Magnetic Ranging While Rotating
US-2015378043-A1 · Dec 31, 2015 · US
US2016209540A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2016209540-A1 |
| Application number | US-201414912901-A |
| Country | US |
| Kind code | A1 |
| Filing date | Aug 21, 2014 |
| Priority date | Aug 21, 2013 |
| Publication date | Jul 21, 2016 |
| Grant date | — |
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A method for obtaining full tensor gain compensated propagation measurements includes processing a full tensor voltage measurement to obtain a fully gain compensated tensor quantity. An electromagnetic logging tool including at least first and second axially spaced transmitters and at least first and second axially spaced receivers is rotated in a subterranean borehole. A plurality of voltage measurements are acquired while rotating to obtain a full tensor voltage measurement which is in turn processed to obtain the fully gain compensated tensor quantity.
Opening claim text (preview).
What is claimed is: 1 . A method for obtaining full tensor gain compensated propagation measurements, the method comprising: (a) rotating an electromagnetic logging tool in a subterranean borehole, the logging tool including at least first and second axially spaced transmitters and at least first and second axially spaced receivers, each of the receivers including a set of collocated linearly independent antennas, each of the transmitters including first and second collocated antennas, at least the first transmitter antenna having a tilted moment with respect to a longitudinal axis of the tool; (b) acquiring a plurality of voltage measurements while rotating the tool in (a), the plurality of voltage measurements obtained using a corresponding plurality of pairs of the transmitters and receivers; (c) fitting the voltage measurements to a harmonic expression to obtain harmonic coefficients; (d) causing a processor to process the harmonic coefficients to construct a full tensor voltage measurement; and (e) causing the processor to process the full tensor voltage measurement to obtain a fully gain compensated tensor quantity. 2 . The method of claim 1 , wherein the processor is a downhole processor. 3 . The method of claim 2 , further comprising: (f) transmitting the fully gain compensated tensor quantity to the surface; and (g) causing a surface computer to invert the fully gain compensated tensor quantity to obtain one or more properties of a subterranean formation. 4 . The method of claim 2 , further comprising: (f) causing the downhole processor to process the fully gain compensated tensor quantity to obtain a fully gain compensated tensor attenuation and a fully gain compensated tensor phase shift. 5 . The method of claim 1 , wherein the second transmitter antenna in each of the first and second transmitters has a transverse moment with respect to the longitudinal axis of the tool. 6 . The method of claim 1 , wherein: (d) further comprises causing the processor to process the harmonic coefficients to obtain first and second sets of full tensor voltage measurements; and (e) further comprises (i) causing the processor to process the first set of full tensor voltage measurements to obtain a first full tensor quantity, (ii) causing the processor to process the second set of full tensor voltage measurements to obtain a second full tensor quantity, and (iii) causing the processor to process the first and second full tensor quantities to obtain the fully gain compensated tensor quantity. 7 . The method of claim 6 , wherein the first set of full tensor voltage measurements are obtained at a toolface angle of zero degrees and the second set of full tensor voltage measurements are obtained at a toolface angle of ninety degrees. 8 . The method of claim 7 , wherein the fully gain compensated tensor quantity 12C is computed in (e) as follows: 12 C = [ 12 ( 0 ) xx 12 ( π 2 ) xx 12 ( 0 ) xy 12 ( π 2 ) xy cot ( β T 1 ) 12 ( 0 ) xz 12 ( 0 ) yx 12 ( π 2 ) yx 12 ( 0 ) yy
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