Method and apparatus for mapping the underground soil

• US 20160187524A1
• Filed: 12/29/2014
• Published: 06/30/2016
• Est. Priority Date: 12/29/2014
• Status: Active Grant

• Current Assignee: Suhami, Avraham
• Original Assignee: Suhami, Avraham
• Inventors: Suhami, Avraham
• Granted Patent: US 9,568,635 B2
• Time in Patent Office: Days
• US Class Current: 1/1
• CPC Class Codes: G01V 3/30 operating with electromagnetic waves

Abstract

The invention describes a method and system, for mapping non-magnetic soils in terms of their local permittivity and velocity of the traversing electromagnetic waves, by measuring the straight-line attenuation and elapsed time between transmitters and receivers located within tubes inserted into the soil.

Claims

1. - A Method and system for mapping the soil using electromagnetic transmitters and receivers inserted within boreholes extending to any practical depth, wherein,

the distance between said electromagnetic transmitters and receivers are maximized by operating at the local resonant frequency (f) of the soil f=(½

π

) [L(μ

)C(∈

)]<sup>−

12</sup> where the resistance is minimal and wherein,

activating the transmitter for a short wavelet time “

Δ

t=(3λ

/V)”

wherein (λ

) is the wavelength and (V) the speed of the radiation in said soil, such that at least one wavelet of radiation reaches the receiver in least-time, hereinafter referred to as the straight-line distance “

SLD”

, and wherein,

the receiver stays shut for a time period equal to the propagation-time “

T₀”

between the transmitter and the receiver, and after said “

T₀”

time, it opens for the short time “

Δ

t” and

wherein,

all events arriving at the receiver are checked for the phase shift “

Δ

φ

”

between their original phase “

φ

₀”

when transmitted, and the current one “

φ

_c”

, and if there is a phase difference “

Δ

φ

=”

φ

_c−

φ

₀”

larger than φ

_min, they are not given access to the receiver, and wherein,

the polarization of all the events arriving at the receiver are passed through a mechanical polarization filter tuned to the same linear polarization, when emitted by the transmitter, so that events with a different polarization are eliminated, and wherein,

both the receiver and the transmitter wait for several “

T₀”

periods, hereinafter referred to as an “

nT₀”

period, where (n)>

(n_min), until all events detected by the receiver subside, and wherein,

the sequence comprising, the transmitter transmitting for Δ

t period, followed by the receiver waiting for “

T₀”

period and opening for a “

Δ

t”

period and shutting back, and then waiting for “

nT₀”

period, is repeated “

m”

times, until the cumulative “

Straight-Line”

events overcome the random noise of the receiver and consequently reach the minimal sensitivity level of the receiver and trigger it, and wherein,

the maximal distance between the transmitter and the receiver at which the receiver is triggered according to the above procedure, is referred to as the maximal “

Straight-Line Distance” and

abbreviated as maximal “

SLD”

.

2. - A Method and system for mapping the soil using electromagnetic transmitters and receivers inserted within boreholes as in claim 1 wherein,

tubes extending to any practical depth, are inserted into their respective boreholes wherein, said tubes and the space between them and the soil, are filled with material that have a composition in terms of conductivity (σ

), permittivity (∈

_r) and permeability (μ

), close to that of the soil, so that the electromagnetic radiation traversing the tube walls and the space between the tube, the transmitter or the receiver, undergo minimal reflection and refraction and wherein,

said tubes, after inserted into their boreholes, are substantially parallel in 3D and equidistant along their length and wherein,

the actual distances between the different levels of said tubes are measured after insertion in the soil, in both directions and any attenuation measurements between the tubes at different levels are corrected for distance discrepancies and wherein

transmitters and receivers controlled by their respective microcontrollers situated at the top of the tubes, may move within the tubes and reach any desired depth, in one of the locomotion means comprising moving along rails affixed to the internal walls of the tubes and, transported within capsules to any desired depth by a winch, wherein,

said microcontrollers may change the positions in space of the transmitters and receivers within capsules, so that their optimal direction of transmission and receipt may be changed to optimize transmitters and receivers at other depth levels at other tubes to intercommunicate.

