Alvin M. Marks v. Polaroid Corporation

237 F.2d 428, 111 U.S.P.Q. (BNA) 60, 1956 U.S. App. LEXIS 5360
CourtCourt of Appeals for the First Circuit
DecidedSeptember 26, 1956
Docket5055_1
StatusPublished
Cited by42 cases

This text of 237 F.2d 428 (Alvin M. Marks v. Polaroid Corporation) is published on Counsel Stack Legal Research, covering Court of Appeals for the First Circuit primary law. Counsel Stack provides free access to over 12 million legal documents including statutes, case law, regulations, and constitutions.

Bluebook
Alvin M. Marks v. Polaroid Corporation, 237 F.2d 428, 111 U.S.P.Q. (BNA) 60, 1956 U.S. App. LEXIS 5360 (1st Cir. 1956).

Opinion

WOODBURY, Circuit Judge.

Alvin M. Marks as the owner of two United States patents, Nos. 2,104,949 and 2,199,227, and Depix Corporation as his exclusive licensee, brought suit in the court below against Polaroid Corporation for infringement of several claims of the patents. Polaroid answered and filed a counterclaim charging both plaintiffs with trademark infringement, unfair competition, and infringement of enumerated claims of three United States patents issued to it as the assignee of Edwin H. Land and a reissue patent, which it owned. These patents are No. - 2,237,567, issued April 8, 1941; No. 2,-328,219, issued April 31, 1943; No. 2,-454,515 issued November 23, 1948; and Reissue No. 23,297, issued November 28, 1950. The plaintiffs replied with a prayer for a declaratory judgment of *429 invalidity of all four of the defendant’s patents. 1

The District Court after hearing entered a judgment in accordance with its opinion wherein it dismissed the plaintiff’s complaint for infringement on the ground that the claims sued upon were either invalid or had not been infringed by the defendant. And it also dismissed the defendant’s counterclaim insofar as it charged the plaintiffs with trademark infringement and unfair competition. It held, however, that some of the claims of the three Land patents remaining in issue under Polaroid’s counterclaim were valid and infringed by Depix Corporation, and that Alvin M. Marks was personally liable for that infringement. Wherefore it enjoined both plaintiffs from further acts of infringement and referred the issue of damages to a master. Both Marks and Depix Corporation appealed, but the appeal of the latter was dismissed for want of diligent prosecution leaving Alvin M. Marks the sole appellant. In that role he does not contest the judgment below insofar as it adjudicates the claims of his patents in issue either invalid or not infringed. His position is that the court below erred in holding any of the claims of the Land patents in issue valid and infringed, that the patents themselves are invalid and unenforceable because obtained by fraud on the Patent Office, that they are unenforceable because they have been misused, and that in any event he is not personally liable for any infringement by Depix Corporation.

The Land patents with which we are concerned are in the light polarizer field and they cover both a product and a process. The plaintiff-appellant in his brief says: “The disclosures of all three may be stated very briefly as being simply to make a polarizer from a sheet of plastic by stretching it, holding it stretched until it is set so that it will not contract, and staining it with a dye at some stage of the process.” This general statement can serve only as the barest of introductions. The problem is a complicated one and to understand it and the conflicting arguments of the parties some exposition of the general principles involved must be attempted.

Oversimplification has its dangers, particularly for tyros. But there is no way of escape for us here, so with no little trepidation we embark on the risky venture of stating in a general way our understanding of the phenomena involved.

The appellant says in his brief, and we do not understand the appellee to disagree, that according to present scientific theory, light consists of vibrations in every direction in a plane perpendicular to the direction of travel of a light beam. That is, if a beam of light coming toward an observer be thought of as the hub or axle of a bicycle wheel coming broadside toward the observer, i. e. with the hub pointed directly at the observer so he could see through it, the vibrations would be represented by the spokes of the wheel.

Now when a beam of light strikes a reflector, such as a polished metal surface, the beam bounces off at an angle equal to the angle of its approach. (The angle of incidence equals the angle of reflection.) This is simple reflection. When a beam of light strikes a transparent object at an angle, such as a pane of glass, it meets resistance, is slowed down and thereby deflected, so that as it enters the glass it turns at an angle and as it emerges from the other surface of the glass it again turns at an angle and resumes its original direction. That is to say, the beam takes a zig-zag course through the glass. This is refraction.

Certain transparent crystals have a different effect upon a beam of light. These crystals, like glass, offer resistance *430 to .the beam of light but, unlike glass, because of their molecular composition, the vibrations in one plane, say the plane horizontal to the surface of the earth represented in our simile by the horizontal spokes of the bicycle wheel, meet less resistance than the vibrations in the vertical plane represented by the up-and-down spokes of the bicycle wheel. Thus the vibrations roughly in one plane are slowed down .more than the vibrations roughly in the other, with the result that two-beams of light .emerge from the crystal,. one having vibrations generally in one plane and the other having vibrations generally in the plane at right angles with it. This is double refraction or birefringence.

Polarization is one step beyond bire-’ fringence in that the vibrations in one plane are to a large extent absorbed by the crystal so that only a single beam of light emerges from it and the vibrations in that beam are largely in a single plane. That is to say, a polarizing crystal not only divides an ordinary beam of light, like a • birefringent crystal, into two beams, one having vibrations largely in one plane and the other having vibra-’ tions largely in the plane at right angles to it, but also largely absorbs the vibrations in one plane. Thus, if a perfect polarizer existed it would cut off all light except that vibrating in a single plane, and if two such polarizers were placed in the path of a beam of light with their planes of polarization at right angles to one another, all light passed by the first polarizer would be cut off by the second. and no light at all would pass through the latter. 2

Dichroism is another name for polarization, and the dichroic ratio, or dichroic constant as it is sometimes called, is a measure of the amount of light that gets through a polarizer and therefore a measure of its merit. The higher the dichroic. ratio the better the polarizer.

The phenomenon of. polarization has been known for at least a century and a half. At first only natural polarizers, such as the Nicol prism and tourmaline,, were known, and they were expensive. About one hundred yea'rs ago a British scientist named Herapath had some success in manufacturing synthetic polarizing crystals which came to be known, as herapathites after their discoverer, but they were slow to make, small in size and expensive, and so never attained commercial success.

This was the state of the polarizer art. until the late 1920’s when two precocious young scientists in their teens, the plaintiff Alvin M. Marks, and the defendant’s patentee, Edwin H. Land, almost simultaneously entered the field. The interest, of both young men stemmed from their, interest in television, and each, independently and without knowledge of the other,. started with Herapath and following his teaching attempted to develop synthetic polarizers of large area. Both failed,, and then each struck out on a path of. his own.

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Bluebook (online)
237 F.2d 428, 111 U.S.P.Q. (BNA) 60, 1956 U.S. App. LEXIS 5360, Counsel Stack Legal Research, https://law.counselstack.com/opinion/alvin-m-marks-v-polaroid-corporation-ca1-1956.