GB1599146A - Seismic method and apparatus - Google Patents

Seismic method and apparatus Download PDF

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Publication number
GB1599146A
GB1599146A GB12766/78A GB1276678A GB1599146A GB 1599146 A GB1599146 A GB 1599146A GB 12766/78 A GB12766/78 A GB 12766/78A GB 1276678 A GB1276678 A GB 1276678A GB 1599146 A GB1599146 A GB 1599146A
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seismic
transducers
liquid
detector
chamber
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Western Geophysical Company of America
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Western Geophysical Company of America
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V1/00Seismology; Seismic or acoustic prospecting or detecting
    • G01V1/16Receiving elements for seismic signals; Arrangements or adaptations of receiving elements
    • G01V1/18Receiving elements, e.g. seismometer, geophone or torque detectors, for localised single point measurements
    • G01V1/181Geophones
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B06GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
    • B06BMETHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
    • B06B1/00Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
    • B06B1/02Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy
    • B06B1/06Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with piezoelectric effect or with electrostriction
    • B06B1/0603Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with piezoelectric effect or with electrostriction using a piezoelectric bender, e.g. bimorph
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V1/00Seismology; Seismic or acoustic prospecting or detecting
    • G01V1/16Receiving elements for seismic signals; Arrangements or adaptations of receiving elements
    • G01V1/18Receiving elements, e.g. seismometer, geophone or torque detectors, for localised single point measurements

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  • Engineering & Computer Science (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Remote Sensing (AREA)
  • Physics & Mathematics (AREA)
  • Environmental & Geological Engineering (AREA)
  • Acoustics & Sound (AREA)
  • Geology (AREA)
  • General Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Geophysics (AREA)
  • Mechanical Engineering (AREA)
  • Geophysics And Detection Of Objects (AREA)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)

Abstract

A long, flexible cable is drawn over the surface of the earth. This cable has liquid-filled detectors which are constructed as geophones (10) and are mounted on the cable at suitable spacings. The seismic cable receives the individual output signals of the geophone. Each geophone supplies an electrical output signal having a polarity which corresponds to the direction of the movement of the earth. Their output signals are transmitted to a processing device, and then it is moved into a different position and the measurement operation is repeated. The geophones have a cylindrical, hollow housing (12) with a chamber (34) in the interior. A liquid (36) of high density, e.g. mercury, mostly fills the chamber (34). The chamber has a flexible base plate (22) which forms a force-measuring or pressure-measuring transducer (27). In addition to the flexible base plate (22), the chamber (34) has a further flexible base plate (22') on the upper side, which likewise forms a measuring transducer (27'). The geophone supplies at its output terminals (56, 58) electrical signals corresponding to the seismic signals. <IMAGE>