3. - A Method and System for mapping the soil as in claim 2, wherein,

the soil'"'"'s permittivity along parallel straight-lines across the depth of a vertical plane under the soil, is relatively uniform, and wherein,

the existence of an underground passageway across a vertical plane under the soil, may be ascertained, by inserting two tubes into the ground, where each tube has both a transmitter and a receiver, at the two sides of said vertical plane, wherein,

the transmitter and receiver in each tube may exchange positions within their respective tubes so that the direction of the radiation is inversed and wherein,

said transmitters and receivers face each other so that the transmission radiation is maximized and approximately equalized in both directions and wherein,

the frequency of the radiation in the 10-100 MHz band where the attenuation in the soil is given approximately by δ

=2/σ

(∈

/μ

)^1/2 where δ

is the distance where the attenuation is (1/e), is selected by the optimal wavelength that maximizes interaction with the target object, and wherein,

a Straight-Line attenuation map of all levels of said vertical plane is built using a transmitter in one tube and a receiver at the same level in the second tube and vice versa exchanging the roles of the transmitter and the receiver and wherein,

the straight-line attenuation at a given depth level is the average of the attenuation measured from both sides and wherein,

the average level of an air cavity is the level whose attenuation is the highest and the attenuation both at levels below and at higher levels, are the same or lesser than the attenuation at the level of the highest attenuation in-between the two tubes, in both directions and wherein,

the lateral position of the air cavity between the two tubes is found by measuring the attenuation between the level of the air cavity at one tube and the respective levels above in the second tube, and vice versa after exchanging the direction of the radiation, the attenuation between the level of the air cavity in the second tube and the respective levels above the level of the air cavity in the first tube and wherein,

the lateral position of the air cavity along the Straight-Line between the tubes is a non-linear function of the attenuation along the straight-lines between the air cavity level transmitter in one tube and the receiver at the level above it in the second tube, and wherein,

said lateral position of the air cavity along the Straight-Line between the tubes may be determined by taking the average level of attenuation as a proportion of the increased attenuation from the highest attenuation level in one tube to one or more levels higher at the opposite tube, when measured in the two opposite directions.

4. - A Method and System for mapping the soil as in claim 2, wherein,

couples of transmitters and receivers are installed back-to-back in a tube, all along the tube, at intervals equal in length to a part of the height of the searched tunnel, wherein

said receivers and transmitters are positioned in 3D so as to face specific transmitters and receivers at the same depth, in a specific neighboring tubes and wherein,

said transmitters or receivers are oriented within their specific tubes so that their horizontal polarizations are in a plane perpendicular to the direction of the tube and wherein,

said transmitters and receivers get their power through a cable that runs all along the length of the tube and may be switched on and off separately, and wherein,

said transmitters and receivers receive their operational instructions from a microcontroller located at the top of the tube, by cable or wireless communications.

5. - A Method and system for mapping the soil using electromagnetic transmitters and receivers inserted within boreholes as in claim 2 wherein,

the soil is not uniform to such a degree, that there are many substantial attenuation discontinuities across parallel Straight-Lines along the depth of the tubes, in which case a full tomography reconstruction of the plane is preferable, in order to delineate the shape of the various layers of the soil with large permittivity discontinuities, and air cavities if any, and wherein,

the radiation transmission between every single transmitter (n_i) along tube (i) and all (n_j) receivers at (n_j) consecutive levels at the opposite tube (j), are measured in both directions, resulting in 2(n_i,j)² Straight-Lines, crossing (n_i,j)² pixels of an area between the tubes, where n_i and n_j are the antennae coordinates along tubes (i) and (j) and d(n_i,j) is the distance between consecutive transmitters as well as the distance between consecutive receivers and wherein,

the distance D between the tubes is smaller than approximately 70% of the maximal distance of transmission (SLD) and wherein,

at high conductivity and in a non-magnetic soil, the velocity in any pixel v_p=(∈

_p)^1/2 and the time to traverse any pixel in any direction may be expressed in terms of the permittivity, as the measurements of the Straight-Line-Distance and time to traverse said distance are known, and wherein,

all Straight-Line measurements are recalibrated for change of directional sensitivity of antennae and wherein,

the permittivity of any ill defined pixel, due to the lack of sufficient number of independent equations related to said pixel, may be defined by assuming that the permittivity of this pixel to be the weighted average of the permittivity of all the surrounding pixels and wherein,

the permittivity map of a D(n_i,n_j)² region within the plane determined by the 2 tubes may be determined by solving the (n_i,j)² independent equations using algebraic reconstruction tomography algorithms with the [(n_i,j)²(∈

_r)] unknowns by finding the inverse of the matrix of the weight coefficients by iterative methods.

6. - A method and system for mapping the soil using electromagnetic transmitters and receivers inserted within boreholes as in claim 2, wherein,

in order to ensure that there are a sufficient number of independent equations relating all (n²) pixels between the two tubes, a transverse tube housing (n) transmitters and (n) receivers is placed on the soil surface, along a line connecting the tops of the 2 tubes inserted in the soil that define the plane whose tomography is to be mapped and wherein, said transverse tube carries an inflatable bottom bag that may be filled with the specific soil over which it operates wherein,

said inflatable bottom bag is inflated in order to establish good contact with the surface over which it stays, in order to impede reflections from the air between the soil surface and its transmitters or receivers, and wherein

all Straight-Line measurements are recalibrated for change of directional sensitivity of antennae and wherein,

said transmitters and receivers exchange radiation with the (n) antennae along each of the the tubes, from (n) positions on the ground between the 2 tubes and wherein,

the (n_i,j)² pixel array between the tubes, is traversed by 2n² additional Straight-Lines that augment the number of independent equations to 3n², thus satisfying the number of independent equations needed, for mapping the (n)×

(n) region between the tubes using an algebraic reconstruction tomography algorithm.

