Metamaterial-based electromagnetic field measurement device

US10422913B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-10422913-B2
Application numberUS-201415311345-A
CountryUS
Kind codeB2
Filing dateNov 7, 2014
Priority dateAug 15, 2014
Publication dateSep 24, 2019
Grant dateSep 24, 2019

How to read this patent

A practical reading order for non-experts. Skip the full description unless you need deep technical detail.

  1. Title

    What the patent document calls the invention.

  2. Abstract

    A short plain-language summary of the technical disclosure.

  3. Assignees and inventors

    Who owns or filed the patent and who is credited as inventor.

  4. Key dates

    Filing, priority, publication, and grant dates set the timeline.

  5. First independent claim

    The legal scope of protection — read this for what is actually claimed.

  6. CPC / IPC classifications

    Technology tags used to group this patent with similar filings.

  7. Citations and related patents

    Prior art links and similar publications in this corpus.

Abstract

Official abstract text for this publication.

An electromagnetic field measuring device utilizes metamaterials to manipulate electromagnetic fields. Such a device is useful in a variety of applications including, for example, downhole gradiometric ranging.

First claim

Opening claim text (preview).

What is claimed is: 1. An electromagnetic field measuring device, comprising: a receiver comprising: a first input path through which to receive an electromagnetic field and thereby produce a first signal by the receiver; and a second input path through which to receive an electromagnetic field and thereby produce a second signal by the receiver; and a first electromagnetic field (“EMF”) rotation medium coupled to the second input path of the receiver, the first EMF rotation medium comprising: an input to receive an electromagnetic field having a first spatial angle, the EMF rotation medium being configured to rotate the first spatial angle to a second spatial angle; and an output through which the electromagnetic field having the second spatial angle travels into the second input path of the receiver to thereby produce the second signal. 2. A device as defined in claim 1 , wherein the first EMF rotation medium is comprised of a metamaterial. 3. A device as defined in claim 1 , wherein the receiver is a magnetic dipole. 4. A device as defined in claim 1 , wherein the receiver is an electric dipole. 5. A device as defined in claim 1 , wherein: the EMF rotation medium is configured to rotate the first spatial angle to a second spatial angle that is substantially 180 degrees out of spatial phase with respect to the first spatial angle; and the receiver is configured to superimpose the first and second signals to thereby produce a signal proportional to a gradiometric measurement. 6. A device as defined in claim 1 , further comprising a second EMF rotation medium coupled to the first input path of the receiver, the second EMF rotation medium comprising: an input to receive an electromagnetic field having a first spatial angle, the second EMF rotation medium being configured to rotate the first spatial angle to a second spatial angle; and an output through which the electromagnetic field having the second spatial angle travels into the first input path of the receiver to thereby produce the first signal. 7. A device as defined in claim 6 , wherein the first and second rotation mediums comprise a substantially symmetric construction with respect to a measurement center of the receiver. 8. A device as defined in claim 6 , wherein: the second spatial angle generated by the first EMF rotation medium is a rotation of substantially 90 degrees with respect to the first spatial angle; the second spatial angle generated by the second EMF rotation medium is a rotation of substantially 90 degrees with respect to the first spatial angle, the rotation of the second EMF rotation medium being in an opposite direction with respect to the rotation of the first EMF rotation medium; and the receiver is configured to superimpose the first and second signals to thereby produce a signal proportional to a gradiometric measurement. 9. A device as defined in claim 1 , wherein: the receiver is located in one wellbore; and a source of the electromagnetic signals is located in a second well. 10. A device as defined in claim 9 , further comprising processing circuitry to calculate a distance between the first and second wells using the first and second signals. 11. A device as defined in claim 9 , wherein the receiver forms part of a wireline or drilling assembly. 12. A method for making an electromagnetic field measurement, the method comprising: receiving an electromagnetic field through a first input path of a receiver and producing a first signal in the receiver; receiving an electromagnetic field into a first electromagnetic field (“EMF”) rotation medium coupled to the receiver; using the first EMF rotation medium, rotating a first spatial angle of the electromagnetic field to a second spatial angle; and receiving the electromagnetic field having the second spatial angle into a second input path of the receiver, and thereby producing a second signal in the receiver. 13. A method as defined in claim 12 , further comprising computing a gradiometric measurement using the first and second signals. 14. A method as defined in claim 13 , wherein rotating the first spatial angle of the electromagnetic field to the second spatial angle comprises rotating the first spatial angle substantially 180 degrees. 15. A method as defined in claim 12 , wherein receiving the electromagnetic field through the first input path of the receiver comprises receiving the electromagnetic field directly from an environment adjacent the receiver. 16. A method as defined in claim 12 , wherein receiving the electromagnetic field through the first input path of the receiver comprises: receiving an electromagnetic field into a second EMF rotation medium coupled to the receiver; using the second EMF rotation medium, rotating a first spatial angle of the electromagnetic field to a second spatial angle; and receiving the electromagnetic field having the second spatial angle into the first input path of the receiver, and thereby producing the first signal in the receiver. 17. A method as defined in claim 16 , wherein: using the first EMF rotation medium, rotating the first spatial angle to the second spatial angle comprises rotating the first spatial angle substantially 90 degrees; and using the second EMF rotation medium, rotating the first spatial angle to the second spatial angle comprises rotating the first spatial angle substantially 90 degrees in a direction opposite the rotation applied by the first EMF rotation medium. 18. A method as defined in claim 12 , wherein: a source of the electromagnetic fields is a first wellbore; the receiver is deployed along a second wellbore; and the method further comprises utilizing the first and second signals to determine a distance between the first and second wellbore. 19. A method as defined in claim 12 , further comprising deploying the receiver along a downhole assembly.

Assignees

Inventors

Classifications

  • using electromagnetic energy or detectors therefor · CPC title

  • Measuring direction or magnitude of magnetic fields or magnetic flux (G01R33/20 takes precedence) · CPC title

  • Measuring gradient · CPC title

  • G01V3/26Primary

    operating with magnetic or electric fields produced or modified either by the surrounding earth formation or by the detecting device (with electromagnetic waves G01V3/30) · CPC title

  • Adaptation for subterranean or subaqueous use · CPC title

Patent family

Related publications grouped by family.

External sources

Frequently asked questions

Answers are generated from the same data shown on this page.

What does patent US10422913B2 cover?
An electromagnetic field measuring device utilizes metamaterials to manipulate electromagnetic fields. Such a device is useful in a variety of applications including, for example, downhole gradiometric ranging.
Who is the assignee on this patent?
Halliburton Energy Services Inc
What technology area does this patent fall under?
Primary CPC classification G01V3/26. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Sep 24 2019 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 3 related publications on this page (citations in our corpus or others sharing the same primary CPC).