Description

(54) SEISMIC METHOD AND APPARATUS (71) We, WESTERN GEOPHYSICAL COMPANY OF AMERICA, a corporation organized and existing under the laws of the State of Delaware, United States of America, having an office at 10001 Richmond Avenue, Houston, Texas 77042, United States of America, do hereby declare the invention, for which we pray that a patent may be granted to us, and the method by which it is to be performed, to be particularly described in and by the following statement This invention relates to liquid-filled geophones for seismic exploration.
In reflection seismic prospecting, the reflected seismic signals are detected with seismic detectors, either geophones or hydrophones, Geophones are typically for land use and hydrophones for marine use. In use, a geophone is coupled to the earth and is responsive to movements thereof. A hydrophone is submerged in water and is responsive to the pressure changes produced therein by the movements of the earth. Either type may be used in shallow waters, typically positioned on the bottom of the body of water. For the sake of simplicity, the term geophone as used herein shall be understood to also include seismic detectors used on or in water.
According to one aspect of the invention, there is provided a seismic detector comprising a chamber having two pressure transducers and containing a "liquid" mass filling a major portion but not all of the chamber so that one of said transducers is decoupled, at least partially, from the "liquid" mass in certain orientations of the detector.
Preferably the transducers are mounted so that in one orientation of the detector only one of the transducers is decoupled, at least partially, from the "liquid" mass and in the opposite orientation only the other transducer is decoupled, at least partially, from the "liquid" mass.
A geophone can therefore be designed according to the invention which requires no self-orienting means, which are expensive and frequently fail during normal field abuse, which has an output signal polarity which can be made to be independent of the inclination of the geophone relative to the vertical, and which, for upwardly and downwardly directed movements of the earth, can be made to produce electric signals of opposite polarities, as is desirable for seismic prospecting.
According to another aspect of the invention, there is provided a method of seismic exploration, comprising the steps of: positioning a plurality of seismic detectors, each comprising a chamber substantially but not completely filled with a "liquid" mass, in random orientations on the earth's surface; measuring the pressures exerted by the masses as a result of excitations of the earth's surface, caused by reflected seismic signals, with a pair of oppositely mounted pressure transducers in each detector; and combining the output signals produced by each transducer pair to determine components of the excitations.
The method comprises in one preferred embodiment, towing a long, flexible member over the earth's surface, the member having liquid-filled geophones mounted thereon or coupled thereto and suitably spaced therealong, and a seismic cable for receiving the individual outputs of the geophones. Each liquid-filled geophone provides an output signal having characteristics corresponding to the direction of the earth's motion. The movement of the earth can be produced by a seismic energy source imparting energy into the earth so as to produce reflected seismic signals therein from underlying layers thereof.Using the preferred embodiment of the geophone, the polarity of the electric signals detected by the geophones and transmitted by the seismic cable to a utilization device is substantially independent of the orientations of the flexible member relative to the earth's surface and of the orientations of the geophones relative to the vertical. In another embodiment of the method of this invention, the geophones are positioned on the earth's surface in a predetermined pattern; their output signals are transmitted to the utilization device; and then the geophones are moved to another location and the process is repeated.
In a simple embodiment of geophone, it may comprise a hollow cylindrical casing defining a chamber therein. A suitable liquid, preferably having a high density, substantially fills the chamber. The chamber has flexible end walls which constitute a force or pressure transducer. The transducers produce electric signals having amplitude and polarity characteristics corresponding to the magnitude and direction of the flexure thereof. When the axis of the geophone is substantially vertical in an upright direction, the liquid in the chamber impinges upon the bottom transducer only, whereas for most inclinations of the geophone the liquid impinges upon both bottom and top flexible transducers. The geophone provides at its output terminals electric signals corresponding to the output signals of the pair of transducers.
In the preferred embodiment, a pair of transducers are "oppositely mounted". In this context, the phrase "oppositely mounted" is intended to mean that the transducers of each pair are separated by at least a substantial portion of the liquid at least for certain orientations of the housing.
Thus according to another aspect of the invention, there is provided a seismic detector comprising a housing including an internal chamber, a "liquid" mass substantially, but not completely, filling the chamber, and a pair of oppositely mounted transducers in the chamber containing the "liquid" mass therebetween for generating output signals in response to seismic signals so that vertical ,components of the seismic signals may be distinguished from horizontal components regardless of the orientation of the housing with respect thereto.
It is preferable to have the planes of sensitivity of the transducers parallel to each other and, in a preferred embodiment, to have these planes perpendicular to a line drawn joining the transducers.
