Ex Parte MogilatovDownload PDFPatent Trial and Appeal BoardDec 17, 201512577424 (P.T.A.B. Dec. 17, 2015) Copy Citation UNITED STA TES p A TENT AND TRADEMARK OFFICE APPLICATION NO. FILING DATE FIRST NAMED INVENTOR 12/577,424 10/12/2009 Vladimir S. Mogilatov 44639 7590 12/21/2015 CANTOR COLBURN LLP- BAKER HUGHES INCORPORATED 20 Church Street 22nd Floor Hartford, CT 06103 UNITED STATES DEPARTMENT OF COMMERCE United States Patent and Trademark Office Address: COMMISSIONER FOR PATENTS P.O. Box 1450 Alexandria, Virginia 22313-1450 www .uspto.gov ATTORNEY DOCKET NO. CONFIRMATION NO. RES4-43521-US (BAT0093US) 4244 EXAMINER PARK,HYUND ART UNIT PAPER NUMBER 2865 NOTIFICATION DATE DELIVERY MODE 12/21/2015 ELECTRONIC Please find below and/or attached an Office communication concerning this application or proceeding. The time period for reply, if any, is set in the attached communication. Notice of the Office communication was sent electronically on above-indicated "Notification Date" to the following e-mail address( es): usptopatentmail@cantorcolbum.com PTOL-90A (Rev. 04/07) UNITED STATES PATENT AND TRADEMARK OFFICE BEFORE THE PATENT TRIAL AND APPEAL BOARD Ex parte VLADIMIR S. MOGILATOV Appeal2013-010999 Application 12/577 ,424 Technology Center 2800 Before HUNG H. BUI, NABEEL U. KHAN, and AMBER L. HAGY, Administrative Patent Judges. KHAN, Administrative Patent Judge. DECISION ON APPEAL Appellant 1 appeals under 35 U.S.C. § 134(a) from the Examiner's Final Rejection of claims 1--4, 6-9, and 11-19, which constitute all the claims pending in this application. Claim 5 was previously canceled. Claim 10 was conditionally allowed if rewritten in independent form. App. Br. 2. We have jurisdiction under 35 U.S.C. § 6(b). We affirm-in-part. 1 According to Appellant, the real party in interest is Baker Hughes Incorporated. App. Br. 1. Appeal2013-010999 Application 12/577 ,424 THE INVENTION Appellant's invention relates to performing transient electromagnetic sounding in a borehole to determine a property of an earth formation. Spec. i-f 1. The Specification explains that the exploration and production of hydrocarbons requires knowledge of subsurface earth formations that may contain reservoirs of the hydrocarbons. Spec. i-f 2. Transient electromagnetic (TEM) sounding at the surface of the earth has been one way of gathering this knowledge. Spec. i-f 2. According to the Specification, traditional TEM sounding at the earth's surface may not be able to reach reservoirs of hydrocarbon located deep inside the earth, and may not be able to discriminate between different distances into the formation. Spec. i-f 4. Appellant's invention seeks to address these drawbacks by employing techniques designed to measure a property of an earth formation deep inside the earth using TEM that can discriminate between different distances into the earth formation. Spec. i-f 5. These techniques call for emitting an electromagnetic pulse with a certain shape that is optimized to induce current in a zone of investigation and to minimize induced current in other zones. Spec. i-f 20. Independent claim 1 is illustrative and is reproduced below: 1. A method for estimating a property of an earth formation in a zone of investigation, the earth formation comprising the zone of investigation and another zone, the method comprising: applying a compound pulse of electromagnetic energy to the earth formation using a transmitter disposed in a borehole penetrating the earth formation, the compound pulse comprising a shape to induce a predominately greater amount of current in the zone of investigation than in the another zone, wherein the compound pulse comprises a first pulse and a second pulse, the first pulse comprising an amplitude whose 2 Appeal2013-010999 Application 12/577 ,424 absolute value is different from an absolute value of the amplitude of the second pulse and a duration of the first pulse being greater than a duration of the second pulse when a polarity of the first pulse is different from a polarity of the second pulse; receiving a response of electromagnetic energy from the current induced by the compound pulse; and estimating the property from the response of electromagnetic energy. REFERENCES and REJECTIONS 1. Claims 1--4, 6-9, and 12-19 stand rejected under 35 U.S.C. § 103(a) as unpatentable over Payton (US 5,955,884; Sept. 21, 1999) and Rocroi (US 4,417,210; Nov. 22, 1983). 2. Claim 11 stands rejected under 35 U.S.C. § 103(a) as unpatentable over Payton, Rocroi, Ekstrom (US 5,675,147; Oct. 7, 1997), and Tabanou (US 2005/0083061; Apr. 21, 2005). ANALYSIS I. Claim 1 Appellant argues the Examiner errs in finding the combination of Payton and Rocroi teaches or suggests the following limitation of claim 1: the compound pulse comprising a shape to induce a predominantly greater amount of current in the zone of investigation than in the another zone comprises a first pulse and a second pulse, the first pulse comprising an amplitude whose absolute value is different from an absolute value of the amplitude of the second pulse and a duration of the first pulse being greater than a duration of the second pulse when a polarity of the first pulse is different from a polarity of the second pulse. 