US20040034472A1 - Methods for measurement, analysis and assessment of ground structure - Google Patents

Methods for measurement, analysis and assessment of ground structure Download PDF

Info

Publication number
US20040034472A1
US20040034472A1 US10/634,539 US63453903A US2004034472A1 US 20040034472 A1 US20040034472 A1 US 20040034472A1 US 63453903 A US63453903 A US 63453903A US 2004034472 A1 US2004034472 A1 US 2004034472A1
Authority
US
United States
Prior art keywords
ground
oscillation
vertical
points
measurement
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Abandoned
Application number
US10/634,539
Inventor
Koji Tokimatsu
Shinichi Kuwayama
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Individual
Original Assignee
Individual
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Individual filed Critical Individual
Priority to US10/634,539 priority Critical patent/US20040034472A1/en
Publication of US20040034472A1 publication Critical patent/US20040034472A1/en
Abandoned legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V1/00Seismology; Seismic or acoustic prospecting or detecting
    • G01V1/003Seismic data acquisition in general, e.g. survey design

Definitions

  • the present invention relates to methods for measurement, analysis and assessment of ground structure.
  • Short-period microseisms include not only substantive waves such as dilatational (P-) waves and S-waves but surface waves such as Rayleigh and Love waves. Since the confirmation or judgement of whether the detected waves are surface waves or not is not performed formed at measurement or analysis, it is impossible to judge whether the dispersion curve obtained is relevant to the surface waves and, hence, to accurately determine the ground structure.
  • phase velocity the velocity of propagation
  • wavelengths dispersions
  • the apparent phase velocity can be computed by averaging the correlation coefficients of the waveforms measured by equi-spaced oscillation sensors in different directions, that this apparent phase velocity varies with different sensor-to-sensor differences due to the influence of higher-order modes, and that when the horizontal and vertical components of the motion of a particle on the ground surface due to propagation of oscillations are detected and synthesized, the locus of rotation or orbit of a particle on the ground surface can be constructed, and that such surface waves are present in short-period microseisms as well.
  • the present invention is directed to a method for measurement, analysis and assessment of surface wave dispersion curves which serve as bases for evaluation of the tetonic and elastic characteristics of the ground by repeated simultaneous measurement of short-period microseisms at a plurality of points in a simple small-scale measuring system wherein 3 or more oscillation sensors are disposed at substantially equal sensor-to-sensor distances within a comparatively small area and inverse analysis of the surface wave dispersion curves at the points of measurement to compute the S-wave velocity of the ground and evaluate the laminar structure and features of the ground.
  • the present invention provides a method for estimating the laminar structure and characteristics of a ground which comprises disposing an oscillation sensor adapted to detect the vertical component or the vertical and horizontal components of oscillations at each of at least 3 points within a comparatively narrow area and thereby measuring microseisms at such plural points simultaneously, if necessary changing the points of measurement and repeating the measurement, and analyzing the vertical oscillation data or vertical and horizontal oscillation data.
  • the present invention is directed to a method for estimating the laminar structure and characteristics of a ground according to said first aspect wherein said microseisms to be measured are short-period microseisms observed at ground level.
  • the present invention is directed to a method according to said first aspect wherein two oscillation sensors are disposed on each of 2 or more straight lines passing through the ground to be measured and dividing the azimuth of 360 degrees into an even-number of sections or straight lines paralleled thereto in such a manner that all sensor-to-sensor-distances are equal on each of said straight lines.
  • the present invention provides a method according to said first aspect wherein said oscillation sensors are disposed at 3 or more points with equal spacings on the circumference of a circle and at one point in the center of the circle, or at a total of at least 4 points.
  • the present invention provides a method according to said first aspect wherein said oscillation sensors are disposed at a pices of a regular triangle and the center of gravity thereof or a total of 4 points.
  • the present invention is directed to a method for estimating the laminar structure and characteristics of a ground which comprises analyzing vertical oscillation data or vertical and horizontal oscillation data as measured simultaneously with oscillation sensors, judging whether the oscillation waves detected by said oscillation sensors are surface waves or not, and extracting and analyzing the surface waves.
  • the present invention is directed to a method for evaluating the laminar structure and characteristics of a ground which comprises analyzing the correlation coefficients and phase differences of oscillation data measured by equi-spaced oscillation sensors at respective frequencies, performing the analysis for each of varying sensor-to-sensor distances, analyzing and computing the fundamental mode of surface waves based on results of the respective analyses and, if necessary, analyzing and completing the higher-mode wavelengths.
  • the present invention relates to a method for estimating the laminar structure and characteristics of a ground which comprises performing the measurement and analysis of microseisms repeatedly until it can be concluded that a relation between phase velocity and wavelength such as to give a sufficiently accurate evaluation of ground structure can be achieved.
  • oscillation sensors for detecting the vertical component or the vertical and horizontal components of a vibration are disposed at 3 or more points within a comparatively small area at ground level and the microseisms are measured simultaneously at said points, if necessary changing the locations of said points of measurement and the resulting vertical oscillation data or vertical and horizontal oscillation data are analyzed.
  • the present invention is concerned with short-period microseisms which can be easily measured at ground level and as such does not require drilling and placement of instruments in the drilled holes or the use of an oscillation source so that the measurement and analysis of ground structure can be easily performed in any location.
  • the network of oscillation sensors for measurement can be set up in a comparatively confined area, the measurement is facilitated and can be performed even in a small plot of land.
  • the P and S waves can be differentiated and the surface waves only be positively measured to provide accurate information on the ground structure.
  • a plurality of oscillation sensors for detecting the vertical component or vertical and horizontal components of oscillations are arranged at 3 or more points in a comparatively small area, the measurements of microseisms at the respective points are simultaneously performed, if necessary varying the locations of said points and repeating the measurements, and the measured vertical oscillation data or vertical and horizontal oscillation data are analyzed to ascertain the laminar structure and characteristics of the ground. Therefore, the laminar structure and other characteristics of the ground can be determined not only expediently, positively and accurately but even when the area available for measurement is confined.
