False operation of the system due to low amplitude compressional waves reaching the receiving transducer is prevented by a threshold circuit 79. Determination of the shear wave attenuation.- In each acoustic transmission cycle, the amplitude of the pulse from the receiver amplifier 72 is sampled and compared, in a gated comparator circuit 102, with the amplitude of a reference source 108. The resulting difference signal at the output of comparator 102 provides an automatic gain control voltage for maintaining the output of amplifier 72 at the reference amplitude of source 108. The control voltage also provides a measure of the attenuation of the shear waves, and is recorded on a meter 21. Details of the transducers, their angular disposition and frequencies used, are given.</p> |
