France Mfg. Co. v. Jefferson Electric Co.

106 F.2d 605, 43 U.S.P.Q. (BNA) 53, 1939 U.S. App. LEXIS 3046
CourtCourt of Appeals for the Sixth Circuit
DecidedSeptember 18, 1939
Docket8121
StatusPublished
Cited by56 cases

This text of 106 F.2d 605 (France Mfg. Co. v. Jefferson Electric Co.) is published on Counsel Stack Legal Research, covering Court of Appeals for the Sixth Circuit primary law. Counsel Stack provides free access to over 12 million legal documents including statutes, case law, regulations, and constitutions.

Bluebook
France Mfg. Co. v. Jefferson Electric Co., 106 F.2d 605, 43 U.S.P.Q. (BNA) 53, 1939 U.S. App. LEXIS 3046 (6th Cir. 1939).

Opinion

HAMILTON, Circuit Judge.

Appellee, Jefferson Electric Company, instituted this action against appellant, France Manufacturing Company, to restrain alleged infringement of mechanical patent No. 1,777,256, applied for July 16, 1928, and issued September 30, 1930, to appellee, assignee of James C. Daley, Edwin G. Goddard and Joseph J. Sola, patentees.

The patent relates to an electric transformer of balanced design and is an improvement on the earlier patent of Daley, et al., No. 1,786,422, of unbalanced design- and for which application was filed November 11, 1927, and issued December 30, 1930. Appellee relies on claims 8, 14 and 19 1 of the patent which the lower court held valid and infringed.

Farraday was the originator of the transformer. He discovered that if two coils of' wire were wound on the same iron or soft steel, magnetic circuit, one primary and the other secondary, and an alternating current 'passed through the primary, it would induce a like current in the secondary. Disregarding the small loss of energy due to eddy currents and other causes, the voltages of the secondary and primary current may be regarded as in the same ratio as the number of turns of wire on the two coils and the current strength in 1 the two coils as in this same ratio inverted. Hence, if desired to raise the voltage and diminish the current from an alternating current dynamo by 100-fold to save the heat loss in long distance transmission, it is necessary only to introduce a step-up transformer, the secondary of which has about one hundred times as many turns of wire as the primary. At the place where it is to be used the high voltage may be reduced again to any desired extent by employing a device that is the reverse of the step-up transformer. Many inventors have turned their genius to the improvement of the details of Farraday’s fundamentally simple device and have developed a transformer with a magnetic core circuit, laminated to reduce eddy currents and with high insulation of the secondary coils from each other and from the primary coils. The mechanical stress and the heating effects during use require careful attention. Differences of phase relations of alternation of the currents form an important part in the field of transformer theory. Various types of connections have been used to meet different problems.

*607 For neon sign work, a step-up transformer is required. The primary, or low-voltage winding consists of perhaps a hundred turns of moderately heavy wire. The secondary, or high voltage winding consists of many thousand turns of smaller wire. For a 15,000-volt transformer, the secondary would have approximately 140 times as many turns as the primary. In luminous tube work, contrary to ordinary transformers, good regulation is not desirable as it maintains the voltage almost constant regardless of the current being drawn from the secondary, but poor regulation is necessary and a transformer for use in neon signs should be built in such a way that as more current is drawn from the secondary, the secondary voltage goes down. Such a transformer, connected to a gas discharge tube, soon reaches a condition of equilibrium, since if too great a current is drawn, the voltage goes down to near zero, and the increased current can no longer flow. If a luminous tube were connected across a transformer having good regulation, the current would increase and as it increased, the resistance of the gas would decrease and as a result still more current would flow. In a short time, the current would become so excessive that either the transformer would burn out or the tube be destroyed.

Transformers for use in neon signs are usually made of an extra iron path in the core called a magnetic shunt which acts as a safety valve. As the current in the secondary increases more of the magnetic lines of force are by-passed by this extra shunt and as a result less of the lines link the secondary winding. As the current in the secondary increases, the voltage across it decreases, thus obtaining the poor regulation. The secondary of a transformer used with a neon sign can be short circuited without harm.

The patent in suit relates to a transformer with a magnetic core surrounding and inclosing the electrical windings, and is suitable for neon signs. It is of the compact housing shell type. Its core structure is composed of two stacks of E-shaped stampings, with its primary or low tension windings disposed about the middle of the central leg of the core. Its secondary or high tension windings are of two separately formed coils disposed at the end of the central leg of the core with one on each side of the low tension or primary winding. The outer ends of these coils are the connecting high tension leads to the neon tubing and the inner ends of the coils are connected electrically and also arranged to ground which creates a midpoint ground for the high tension winding.

Magnetic shunts composed of small stacks of laminations placed transversely of the main central and two outer legs of the core structure are located on each side of the primary coil. Small gaps are left at the ends of the shunts tightly filled with non-magnetic material. The arrangement of the transformer is referred to in the art as balanced, which means dividing the secondary windings with the primary between and with two magnetic shunt paths on opposite sides of the primary so as to come between it and each of the secondary coils.

In the prior art, Elihu Thompson was known as the “father” of electric safety grounding because he introduced the grounded secondary in the transformer as a means of saving life. In his patent No. 400,515, issued April 2, 1899, he stated the object of his 1 invention was to construct a device of a self-regulating character resulting in an automatic adjustment or regulation of the current or potential in the coil forming the secondary when the resistance or current in the same varies. He proposed to do this by a combination with one or the other or both currents of the induction coil of an iron core included in the alternating or varying current circuits with parts brought into definite proximity to form a partial magnetic closure of the magnetic circuit of the core of a definite set value, according to the nature of the regulation of current or the potential desired in the induced circuit, such magnetic circuit being formed independently of the magnetic current which threads both coils of the converter. He used magnetic shunts.

It was also known to the art that a ground connection at the midpoint of the secondary was a useful protective measure where the secondary produced high voltage, but this device, when used in an unbalanced transformer, created the hazard of double current when a short circuit occurred and burned out the transformer without injuring the tubes, electrodes or wiring.

In Fessenden’s induction coil, patent No. 64,390, issued July 24, 1900, he stated in order to prevent arcing between the primary and secondary coils, each should be grounded on the core. In the General Electric Review, Vol. 20, Issue No. 12, December, 1917, E. D. Treanor of the Transformer Engineering Department of the General *608

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106 F.2d 605, 43 U.S.P.Q. (BNA) 53, 1939 U.S. App. LEXIS 3046, Counsel Stack Legal Research, https://law.counselstack.com/opinion/france-mfg-co-v-jefferson-electric-co-ca6-1939.