Deep Welding, Inc. v. Sciaky Bros., Inc.

417 F.2d 1227
CourtCourt of Appeals for the Seventh Circuit
DecidedNovember 24, 1969
Docket16707_1
StatusPublished
Cited by50 cases

This text of 417 F.2d 1227 (Deep Welding, Inc. v. Sciaky Bros., Inc.) is published on Counsel Stack Legal Research, covering Court of Appeals for the Seventh Circuit primary law. Counsel Stack provides free access to over 12 million legal documents including statutes, case law, regulations, and constitutions.

Bluebook
Deep Welding, Inc. v. Sciaky Bros., Inc., 417 F.2d 1227 (7th Cir. 1969).

Opinion

KERNER, Circuit Judge.

Plaintiff (Deep Welding) sued defendant (Sciaky) charging infringement of plaintiff’s United States Patent No. 2,-987,610 (Steigerwald) covering a method of welding using a controlled electron beam. Defendant asserted as affirmative defenses the invalidity of the patent, laches, and unclean hands (allegedly resulting from the establishment of a limited monopoly in unpatented electron beam welding machines by a parent corporation of plaintiff through improper use of the patent). The trial court found the patent valid, rejected Sciaky’s other defenses, found some infringement and ordered the case referred to a master for an accounting. Sciaky appealed asserting as error the finding of validity of the patent. On this ground, we reverse.

It is axiomatic that findings in patent cases are like those in any other case in that they are entitled to our respect and should not be set aside unless clearly erroneous under Federal Rule of Civil Procedure 52(a). Armour Research Foundation v. C. K. Williams & Co., Inc., 280 F.2d 499, 503 (7th Cir. 1960), and O’Brien v. O’Brien, 202 F.2d 254, 256 (7th Cir. 1953). See also 41 Mod.Fed. Prac.Dig., Patents key nos. 324(5%) (a)-(c) (1961 and supps.). The major exception to this axiom is in situations where the evidence is documentary or where it involves the actual examination of a product or a device in operation. In such situations, the Court of Appeals has the right to interpret such evidence for itself and is as equally competent as the trial court to do so. See, e. g., Southern States Equipment Corp. v. USCO Power Equipment Corp., 209 F.2d 111, 117-118 (5th Cir. 1953); Plax Corp. v. Elmer E. Mills Corp., 204 F.2d 302, 308 (7th Cir. 1953); Stewart-Warner Corp. v. Lone Star Gas Co., 195 F.2d 645, 647-648 (5th Cir. 1952); Falkenberg v. Golding, 195 F.2d 482, 486 (7th Cir. 1952); and Armour Pharmaceutical Co. v. Richardson-Merrell, Inc., 396 F.2d 70, 72 (3rd Cir. 1968). See generally 15, Mod.Fed.Prac.Dig., Courts key no. 406.3(12) (1960 and supps.). Careful analysis of the evidence below, both documentary and testimonial and by way of exhibits showing welds made by the process in question, convinces us that this *1230 case is determinable upon its documentary evidence. We find ourselves in the same position as did an earlier panel of this Court in Charles Peckat Mfg. Co. v. Jacobs, 178 F.2d 794, at 802 (7th Cir. 1949), cert. denied, 339 U.S. 915, 70 S.Ct. 575, 94 L.Ed. 1340 (1950), which held:

Findings of fact are not to be upset unless they are clearly erroneous; a court of review will not interfere with them, in the absence of a very obvious showing of error. Graver Tank & Mfg. Co., Inc. v. Linde Air Products Co., 336 U.S. 271, 69 S.Ct. 535, [93 L.Ed. 672]. But the ultimate question of patentability is whether the device meets the requirement of the statute. 35 U.S.C.A. § 31. Here we have a finding of fact of anticipation because of existing prior art patents. Each of these documents was before the trial court and is before us. Their interpretation, in view of the statute, is as open to us as to the District Court. True, there was some parol testimony in the court below, but we find that it did not in any way throw light upon the question of anticipation by the prior art. Consequently we feel free to review the evidence bearing upon anticipation by the prior patents.

1. THE PROCESS IN ISSUE

The process here involved is one in which a particle accelerator (electron gun) utilizing electron beam currents ranging from approximately 9 to 250 milliamps supplies accelerating voltages to the electrons of as little as 10 and as high as 30 KeV. 1 The beam thus generated passes through a focusing coil which narrows it at the impingement site on the pieces to be welded so as to put the greatest amount of power into the smallest possible area. The welding process is performed in a vacuum chamber reduced to a pressure on the order of 1 x 1(H mm. Hg so as to minimize contamination and beam interference and scattering. Lastly, the machine is set so that either the gun or the work moves at a speed which insures that a weld will be achieved rather than a hole or a channel. Beam current and focus, accelerating potential, and welding speed are all variable and the correct settings for any given operation will depend on the characteristics of the metals to be joined and the thickness to be penetrated by the beam. The latter depends not only on the thickness of the metal pieces but also upon the type of weld to be made. 2

The process represents a considerable advance over older methods of welding which depended upon heat transfer by conduction. In older welding methods, e. g., metal inert gas welding, in the absence of bevelling, the heat of the torch flame melts a surface portion of the metal creating a molten puddle. Continued application of the flame causes the puddle to propagate itself by continuing to melt solid metal with the heat of the molten metal at the interface of the two. Such welds typically exhibit a hemispherical shape in which the ratio of width to depth is on the order of 2 to 1 though, in some cases, unity may be achieved. Width is measured at the widest part of the weld.

In electron beam welding, two modes are available. In the first, beam strength is low and the weld is caused by the propagation of heat from a molten puddle formed at the point of beam impact. Welds thus achieved are substantially similar to metal inert gas welds.

In the second mode, electron beam welding is performed by the process at issue. The beam is set above a “threshold value” for the pieces to be joined and penetrates deeply into them diffusing its energy throughout the depth of penetra *1231 tion. The penetration of the beam into the material affords the electrons an opportunity to transfer energy and create heat throughout the depth of penetration thus creating a deep narrow molten zone which quickly solidifies. 3 The resultant weld is deep, rather than shallow, narrow, rather than wide, and exhibits typical width to depth ratios from 1 to 3 through 1 to 30 and, in some instances, more. 4 These welds are known as “deep welds.”

The crucial factor involved in the production of deep welds is the threshold value of the material to be welded.

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