Ex Parte Olsson et alDownload PDFPatent Trial and Appeal BoardApr 26, 201712756068 (P.T.A.B. Apr. 26, 2017) Copy Citation United States Patent and Trademark Office 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 APPLICATION NO. FILING DATE FIRST NAMED INVENTOR ATTORNEY DOCKET NO. CONFIRMATION NO. 12/756,068 04/07/2010 Mark S. Olsson SEEK 09-156-201 9872 13235 7590 04/28/2017 Steven P Tietsiwnrth EXAMINER 3527 Talbot St. TAYLOR JR, DUANE N San Diego, CA 92106 ART UNIT PAPER NUMBER 2626 NOTIFICATION DATE DELIVERY MODE 04/28/2017 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): tietsworth@cox.net steven. tietsworth @ seescan.com PTOL-90A (Rev. 04/07) UNITED STATES PATENT AND TRADEMARK OFFICE BEFORE THE PATENT TRIAL AND APPEAL BOARD Ex parte MARK S. OLSSON, RAY MEREWETHER, LONI M. CANEPA, ALEXANDER L. WARREN, AMOS H. JESSUP, MICHAEL J. MARTIN, and GEORGE L. JEMMOTT Appeal 2017-000604 Application 12/756,068 Technology Center 2600 Before JOSEPH L. DIXON, JAMES R. HUGHES, and ERIC S. FRAHM, Administrative Patent Judges. DIXON, Administrative Patent Judge. DECISION ON APPEAL Appeal 2017-000604 Application 12/756,068 STATEMENT OF THE CASE Appellants appeal under 35 U.S.C. § 134(a) from a rejection of claims 1—23. We have jurisdiction under 35 U.S.C. § 6(b). We affirm-in-part. The invention relates to a magnetic manual user interface device, such as a joystick (Spec. 1:12—13). In one embodiment, a ball and socket joystick is comprised of a manual actuator connected to a spherical magnet that is suspended within a cylindrical bore of an annular magnet (Spec. 12:8—17). The spherical magnet and the annular magnet have oppositely oriented north-south magnetic axes, which causes the spherical magnet to return to a vertical position after the actuator is deflected, or to a neutral position within the annular magnet after the actuator is pulled upwards away from the printed circuit board of the joystick (Spec. 13:7—24; Fig. 2B). A sensor below the spherical magnet detects its movement (Spec. 13:1—6). Claims 1 and 10, reproduced below, are illustrative of the claimed subject matter: 1. A manual user interface device, comprising: a manual actuator having an axis; an annular magnet having a central bore; a substantially spherical magnet that can be operatively coupled to the manual actuator, the spherical magnet being positioned in the bore of the annular magnet, the magnetic axes of the magnets being substantially co-axial, and the polarity of the magnets being oppositely oriented such that the interaction of their magnetic fields provides restoring forces that urge the spherical magnet so that its axis is aligned with a neutral axis; and 2 Appeal 2017-000604 Application 12/756,068 a three-axis magnetic sensor positioned to detect changes in a magnetic field due to movement of the spherical magnet and generate signals representative of the direction and amount of movement of the spherical magnet relative to the neutral axis. 10. A manual user interface device, comprising: a manual actuator having an axis; a plurality of magnets arranged in a concentric relationship with at least one of the magnets being operatively coupled to the manual actuator and the polarity of the magnets being oriented such that the interaction of their magnetic fields provides restoring forces that urge the coupled magnet so that its magnetic axis is aligned with a neutral axis; and a three-axis magnetic sensing element for sensing magnetic fields in three-axes at a point in space and positioned to detect changes in a magnetic field due to movement of the operatively coupled magnet and generate signals representative of the movement of the operatively coupled magnet relative to the neutral axis. The prior art relied upon by the Examiner in rejecting the claims on REFERENCES appeal is: Takatsuka Lewis Ameson Phan Le Hoyt Arita Chen US 5,959,863 Sept. 28, 1999 US 6,515,650 Feb. 4,2003 US 7,081,883 July 25, 2006 US 8,054,291 Nov. 8,2011 US 2001/0024192 A1 Sept. 27, 2001 US 2006/0146018 A1 July 6, 2006 US 2008/0184799 A1 Aug. 7, 2008 3 Appeal 2017-000604 Application 12/756,068 REJECTIONS The Examiner made the following rejections: Claims 1, 10—13, 15—18, 21, and 23 stand rejected under 35 U.S.C. § 103(a) as being unpatentable over Phan Le, Takatsuka, and Hoyt. Claims 2, 3, and 19 stand rejected under 35 U.S.C. § 103(a) as being unpatentable over Phan Le, Takatsuka, Hoyt, and Lewis. Claims 4 and 5 stand rejected under 35 U.S.C. § 103(a) as being unpatentable over Phan Le, Takatsuka, Hoyt, and Arita. Claims 6—9 stand rejected under 35 U.S.C. § 103(a) as being unpatentable over Phan Le, Takatsuka, Hoyt, and Ameson. Claim 14 stands rejected under 35 U.S.C. § 103(a) as being unpatentable over Phan Le, Takatsuka, Hoyt, and Chen. Claims 20 and 22 stand rejected under 35 U.S.C. § 103(a) as being unpatentable over Phan Le, Takatsuka, Hoyt, Ameson, and Lewis. ANALYSIS Claims 1—9 and 20—23 Regarding