The transducers can thus generate output signals in response to pressure exerted upon them by the interaction of the liquid mass and the transducers resulting from excitations of the earth's surface caused by reflected seismic signals. In particular, such a geophone is primarily sensitive to accelerations of the earth's surface. Such accelerations are typically in the range of 10 to 1000 hertz and of the order of less than 3 percent of the acceleration due to gravity. The excitations of the earth's surface to which this device is sensitive may be considered to have both vertical and horizontal components.
The sensitivity of any geophone to vertical and horizontal components may be controlled by the manner in which the output signals of the individual transducers in a pair are combined.
The preferred form of geophone may be made sensitive primarily to vertical components by combining the individual transducer outputs by addition. The polarity of the sum will then indicate the direction of the vertical component without regard to the orientation of the geophone with respect to the vertical. That is, positive polarity may be used to indicate vertical components directed toward the center of the earth and negative polarity to indicate vertical components directed away from the center of the earth. If the dimensions of the chamber, and the proportion of the chamber filled with the liquid, are carefully chosen, the amplitude of the sum may be made constant for a given vertical component regardless of orientation of the housing.The components of the output signals from each transducer generated in response to horizontal components are of opposite polarity from each other and of equal magnitudes. They will therefore cancel each other when combined by addition.
On the other hand, the outputs of the transducers in each pair may be combined by subtraction. If the geophones are positioned approximately on their sides, the signal resulting from the subtraction is then proportional only to the horizontal components. All signals representing vertical components will be cancelled by the subtraction because, in this orientation, the output signals from each transducer generated in response to vertical components will be equal in magnitude and of the same polarity.
It is, therefore, particularly convenient to position the geophones approximately on their sides and record the output signals from each transducer in a pair separately. The signals may thereafter be combined, by addition and by subtraction, to determine both horizontal and vertical components without having to reorient the geophones.
Additional pairs of oppositely mounted flexible transducers may be added to increase the accuracy and amplitude of the resulting output signals.
The output signals from the transducers in each pair may be combined by addition and/or subtraction, in parallel or series, with the signals from transducers in other pairs or may be transmitted separately according to the needs of a particular situation.
For a better understanding of the invention and to show how the same may be carried into effect, reference will now be made, by way of example, to the accompanying drawings, in which: Fig. 1 is a sectional view in elevation of a preferred embodiment of geophone; Fig. 2 illustrates the operation of the geophone for inclinations thereof from upright to upside-down for upwardly-directed movements of the earth; Fig. 3 is similar to Fig. 2 but for downwardly directed earth movements; Fig. 4 illustrates the installation of the geophone onto a towed seismic cable; Fig. 5 illustrates a preferred method of seismic prospecting; Fig. 6 is a perspective view of a housing for the geophone; Fig. 7 illustrates the attachment of the geophone housings, shown in Fig. 6, onto a seismic spread cable, and the use of the spread cable for seismic prospecting illustrated in Fig. 5;; Fig. 8 is a sectional view illustrating a geophone having a rectangular cross-section; and Fig. 9 is a view similar to Fig. 8 with an elliptical cross-section.
The preferred embodiment of the liquid geophone, generally designated as 10, comprises a metal housing 12 having a circular cross-section (Fig. 1). Housing 12 can also have a rectangular cross-section (Fig. 8), an elliptical cross-section (Fig. 9), or variations thereof depending on the desired sensitivity of geophone response.
In Fig. 1 housing 12 has bottom and top covers 14 and 16 which hermetically seal its inner cylindrical cavity 18. A split ring 20 rests on the bottom cover 14 and provides a support for a circular conductive wall 22 to the underface of which is secured a crystal 24 having a silver electrode 26. Throughout the description and to the extent possible, similar parts are designated with the same reference characters followed by a prime('). A split annular ring 20' abuts against the top cover 16 and provides a support for a circular conductive wall 22' to the top face of which is secured a crystal 24' having a silver electrode 26'. Housing 12 is lined with a tubular plastics casing 30 (Figs. 1, 8, 9) extending between bottom and top covers 14, 16. Walls 22, 22' abut against O-rings 32, 32', positioned on shoulders 33, 33', respectively, formed in casing 30.The walls 22, 22' are secured to the shoulders 33, 33' by the annular rings 20, 20', respectively. Walls 22, 22', are flexible and their flexures are sensed by their crystals 24, 24', respectively. Thus, each flexible wall and the crystal mounted thereon consitutes a conventional force or pressure transducer. The transducers formed by walls 22, 22' and their respective crystals 24, 24' are generally designated as 27, 27', respectively.
For the purposes of this description, transducers 27 and 27' are assumed to be mounted so that they will generate signals of the same polarity when a force or pressure causes them to bend outwardly away from liquid 36.
Additional pairs of oppositely mounted flexible transducers (not shown) may be added to increase the accuracy and amplitude of the resulting output signals.
Housing 12 may also be made of a nonmetal, such as plastics, eliminating the need for tubular plastics casing 30. Walls 22 and 22' need not be made of conductive material except to the extent required to provide an electrical connection to crystals 24 and 24'.
