Poulsen v. Coe

119 F.2d 188, 73 App. D.C. 324, 48 U.S.P.Q. (BNA) 673, 1941 U.S. App. LEXIS 3668
CourtCourt of Appeals for the D.C. Circuit
DecidedMarch 17, 1941
DocketNo. 7380
StatusPublished
Cited by7 cases

This text of 119 F.2d 188 (Poulsen v. Coe) 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
Poulsen v. Coe, 119 F.2d 188, 73 App. D.C. 324, 48 U.S.P.Q. (BNA) 673, 1941 U.S. App. LEXIS 3668 (D.C. Cir. 1941).

Opinion

STEPHENS, Associate Justice.

This is an appeal from a decree of the District Court of the United States for the District of Columbia dismissing, after a hearing on the' merits, a bill in equity seeking, under Rev.Stat. § 4915, 35 U.S.C.A. § 63, an order authorizing the appellee Commissioner of Patents to issue to the appel[189]*189lants Poulsen and Petersen a patent on their application for letters patent, Serial No. 563,447, filed December 17, 1931, with claims 49, 70, 72, 73, 74, 76, 77, 78 and 79. Claims 72, 73 and 74 are process claims; the others are claims for a machine, informally denominated a system or apparatus. All of the claims relate to the recording of sound on films such as are used in the making of talking motion pictures. All, except claim 70, were rejected by the Commissioner as lacking invention over the prior art; claim 70, as not sufficiently definite to meet the requirements of Rev.Stat. § 4888, 35 U.S.C.A. § 33. The District Court in dismissing the appellants’ bill apparently accepted the views of the Patent Office with respect to each of the claims. The references relied upon in the Patent Office were:

Sacia 1,623,756' April 5, 1927

Hanna 1,888,724 November 22, 1932

Robinson 1,854,159 April 12, 1932

Hewlett 1,853,812 April 12, 1932

Sacia was not urged at the trial below. On this appeal the reliance in the Commissioner’s brief is upon Robinson and Hewlett alone. In this opinion we shall therefore disregard both Sacia and Hanna.

The basic process of sound recording in connection with the production of motion pictures is the transformation of tonal variations produced by a sound source into variations in the magnitude of current in an electric circuit, and then into light variations which are recorded by exposure to them of a moving logitudinal strip of film called a sound track. An understanding of this case requires a brief description of the art as it existed prior to the references relied on in the appeal, and as it existed in view of those references, as well as a description of the appellants’ apparatus and method. Such description can best be made in terms of Illustrations I and II below.1

The art prior to Robinson and Hewlett: As sound to be recorded emanates from its source, it produces pressure vibrations usually spoken of as sound waves which are intercepted by a microphone. This, by means of a diaphragm, converts the mechanical energy of the sound waves into electric energy in the form of an alternating current with vibrational characteristics which are identical with those of the sound waves. The conduits of this alternating current appear in Illustration I at the points marked a a.

Illustration I

d

[190]*190These conduits, passing first through an amplifier, connect the microphone to an oscillograph2 loop b b' to which is attached a mirror c. The oscillation of this mirror, and, in consequence, of a light beam reflected from it in the manner described below, varies in accordance with the changing magnitude of the alternating current vibrations — which itself of course varies in accordance with the variation in amplitude of the sound waves which enter the microphone. The beam of light to be reflected by the mirror upon the moving film is produced by a lamp whose rays pass through a rectangular mask containing a condenser lens which focuses the bundle of rays upon the mirror. When reflected by this mirror toward the film the light bundle thus produced strikes a screen in which there is a horizontal slit, so that there flows on toward the film only that portion of the bundle of light which passes through the slit; and this portion of the bundle is itself, through an objective lens, focused into a fine, transversely disposed line of light which vibrates horizontally upon the sound track, d d', moving downward in a perpendicular plane. In this manner the recording end of the line of light produces upon the film when developed a negative representation of the light vibrations — which themselves correspond exactly to the original vibrations from the sound source.3 The squares e e shown in Illustration I represent sprocket holes by means of which the film is fitted over moving sprockets which carry it downward. The shaded surfaces are those portions of the film upon which the visual images are recorded.4

In the art prior to Hewlett and Robinson, the oscillograph mirror was so adjusted mechanically that when no sound was being produced and therefore no current was passing through the oscillograph loop, the recording end of the line of light was placed exactly in the middle of the sound track. In Figure A of Illustration II there appears graphically the vibration pattern produced by the apparatus thus far described, with the oscillograph mirror set as just stated.

It will be noted that the peaks of the waves described by the recording end of the line of light are symmetrical with respect to a median line or axis a a — sometimes referred to as the “zero line,” which is midway between the sides of the sound track. It is thus shown that under conditions of silence one half the sound track is exposed and the other half unexposed. That is to say, in this stage of the art, when there was no oscillation of the oscillograph mirror, the transversely disposed line of light [191]*191upon the sound track would expose only that portion of the latter designated b b' in Figure A.5

Illustration II

Figure A Normal Sound Track (variable area)

Figure C Sound Track of Robinson & Hewlett

Figure D Sound Track of Petersen & Poulson

But in this stage of the art there was a serious problem. When sound recorded upon a sound track in light variations as above described is to be reproduced for the

benefit of a theatre audience, a fixed light source is sharply focused upon and shines through a positive, produced by printing the developed film record negative, while the former is moved in front of a photoelectric cell.6 The cell thus “sees” the linear variations in light and functions to trans[192]*192mute them into corresponding electric variations which are amplified to a desired degree and are then led into and actuate the diaphragm of the conventional loud speaker. The resultant vibrations in this diaphragm produce pressure vibrations in the air which are accurate counterparts of those which came from the original sound source. Thus listeners hear sound which is a virtual copy of the original. Since the photoelectric cell is actuated by light variations, sound is not reproduced when there is no vibration of the recording line of light upon the sound track and when, therefore, the latter is half exposed and half unexposed, as shown in that portion of Figure A marked b b' and c c.

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Bluebook (online)
119 F.2d 188, 73 App. D.C. 324, 48 U.S.P.Q. (BNA) 673, 1941 U.S. App. LEXIS 3668, Counsel Stack Legal Research, https://law.counselstack.com/opinion/poulsen-v-coe-cadc-1941.