General Electric Co. v. Alexander

277 F. 290, 1921 U.S. Dist. LEXIS 901
CourtDistrict Court, S.D. New York
DecidedOctober 29, 1921
StatusPublished
Cited by14 cases

This text of 277 F. 290 (General Electric Co. v. Alexander) is published on Counsel Stack Legal Research, covering District Court, S.D. New York primary law. Counsel Stack provides free access to over 12 million legal documents including statutes, case law, regulations, and constitutions.

Bluebook
General Electric Co. v. Alexander, 277 F. 290, 1921 U.S. Dist. LEXIS 901 (S.D.N.Y. 1921).

Opinion

MAYER, Circuit Judge.

The patents and the art here considered were fully discussed in previous opinions of the Circuit Court of Appeals and of this court. General Electric Co. v. Laco-Philips, 233 Fed. 96, 147 C. C. A. 166, affirmed 233 Fed. 96, 147 C. C. A. 166. General Flee. Co. v. Nitro-Tungsten Lamp Co. (D. C.) 261 Fed. 606, affirmed (C. C. A.) 266 Fed. 994.

The Just and Hanaman patent is now attacked upon the ground (a) of invalidity and (b) non-infringement. The Langmuir patent is attacked upon the ground of invalidity.

[291]*291The bulk of the record is quite disproportionate to the simplicity of all but one of the questions involved. This extensive record is due in part to the fact that the court felt that the widest opportunity should be given to put forward almost any conceivable fact, experiment, or theory directed against validity or infringement as the case might be, in order that litigation, in any event, as to the validity of these patents should some day come to an end, one way or the other. If, in view of prior litigations, it he ultimately held in this case that the claims of these patents are valid, it is difficult to imagine what new matter can later be brought forth.

This introduction is regarded as desirable because otherwise the reason for the brevity of this opinion on certain points might not be understood. The three questions supra will be discussed in inverse order.

[1] 1. The Langmuir Patent. There is not a shred of merit to the present attack on validity. The previous case was ably tried for the defense by experienced counsel who did not neglect anything of consequence. The British Sinding-Larsen (Thompson) patent, No. 18,968 of 1899, was fully considered in the Nitro-Tungsten record.

Now it is claimed that the American Sinding-Larsen patent, No. 672,019, invalidates the Langmuir patent. The British and American patents are the same, except that the British patent mentions the pressure of four atmospheres, while the American patent does not specify the pressure, though it calls for a pressure above atmospheric.

No Sinding-Larsen lamps have ever been used, not because of the osmium lamp, but because the Sinding-Larsen theory was wholly wrong. As Langmuir testified:

“The point, is that the whole theory of the inventor is a false theory, but the theory shows very distinctly that he had in mind that an external pressure on the material of the filament would improve the life of the filament.
“As a matter of fact, we know to-day, and even Sinding-Larsen could have calculated it in liis time, that the pressure on the material of the filament, instead of on the vapor from the filament, would cause an increased rate of evaporation of the filament, and not a decrease. The whole theory is wrong, thermodynamically wrong. You can calculate through rigorous methods that the effect would be just the opposite of what he expeels. As a matter of fact, the penetration of a gas into the pores of a filament, if the phenomena'are dependent upon the evaporation, could not have any material effect upon the evaporation of the filament.”

Sinding-Larsen himself, in his British patent, No. 19,945 of 1900, realized the futility of his earlier patent.

Further, the material in the Sinding-Larsen lamp was carbon, and carbon will not do in the Langmuir co-ordination. The experiments or demonstrations on this score in court are not guides, because life is a basic factor in tests as to lamp efficiency. The point is, as Langmuir said:

“That producing a lamp * * * and running it for a couple of minutes at a high efficiency has no significance whatever as an indication of what a lamp is capable of doing.”

The Hop felt lamp (patent No. 29,285) consists of a small glass tube bent to the shape of an U, containing a drop of mercury and also [292]*292containing, substantially in its center, a carbon filament, the whole surrounded by an external bulb like that of an ordinary lamp. The presence of the carbon filament is sufficient to exclude this patent from further consideration, and its theory as to the vapor of mercury which surrounds the filament after the drop of mercury evaporates, being raised to an intense white heat, is not Langmuir’s invention.

The same general observations apply to the extract from the Electrotechnische Zéitschrift. In brief, there is nothing of' theoretical or practical value in this Hopfelt patent, and, like other prior art, it was a failure.

Claims 4, 5, 12, and 13 are held valid and infringed. The remaining claims need not he considered.

[2] 2. Infringement of lust and Hanaman Patent. The opinion of this court as to this patent unanimously adopted by the Circuit Court of Appeals indicated that this patent disclosed invention of a high order in an art which performs a great service to mankind.

The construction of claims of such a patent will not turn upon dictionary fine distinctions. The courts must always ascertain what the claims mean in the light- of the state of the art and the accomplishment of the inventor.

Practical experience demonstrated the desirability of counteracting what is known as “offsetting,” infra, and for that purpose one of the means or methods employed is to introduce the rare earth oxide known as “thoria.” It is contended that thoria does not cohere, and that the tungsten is not pure nor homogeneous, and hence that there is not infringement of the claims. These claims are as follows:

“(1) A filament for incandescent lights consisting of tungsten in a coherent metallic state and homogeneous throughout.
“(2) A filament for incandescent lights consisting throughout of substantially pure metallic tungsten of high fusing point and electrically conductive, the light emitting properties of the filament being due «to the coherent, homogeneous metallic nature of the tungsten.
“(3) A ‘filament for electric incandescent lights comprising dense, coherent tungsten metal, having its fusing point approximately 3,200“ C., and capable of incandescent efficiency at the rate of less than one watt per candle power and substantially free from perceptible disintegration at that efficiency.”

When Coolidge’s drawn wire tungsten filament (referred to in the Tungsten Lamp Case) was used, it was found that it differed from the squirted filament (of Just .and Hanaman)” in that, when used on an alternating current circuit, it was sometimes subject to what is known as “offsetting,” and this offsetting has to do only with the life of the filament. As'the drawn filament is operated in a lamp, the fibers of which it is composed tend to reform as crystals. This crystal formation may, on an A. C. circuit, produce crystal boundary planes at right angles to the length of the filament, which are planes of mechanical weakness at the temperature at which the filament runs. On these planes slipping may occur, causing one part of the filament to offset laterally from another part. This effect is disadvantageous, as a part of the filament (especially small vacuum lamp filaments) will grow too hot and burn out at the point affected.

Of several ways of preventing this, one is the introduction of thoria. This thoria is in practice usually introduced by a process de[293]

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Bluebook (online)
277 F. 290, 1921 U.S. Dist. LEXIS 901, Counsel Stack Legal Research, https://law.counselstack.com/opinion/general-electric-co-v-alexander-nysd-1921.