The output signals from pressure transducer 27 are conducted through a pair of wires 51, 52, and the output signals from pressure transducer 27' are conducted through a pair of wires 51', 52'. Wires 51, 52 pass through a slit 53 in ring 20, a longitudinal groove 54 in the outer wall of casing 30, then through a slit 53' in ring 20'. The output signals carried by wires 51, 52 and 51', 52' can be added, either in series or in parallel, at a pair of the geophone's output terminals 56, 58, extending through top cover 16. On the other hand the wires 51, 52, 51' and 52' can be connected to four output terminals (not shown).
When the wires are connected to four output terminals, the outputs of each transducer of the pair may be recorded or otherwise utilized separately. Addition and/or subtraction may be then accomplished during recording or afterwards. As another alternative, the output signals carried by wires 51, 52 and 51', 52' can be subtracted from each other, either in series or in parallel, at output terminals 56 and 58.
The inner space confined between the transducers and the inner cylindrical wall of casing 30 forms a chamber 34 which is substantially fully, but not completely, filled by a liquid 36 serving as the inertial mass for the geophone 10. It is therefore desired that the liquid 36 have a high density, and a suitable such liquid is mercury. In the preferred embodiment, liquid 36 fills approximately 90% of the space in chamber 34, leaving approximately 10% of available space for expansion of the liquid due to temperature changes within the operating temperature range for the geophone.
The terms "substantially" and "substantially fully" when used to designate the degree to which the chamber is filled by the liquid, shall be understood to include all degrees of such filling beyond 50% full in which the upper transducer is at least partially decoupled from the liquid when the geophone is in an upright position. The term "liquid" as used herein is intended to include other fluids, such as powdered metals, which are suitable for use as inertial masses in geophones of the type described herein.
The action of the inertial liquid 36 on the pressure transducers 27, 27' will now be illustrated with reference to Figs. 2 and 3, wherein only the operational parts of the geophone are shown, that is, casing 30 and its associated bottom and top transducers 27, 27'. The solid lines illustrate the positions of the flexible walls 22, 22' when the transducers are at rest, and the dotted lines illustrate their deflected positions produced by the pressures of the inertial liquid reacting to the earth motion.
In Fig. 2 geophone 10 is shown positioned over the earth's surface 40 at various inclinations from an upright position A to an inverted upside-down position E. The earth is assumed to undergo upward movements, represented by the arrows 42, which are transmitted to the inertial liquid 36 which, in turn, produces a force or pressure outwardly directed with respect to the axis of casing 30.
Thus, in position A transducer 27 will bend outwardly toward cover 14, and transducer 27' will bend neither outwardly nor inwardly, since it is decoupled from the inertial liquid 36. In position B, at an inclination of 45 from vertical, transducer 27 will bend outwardly toward cover 14, and transducer 27' will bend outwardly toward cover 16. The same applies for position C corresponding to an inclination of 90' wherein the geophone lies completely on its side, and for position D corresponding to an inclination of 135 . In the fully-inverted, upside-down position E corresponding to an inclination of 180o, transducer 27' bend outwardly toward cover 16, and transducer 27 will bend neither inwardly nor outwardly, since in this position it is decoupled from liquid 36.
Thus, for all positions from 0" to 180 relative to the upright position A, either one or both of the pressure transducers 27, 27' will sustain an outwardly-directed deflection.
The transducers 27, 27' will therefore produce electric signals 43 of the same polarity for all the outwardly-directed flexures.
As the level of degree of filling of chamber 34 with liquid 36 is increased, another effect becomes noticable. At sufficiently high degrees of filling the top transducer in the vertical position may no longer be completely decoupled even though liquid 36 does not actually impinge upon this transducer.
That is, transducer 27' in position A and trawnsducer 27 in position E may each exhibit a tendency to move inwardly in response to upward motions of the earth as represented by arrows 42. In such situations this top transducer will generate an output signal of the opposite polarity from the other transducer of the pair. The amplitude of this opposite polarity output will always be no greater than the amplitude of the output of the lower transducer. Geophone output signal 43, which is the sum of the ouput signals of transducers 27 and 27', will therefore always have the same polarity for all vertical components in the same direction without regard to the orientation of the geophone with respect to the vertical.
The degree of filling of chamber 34 has a different effect on the amplitude of geophone output signal 43 in position A or E than it has on the amplitude of signal 43 in positions B, C, or D. The amount of variation in the amplitude of signals 43 for the same accelerations in various geophone orientations may therefore be controlled somewhat by changing the degree of filling of chamber 34. The amplitude of the output signal from a transducer in response to a particular amplitude of excitation is primarily controlled by the height of liquid above the transducers in that particular orientation.
The partial decoupling of on transducer in certain orientations may be utilized in order to configure a geophone in which the sensitivity, that is, the ratio of the amplitude of the output signal to the amplitude of the detected component, is not effected by the orientation of the geophone with respect to the vertical.
