Armstrong v. Levy

29 F.2d 953, 58 App. D.C. 293, 1928 U.S. App. LEXIS 2853
CourtCourt of Appeals for the D.C. Circuit
DecidedDecember 3, 1928
DocketNo. 2085
StatusPublished
Cited by4 cases

This text of 29 F.2d 953 (Armstrong v. Levy) is published on Counsel Stack Legal Research, covering Court of Appeals for the D.C. Circuit primary law. Counsel Stack provides free access to over 12 million legal documents including statutes, case law, regulations, and constitutions.

Bluebook
Armstrong v. Levy, 29 F.2d 953, 58 App. D.C. 293, 1928 U.S. App. LEXIS 2853 (D.C. Cir. 1928).

Opinion

ROBB, Associate Justice.

Appeal from a decision of the Patent Office in an interference proceeding in which priority was awarded the senior party.

The 'invention relates to a radio receiver, in which descent from the high or received frequency to the voice or signal frequency is made in two steps instead of one, as in the conventional receiver, and in which amplification is used at the intermediate frequency stage.

Levy filed in France on August 4, 1917. An application was filed here on August 12, 1918, substantially like the French application. Armstrong filed February 8,1919, and a patent was issued to him on June 8, 1920.

If the two applications disclose common subject-matter, the Armstrong patent was inadvertently issued, for under our rulings Levy’s United States application has the “same force and effect as the same application would have if filed in this country on the date” of the French application. See Seror v. Dick, 55 App. D. C. 151, 3 F.(2d) 92; Kling v. Haring, 56 App. D. C. 153, 11 F. (2d) 202; Giesler v. Moulet, 56 App. D. C. 196, 11 F.(2d) 911; Lamb v. Guillemard, 56 App. D. C. 234, 12 F.(2d) 175.

Levy copied the claims of the Armstrong application. Claim 32, here reproduced, is illustrative of the group: “The method of receiving and amplifying high frequency oscillations whereby the incoming energy is utilized to produce oscillations of a different locally predetermined high frequency which are then amplified and the resultant energy utilized to produce oscillations of a second different, locally predetermined, high frequency, which are then amplified, detected and indicated.” The Primary Examiner rejected them on two grounds: The first, and perhaps the main, ground was that the term “high frequency” as used in the claims should,, in the light of the Armstrong disclosure, be restricted to very high frequencies; and the second was that while Levy, in describing the system of his Fig. 7, stated that it could be modified by adding amplifiers at the points [954]*954indicated in dotted lines and also by adding tbe local source of high, frequency indicated by dotted lines at 65, there was lacking any clear statement that both of these modifications were to be used in or applied to the system of Mg. 7 at one and the same time, and that therefore he could not make the claims.

[953]*953

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223 F.2d 926 (Customs and Patent Appeals, 1955)
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Bluebook (online)
29 F.2d 953, 58 App. D.C. 293, 1928 U.S. App. LEXIS 2853, Counsel Stack Legal Research, https://law.counselstack.com/opinion/armstrong-v-levy-cadc-1928.