  • the laminar structure and other characteristics of the ground can be determined without calling for drilling of holes or the use of an oscillation source in addition to realization of the effects achieved by the first aspect of the invention.
  • two oscillation sensors are arranged on two or more straight lines passing through the ground to be measured and dividing the azimuth of 360 degrees into an even-number sections or straight lines parallel thereto in such a manner that the distance between the oscillation sensors is constant on each of said straight lines, with the result that, in addition to the effects of the first aspect of the invention, the field installation of the oscillation sensors is facilitated and, moreover, because the sensor-to-sensor distance is constant in different directions, the accuracy of measurement and analysis is improved.
  • the vertical oscillaton data or vertical and horizontal oscillation data measured simultaneously by said oscillation sensors are analyzed to see whether the oscillation waves detected by the oscillation sensors are surface waves or not and the laminar structure and other characteristics of the ground are still more accurately estimated from the accurate dispersion curves constructed by extraction and selective analysis of the surface waves.
  • the correlation coefficients and phase differences of the oscillation data measured by oscillation sensors disposed at equal spacings for the respective wavelength are analyzed, varying the sensor-to-sensor difference and repeating the measurements and, based on results of the respective analyses, the fundamental mode of the surface waves is analyzed and computed. If necessary the wavelength of the higher mode is analyzed and computed to assess the laminar structure and characteristics of the ground. Therefore, in addition to the effects of the first to the sixth aspect of the invention, the higher mode surface waves which could not be easily isolated in the past can be neatly isolated for insuring a further improvement in the accuracy of assessment of ground structure.
  • the measurement of microseisms and the analysis of measured microseisms data are continued until a relationship between phase velocity and wavelength such that the ground structure can be determined with sufficient accuracy is obtained so that the laminar structure and characteristics of the ground can be determined expediently, rapidly and accurately on a real-time basis.
  • FIG. 1 is a view showing the arrangement of oscillation sensors in an embodiment of the present invention
  • FIG. 2 is a schematic view showing the measurement, analysis and assessment system of the same
  • FIGS. 3 and 4 each is a flow chart for illustrating the procedure of said analysis and assessment
  • FIG. 5 is a schematic view showing the measured and theoretical dispersion curves
  • FIG. 6 is a tectonic characteristic diagram obtained by inverse analysis of the same according to the elastic wave propagation theory.
  • FIGS. 7 ( a ) through ( d ) are other arrangements of oscillation sensors.
  • FIGS. 1 and 2 which illustrate a typical arrangement of oscillation sensors and a schematic representation of the system embodying the principles of the invention
  • a three-component oscillation sensor 1 for detecting the vertical component of oscillation and the bidirectional horizontal component of oscillation as disposed in one position at ground level and a plurality of vertical-component oscillation sensors 2 a , 2 b and 2 c as disposed at positions corresponding to the apices B 1 through B 3 of a regular triangle with the length of one side being R and the center of gravity coinciding with said one point A.
  • the above-mentioned oscillation sensors 1 and 2 a through 2 c each comprises a speedometer and a displacement meter. In the above arrangement, the short-period microseisms are simultaneously measured.
  • the detection signal outputs from the respective oscillation sensors 1 and 2 a through 2 c are amplified by a signal amplifier 3 (FIG. 2) and then, fed to a data analyzer-assessor means 5 , comprised of a microcomputer, through an A/D converter 4 (interface).
  • the data analyzer/assessor means 5 analyzes the input data according to the processing flow shown in FIG. 3 to compute provisional dispersion curves and displays the curves on a cathode-ray tube CRT 6 .
  • the vertical and horizontal oscillation detection signal outputs from the oscillation sensors 1 and 2 a through 2 c located at points A and B 1 through B 3 are respectively amplified in the signal amplifier 3 and, after A/D conversion, are fed to said data analyzer/assessor means 5 for data analysis (( 1 ) in FIG. 3).
  • the oscillation data are filtered (( 2 ), FIG. 3) and subjected to spectrum analysis inclusive of FFT (high-speed Fourier transformation) to determine the coherence, correlation coefficient and phase difference of waves detected by the plural equi-spaced oscillation sensors for each of the frequencies (f) involved (FIG. 3, ( 3 )).
  • FFT high-speed Fourier transformation
  • the provisional dispersion curves determined by measurements for regular triangles varying in length of their sides (FIG. 4, ( 1 )-( 2 )) and if all the provisional dispersion curves are identical, they are taken as the final dispersion curves ( 3 ). If they are different, the fundamental mode and the higher-order mode are respectively isolated and the degree of predominance is determined for each frequency ( 4 ). Finally the final dispersion curve is determined.
  • the measured dispersion curve is represented by the mark “o” and the ground structure determined by said inverse analysis is shown in FIG. 6.
  • the solid line represents the theoretical dispersion curve of the ground, which is well consistent with the measured values, indicating that the characteristics of the ground can be determined with reliable accuracy.
  • FIG. 7( a ) shows an example of arrangement where oscillation'sensors 2 a through 2 e are disposed at apices of a regular pentagon, with an additional oscillation sensor 1 being disposed at the center of gravity of the pentagon.
  • FIG. 7( b ) is an example of arrangement in which six oscillation sensors 2 a through 2 f are disposed at apices of a regular hexagon.
  • oscillation sensors 1 and 2 a through 2 d are disposed at apices of three equilateral triangles each rotated through 45 degrees and having one of the apices in common.
  • the circumference of a circle is equally divided into 12 sections and oscillation sensors 1 and 2 a through 2 f are disposed on 6 of said circumferential sections and in the center of gravity.
  • the length of one side is about 30 cm at the minimum and about 30 m at the maximum.
  • the minimum length is about 20 cm and the maximum is about 20 m, in terms of the radius of a circle, so that the scale of measurement can be as much smaller.

Landscapes

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

Abstract

For determination of the laminar structure and other characteristics of a ground, oscillation sensors for detecting the vertical component or vertical and horizontal components of oscillations are disposed at three or more points within a comparatively small area at ground level to simultaneously measure microseisms at the respective points, if necessary with locations of said points being varied and measurements be performed at the respective locations and the vertical oscillation data or vertical and horizontal oscillation data thus generated are analyzed. This method not only permits an expedient, positive and accurate assessment of the laminar structure and other characteristics of the ground but also permits the measurement of ground structure even when the area available for measurement is small.