In the preferred embodiment, the ratio of the diameter to height of the enclosed column of liquid 36 is chosen such that the amplitude of signals 43 remains substantially constant for all positions A through E of the geophone, i.e., from its upright to upsidedown positions.
Geophone 10 may therefore be used in geophysical exploration to detect seismic reflections without careful positioning. That is, a series of such geophones may be positioned in random orientations and yet generate output signals having the correct amplitudes and polarities to represent vertical components of acceleration of the earth's surface.
In fact, geophone 10 may be made responsive only to vertical components. That is, horizontal components cause transducers 27 and 27' to respond in a manner in which the effects of such horizontal components are cancelled by the addition of the outputs of the transducers to form signals 43.
For ease of illustration, the effects of a horizontal component will be described assuming acceleration from left to right. The effects of horizontal components in any direction may be understood therefrom. In position A, horizontal components have no effect on either transducer because the acceleration is parallel to the surface of the transducers. In position B, transducer 27' will deflect inward and transducer 27 will deflect outward. The same applies for positions C and D. In position E there will be no net effect as noted above. In position C the amount of deflection and therefore the am plitudes of the output signals of transducers 27 and 27' will be equal.In positions B and D the ratio of the diameter to height of the enclosed column (when viewed in Position A) may be chosen, and the degree of filling of chamber 34 with liquid 36 may be adjusted, so that the amplitudes of the output signals of transducers 27 and 27' are approximately equal. Since these signals are of opposite polarity, they wll cancel when the outputs of transducers 27 and 27' are added to produce signal 43.
In this manner it can be seen that geophone 10 may be made to be sensitive only to vertical and not to horizontal components.
That is, the effective sensitive axis of geophone 10 automatically remains oriented to the vertical without regard to the actual orientation of the device.
As noted above, in position C, the amplitudes of the output signals resulting from horizontal components are equal in amplitude but opposite in polarity. When combined by subtraction these signals will not cancel but will reinforce each other. Signal 43 formed in this manner will therefore be proportional to the effects of horizontal components. Further, the output signals resulting from vertical components produced by transducers 27 and 27' in position C are equal in amplitude and of the same polarity.
Combination by subtraction will therefore result in cancellation. When the output signals of transducers 27 and 27' in position C are combined by subtraction, the resultant geophone output signal 43 contains the effects of horizontal components but not vertical components. As geophone 10 is changed in orientation from position C to positions B or D the amplitude of geophone output signal 43 formed by subtraction is reduced as a function of the cosine of the angle of orientation with respect to the horizontal. When position A or E is reached, output signal 43 is not representative at all of the horizontal components.
It is therefore particularly convenient to utilize a plurality of geophones 10 in substantially horizontal positions to detect reflected seismic signals. The outputs of individual transducers 27 and 27' of each pair may then be separately transmitted to the utilization device for combination by addition and subtraction in the utilization device or for recording and later combination so that both vertical and horizontal components may be determined for the same location on the surface of the earth by one of geophones without repositioning.
The description of Fig. 3 is similar to that of Fig. 2, except that the earth's movements, represented by the arrows 42', are now assumed to be directed downwardly, causing inwardly-directed flexures resulting from relief of static pressure of the inertial liquid and the spring action of the flexible walls 22, 22'.
As illustrated in Fig. 3, for all positions of geophone 10 from its upright position A to its upside-down inverted position E, the transducers 27, 27' will flex inwardly, that is, away from their respective covers 14, 16. The transducers 27, 27' will therefore produce electric signals 43', having a polarity opposite to the polarity of the electric signals 43 produced by transducers 27, 27' in response to the upwardly-directed movements of the earth, as shown in Fig. 2.
The design of geophone 10 makes it relatively easy to maintain the desired ratio, between the mass of the inertial liquid 36 and the mass of the remaining components of the geophone including housing 12, greater than one. Such a ratio is favorable for seismic prospecting, as described in U.S. Patent No.
3,067,404. In the prior art utilizing selfaligning means, such as gimbal mounts, for orienting the geophone, the heavy mass of such means makes it virtually impossible to achieve said desired ratio.
The geophone 10 can be housed in a suitable housing 60 (Fig. 4) which is protected by a resilient sleeve whose ends are suitably secured by a tape 65 to the outer sleeve of a towable seismic cable 62. A pair of wires 66, 67 interconnect the ouput terminals of the geophone with a pair of of conductors in seismic cable 62. If sensitivity to both vertical and horizontal components is desired, one additional pair of wires, not shown, will be required to connect the geophone with one additional pair of conductors, not shown, in seismic cable 62.
Thus cable 62 may have associated therewith and interconnected therein a plurality of suitable spaced-apart geophones. In accordance with a very important aspect of this embodiment, each geophone can lie on its side, as shown in Fig. 4, yet still be fully operative and responsive, as shown in Figs.