7. - A method and system for mapping the soil using electromagnetic transmitters and receivers inserted within boreholes as in claim 5, wherein,

the mapping of the plane between 2 tubes is performed in successive steps by mapping overlapping square (n_ij²) regions, starting with a first region bordering with the soil as in claim 6 wherein,

the permittivity of any ill defined pixel in a region bordering with a previously mapped region is copied from said previously mapped region that is well defined.

8. - A method and system for mapping the soil using electromagnetic transmitters and receivers inserted within tubes as in claim 2, and mobile transmit/receive electromagnetic antennae on wheels that move on the ground, thereinafter referred to as “

mobile scanners”

, and wherein,

said transmit/receive antennae may be directed in the directions of respective antennae located within tubes, and wherein,

said mobile scanners carry inflatable bottom bags that may be filled with the specific soil over which the specific mobile scanner operates and inflating it before it transmits or receives radiation in the direction of the antennae in one of the tubes, so that any reflection from the soil surface is minimized and wherein,

the exact positions of said mobile transmit/receive antennae are determined by various sensors, including high resolution GPS receivers and wherein,

said mobile scanners transmit and receive radiation from each of the (n) antennae along each of the tubes, from (k,l) positions on the ground between the tubes and wherein,

the volumetric voxel array between the tubes, is traversed by (m) additional Straight-Lines that augment the number of independent equations needed to solve the equations, specifically in the region close to the soil surface and wherein,

all Straight-Line measurements are recalibrated for change of directional sensitivity of the antennae and wherein,

the total number of equations formed by 2 tubes and the mobile scanner scanning the line between the 2 tubes at (n) number of steps, is 3n², for an area of n² pixels, and wherein,

the total number of equations formed by 3 vertical tubes and a mobile scanner covering the triangular area of (n²/2) between the 3 tubes, for a volume of n³/2 voxels, is 1.8 n³, and wherein,

the total number of equations formed by 4 tubes and the mobile scanner covering the area of n² pixels between the 4 tubes of volume of n³ voxels, is 4.06n³, and wherein,

the combination of underground structures defined by 2, 3, and 4 tubes and a mobile scanner enable to form a number of independent equation larger than the minimal number of equations needed to determine the values of the voxels within the region between the tubes and the mobile scanner for mapping said regions using an algebraic reconstruction tomography algorithm.

9. - A method and system for mapping the soil as in claim 8, for mapping the soil layers close to the surface, one layer after the other, using at least 2 mobile scanners wherein, a decision may be made whether the mapped area is suitable for inserting a long tube containing antennae along its length wherein,

said mobile scanners, located at a mutually short distance, transmit in unison short electromagnetic pulses into the soil, in directions that overlap at an approximate depth roughly determined by the time-window of the back-scattered radiation detected by the receivers of said mobile scanners in unison, and wherein,

changing the directions of the radiation transmitted in unison by both mobile scanners, the time-window for detecting the back-scattered radiation, and appropriately increasing the intensity of the radiation in order to compensate for the increased distance of the following layer, and wherein,

repeating said process above, enables to measure the density of consecutive layers where said tube is to be inserted until such depth that the soil around the tube may be mapped using the antennae within the tube and one mobile scanner.

10. - A method and system for mapping the soil using electromagnetic transmitters and receivers as in claim 8 wherein,

said transmit/receive antennae are located within one tube whose length is 70% of the maximal SLD hereinafter denoted as (L) and wherein,

said electromagnetic antennae may be directed in the directions of respective antennae located within one or more mobile transmit/receive antennae on wheels, that move on the ground, and wherein,

all Straight-Line measurements between the antennae in the tube and the mobile antennae are recalibrated for change in the directional sensitivity of said antennae and wherein,

the volume of the soil cone around the tube that can be imaged is [(π

L²)L/3] and wherein,

the surface of the base of the cone being (π

L²) and the height of the cone having L levels of transmitter/receivers along the depth of the tube, [(π

L²)L] straight-line equations may be generated, 3 times the number of the needed equations to solve the values of the [(π

L²)L/3] voxels around the tube, consequently enabling to find the values of the (π

L³/3) voxels around the tube using an algebraic reconstruction tomography algorithm.

