General Electric Co. v. Corliss

160 F. 672, 87 C.C.A. 560, 1908 U.S. App. LEXIS 4250
CourtCourt of Appeals for the Second Circuit
DecidedMarch 10, 1908
DocketNo. 139
StatusPublished
Cited by1 cases

This text of 160 F. 672 (General Electric Co. v. Corliss) is published on Counsel Stack Legal Research, covering Court of Appeals for the Second Circuit 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. Corliss, 160 F. 672, 87 C.C.A. 560, 1908 U.S. App. LEXIS 4250 (2d Cir. 1908).

Opinion

LACOMBE, Circuit Judge.

The motor of the patent is an induction motor; a quotation from appellee’s brief will sufficiently indicate the characteristics of that type and make the specifications, hereafter to be quoted, more intelligible:

“Induction motors are those in which the coils of the field magnets are traversed by an alternating current brought from the outside source of supply, but the rotating armature has absolutely no connection with any outside source of supply. The currents traversing the closed rings or coils on the armature and producing the armature magnets are induced there by reason of the changing volume and direction of the magnetism produced by the field coils. There are no brushes and commutators such as are used with the direct current motor, and therefore there is at hand no such definite means of causing the armature currents to flow in the direction and at the places and times necessary for producing such magnetism in the armature as will start the motor and cause continuous rotation.”

. As complainant’s expert expresses it:

“The constructor has no way of controlling these currents except through the control of the magnetic field itself, and to determine their position, strength, and time of reversal he can depend only upon the production of a [673]*673correct physical structure. Therefore by his structure he determines his magnetic field, and by bis magnetic field he determines both his arum lure currents and the reaction between these currents and field to produce motion.”

In motors of this type the theory of rotation of the armature is this: On the field there is a succession of magnets and on the armature a like succession of them — each magnet being produced by a flow of current through a coil or ring which surrounds the iron which constitutes such magnet. When the current flows one way the magnet becomes a north pole, when it flows the other way, it becomes a south pole, and, since with an alternating current the direction of the current is constantly and rapidly changing, the polarity of the iron around which it flows (which for convenience we will call the tooth, although the tooth does not necessarily physically project) is changing polarity in like manner. Continuous movement of rotation — we refer again to complainant’s brief — is produced by the arrangement of these two series of magnets. If we have a straight bar magnet pivoted at its middle point so that it may rotate, and if its north pole is brought near the south pole of a magnet, stationary as are the magnets of the field, such north pole will rotate until it comes as near as it can — that is, opposite — the south pole of the stationary magnet, and then it would stop, for it has moved as near to the attracting pole as it can. Each single tooth with its corresponding tooth on the opposite side of the axis of the armature may be considered such a pivoted straight bar magnet. When the north pole of the rotating bar magnet has come opposite the attracting south pole in the field magnet it would stop, as we have seen, but if as it drew near such south pole that pole were moved further along the north pole would pursue it, and rotation be continued. The same effect would be produced by changing in some way the pivoted north pole to a south pole after it had moved to the stationary south pole and providing another stationary north pole at a location a little further along in the arc of rotation, in which case the stationary south pole would repel the new pivoted south pole, and the succeeding stationary north pole would attract the moving south pole; and if this last-mentioned south pole were then again changed to a north pole and another stationary south pole were created a little further along in the arc of rotation, the pivoted north pole would move to it. If this were repeated all around the arc of movement, the rotation would be continuous. Although this theory may be thus simply stated it is apparently no easy matter so to arrange all parts that the changes of polarity are effected at the necessary moment of time and with the moving parts in such relation to the stationary parts that rotation may be continuous.

For simplicity of description we have spoken of the magnets of the armature as teeth of iron surrounded by a conducting coil or ring, but it is understood that each coil or ring itself when current is induced in it acts like a magnet and changes polarity wifli every change of direction of the induced current. In the art of effecting continuous rotation by changing polarity of the magnet through changes of current direction, a difficulty presented itself, and it is to the overcoming of such difficulty that the device of the patent is directed. Whether we speak of teeth or whether we speak of coils it will happen in a device [674]*674where all the poles grouped around the arc of rotation are symmetrical that “dead points” will be developed; momentum might keep the motor going, but they would have a locking or checking action which it is desirable to eliminate. A single tooth when exactly opposite another tooth of like polarity would be repelled, but whether that repulsion would tend to rotate it forward or backward would depend upon what were at the precise moment of time the mutual relations of all other teeth (or groups of teeth) and the field magnets opposite to which they were located. So with the armature coils. One of them having been repelled from one of the field magnets may come into the sphere of influence of the next magnet, which acts in the same way that the first magnet did and tends to repel the coil and to prevent it from moving further. In other words, it is caught between the two magnets and locked in position. It is unnecessary to go at any further length into the details of what takes place, or may take place. It is safe to assume that this opinion will not be read by any one who is not already more familiar with the obscure and invisible movements of electric and magnetic currents than this court is, despite the exhaustive and able briefs and arguments which have been submitted; it is sufficient to indicate that we understand that there is a double locking action to be overcome, and that, in motors of this type it can be overcome only by structural arrangements, not by brushes or commutators. Another excerpt from complainant's brief says:

"If we assume the field magnets are increased in number so that they fill the entire circumference, and if we assume there are mounted on the axis of the armature the same number of armature coils that there are field magnets, it will be seen that in accordance with the locking action which we have described with reference to one armature coil, all of such coils will come into locking position at the same time, each coil standing at a position intermediate between each of the nearest two field magnets.”

It appears that the same effect is produced when each iron tooth of the armature is exactly opposite an iron tooth of the field. If each two of such opposed teeth are of the same polarity all would be repelled, if each were of opposite polarity, all would be attracted at the same time and the tendency would be to lock the machine. It further appears that it makes no difference whether the poles of the field are exactly equal in number to the teeth or coils of the armature; a symmetrical relation may be as readily established when there are two, or three, or more teeth or coils to be positioned relatively to each magnet pole.

Complainant thus summarizes the device of the patent:

“Mr. Eickemeyer, in order to

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Bluebook (online)
160 F. 672, 87 C.C.A. 560, 1908 U.S. App. LEXIS 4250, Counsel Stack Legal Research, https://law.counselstack.com/opinion/general-electric-co-v-corliss-ca2-1908.