Description

    BACKGROUND OF THE INVENTION
  • 1. Technical Field [0001]
  • The present invention relates to methods for measurement, analysis and assessment of ground structure. [0002]
  • 2. Background Art [0003]
  • To determine the structure and characteristics of the surface layer of the ground, it has heretofore been necessary to drill a plurality of holes in the ground and insert or indwell instruments and ancillary devices into the holes and also to employ a source of oscillation for generating waves to be measured. It should, therefore, be obviously of great benefit if it were ever possible to know the,structure and characteristics of the surface layer of the ground without any of such efforts and contrivances. To this end, it might be contemplated to measure and analyze the oscillatory waves or microseisms observed in the surface layer of the ground. However, up to the present time, there is not known a measuring technology or a system of instrumental analysis, by means of which short-period microseisms could be measured with sufficient accuracy to estimate the tectonic and other characteristics of the surface layer of the ground inclusive of the velocity of shear (S) waves. [0004]
  • Furthermore, the prior art system designed to simultaneously measure short-period microseisms at a plurality of points to thereby delineate the ground structure has the following disadvantages. [0005]
  • A. Since the spacings of oscillation sensors must be large, that is to say the scale of measurement must be large, a large free area is required and it is time-consuming to connect the cords from the respective oscillation sensors for cental analysis. Moreover, because the large number of oscillation sensors are required, the analytical procedure is scaled up to the extent that the method cannot be utilized advantageously in the field. [0006]
  • B. Since the network of oscillation sensors is not tailored to improvement in measuring accuracy or resolution of high-order modes, the reliability of the measured dispersion curve is low. [0007]
  • C. Short-period microseisms include not only substantive waves such as dilatational (P-) waves and S-waves but surface waves such as Rayleigh and Love waves. Since the confirmation or judgement of whether the detected waves are surface waves or not is not performed formed at measurement or analysis, it is impossible to judge whether the dispersion curve obtained is relevant to the surface waves and, hence, to accurately determine the ground structure. [0008]
  • D. Since short-period waves include higher-modes surface waves, it is impossible to compute an accurate surface wave dispersion curve and, hence, to ascertain the surface layer structure of the ground unless some means for removing or separating these waves are available. [0009]
  • E. Since the dispersion curve cannot be computed real-time from field values, there is no knowing whether measurements were made with acceptable accuracy. [0010]
  • OBJECT OF THE INVENTION
  • It is an object of the present invention to provide a method for measurement, analysis and assessment of ground structure whereby the laminar structure and characteristics of the ground can be determined quickly, expediently and accurately through simultaneous ground-level observation and analysis of short-period microseisms even in a confined available land. [0011]
  • It is another object of the present invention to provide a method for measurement, analysis and assessment of ground structure which does not call for drilling of holes or the use of an oscillation source. [0012]
  • It is a further object of the invention to provide a method for measurement, analysis and assessment of ground structure in which the accuracy of measurement and analysis has been improved by using a network of substantially equi-spaced oscillation sensors which facilitates field sensor positioning as well. [0013]
  • It is another object of the present invention to provide a method for measurement, analysis and assessment of ground structure by which the laminar structure and characteristics of the ground can be ascertained with accuracy through selective extraction of surface waves. [0014]
  • It is still another object of the present invention to provide a method for measurement, analysis and assessment of ground structure by which the accuracy of assessment of the ground structure can be improved by a collective analysis of data obtained by repeated measurement using dissimilar sensor-to-sensor distances. [0015]
  • It is still another object of the present invention to provide a method for measurement, analysis and assessment of ground structure by which the laminar structure and characteristics of the ground can be evaluated conveniently and accurately on a real-time basis. [0016]
  • SUMMARY OF THE INVENTION
  • The present invention is predicated on the facts that when surface waves such as Rayleigh waves are propagated through a horizontal multi-layer ground structure, phase velocity (the velocity of propagation) varies with different wavelengths (dispersions), that the apparent phase velocity can be computed by averaging the correlation coefficients of the waveforms measured by equi-spaced oscillation sensors in different directions, that this apparent phase velocity varies with different sensor-to-sensor differences due to the influence of higher-order modes, and that when the horizontal and vertical components of the motion of a particle on the ground surface due to propagation of oscillations are detected and synthesized, the locus of rotation or orbit of a particle on the ground surface can be constructed, and that such surface waves are present in short-period microseisms as well. As such, the present invention is directed to a method for measurement, analysis and assessment of surface wave dispersion curves which serve as bases for evaluation of the tetonic and elastic characteristics of the ground by repeated simultaneous measurement of short-period microseisms at a plurality of points in a simple small-scale measuring system wherein 3 or more oscillation sensors are disposed at substantially equal sensor-to-sensor distances within a comparatively small area and inverse analysis of the surface wave dispersion curves at the points of measurement to compute the S-wave velocity of the ground and evaluate the laminar structure and features of the ground. [0017]
  • In the first aspect, the present invention provides a method for estimating the laminar structure and characteristics of a ground which comprises disposing an oscillation sensor adapted to detect the vertical component or the vertical and horizontal components of oscillations at each of at least 3 points within a comparatively narrow area and thereby measuring microseisms at such plural points simultaneously, if necessary changing the points of measurement and repeating the measurement, and analyzing the vertical oscillation data or vertical and horizontal oscillation data. [0018]
  • In the second aspect, the present invention is directed to a method for estimating the laminar structure and characteristics of a ground according to said first aspect wherein said microseisms to be measured are short-period microseisms observed at ground level. [0019]
  • In the third aspect, the present invention is directed to a method according to said first aspect wherein two oscillation sensors are disposed on each of 2 or more straight lines passing through the ground to be measured and dividing the azimuth of 360 degrees into an even-number of sections or straight lines paralleled thereto in such a manner that all sensor-to-sensor-distances are equal on each of said straight lines. [0020]