2C and 3C, to upwardly and downwardly directed earth's movements represented by the arrows 42 and 42', respectively.
In accordance with one embodiment of the method of the invention, the seismic cable 62 together with its geophones is towed with a seismic truck 72 having a utilization device such as a recorder 73 therein which receives and records the signals from cable 62. Cable 62 can be wound on and unwound from a rotatably-mounted spool 70, and the seismic energy needed for seismic exploration can be imparted into the earth by a suitable seismic energy source 74.
In an alternative embodiment of the method of the invention, each geophone 10 is housed in a housing 90 (Fig. 6) and the output terminals of the geophone are connected to a lead-in, short cable 91 which extends from a spread cable 93. The seismic crew positions cable 93 on the earth's surface 40, with the housings 90 disposed in any desired detection pattern, but housings 90 need not be oriented in any particular direction with respect to the vertical.
Instead of employing crystal pressure sensors, 24, 24', typically made of a piezoceramic material, other pressure sensors can equally be employed, as will be apparent to those skilled in the art.
WHAT WE CLAIM IS: 1. A seismic detector comprising a chamber having two pressure transducers and containing a "liquid" mass filling a major portion but not all of the chamber so that one of said transducers is decoupled, at least partially, from the "liquid" mass in certain orientations of the detector.
2. A seismic detector according to claim 1, wherein the transducers are mounted so that in one orientation of the detector only one of the transducers is decoupled, at least partially, from the "liquid" mass and in the opposite orientation only the other transducer is decoupled, at least partially, from the "liquid" mass.
3. A seismic detector according to claims 1 or 2 and comprising means for combining the output signals from the transducers by addition so that the polarity of the sum represents the direction of vertical components of incident seismic signals regardless of the orientation of the housing with respect thereto.
4. A seismic detector according to claim 3, wherein the magnitude of the sum represents the magnitude of the vertical components, regardless of the orientation of the detector with respect to the surface of the earth.
5. A seismic detector comprising a housing including an internal chamber, a "liquid" mass substantially, but not completely, filling the chamber, and a pair of oppositely mounted transducers in the chamber containing the "liquid" mass therebetween for generating output signals in response to seismic signals so that vertical components of the seismic signals may be distinguished from horizontal components regardless of the orientation of the housing with respect thereto.
6. A seismic detector according to claim 5, further comprising means for distinguishing between the vertical and horizontal components of the seismic signals regardless of the orientation of the housing with respect thereto.
7. A seismic detector according to claim 5 or 6, and comprising means for combining the output signals from each transducer by addition so that the magnitude of the sum thereof represents the magnitude of the vertical components of the seismic signals, regardless of the orientation of the housing with respect thereto.
8. A seismic detector according to claim 4 or 7, wherein the amplitude of the sum of the transducer output signals is substantially the same for vertical components of equal magnitude regardless of the orientation of the detector with respect thereto.
9. A seismic detector according 'to any one of the preceding claim, wherein the dimensions of the portion of the chamber filled by the "liquid" mass are selected so that the detector is substantially equally sensitive to vertical components regardless of the orientation of the detector with respect thereto.
10. A seismic detector according to any one of the preceding claims, wherein there are means for combining the output signals from the transducers by subtraction so that the result thereof represents the horizontal components of seismic signals when the detector is oriented so that a line drawn from one transducer to the other has a component in the horizontal direction.
11. A seismic detector according to claim 10, wherein the sensitivity of the detector is a function of the cosine of the angle between the line and the horizontal.
12. A seismic detector according to any one of the preceding claims, wherein the "liquid" mass is substantially contained between the transducers.
13. A seismic detector according to any one of the preceding claims, wherein the two transducers have substantially parallel planes of sensitivity.
14. A seismic detector according to claim 13, wherein the planes are perpendicular to a line drawn from one to the other of the transducers.
15. A seismic detector according to any one of the preceding claims, wherein each transducer comprises a flexible wall forming one portion of the chamber, and means to detect deflection of the flexible wall.
16. A seismic detector according to claim 15, wherein the deflection detection means is a piezo-electric crystal.
17. A seismic detector according to claim 15 or 16, wherein the chamber is a right circular cylinder and the flexible walls form respective circular ends thereof.
18. A method of seismic exploration, comprising the steps of: positioning a plurality of seismic detectors, each comprising a chamber substantially but not completely filled with a "liquid" mass, in random orientations on the earth's surface; measuring the pressures exerted by the masses as a result of excitations of the earths surface, caused by reflected seismic signals, with a pair of oppositely mounted pressure transducers in each detector; and combining the output signals produced by each transducer pair to determine components of the excita
**WARNING** end of DESC field may overlap start of CLMS **.

