Application of John P. Glass

347 F.2d 604, 52 C.C.P.A. 1651
CourtCourt of Customs and Patent Appeals
DecidedJune 24, 1965
DocketPatent Appeal 7300
StatusPublished

This text of 347 F.2d 604 (Application of John P. Glass) is published on Counsel Stack Legal Research, covering Court of Customs and Patent Appeals primary law. Counsel Stack provides free access to over 12 million legal documents including statutes, case law, regulations, and constitutions.

Bluebook
Application of John P. Glass, 347 F.2d 604, 52 C.C.P.A. 1651 (ccpa 1965).

Opinion

SMITH, Judge.

This appeal calls for review of a decision of the Patent Office Board of Appeals, adhered to on reconsideration, wherein the board sustained certain of the examiner’s rejections of various claims in appellant’s application serial No. 699,563, filed November 29, 1957, for “Laminated Cores.” Two claims were allowed by the examiner, and the board reversed the examiner’s rejection of four more. The claims urged on this appeal, therefore, are 21, 22, 24-26, 28-30, 32-35, 37-43, 46 and 47. The board, in addition to affirming the examiner’s rejection of all these claims as unpatentable over the prior art, itself rejected claims 39, 46 and 47 for failure to comply with 35 U.S.C. § 112. That rejection was made in accordance with Rule 196(b).

The following background is helpful in understanding appellant’s claimed invention : Magnetic materials which are commonly used to form laminated cores in many electromagnetic inductive devices normally have a permeability curve (flux density plotted as a function of magnetizing force) which is not linear. For example, appellant’s specification shows a permeability curve for a ring-shaped lamination of a typical 50/50 alloy of iron and nickel. The curve, rather than approximating a straight line, has two distinct “knees.” In the region of the lower knee (at low values of magnetizing force) the flux density is less than it would be if the curve were a straight line, and in the region of the upper knee (at somewhat higher values of magnetizing force) the flux density is greater than the corresponding straight line value.

In many applications, such as in synchro resolvers and other precision inductive devices, this nonlinearity is undesirable because it introduces harmonics. Appellant’s goal, therefore, is to raise the lower knee and depress the upper knee of the permeability curve, so as to make the curve as linear as possible over the working range of the device. As stated in his specification:

The objects of this invention are accomplished by brinelling selected areas of the laminations which make up the core of the transformer, or the rotor or stator of the synchro. This brinelling is an operation whereby portions of the lamination are dimpled by being subjected to compressive forces which compress a local area in the annealed lamination and cause the metal to flow, and thereby subject the area of the lamination surrounding the compressed or dimpled portion to tension stress. The portion of the lamination which is under the highest tension has the highest permeability at lower magnetizing forces, and the portion of the lamination which is most severely deformed by the compressive force applied to it under the brinelling tools is physically much harder than before and magnetically less permeable in the higher ranges of magnetizing force. By controlling and selecting the relative compressive and tension areas of lamination and the amount of stretching under the brinelling tools, the desired result of making the permeability curve more linear is obtained.

Claim 21 is fairly illustrative of those on appeal and reads as follows:

21. A method of forming an electrical inductive device, comprising brinelling selected areas of an annealed ferromagnetic lamination in order to introduce tension stress into the bulk of the lamination to improve the magnetization curve of said device over its operating range and to suppress third harmonics, and to increase permeability at low values of magnetizing force and decrease it at somewhat higher values of magnetizing force so as to im *606 part to said lamination a permeability curve which is more linear than a similar lamination which has not been so treated, and assembling a plurality of the treated laminations in an inductive device.

Claims 22 and 24 are drawn to a similar method, except that they call for “coining” and simply “stressing,” respectively, in place of brinelling. Claim 32 recites a “process of introducing tension stress into selected areas” of a lamination by brinelling. With minor variations, similar language is used in other claims; thus: “shot blasting” (claim 29), “sandblasting” (claim 30), “coining” (claim 33) and “compressively deforming” (claim 28). Claim 38 is similar to claim 28, except that it begins “A process of treating a ferromagnetic lamination”; in like manner, claim 40 is similar to claim 24. Claim 43 recites “in the method of improving the magnetization curve of a ferromagnetic lamination,” the step of compressing portions of the surface thereof.

Claims 34 and 35 define the invention in a somewhat different way, reciting a “new use” of the processes of brinelling and coining, respectively. Claims 25, 26, 41 and 42 claim an annealed ferromagnetic lamination per se, always with the limitation that the permeability curve be more linear than that of a similar unstressed lamination. Claim 37 recites “An improved electrical inductive device” having such laminations. Finally, claims 39, 46 and 47 recite “A method of improving the magnetization curve of an electrical inductive device,” and include specific limitations as to alloy and values on the magnetization curve.

The references finally relied on by the Patent Office are Garbarino patent No. 2,565,303 issued August 21, 1951, and Neurath patent No. 2,920,296 issued January 5, 1960. The examiner rejected all of the appealed claims as “unpatentable over” either Neurath or Garbarino. The board sustained the rejection of all claims on Garbarino but reversed the rejection based on Neurath as to all claims except 26 and 37. From the tenor of the examiner’s answer and the board’s decisions, it is evident that the rejection was one for obviousness under 35 U.S.C. § 103. We are thus required to determine whether the board was correct in holding that the subject matter defined by the appealed claims would have been obvious, as a whole, to a person having ordinary skill in this art at the time the invention was made (here the filing date).

Garbarino is directed to reducing the noise caused by vibration at butt gaps in laminated magnetic cores. As Garbarino puts it:

An analysis which I have made shows that the magnetic flux crossing from one laminar layer to another to by-pass a butt gap has its greatest density close to the butt gap. In other words, most of the flux in any given laminar layer waits until it reaches the very edge of the butt gap before it crosses in a perpendicular plane to the adjacent laminar layers, and very little of the flux passes over to the adjacent laminar layers before reaching the edge of the butt gap. This flux passage at the edge of the butt gaps causes mechanical forces which can be shown to be proportional to the square of flux density. It is this concentration of flux at the edge of the butt gaps which is an important factor in causing the laminar vibrations which raise the noise level of the magnetic core.

Garbarino’s proposed solution to the noise problem is

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347 F.2d 604, 52 C.C.P.A. 1651, Counsel Stack Legal Research, https://law.counselstack.com/opinion/application-of-john-p-glass-ccpa-1965.