  • In the fourth aspect, the present invention provides a method according to said first aspect wherein said oscillation sensors are disposed at 3 or more points with equal spacings on the circumference of a circle and at one point in the center of the circle, or at a total of at least 4 points. [0021]
  • In the fifth aspect, the present invention provides a method according to said first aspect wherein said oscillation sensors are disposed at a pices of a regular triangle and the center of gravity thereof or a total of 4 points. [0022]
  • In the sixth aspect, the present invention is directed to a method for estimating the laminar structure and characteristics of a ground which comprises analyzing vertical oscillation data or vertical and horizontal oscillation data as measured simultaneously with oscillation sensors, judging whether the oscillation waves detected by said oscillation sensors are surface waves or not, and extracting and analyzing the surface waves. [0023]
  • In the seventh aspect, the present invention is directed to a method for evaluating the laminar structure and characteristics of a ground which comprises analyzing the correlation coefficients and phase differences of oscillation data measured by equi-spaced oscillation sensors at respective frequencies, performing the analysis for each of varying sensor-to-sensor distances, analyzing and computing the fundamental mode of surface waves based on results of the respective analyses and, if necessary, analyzing and completing the higher-mode wavelengths. [0024]
  • In the eighth aspect, the present invention relates to a method for estimating the laminar structure and characteristics of a ground which comprises performing the measurement and analysis of microseisms repeatedly until it can be concluded that a relation between phase velocity and wavelength such as to give a sufficiently accurate evaluation of ground structure can be achieved. [0025]
  • Thus, in accordance with the present invention, oscillation sensors for detecting the vertical component or the vertical and horizontal components of a vibration are disposed at 3 or more points within a comparatively small area at ground level and the microseisms are measured simultaneously at said points, if necessary changing the locations of said points of measurement and the resulting vertical oscillation data or vertical and horizontal oscillation data are analyzed. By measuring microseisms with a small network of oscillation sensors, the accuracy of assessment of the surface structure of the ground can be improved and a system enabling a rapid field measurement, analysis and assessment can be constructed. Therefore, the laminar structure and characteristics of the ground can be estimated expediently, positively and accurately. [0026]
  • Furthermore, the present invention is concerned with short-period microseisms which can be easily measured at ground level and as such does not require drilling and placement of instruments in the drilled holes or the use of an oscillation source so that the measurement and analysis of ground structure can be easily performed in any location. [0027]
  • Moreover, since the network of oscillation sensors for measurement can be set up in a comparatively confined area, the measurement is facilitated and can be performed even in a small plot of land. [0028]
  • In addition, when the vertical and horizontal oscillation data are analyzed and the locus of rotation of a particle on the ground surface due to propagation of oscillations is constructed and the analysis and assessment are carried out on confirming that the measured waves are surface waves, the P and S waves can be differentiated and the surface waves only be positively measured to provide accurate information on the ground structure. [0029]
  • Moreover, when oscillation sensors are disposed in a network wherein sensor-to-sensor distances are substantially equal and the measurement of waves is repeated varying the sensor-to-sensor distances, the high-mode surface waves can be isolated from the fundamental mode, with the result that a highly accurate relation of dispersion wave to wavelength can be obtained. It is because the analytical system is constructed using a microcomputer that the assessment can be obtained on the spot. [0030]
  • Moreover, when it is so arranged that the measurement of microseisms, amplification of detected signals and the analysis and assessment of data are automatically performed as a sequence, the relationship between dispersion curve and wavelength can be more accurately determined in the field. [0031]
  • EFFECTS OF THE INVENTION
  • In accordance with the present invention, a plurality of oscillation sensors for detecting the vertical component or vertical and horizontal components of oscillations are arranged at 3 or more points in a comparatively small area, the measurements of microseisms at the respective points are simultaneously performed, if necessary varying the locations of said points and repeating the measurements, and the measured vertical oscillation data or vertical and horizontal oscillation data are analyzed to ascertain the laminar structure and characteristics of the ground. Therefore, the laminar structure and other characteristics of the ground can be determined not only expediently, positively and accurately but even when the area available for measurement is confined. [0032]
  • In the second aspect of the present invention wherein said microseisms to be measured are short-period microseisms observed on the surface of the ground, the laminar structure and other characteristics of the ground can be determined without calling for drilling of holes or the use of an oscillation source in addition to realization of the effects achieved by the first aspect of the invention. [0033]
  • According to the third aspect of the invention, two oscillation sensors are arranged on two or more straight lines passing through the ground to be measured and dividing the azimuth of 360 degrees into an even-number sections or straight lines parallel thereto in such a manner that the distance between the oscillation sensors is constant on each of said straight lines, with the result that, in addition to the effects of the first aspect of the invention, the field installation of the oscillation sensors is facilitated and, moreover, because the sensor-to-sensor distance is constant in different directions, the accuracy of measurement and analysis is improved. [0034]
  • Comparable effects are obtained in the fourth and fifth inventions. [0035]
  • In accordance with the sixth aspect of the present invention, the vertical oscillaton data or vertical and horizontal oscillation data measured simultaneously by said oscillation sensors are analyzed to see whether the oscillation waves detected by the oscillation sensors are surface waves or not and the laminar structure and other characteristics of the ground are still more accurately estimated from the accurate dispersion curves constructed by extraction and selective analysis of the surface waves. [0036]
  • In accordance with the seventh aspect of the present invention, the correlation coefficients and phase differences of the oscillation data measured by oscillation sensors disposed at equal spacings for the respective wavelength are analyzed, varying the sensor-to-sensor difference and repeating the measurements and, based on results of the respective analyses, the fundamental mode of the surface waves is analyzed and computed. If necessary the wavelength of the higher mode is analyzed and computed to assess the laminar structure and characteristics of the ground. Therefore, in addition to the effects of the first to the sixth aspect of the invention, the higher mode surface waves which could not be easily isolated in the past can be neatly isolated for insuring a further improvement in the accuracy of assessment of ground structure. [0037]