Claims (24)

**WARNING** start of CLMS field may overlap end of DESC **. 40, with the housings 90 disposed in any desired detection pattern, but housings 90 need not be oriented in any particular direction with respect to the vertical. Instead of employing crystal pressure sensors, 24, 24', typically made of a piezoceramic material, other pressure sensors can equally be employed, as will be apparent to those skilled in the art. WHAT WE CLAIM IS:
1. A seismic detector comprising a chamber having two pressure transducers and containing a "liquid" mass filling a major portion but not all of the chamber so that one of said transducers is decoupled, at least partially, from the "liquid" mass in certain orientations of the detector.
2. A seismic detector according to claim 1, wherein the transducers are mounted so that in one orientation of the detector only one of the transducers is decoupled, at least partially, from the "liquid" mass and in the opposite orientation only the other transducer is decoupled, at least partially, from the "liquid" mass.
3. A seismic detector according to claims 1 or 2 and comprising means for combining the output signals from the transducers by addition so that the polarity of the sum represents the direction of vertical components of incident seismic signals regardless of the orientation of the housing with respect thereto.
4. A seismic detector according to claim 3, wherein the magnitude of the sum represents the magnitude of the vertical components, regardless of the orientation of the detector with respect to the surface of the earth.
5. A seismic detector comprising a housing including an internal chamber, a "liquid" mass substantially, but not completely, filling the chamber, and a pair of oppositely mounted transducers in the chamber containing the "liquid" mass therebetween for generating output signals in response to seismic signals so that vertical components of the seismic signals may be distinguished from horizontal components regardless of the orientation of the housing with respect thereto.
6. A seismic detector according to claim 5, further comprising means for distinguishing between the vertical and horizontal components of the seismic signals regardless of the orientation of the housing with respect thereto.
7. A seismic detector according to claim 5 or 6, and comprising means for combining the output signals from each transducer by addition so that the magnitude of the sum thereof represents the magnitude of the vertical components of the seismic signals, regardless of the orientation of the housing with respect thereto.
8. A seismic detector according to claim 4 or 7, wherein the amplitude of the sum of the transducer output signals is substantially the same for vertical components of equal magnitude regardless of the orientation of the detector with respect thereto.
9. A seismic detector according 'to any one of the preceding claim, wherein the dimensions of the portion of the chamber filled by the "liquid" mass are selected so that the detector is substantially equally sensitive to vertical components regardless of the orientation of the detector with respect thereto.
10. A seismic detector according to any one of the preceding claims, wherein there are means for combining the output signals from the transducers by subtraction so that the result thereof represents the horizontal components of seismic signals when the detector is oriented so that a line drawn from one transducer to the other has a component in the horizontal direction.
11. A seismic detector according to claim 10, wherein the sensitivity of the detector is a function of the cosine of the angle between the line and the horizontal.
12. A seismic detector according to any one of the preceding claims, wherein the "liquid" mass is substantially contained between the transducers.
13. A seismic detector according to any one of the preceding claims, wherein the two transducers have substantially parallel planes of sensitivity.
14. A seismic detector according to claim 13, wherein the planes are perpendicular to a line drawn from one to the other of the transducers.
15. A seismic detector according to any one of the preceding claims, wherein each transducer comprises a flexible wall forming one portion of the chamber, and means to detect deflection of the flexible wall.
16. A seismic detector according to claim 15, wherein the deflection detection means is a piezo-electric crystal.
17. A seismic detector according to claim 15 or 16, wherein the chamber is a right circular cylinder and the flexible walls form respective circular ends thereof.
18. A method of seismic exploration, comprising the steps of: positioning a plurality of seismic detectors, each comprising a chamber substantially but not completely filled with a "liquid" mass, in random orientations on the earth's surface; measuring the pressures exerted by the masses as a result of excitations of the earths surface, caused by reflected seismic signals, with a pair of oppositely mounted pressure transducers in each detector; and combining the output signals produced by each transducer pair to determine components of the excita
tions.
19. A method according to claim 18, wherein the combining step includes the step of combining the output signals by addition to determine the vertical components.
20. A method according to claim 18 or 19, wherein the degree of filling of each detector is such that the sensitivity of the detector to vertical components is the same in all directions.
21. A method according to claim 18, 19 or 20, wherein the detectors are positioned in horizontal orientations and the combining step includes the step of combining the output signals by subtraction to determine the horizontal components of the excitations.
22. A method according to claims 19 and 21, wherein the combining step includes the steps of combining the output signals by addition and by subtraction to separately determine the vertical and the horizontal components of the excitations.
23. A seismic detector substantially as hereinbefore described with reference to Figure 1 or Figure 1 as modified by Figure 4, 6, 8 or 9 of the accompanying drawings.
24. A seismic exploration method substantially as hereinbefore described with reference to the accompanying drawings.
GB12766/78A 1977-04-01 1978-03-31 Seismic method and apparatus Expired GB1599146A (en)