3 Appeal2013-010999 Application 12/577 ,424 See App. Br. 5. Specifically, Appellant argues: Payton does not discuss and is not directed to focusing the electrical energy to a zone of investigation to "to [sic] induce a predominately greater amount of current in the zone of investigation than in the another zone," as recited by Claim 1. In fact, the transmission is in three orthogonal directions in Payton. App. Br. 6. Regarding Rocroi, Appellant argues that because Rocroi teaches compound pulses that have a linear average of zero, "the compound pulse cannot also have 'a shape to induce a predominantly greater amount of current in the zone of investigation than in the another zone."' App. Br. 8. Appellant reasons that: if the first pulse has a positive polarity, the negative polarity pulse (second pulse) would be required by Rocroi to have a greater amplitude (in order to provide a linear average of zero). The negative polarity pulse (of greater amplitude) is likely to adversely affect the current induced in the zone of investigation as well as in another zone. And, if the first pulse has a negative polarity, the positive polarity pulse (second pulse) would be required by Claim 1 to have a smaller duration. A negative polarity pulse that precedes the positive polarity pulse would not eliminate the currents induced (by the positive polarity pulse) in the another zone (outside the zone of investigation). Id. Further, in response to the Examiner's findings that Figure 13 of Rocroi teaches a compound pulse as recited in claim 1, Appellant argues the labels "first" and "second" convey an order and that Examiner's assignment of the first and second to the pulses of Figure 13 is not consistent with this order. Reply Br. 2. We are unpersuaded by Appellant's arguments regarding Payton because they are not commensurate with the scope of the claim. The claim 4 Appeal2013-010999 Application 12/577 ,424 does not preclude a transm1ss10n of the compound pulse in three orthogonal directions, so long as the pulse has a shape that induces a predominantly greater amount of current in the zone of investigation. The Examiner finds "Payton specifically teaches applying electromagnetic energy to the formation at selected frequencies and waveforms that will maximize the radial depth of penetration of the magnetic and electric energy into the target formation (Col. 3, lines 40-46)." Ans. 7. The Examiner's findings are supported by evidence and we therefore agree that the pulse taught in Payton induces a "predominantly greater amount of current in the zone of investigation than in the another zone," as recited in claim 1. Likewise, Appellant's arguments regarding Rocroi are also not commensurate with the scope of claim 1. The claim does not preclude a compound pulse where the amplitude of the negative polarity pulse is greater than that of the positive polarity pulse. Similarly, the claim does not preclude a negative polarity pulse from preceding a positive polarity pulse. Appellant's argument that the recitation of "first" and "second" in claim 1 conveys an order is unpersuasive in light of dependent claim 4, which requires the first pulse to be applied before the second pulse. See Liebel- Flarsheim Co. v. Medrad, Inc., 358 F.3d 898, 911 (Fed. Cir. 2004) ("[T]he presence of a dependent claim that adds a particular limitation raises a presumption that the limitation in question is not found in the independent claim.") The Examiner finds, and we agree, Figure 13 of Rocroi teaches a compound pulse that comprises a first pulse (134) and a second pulse (133) where the absolute value of the amplitude of the first pulse is different than that of the second pulse and the duration of the first pulse is greater than that of the second pulse. Ans. 5. 5 Appeal2013-010999 Application 12/577 ,424 Accordingly, we sustain the Examiner's rejection of claim 1. II. Claims 2, 3, 6-9, and 11-19 We also sustain the Examiner's rejection of claims 11, 13, and 14--19 for which Appellant does not present separate arguments for patentability. See App. Br. 9-10. Regarding claims 2--4, 6-9, and 12, although Appellant contends that these claims "recite additional features that are not taught by the combination of Payton and Rocroi," other than for claim 4, Appellant does not present any arguments or reasoning to support such a contention. For this reason, we also sustain the Examiner's rejection of claims 2, 3, 6-9, and 12. See, e.g., In re Geisler, 116 F.3d 1465, 1470 (Fed. Cir. 1997) (attorney arguments or conclusory statements are insufficient to rebut a prima facie case). III. Claim 4 Dependent claim 4 recites "the first pulse is applied before the second pulse and the amplitude of the first pulse is greater than the amplitude of the second pulse." App. Br. 12 (Claims App'x). Appellant argues Rocroi does not teach this limitation "because a compound pulse in which a first pulse is greater in amplitude than the second pulse and has a greater duration (as required by Claim 1, from which Claim 4 depends) could not provide a linear average of zero as required by Rocroi." App. Br. 9. We agree. Figure 13 of Rocroi shows that a pulse with greater duration (134) is applied second in time, not first, and thus does not satisfy the limitations of claim 4. We note that the Examiner acknowledges this deficiency but concludes that "it would have been obvious ... to use the teachings of Rocroi ... and try the compound pulse" as recited in claim 4. 6 Appeal2013-010999 Application 12/577 ,424 The Examiner's conclusion is not supported by the evidence and therefore we do not sustain the rejection of claim 4. IV. Other Issues Although the independent claims are drafted in a variety of forms, including a method, an apparatus, and a computer program, we note that the inventive concept encompassed by the independent claims is directed to the shape of the electromagnetic pulse of energy applied by a transmitter. Such a pulse is per se patent ineligible. In re Nuijten, 500 F.3d at 1351-57. Thus, should there be further prosecution of this application (including any review for allowance), the Examiner may wish to review the claims for compliance under 35 U.S.C. § 101 in light of the Federal Circuit's decision in In re Nuijten, 500 F.3d 1346 (Fed. Cir. 2007). DECISION The Examiner's rejection of claims 1-3, 6-9, and 11-19 is affirmed. The Examiner's rejection of claim 4 is reversed. No time period for taking any subsequent action in connection with this appeal may be extended. See 37 C.F.R. § 1.136(a)(l )(iv). AFFIRMED-IN-PART kme 7 Copy with citationCopy as parenthetical citation