  • In accordance with the eighth aspect of the invention, the measurement of microseisms and the analysis of measured microseisms data are continued until a relationship between phase velocity and wavelength such that the ground structure can be determined with sufficient accuracy is obtained so that the laminar structure and characteristics of the ground can be determined expediently, rapidly and accurately on a real-time basis.[0038]
  • BRIEF DESCRIPTION OF THE DRAWINGS
  • FIG. 1 is a view showing the arrangement of oscillation sensors in an embodiment of the present invention; [0039]
  • FIG. 2 is a schematic view showing the measurement, analysis and assessment system of the same; [0040]
  • FIGS. 3 and 4 each is a flow chart for illustrating the procedure of said analysis and assessment; [0041]
  • FIG. 5 is a schematic view showing the measured and theoretical dispersion curves; [0042]
  • FIG. 6 is a tectonic characteristic diagram obtained by inverse analysis of the same according to the elastic wave propagation theory; and [0043]
  • FIGS. [0044] 7(a) through (d) are other arrangements of oscillation sensors.
  • DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS
  • The preferred embodiments of the present invention are described in detail. [0045]
  • Referring to FIGS. 1 and 2 which illustrate a typical arrangement of oscillation sensors and a schematic representation of the system embodying the principles of the invention, a three-[0046] component oscillation sensor 1 for detecting the vertical component of oscillation and the bidirectional horizontal component of oscillation as disposed in one position at ground level and a plurality of vertical- component oscillation sensors 2 a, 2 b and 2 c as disposed at positions corresponding to the apices B1 through B3 of a regular triangle with the length of one side being R and the center of gravity coinciding with said one point A.
  • The above-mentioned [0047] oscillation sensors 1 and 2 a through 2 c each comprises a speedometer and a displacement meter. In the above arrangement, the short-period microseisms are simultaneously measured.
  • The detection signal outputs from the [0048] respective oscillation sensors 1 and 2 a through 2 c are amplified by a signal amplifier 3 (FIG. 2) and then, fed to a data analyzer-assessor means 5, comprised of a microcomputer, through an A/D converter 4 (interface).
  • The data analyzer/assessor means [0049] 5 analyzes the input data according to the processing flow shown in FIG. 3 to compute provisional dispersion curves and displays the curves on a cathode-ray tube CRT 6.
  • The measurement, analysis and assessment functions of the system are described in detail below, referring to the flow charts shown in FIGS. 3 and 4. [0050]
  • Referring back to FIG. 1, the vertical and horizontal oscillation detection signal outputs from the [0051] oscillation sensors 1 and 2 a through 2 c located at points A and B1 through B3 are respectively amplified in the signal amplifier 3 and, after A/D conversion, are fed to said data analyzer/assessor means 5 for data analysis ((1) in FIG. 3).
  • The oscillation data are filtered (([0052] 2), FIG. 3) and subjected to spectrum analysis inclusive of FFT (high-speed Fourier transformation) to determine the coherence, correlation coefficient and phase difference of waves detected by the plural equi-spaced oscillation sensors for each of the frequencies (f) involved (FIG. 3, (3)). When there is horizontal component data (FIG. 3, (4)), the direction of approach of the dominant wave is determined (FIG. 3, (5)), the horizontal component data measured by oscillation sensors 1 and 2 a through 2 c are analyzed in a direction perpendicular to the direction of approach of the waves (FIG. 3, (6)), and the movements of the ground surface in the planes parallel and perpendicular to the direction of approach of the waves are determined as the locus of rotation of a particle on the ground surface (FIG. 3, (7)). Then, it is inquired if the predominant seismic wave is a surface wave or not (FIG. 3, (8)). If the answer is affirmative, a provisional dispersion curve (FIG. 3, (9)) is computed for the frequency relevant to the surface wave.
  • The above series of measurement, analysis and assement is performed with the length of sides of the tringle at the apices of which said [0053] oscillation sensors 2 a, 2 b and 2 c are situated being varied from 50 cm to 1 m to 2 m to 5 m and to 10 m or, alternatively, with a plurality of regular triangles varying in the length of sides being laid out and said oscillation sensors are disposed at the apices of each triangle.
  • Then, the provisional dispersion curves determined by measurements for regular triangles varying in length of their sides (FIG. 4, ([0054] 1)-(2)) and if all the provisional dispersion curves are identical, they are taken as the final dispersion curves (3). If they are different, the fundamental mode and the higher-order mode are respectively isolated and the degree of predominance is determined for each frequency (4). Finally the final dispersion curve is determined.
  • With respect to the dispersion curve thus determined, inverse analysis based on the theory of elastic wave propagation is carried out to estimate the laminar structure and characteristics of the ground. [0055]
  • In FIG. 5, the measured dispersion curve is represented by the mark “o” and the ground structure determined by said inverse analysis is shown in FIG. 6. In FIG. 5, the solid line represents the theoretical dispersion curve of the ground, which is well consistent with the measured values, indicating that the characteristics of the ground can be determined with reliable accuracy. [0056]
  • Now, the measurement of microseisms and the analysis of measured microseisms are automatically continued until it can be judged that the relationship between phase velocity and wavelength which would be conducive to a sufficiently accurate structural determination. In this manner, the laminar structure and characteristics of the ground can be determined expediently and accurately on a real-time basis. [0057]
  • FIG. 7([0058] a) shows an example of arrangement where oscillation'sensors 2 a through 2 e are disposed at apices of a regular pentagon, with an additional oscillation sensor 1 being disposed at the center of gravity of the pentagon.
  • FIG. 7([0059] b) is an example of arrangement in which six oscillation sensors 2 a through 2 f are disposed at apices of a regular hexagon. In the arrangement illustrated in FIG. 7(c), oscillation sensors 1 and 2 a through 2 d are disposed at apices of three equilateral triangles each rotated through 45 degrees and having one of the apices in common. In the arrangement shown in FIG. 7(d), the circumference of a circle is equally divided into 12 sections and oscillation sensors 1 and 2 a through 2 f are disposed on 6 of said circumferential sections and in the center of gravity.
  • In the arrangement of FIG. 1 wherein short-period microseisms are subjects of measurement, the length of one side is about 30 cm at the minimum and about 30 m at the maximum. In contrast, in the arrangements shown in FIG. 7, the minimum length is about 20 cm and the maximum is about 20 m, in terms of the radius of a circle, so that the scale of measurement can be as much smaller. [0060]

