Differential target antenna coupling (“DTAC”) data corrections
View Patent ↗The present invention features a unique system of interdependent methods to greatly improve data acquired via the Differential Target Antenna Coupling (“DTAC”) method, which transmits electromagnetic (“EM”) fields and measures the primary EM field and the secondary EM fields generated in subsurface targets. These new data correction techniques provide improvements, in orders of magnitude, to the measured DTAC response accuracy. This improvement allows for greater depth of investigation, improved target location, and enhanced target characteristics.
1. A method for removing an influence of a primary electromagnetic (“EM”) field from a set of secondary EM field measurements to enhance detection and analysis of a subsurface target by a subsurface imaging and detection system employing differential target antenna coupling (“DTAC”), wherein a secondary EM field is produced as a result of interactions between the primary EM field and a subsurface environment, the method comprising:
(a) selecting a reference frequency ( 200 ) from a plurality of received frequencies, wherein data at the reference frequency comprises a set of residual primary EM field data and a set of secondary EM field data;
(b) measuring a horizontal EM field component ( 201 ) of a secondary magnetic field at the reference frequency and measuring or calculating a vertical EM field component of an in-phase EM field at the reference frequency;
(c) computing an orthogonality correction angle ( 203 ), wherein the subsurface imaging and detection system has a receiver-coil, wherein the orthogonality correction angle is a mathematical difference between a present receiver-coil orientation angle and an orientation of the receiver-coil when the receiver-coil is orthogonal to the in-phase EM field;
(d) measuring a horizontal EM field component of an in-phase magnetic field and measuring or calculating a vertical EM field component of an in-phase magnetic field ( 204 ) at a first data frequency, where the first data frequency is one of the plurality of received frequencies;
(e) calculating a present inclination angle of the receiver-coil relative to the primary field at the first data frequency ( 205 ) using the horizontal EM field component of the in-phase EM field at the first data frequency and the vertical EM field component of the in-phase EM field at the first data frequency;
(f) computing an orthogonality corrected in-phase EM field ( 206 ) for the first data frequency using the orthogonality correction angle and the present inclination angle of the receiver-coil; and
(g) repeating steps (a) through (f) to obtain a corrected in-phase EM field for each of the plurality of received frequencies,
wherein the method is for removing the primary in-phase EM field while maintaining the secondary in-phase EM field as the primary in-phase EM field changes.
2. The method of claim 1 , wherein each corrected in-phase EM field, comprising an in-phase response and a quadrature response, is calibrated by:
(a) adjusting a magnitude, or a real part, of a gain response of a receiver, operatively coupled to the receiver antenna, until an in-phase component of a B x and B y orthogonality corrected field at an original primary EM field value and an in-phase component of the B x and B y orthogonality corrected field at a changed primary EM field value are equal, where the receiver is operatively coupled to the receiver-coil; and
(b) amending a phase, or an imaginary part, of the gain response of the receiver until a quadrature component of the B x and B y field at an original primary field value and a quadrature component of the B x and B y orthogonality corrected field at a changed primary field value are equal.
3. The method of claim 1 further comprising calculating the present inclination angle of the receiver-coil relative to the primary EM field at the reference frequency using the horizontal EM field component of the in-phase EM field at the reference frequency and the vertical EM field component of the primary EM field at the reference frequency.