independent claim 1, the Examiner finds the combination of Phan Le, Takatsuka, and Hoyt discloses all the recited limitations, including that Phan Le teaches “a substantially spherical magnet that can be operatively coupled to the manual actuator,” that Takatsuka teaches “an annular magnet having a central bore,” and that Phan Le and Takatsuka collectively teach “the spherical magnet being positioned in the bore of the annular magnet” (Final Act. 5—6). Appellants contend Phan Le does not disclose a spherical magnet, but rather a sphere of magnetic material (see App. Br. 4—7). Appellants also contend Takatsuka teaches the opposite of 4 Appeal 2017-000604 Application 12/756,068 the claimed actuator-coupled magnet located within the bore of an annular magnet, because the magnet attached to an actuator in Takatsuka’s device is located outside of, not within the bore of, another magnet (see App. Br. 9— 10). We are persuaded the Examiner erred. Phan Le discloses an embodiment of a device with a sensor arrangement, shown in Figure 10, that includes a sphere 44 “made of magnetic material” coupled to a joystick 49 where “[i]n the rest position, the joystick stands upright, the magnetic force produced by the permanent magnet [46] is responsible for this” (Phan Le 1 61; Fig. 10). Appellants argue Phan Le’s sphere is not a magnet, but merely magnetic material that is affected by the magnetic field of the permanent magnet located beneath the sphere (see App. Br. 4—7). However, the Examiner responds by asserting the rejection is based on the combination of Phan Le’s Figure 10 and Figure 13 embodiments, where Figure 13 shows a spherical magnet (Ans. 23). Appellants do not contest the Examiner’s combination of Phan Le’s Figure 10 and Figure 13 embodiments to meet the claim 1 limitation of “a substantially spherical magnet that can be operatively coupled to the manual actuator.” Rather, Appellants’ arguments focus solely on Phan Le’s Figure 10 embodiment (see App. Br. 4—7; Reply Br. 1—2). Accordingly, we are not persuaded the Examiner erred in finding Phan Le teaches a spherical magnet coupled to an actuator. We are, however, persuaded the Examiner erred in concluding the combination of Phan Le with Takatsuka discloses the claim 1 limitation “the spherical magnet being positioned in the bore of the annular magnet.” Takatsuka teaches a pointing device that has a ring-like magnet 12 that is moved via a switch cover 15, where the magnet’s movement is detected by magnetic sensors 11 (Takatsuka, col. 5,1. 43—col. 6,1. 4; Fig. 2B). In the 5 Appeal 2017-000604 Application 12/756,068 base embodiment, a silicon resin 13 helps return the magnet 12 to its original position after an external force is removed (Takatsuka, col. 5,1. 64—col. 6,1. 4; Fig. 2B); but in another embodiment, an additional ring-like magnet is positioned inside the movable ring-like magnet to aid in returning the movable ring-like magnet to its original position and reduce wear of the silicon resin (see Takatsuka, col. 7,11. 30-44; Fig. 5). Takatsuka’s Figure 5 shows this other embodiment with the inner ring-like magnet 49 and the outer ring-like magnet 42 being oppositely polarized such that the outer portion of magnet 49 repels the inner portion of magnet 42, thus forcing magnet 42 into a position centered around magnet 49. However, contrary to the claimed invention, in which the spherical magnet coupled to the actuator is located inside the annular magnet that provides restoring forces, Takatsuka’s movable ring-like magnet 42 is located outside the ring-like magnet 49 that provides restoring forces. Accordingly, Takatsuka does not suggest placing Phan Le’s spherical magnet coupled to an actuator inside an annular magnet. Moreover, Takatsuka’s concentric ring-like magnets are each polarized from inside to outside (see Takatsuka, Fig. 5), whereas Phan Le’s spherical magnet is polarized from top to bottom (see Phan Le, Fig. 13). Thus, even if a spherical magnet polarized from top to bottom and coupled to an actuator— as taught by Phan Le (see Phan Le, Figs. 10, 13)—were situated inside one of Takatsuka’s ring-like magnets, the inside to outside polarization of the ring-like magnet would not urge the actuator into a proper vertical position to function as a joystick. Accordingly, we find Phan Le in view of Takatsuka does not disclose “the spherical magnet being positioned in the bore of the annular magnet, the magnetic axes of the magnets being substantially co-axial, and the polarity of the magnets being oppositely 6 Appeal 2017-000604 Application 12/756,068 oriented such that the interaction of their magnetic fields provides restoring forces that urge the spherical magnet so that its axis is aligned with a neutral axis,” as recited in claim 1. We are, therefore, constrained by the record to find the Examiner erred in rejecting independent claim 1, independent claim 20 which recites commensurate limitations, and