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US78353177A 1977-04-01 1977-04-01
US88716578A 1978-03-16 1978-03-16

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CA (1) CA1116285A (en)
CH (1) CH633372A5 (en)
DE (1) DE2813487A1 (en)
FR (1) FR2386056A1 (en)
GB (1) GB1599146A (en)
IE (1) IE46597B1 (en)
IT (1) IT1156186B (en)
MX (1) MX145829A (en)
NL (1) NL7803500A (en)
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1983000564A1 (en) * 1981-08-13 1983-02-17 Carpenter, Allan, Lloyd Hydrophone cable
GB2224121A (en) * 1988-10-08 1990-04-25 Roy Wyatt Improvements in or relating to arrays of geophones suitable for towing over ice

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
AT229599B (en) * 1962-04-10 1963-09-25 Oemv Ag Mechanoelectric converter
US3270565A (en) * 1962-12-26 1966-09-06 Wilbur W Hawley Omnidirectional acceleration device
US3555503A (en) * 1968-12-31 1971-01-12 Electronic Systems Inc Acceleration dependent phase control seismic exploration
GB1385971A (en) * 1971-05-03 1975-03-05 Western Geophysical Co Seismic detector conveyances
US3813744A (en) * 1972-12-08 1974-06-04 Seismic Logs Geophone treatment

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1983000564A1 (en) * 1981-08-13 1983-02-17 Carpenter, Allan, Lloyd Hydrophone cable
GB2224121A (en) * 1988-10-08 1990-04-25 Roy Wyatt Improvements in or relating to arrays of geophones suitable for towing over ice

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SE7803556L (en) 1978-10-02
FR2386056A1 (en) 1978-10-27
NO781063L (en) 1978-10-03
DE2813487A1 (en) 1978-10-19
NO149943B (en) 1984-04-09
IT1156186B (en) 1987-01-28
BE865476A (en) 1978-10-02
CA1116285A (en) 1982-01-12
CH633372A5 (en) 1982-11-30
DE2813487C2 (en) 1988-06-01
NO149943C (en) 1984-07-18
IE46597B1 (en) 1983-07-27
MX145829A (en) 1982-04-05
NL7803500A (en) 1978-10-03
SE430544B (en) 1983-11-21
FR2386056B1 (en) 1984-11-16
IE780645L (en) 1978-10-01
IT7848664A0 (en) 1978-03-30

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Legal Events

Date Code Title Description
PS Patent sealed [section 19, patents act 1949]
732 Registration of transactions, instruments or events in the register (sect. 32/1977)
PE20 Patent expired after termination of 20 years

Effective date: 19980330