Claims (8)

What is claimed is:
1. A method for estimating the laminar structure and other characteristics of a ground which comprises disposing an oscillation sensor adapted to detect the vertical component or the vertical and horizontal components of oscillations at each of at least 3 points within a comparatively small area at ground level to simultaneously measure microseisms at such plural points, if necessary changing the locations of said points of measurement and repeating the measurements, and analyzing the vertical oscillation data or vertical and horizontal oscillation data.
2. A method for estimating the laminar structure and other characteristics of a ground according to claim 1 wherein said microseisms to be measured are short-period microseisms observed at ground level.
3. A method according to claim 1 wherein two oscillation sensors are disposed on each of 2 or more straight lines passing through the ground to be measured and dividing the azimuth of 360 degrees into an even-number of equal sections or straight lines paralled thereto in such a manner that sensor-to-sensor distances are equal on said straight lines.
4. A method according to claim 1 wherein said oscillation sensors are disposed at 3 or more points at qual spacings on the circumference of a circle and at one point in the center of the circle, or at a total of at least 4 points.
5. A method according to claim 1 wherein said oscillation sensors are disposed at apices of a regular triangle and the center of gravity thereof or a total of 4 points.
6. A method for estimating the laminar structure and characteristics of a ground according to any of claims 1 to 6 which comprises analyzing vertical oscillation data or vertical and horizontal oscillation data as measured simultaneously with said oscillation sensors, judging whether the oscillation waves detected by said oscillation sensors are surface waves or not, and extracting and analyzing the surface waves.
7. A method for estimating the laminar structure and characteristics of a ground according to any of claims 1 to 6, which comprises analyzing the correlation coefficient and phase difference of oscillation data measured by equi-spaced oscillation sensors for each frequency, performing the analysis repeatedly with sensor-to-sensor distances varied, analyzing and computing the fundamental mode of surface waves based on results of the respective analyses and, if necessary, analyzing and computing the higher-mode wavelengths.
8. A method for estimating the laminar structure and characteristics of a ground according to any of claims 1 to 7 which comprises performing the measurement and analysis of microseisms repeatedly until it can be concluded that a relation between phase velocity and wavelength such as to give a sufficiently accurate assessment of ground structure is achieved.
US10/634,539 1990-04-28 2003-08-04 Methods for measurement, analysis and assessment of ground structure Abandoned US20040034472A1 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
US10/634,539 US20040034472A1 (en) 1990-04-28 2003-08-04 Methods for measurement, analysis and assessment of ground structure

Applications Claiming Priority (9)

Application Number Priority Date Filing Date Title
JP11222190A JP2958362B2 (en) 1990-04-28 1990-04-28 Measurement, analysis and judgment method of ground structure
JP2-112221 1990-04-28
US68621691A 1991-04-16 1991-04-16
US21012094A 1994-03-16 1994-03-16
US34096594A 1994-11-17 1994-11-17
US57391495A 1995-12-18 1995-12-18
US08/887,686 US6253870B1 (en) 1990-04-28 1997-07-03 Methods for measurement, analysis and assessment of ground structure
US09/638,681 US6612398B1 (en) 1990-04-28 2000-08-15 Methods for measurement, analysis and assessment of ground structure
US10/634,539 US20040034472A1 (en) 1990-04-28 2003-08-04 Methods for measurement, analysis and assessment of ground structure

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
US09/638,681 Continuation US6612398B1 (en) 1990-04-28 2000-08-15 Methods for measurement, analysis and assessment of ground structure

Publications (1)

Publication Number Publication Date
US20040034472A1 true US20040034472A1 (en) 2004-02-19

Family

ID=14581285

Family Applications (3)

Application Number Title Priority Date Filing Date
US08/887,686 Expired - Fee Related US6253870B1 (en) 1990-04-28 1997-07-03 Methods for measurement, analysis and assessment of ground structure
US09/638,681 Expired - Fee Related US6612398B1 (en) 1990-04-28 2000-08-15 Methods for measurement, analysis and assessment of ground structure
US10/634,539 Abandoned US20040034472A1 (en) 1990-04-28 2003-08-04 Methods for measurement, analysis and assessment of ground structure

Family Applications Before (2)

Application Number Title Priority Date Filing Date
US08/887,686 Expired - Fee Related US6253870B1 (en) 1990-04-28 1997-07-03 Methods for measurement, analysis and assessment of ground structure
US09/638,681 Expired - Fee Related US6612398B1 (en) 1990-04-28 2000-08-15 Methods for measurement, analysis and assessment of ground structure

Country Status (8)

Country Link
US (3) US6253870B1 (en)
EP (2) EP0455091B1 (en)
JP (1) JP2958362B2 (en)
CN (1) CN1033406C (en)
CA (1) CA2040977C (en)
DE (1) DE69130000T2 (en)
ES (1) ES2122963T3 (en)
RU (1) RU2106000C1 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20130100769A1 (en) * 2011-10-19 2013-04-25 Global Microseismic Services, Inc. Microseismic Data Acquisition Array and Corresponding Method