11. - A method and system for discovering underground passageways in a relatively uniform soil, as in claim 3, wherein,

tubes where the transmitters and receivers are located, follow a substantially triangular meandering route, with approximately 70% of maximal SLD between the tubes and wherein,

the direction in 3D of an underground passageway that crosses more than one of the inter-tube routes, may be determined by parallel-line scanning the soil between the tubes and wherein,

the 3D direction of passageways may be determined from its 2D cross sections determined from the 2D parallel line maps of the planes between tubes.

12. - A method and system for discovering underground passageways in a non-uniform soil, as in claim 6 wherein,

tubes where the transmitters and receivers are located, follow a substantially triangular, meandering route, with approximately 70% maximal SLD between the tubes and wherein, the full map of the inter-tube planes are reconstructed using an algebraic reconstruction algorithm and wherein,

the direction in 3D of an underground passageway that crosses more than one of the inter-tube planes, may be determined by correlating the 2D regions having a permittivity ∈

_r=1, in the reconstructed inter-tube maps.

13. - A Method and system for mapping the soil as in claim 1 wherein,

the resonant frequency of the electromagnetic antennae that have to equal the resonant frequency of the soil layers that change from one layer to another and from one day to another depending on the climate, may be recalibrated in real-time, and wherein,

said recalibration consists in changing the physical distance between the electrical ground and the back of the radiating surface of the antenna facing the electrical ground, wherein, the back of the radiating surface of the antenna is coated with a high dielectric constant material, and wherein

said physical distance is changed by remotely controlled mechanical means placed between the electrical ground and a back plate, and wherein,

changing the average permittivity of the space between the radiating surface, and the electrical ground, changes the resonant frequency of the antennae and wherein,

equating the resonant frequency of the antennae to that of the soil is achieved successively by measuring the straight line transmission of the radiation while changing the resonant frequency of the of the transmitter and receiver until maximal transmission distance is achieved.

14. - A Method and system for mapping the soil as in claim 2 wherein,

the tubes are made of plastic material that can withstand high temperatures and sections of stainless steel tubing adjoined to sections of the plastic tubing in order to strengthen the entire structure and wherein,

the permittivity of the plastic material of said tube is close to that of the soil adhering to, and wherein,

the tube inserted into a borehole is built modularly from sections that can be inter-connected through flexible joints and enable filling the space between the borehole and each of the tube sections, gradually with material that bridge the difference in permittivity. between said tube and the borehole and wherein,

meander-lined loop antennas built with one of high conductivity materials comprising copper, silver, graphene and stanine derived materials are inscribed onto the plastic surface of the tubes at consecutive levels along its length and wherein,

the power to the loop antennae is supplied by a power supply situated at the top of the tube through a cable affixed to the inner wall of the tube with connections through the wall to specific loop antennae and wherein

said loop antennae connect to their power source through a switch that may be activated by said microcontroller and wherein,

the power of the loop antenna is multiplied manifold by inserting within the loop, adjacent to the internal wall of the tube, an array of soft ferrite rods of low magnetic coercivity that can follow the frequency of the current circulating in the loop, and consequently multiply the radiation intensity many folds, and wherein,

said arrays of ferrite rods may be one of lowered to the desired level inside a loop antenna by a winch controlled by the microcontroller and be affixed to the internal wall of the tube adjacent to the inscribed loop and wherein,

the tubes include electrical conductors traversing its walls at consecutive levels along the loop antennas for the purpose of measuring the conductance (σ

) of the soil between tubes.

15. - A Method and system for mapping the soil as in claim 12 wherein,

the tube has a rectangular cross section, wherein,

the meander looped antenna is wound around a thin rectangular shaped thin core containing an array of ferrite rods with circular holes traversing the lengths of said rods, and wherein,

said ferrite rods are cooled by a heat exchanger that circulates a low temperature evaporation liquid, in a closed loop with a heat sink that liquefies back said liquid, and wherein,

said antenna may be transported to any depth along the rectangular tube by an elevator-like mechanism.

16. - A Method and system for mapping the soil as in claim 12 wherein,

magnetic antennae composed of meander-lined elliptic looped coils of several lateral rounds inscribed on the surface of the tube, and wherein,

the axial direction of said loops is perpendicular to the longitudinal direction of the tube and wherein,

4 loops, each facing the 4 directions at 90°

of the other, are inscribed on the surface of the tube and wherein,

a circular platform supported by a cable unfolded by a motor on top of the tube may reach any level within the tube, wherein said motor is controlled by a microcontroller on the top of said tube and wherein,

said platform carries 4 bundles of soft ferrite rods, each bundle perpendicular to the other and wherein,

said ferrite rods are positioned behind the elliptical meander-lined loops inscribed on the surface of the loop and wherein,

said magnetic loop antenna impervious to changes in permeability and conductivity may be used as short range underground antennae.