dependent claims 2—9 and 21—23 for similar reasons. Claims 10—19 Although Appellants argue independent claim 10 based on the same arguments presented for independent claim 1 (see App. Br. 13), we note the claim 1 features discussed above—“a substantially spherical magnet that can be operatively coupled to the manual actuator, the spherical magnet being positioned in the bore of the annular magnet”—are not recited in claim 10. Rather, claim 10 recites the broader limitations “a plurality of magnets arranged in a concentric relationship with at least one of the magnets being operatively coupled to the manual actuator.” Accordingly, Appellants’ arguments discussed above are not persuasive with respect to claim 10, because they are not commensurate in scope with claim 10. Appellants also contend Hoyt fails to teach “a three-axis magnetic sensor” (App. Br. 10-11), which is recited in claim 10, but we are not persuaded by this argument. Specifically, Appellants argue “the purported sensor in Hoyt is ... at most, a grouping of several separate and distinct discrete sensors. . . . Hoyt makes it clear that these are multiple separate sensing devices, not a ‘sensor’ as claimed” (App. Br. 11; see also Reply Br. 3). However, the Specification provides that the sensor may include multiple “magnetic field sensing elements in the form of Hall effect devices 7 Appeal 2017-000604 Application 12/756,068 and circuitry configured to select and/or interpolate between the outputs of the Hall effect devices.” Accordingly, we find the broadest reasonable interpretation of a “magnetic sensor” encompasses several Hall effect elements acting collectively to sense the position of an actuator. Hoyt discloses a “six axis joystick 110” that uses “Hall-effect sensor arrays 170, 172, 174, and 176 that are mounted to a circuit board 178” where “[e]ach Hall-effect sensor array includes individual Hall-effect sensors A, B, and C” (Hoyt, col. 7,11. 53—57 (emphasis omitted)). Appellants have not shown Hoyt’s sensor array fails to teach “a three-axis magnetic sensor” as recited in claim 10 and construed according to the broadest reasonable interpretation in light of the Specification. Additionally, Appellants contend the Examiner’s combination of references is improper (App. Br. 11—13). Specifically, Appellants argue [cjombining Phan Le with Takatsuka makes no sense as Takatsuka describes an inner fixed magnet to purportedly provide restorative force, while Phan Le, as well as the presently claimed invention, rely on the inner magnet to be moveable with an attached actuator. . . . Accordingly, combining them as the Examiner has done merely reflects hindsight bias .... (App. Br. 12). This argument, however, is not persuasive because claim 10 does not specify whether an inner or outer magnet is coupled to the actuator. The Examiner’s reliance on Phan Le for claim 10 is superfluous because the Examiner’s citations to Takatsuka and Hoyt provide a prima facie case of obviousness that addresses all the limitations actually recited in claim 10 (see Final Act. 8—9). Appellants also argue “the Examiner claims that one [sic] it would be obvious to combine the references to ‘provide a less sensitive sensor array compared to inductive sensing’—this assertion by the Examiner has nothing 8 Appeal 2017-000604 Application 12/756,068 to do with Appellant’s invention, and in fact a more sensitive sensor would likely work better” (App. Br. 13). However, “any need or problem known in the field of endeavor at the time of invention and addressed by the [application] can provide a reason for combining the elements in the manner claimed.” KSRInt’l Co. v. Teleflex Inc., 550 U.S. 398, 420 (2007). Further, the Examiner’s combination is bolstered by the Supreme Court’s recognition in KSR that “when a[n] [application] claims a structure already known in the prior art this is altered by the mere substitution of one element for another known in the field, the combination must do more than yield a predictable result.” 550 U.S. at 416. Here, the Examiner has proposed substituting one magnetic field sensor for another magnetic field sensor, i.e., Hoyt’s Hall- effect sensor array (see Final Act. 9). Appellants have not shown this substitution would yield unpredictable results, or would render the combination inoperable. We are, therefore, not persuaded the Examiner erred in rejecting independent claim 10, and claims 11—19 not specifically argued separately. CONCLUSION The Examiner erred in rejecting claims 1—9 and 20—23, but did not err in rejecting claims 10-19 under 35 U.S.C. § 103(a). DECISION For the above reasons, the Examiner’s rejection of claims 1—9 and 20— 23 is reversed, and the Examiner’s rejection of claims 10—19 is affirmed. No time period for taking any subsequent action in connection with this appeal may be extended under 37 C.F.R. § 1.136(a)(l)(iv). AFFIRMED-IN-PART 9 Copy with citationCopy as parenthetical citation