Measurement compensation using multiple electromagnetic transmitters

Patent metadata

Field	Value
Publication number	US-10012753-B2
Application number	US-201414784597-A
Country	US
Kind code	B2
Filing date	Apr 15, 2014
Priority date	Apr 17, 2013
Publication date	Jul 3, 2018
Grant date	Jul 3, 2018

Abstract

Systems, methods, and devices for compensating for environmental conditions on electromagnetic measurements are provided. For example, a downhole logging tool may include a first transmitter coil, a second transmitter coil, and a first receiver coil. The first transmitter coil may provide a first magnetic signal in a wellbore having a conductive casing. The second transmitter coil may provide a second magnetic signal in the wellbore. The first receiver may obtain a first measurement relating to the first magnetic signal and a second measurement relating to the second magnetic signal. The first receiver coil may be near enough to the first transmitter coil and the second transmitter coil to obtain measurements predominantly in the near field eddy current regime. A ratio of the first measurement and the second measurement may cancel environmental dependencies of the first receiver coil.

First claim

What is claimed is:

1. A downhole logging system configured to obtain electromagnetic measurements relating to a Z-property of a conductive casing in a wellbore, the system comprising:
a first transmitter coil configured to provide, at a first time, a first magnetic signal of a first frequency in a wellbore having the conductive casing;
a second transmitter coil configured to provide, at a second time, a second magnetic signal of the first frequency in the wellbore; and
a first receiver coil configured to obtain:
a first measurement, at the first time, of magnetic fields due at least in part to eddy currents flowing on the conductive casing that are caused at least in part by the first magnetic signal; and
a second measurement, at the second time, of magnetic fields due at least in part to eddy currents flowing on the conductive casing that are caused at least in part by the second magnetic signal;

wherein the first receiver coil is near enough to the first transmitter coil and the second transmitter coil to obtain measurements predominantly in the near field eddy current regime,
wherein the first measurement and the second measurement depend at least in part on a temperature of the first receiver coil; and
data processing circuitry configured to determine a value independent of the temperature that relates to a Z-property of the casing in the wellbore based at least in part on the first measurement and the second measurement.

2. The downhole logging system of claim 1 , wherein the first time and the second time are configured to take place sufficiently near to one another such that the first receiver coil is subject to approximately the same environmental conditions at the first time as the second time.

3. The downhole logging system of claim 1 , wherein the first receiver coil is spaced a first distance from the first transmitter coil and a second distance from the second transmitter coil, wherein the second distance is greater than the first distance.

4. The downhole logging system of claim 3 , wherein the first distance is between approximately 0.5-10 inches and the second distance is between approximately 0.5-10 inches.

5. The downhole logging system of claim 1 , wherein the first receiver coil, the first transmitter coil, and the second transmitter coil are disposed generally longitudinally through a downhole logging tool, wherein the first receiver coil is disposed between the first transmitter coil and the second transmitter coil.

6. The downhole logging system of claim 1 , wherein:
the first transmitter coil is configured to provide, at a third time, a third magnetic signal of a second frequency and, at a fourth time, a fourth magnetic signal of a third frequency;
the second transmitter coil is configured to provide, at a fifth time, a fifth magnetic signal of the second frequency and, at a sixth time, a sixth magnetic signal of the third frequency; and
the first receiver is configured to obtain:
a third measurement, at the third time, of magnetic fields due at least in part to eddy currents flowing on the conductive casing that are caused at least in part by the third magnetic signal;
a fourth measurement, at the fourth time, of magnetic fields due at least in part to eddy currents flowing on the conductive casing that are caused at least in part by the fourth magnetic signal;
a fifth measurement, at the fifth time, of magnetic fields due at least in part to eddy currents flowing on the conductive casing that are caused at least in part by the third magnetic signal; and
a sixth measurement, at the sixth time, of magnetic fields due at least in part to eddy currents flowing on the conductive casing caused that are at least in part by the sixth magnetic signal.

7. The downhole logging system of claim 1 , wherein the first frequency is greater than or equal to approximately 100 Hz.

8. The downhole logging system of claim 7 , wherein the first frequency is between approximately 10-10,000 Hz, the second frequency is between approximately 100-50,000 Hz, and the third frequency is between approximately 1-1000 kHz.

9. The downhole logging system of claim 1 , comprising a second receiver coil also configured to obtain measurements at the first and second times of magnetic fields due at least in part to eddy currents flowing on the conductive casing that are caused at least in part by the first magnetic signal or the second magnetic signal.

10. The downhole logging system of claim 1 , wherein the value relating to the Z-property comprises a ratio of the first measurement and the second measurement.

11. The downhole logging system of claim 10 , wherein the data processing circuitry is configured to determine the Z-property of the casing using a lookup table that relates the ratio to the Z-property or a formula that that relates the ratio to the Z-property, or both.

12. The downhole logging system of claim 1 , wherein the first measurement accords with the following relationship:
R T1 ( f )= g ( f ) S T1 ( f ) e iϕ(f) ,

where R T1 (f) represents the first measurement, f represents a frequency of the first signal and the second signal, g(f) represents a temperature-dependent gain response of the first receiver coil, ϕ(f) represents a temperature-dependent phase response of the first receiver coil, and S T1 (f) represents an output of the first receiver coil that is based on a response by the conductive casing to the first signal; and
wherein the second measurement accords with the following relationship:
R T2 ( f )= g ( f ) S T2 ( f ) e iϕ(f) ,

where R T2 (f) represents the second measurement, f represents the frequency of the first signal and the second signal, g(f) represents the temperature-dependent gain response of the first receiver coil, ϕ(f) represents the temperature-dependent phase response of the first receiver coil, and S T2 (f) represents an output of the first receiver coil that is based on a response by the conductive casing to the second signal.

13. The downhole logging system of claim 1 , wherein the first transmitter, second transmitter and first receiver and at least part of the data processing circuitry are disposed within a wireline downhole tool or a logging-while-drilling tool.

14. A method comprising:
moving a downhole tool into a borehole with a conductive casing; wherein the downhole tool comprises:
a first transmitter coil configured to provide, at a first time, a first magnetic signal of a first frequency in a wellbore having the conductive casing;
a second transmitter coil configured to provide, at a second time, a second magnetic signal of the first frequency in the wellbore; and
a first receiver coil configured to obtain:
a first electromagnetic measurement, at the first time, of magnetic fields due at least in part to eddy currents flowing on the conductive casing that are caused at least in part by the first magnetic signal; and
a second electromagnetic measurement, at the second time, of magnetic fields due at least in part to eddy currents flowing on the conductive casing that are caused at least in part by the second magnetic signal;

wherein the first receiver coil is near enough to the first transmitter coil and the second transmitter coil to obtain measurements predominantly in the near field eddy current regime;
obtaining the first electromagnetic measurement;
obtaining the second electromagnetic measurement; and
taking a ratio of the first electromagnetic measurement and the second electromagnetic measurement to reduce or eliminate dependencies of the first and second measurements to at least one environmental condition on the receiver

Assignees

• Schlumberger Technology Corp

Inventors

• Nichols Edward
• Legendre Emmanuel
• Le Calvez Jean-Luc

Classifications

• G01V3/28 Primary

  using induction coils · CPC title

• E21B47/092

  by detecting magnetic anomalies · CPC title

• G01V3/38

  Processing data, e.g. for analysis, for interpretation, for correction · CPC title

• E21B47/00

  Survey of boreholes or wells (monitoring pressure or flow of drilling fluid E21B21/08) · CPC title

• E21B47/0905

  Fixed Constructions · mapped topic