Determining cement impedance from a formation boundary
US-9606254-B2 · Mar 28, 2017 · US
US10114138B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10114138-B2 |
| Application number | US-201615338865-A |
| Country | US |
| Kind code | B2 |
| Filing date | Oct 31, 2016 |
| Priority date | Dec 15, 2015 |
| Publication date | Oct 30, 2018 |
| Grant date | Oct 30, 2018 |
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A method includes performing pulse echo measurements using a pulse echo tool. The method also includes detecting a casing collar using the pulse echo measurements performed by the pulse echo tool. The method further includes estimating a tool response of the pulse echo tool response at the casing collar using one or more processors based on the pulse echo measurement at the casing collar. The method also includes and removing the pulse echo tool response estimation from at least some of the pulse echo measurements not at the casing collar.
Opening claim text (preview).
What is claimed is: 1. A method, comprising: performing pulse echo measurements using a pulse echo tool, wherein the pulse echo tool comprises a transducer; detecting a casing collar using the pulse echo measurements performed by the pulse echo tool; estimating a tool response of the pulse echo tool response at the casing collar using one or more processors based on the pulse echo measurement at the casing collar; and removing the pulse echo tool response estimation from at least some of the pulse echo measurements not at the casing collar. 2. The method of claim 1 , wherein the pulse echo tool is centered in a wellbore. 3. The method of claim 1 , wherein the pulse echo tool is eccentered in a wellbore. 4. The method of claim 1 , wherein the transducer is configured to emit a sonic pulse. 5. The method of claim 1 , wherein the transducer is configured to emit an ultrasonic pulse. 6. The method of claim 1 , wherein the pulse echo measurement is obtained by the transducer. 7. The method of claim 1 , wherein the transducer comprises a single emitter-receiver that operates at approximately a few hundred kilohertz. 8. The method of claim 1 , wherein the pulse echo tool response at the casing collar substantially comprises only coherent noise. 9. The method of claim 1 , wherein the pulse echo measurement comprises a measurement of an acoustic interaction between an acoustic pulse and a casing comprising a first thickness. 10. The method of claim 9 , wherein the casing collar comprises a second thickness greater than the first thickness. 11. The method of claim 10 , wherein the second thickness results in no or very little amplitude resonance when measured by the pulse echo tool. 12. The method of claim 10 , wherein the second thickness corresponds to an amplitude resonance that is lower than a threshold amplitude resonance. 13. The method of claim 1 , wherein the pulse echo tool response is estimated based on statistical criteria. 14. A tangible, non-transitory, machine-readable-medium, comprising machine readable instructions to: cause a transducer of a pulse echo tool to perform pulse echo measurements; detect a casing collar using the pulse echo measurements performed by the pulse echo tool; estimate a tool response of the pulse echo tool response at the casing collar based on the pulse echo measurement at the casing collar; and remove the pulse echo tool response estimation from at least some of the pulse echo measurements not at the casing collar. 15. The tangible, non-transitory, machine-readable-medium from claim 14 , wherein the pulse echo measurement comprises a measurement of an acoustic interaction between an acoustic pulse and a casing comprising a first thickness. 16. The machine-readable-medium of claim 15 , wherein the casing collar comprises a second thickness greater than the first thickness, wherein the second thickness corresponds to no or very little amplitude resonance when measured by the pulse echo tool. 17. The machine-readable-medium of claim 15 , wherein the casing collar comprises a second thickness greater than the first thickness, wherein the second thickness corresponds to an amplitude resonance that is lower than a threshold amplitude resonance.
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