Families Citing this family (36)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2958362B2 (en) * 1990-04-28 1999-10-06 孝次 時松 Measurement, analysis and judgment method of ground structure
RU2030766C1 (en) * 1993-01-05 1995-03-10 Виктор Никифорович Лисин Method of seismic prospecting
JP2743975B2 (en) * 1993-06-21 1998-04-28 財団法人鉄道総合技術研究所 Ground liquefaction determination method
GB9906995D0 (en) * 1998-09-16 1999-05-19 Geco Prakla Uk Ltd Seismic detection apparatus and related method
US7028772B2 (en) * 2000-04-26 2006-04-18 Pinnacle Technologies, Inc. Treatment well tiltmeter system
GB2372568B (en) * 2001-02-26 2004-05-12 Abb Offshore Systems Ltd Seismic detection
JP3617036B2 (en) * 2001-05-22 2005-02-02 ビイック株式会社 Ground exploration device and analysis program used therefor
US7330799B2 (en) * 2001-12-21 2008-02-12 Société de commercialisation des produits de la recherche appliquée-Socpra Sciences et Génie s.e.c. Method and algorithm for using surface waves
CA2365336A1 (en) * 2001-12-21 2003-06-21 Universite De Sherbrooke Method and algorithm for using surface waves
JP4071988B2 (en) * 2002-04-30 2008-04-02 応用地質株式会社 Ground survey method using S-wave amplitude associated with impact penetration
US8235844B2 (en) 2010-06-01 2012-08-07 Adams Golf Ip, Lp Hollow golf club head
US6985816B2 (en) * 2003-09-15 2006-01-10 Pinnacle Technologies, Inc. Methods and systems for determining the orientation of natural fractures
US20060081412A1 (en) * 2004-03-16 2006-04-20 Pinnacle Technologies, Inc. System and method for combined microseismic and tiltmeter analysis
AU2005238921A1 (en) * 2004-04-21 2005-11-10 Halliburton Energy Services, Inc. Microseismic fracture mapping using seismic source timing measurements for velocity calibration
FR2870006B1 (en) * 2004-05-07 2006-06-23 Sismocean Soc Par Actions Simp PROCESS FOR AUSCULATING SOIL IN NEAR SURFACE AND / OR IN BASEMENT FOR DETECTION OF LOCAL HETEROGENEITIES IN THE ENVIRONMENT
GB2419410B (en) * 2004-10-20 2008-05-21 Vetco Gray Controls Ltd Sensor configuration
US7676326B2 (en) * 2006-06-09 2010-03-09 Spectraseis Ag VH Reservoir Mapping
WO2008001335A2 (en) * 2006-06-30 2008-01-03 Spectraseis Ag Vh signal integration measure for seismic data
WO2008142495A1 (en) * 2007-05-17 2008-11-27 Spectraseis Ag Seismic attributes for reservoir localization
WO2009120401A1 (en) * 2008-03-28 2009-10-01 Exxonmobil Upstream Research Company Characterizing spatial variablility of surface waves in seismic processing
US8632419B2 (en) 2010-03-05 2014-01-21 Callaway Golf Company Golf club head
US8821312B2 (en) 2010-06-01 2014-09-02 Taylor Made Golf Company, Inc. Golf club head having a stress reducing feature with aperture
US8827831B2 (en) 2010-06-01 2014-09-09 Taylor Made Golf Company, Inc. Golf club head having a stress reducing feature
US9089749B2 (en) 2010-06-01 2015-07-28 Taylor Made Golf Company, Inc. Golf club head having a shielded stress reducing feature
WO2012015520A1 (en) 2010-07-26 2012-02-02 Exxonmobil Upstream Research Company Seismic acquisition method for mode separation
US8585510B1 (en) 2010-08-30 2013-11-19 Callaway Golf Company Golf club head with improved aerodynamic characteristics
US8715102B1 (en) 2011-03-10 2014-05-06 Callaway Golf Company Adjustable golf club shaft and hosel assembly
US8684859B1 (en) 2011-03-10 2014-04-01 Callaway Golf Company Adjustable golf club shaft and hosel assembly
US8753221B1 (en) 2012-01-26 2014-06-17 Callaway Golf Company Adjustable golf club shaft and hosel assembly
US10466376B2 (en) 2013-06-03 2019-11-05 Cgg Services Sas Device and method for velocity function extraction from the phase of ambient noise
CN103412322B (en) * 2013-08-13 2015-10-28 中国科学院武汉岩土力学研究所 A kind of micro seismic monitoring three component sensor
JP6672977B2 (en) * 2016-04-19 2020-03-25 株式会社大林組 Ground estimation method
EP3635185A1 (en) * 2017-06-09 2020-04-15 Volvo Construction Equipment AB An information system for a working machine
CN108152854B (en) * 2017-11-30 2020-02-07 福建省建筑设计研究院有限公司 Micro-motion power spectral density-based nondestructive detection method and application thereof
CN110031893A (en) * 2019-04-19 2019-07-19 中国电建集团铁路建设有限公司 Drilling surveys new method with combining the subway engineering of fine motion detection
US11786784B1 (en) 2022-12-16 2023-10-17 Topgolf Callaway Brands Corp. Golf club head

Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3344881A (en) * 1966-09-27 1967-10-03 Marathon Oil Co Seismic detection method
US3506957A (en) * 1968-06-28 1970-04-14 Dresser Ind Strong motion recorder using velocity geophone
US3812457A (en) * 1969-11-17 1974-05-21 Shell Oil Co Seismic exploration method
US3893066A (en) * 1974-02-25 1975-07-01 Mark Products Apparatus and method for adjusting the output of a plurality of geophones to eliminate the effect of variations in the near surface character of the earth
US4403312A (en) * 1980-12-30 1983-09-06 Mobil Oil Corporation Three-dimensional seismic data gathering method
US4554648A (en) * 1980-07-03 1985-11-19 The United States Of America As Represented By The Secretary Of The Army Electronic earth seismic noise measuring method
US4649524A (en) * 1983-07-05 1987-03-10 Potash Corporation Of Saskatchewan Mining Limited Integrated acoustic network
US4935905A (en) * 1989-08-04 1990-06-19 Terra Linda Canada, Inc. Method and apparatus for seismic exploration
US5010976A (en) * 1989-10-04 1991-04-30 Atlantic Richfield Company Characterization of the full elastic effect of the near surface on seismic waves
US5029145A (en) * 1990-05-29 1991-07-02 Amoco Corporation Methods of geophysical exploration
US6253870B1 (en) * 1990-04-28 2001-07-03 Koji Tokimatsu Methods for measurement, analysis and assessment of ground structure

Family Cites Families (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
SU705398A1 (en) * 1977-09-19 1979-12-25 Сибирское Особое Конструкторское Бюро Научно-Производственного Объединения "Союзгеофизика" Automatic seismic station
SU1000971A1 (en) * 1980-05-07 1983-02-28 Институт геологии и геофизики СО АН СССР Device for seismic sign al recognition
SU1022090A1 (en) * 1981-04-06 1983-06-07 Sedin Aleksandr M Method of seismic prospecting
JPS6089788A (en) * 1983-10-21 1985-05-20 Agency Of Ind Science & Technol Surveying method of earthquake on ground surface and ground surface type geophone
JPS6089783A (en) * 1983-10-24 1985-05-20 Nissan Motor Co Ltd Ultrasonic distance detector
SU1377795A1 (en) * 1986-03-26 1988-02-28 Научно-производственное объединение "Рудгеофизика" Method of seismic prospecting
JPS6341500A (en) * 1986-08-07 1988-02-22 Takeda Chem Ind Ltd Human interferon-alpha derivative
SU1513408A1 (en) * 1986-11-10 1989-10-07 Всесоюзный Научно-Исследовательский Институт Геофизических Методов Разведки Method of seismic study of earthъs crust and mantle
SU1434378A1 (en) * 1987-03-09 1988-10-30 Институт физики Земли им.О.Ю.Шмидта Method of short-time forecasting of powerful earthquakes
DE3736873A1 (en) * 1987-10-30 1989-05-11 Adalbert Hayduk ARRANGEMENT FOR SHORT-TERM EARTHQUAKE PREDICTION
SU1589230A1 (en) * 1988-04-13 1990-08-30 Институт физики Земли им.О.Ю.Шмидта Method of seismic investigations of deposits of oil and gas

Patent Citations (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3344881A (en) * 1966-09-27 1967-10-03 Marathon Oil Co Seismic detection method
US3506957A (en) * 1968-06-28 1970-04-14 Dresser Ind Strong motion recorder using velocity geophone
US3812457A (en) * 1969-11-17 1974-05-21 Shell Oil Co Seismic exploration method
US3893066A (en) * 1974-02-25 1975-07-01 Mark Products Apparatus and method for adjusting the output of a plurality of geophones to eliminate the effect of variations in the near surface character of the earth
US4554648A (en) * 1980-07-03 1985-11-19 The United States Of America As Represented By The Secretary Of The Army Electronic earth seismic noise measuring method
US4403312A (en) * 1980-12-30 1983-09-06 Mobil Oil Corporation Three-dimensional seismic data gathering method
US4649524A (en) * 1983-07-05 1987-03-10 Potash Corporation Of Saskatchewan Mining Limited Integrated acoustic network
US4935905A (en) * 1989-08-04 1990-06-19 Terra Linda Canada, Inc. Method and apparatus for seismic exploration
US5010976A (en) * 1989-10-04 1991-04-30 Atlantic Richfield Company Characterization of the full elastic effect of the near surface on seismic waves
US6253870B1 (en) * 1990-04-28 2001-07-03 Koji Tokimatsu Methods for measurement, analysis and assessment of ground structure
US6612398B1 (en) * 1990-04-28 2003-09-02 Koji Tokimatsu Methods for measurement, analysis and assessment of ground structure
US5029145A (en) * 1990-05-29 1991-07-02 Amoco Corporation Methods of geophysical exploration

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20130100769A1 (en) * 2011-10-19 2013-04-25 Global Microseismic Services, Inc. Microseismic Data Acquisition Array and Corresponding Method
US9354336B2 (en) * 2011-10-19 2016-05-31 Global Ambient Seismic, Inc. Microseismic data acquisition array and corresponding method

Also Published As

Publication number Publication date
EP0455091B1 (en) 1998-08-19
CA2040977C (en) 2000-03-07
JP2958362B2 (en) 1999-10-06
US6253870B1 (en) 2001-07-03
ES2122963T3 (en) 1999-01-01
CN1057112A (en) 1991-12-18
JPH0412291A (en) 1992-01-16
EP0455091A3 (en) 1993-02-10
DE69130000T2 (en) 1999-05-12
RU2106000C1 (en) 1998-02-27
EP0455091A2 (en) 1991-11-06
EP0845688A2 (en) 1998-06-03
CA2040977A1 (en) 1991-10-29
US6612398B1 (en) 2003-09-02
CN1033406C (en) 1996-11-27
DE69130000D1 (en) 1998-09-24
EP0845688A3 (en) 1998-07-29

Similar Documents

Publication Publication Date Title
US6253870B1 (en) Methods for measurement, analysis and assessment of ground structure
EP1331490B1 (en) Sound source probing system
US6138512A (en) Method and apparatus for determining source location of energy carried in the form of propagating waves through a conducting medium
US7162043B2 (en) Microphone array sound source location system with imaging overlay
EP2293117B1 (en) VH Signal Integration Measure for Seismic Data
RU2144684C1 (en) Method of formation of vertical seismic sections in process of drilling of holes
US5406530A (en) Pseudo-random binary sequence measurement method
JPH02212734A (en) Apparatus and method for detecting change in structual integrity of structural member
JPH0374349B2 (en)
US8639442B2 (en) Identifying invalid seismic data
CN107153224B (en) Wave detector dynamic performance integrated test and evaluation method
EP0685078B1 (en) Location of buried conductors
KR101368196B1 (en) Apparatus for measuring wave transmission velocity and method for measuring wave transmission velocity using thereof
JP3919015B2 (en) Method and apparatus for nondestructive inspection of trees using acoustic tomography
CN113189641B (en) Two-channel multi-mode Rayleigh wave underground detection system and method
US4697456A (en) Leakage test for liquid containment
JPH0511895B2 (en)
EP1769267B1 (en) Movement detection system and method
CN115450268A (en) Disk supporting pile detection device and method
US20050162974A1 (en) Resonance scattering seismic method
US4875197A (en) Method and apparatus for determining propagation velocities of elastic waves in a borehole
Baziw et al. Quality Assessment of Seismic Data Sets and the Impact on Interval Velocity Estimates in DST
JP2006292415A (en) Survey method of cavity
CN108627237A (en) A kind of autocorrelation analysis signal processing method based on distributed optical fiber sensing system
WO2023106418A1 (en) Magnetic exploration system

Legal Events

Date Code Title Description
STCB Information on status: application discontinuation

Free format text: ABANDONED -- FAILURE TO RESPOND TO AN OFFICE ACTION