Carl Schenck, A.G. v. Nortron Corp.

570 F. Supp. 810, 1982 U.S. Dist. LEXIS 10213
CourtDistrict Court, M.D. Tennessee
DecidedDecember 21, 1982
DocketCiv. A. 80-3278
StatusPublished

This text of 570 F. Supp. 810 (Carl Schenck, A.G. v. Nortron Corp.) is published on Counsel Stack Legal Research, covering District Court, M.D. Tennessee primary law. Counsel Stack provides free access to over 12 million legal documents including statutes, case law, regulations, and constitutions.

Bluebook
Carl Schenck, A.G. v. Nortron Corp., 570 F. Supp. 810, 1982 U.S. Dist. LEXIS 10213 (M.D. Tenn. 1982).

Opinion

MEMORANDUM

JOHN T. NIXON, District Judge.

The plaintiff Carl Schenck A.G. brings this action to recover damages for an alleged infringement of U.S. Patent No. 3,182,511 (the “511” patent or “Federn” patent). For the reasons stated, this Court concludes that the plaintiff should prevail on its claim of patent infringement. Pursuant to Fed.R.Civ.P. 52, the following will constitute the Court’s findings of fact and conclusions of law.

The plaintiff alleges that the defendant Nortron Corporation’s Model 7402 wheel balancing machine incorporates the invention described in claims 1, 2 and 5 of the 511 patent. The invention disclosed in the patent was discovered in the early 1960’s by Schenck employees Klaus Federn, Heinrick Geiss and Alfred Seibert. The defendant challenges the validity of the patent on several independent grounds and disputes plaintiff’s allegation of infringement.

I.

The issues presented necessitate a brief discussion of some of the principles of wheel balancing drawn primarily from the testimony of the plaintiff’s expert witness Dr. Douglas Muster, of the University of Houston. The following constitutes factual findings by the Court presented as background for the Court’s analysis in Part III of this Memorandum.

Imbalance in automobile tires and in rotors in general is a result of an unequal distribution of mass with respect to a desired axis of rotation. When an imbalanced rotor is set in motion, the mass imbalance generates a force. This force, if viewed in a reference frame that rotates with the rotor, is called the centrifugal force and its magnitude depends upon the mass imbalance and on the square of the frequency of rotation. Rotation of an imbalanced rotor also generates a twisting force in situations when the center of gravity of the rotor is on the axis of rotation but the opposite ends of the rotors are equally out of balance. The twisting force is only present while the rotor is in motion and its magnitude depends upon the frequency of rotation.

The plaintiff, the defendant and the industry have adopted the following technique to measure the centrifugal and twisting forces generated by rotors in motion. The technique requires mounting the rotor on at least two bearings atop carefully designed pedestals. The motion of the axis of rotation at each pedestal then may be observed and measured.

Prior to 1960, the soft-bearing method, which is extremely sensitive and accurate, was used to balance rotors. This method allowed the axis of rotation to move with relative freedom in the measuring direction and inhibited motion in other directions. Using this method, a rotor if mounted on two pedestals and set in motion vibrates with an amplitude (dimension of displacement) of vibration indicative of the force of imbalance; so long as the frequency of rotation and the fundamental frequency of the vibratory mass are properly chosen. These frequencies must be chosen such that the frequency of rotation exceeds twice the fundamental or natural frequency (critical speed) of the system composed of the pedestal and the mass it supports. The soft-bearing method, however, has numerous disadvantages. Because the axis of rotation is not fixed, the motion of an unbalanced rotor is not a simple rotation. As a result, the balancing of a single rotor requires calibration runs and numerous measurements until the proper correction weight is in place. In addition, the speed at which the rotor rotates must exceed the critical speed when resonance may cause so large an amplitude of vibration as to damage the *812 measuring system or make the measurement dangerous.

Neither the plaintiff’s patent nor the defendant’s wheel balancing machine uses a soft-bearing method to solve the problem of measuring imbalance in rotors. Instead, the parties rely on what has been termed a hard-bearing method. This method has been available since at least the early 1920’s when it was described in U.S. Patent 1,599,922. But only since 1960 has the hard-bearing method grown from infrequent use to become the dominant method for the balancing of rotors. A pedestal for a hard-bearing balancer, as the name implies, is significantly stiffer or more resistant to the motion in the measuring direction than its soft-bearing counterpart for balancing a given rotor. A pedestal to be used in a hard-bearing machine also has some form of transducer, which gives a direct reading of the force of imbalance, rather than measuring the amplitude of displacement caused by the imbalance as in a soft-bearing machine. Otherwise, the apparatus used in a hard-bearing balancer is quite similar to that used in a soft-bearing machine.

Professor Muster’s testimony, which the Court finds credible established that a given pedestal could be used in either a hard or soft-bearing machine. The critical factor in determining whether a pedestal is suitable for hard or soft balancing is the relationship between the intended frequency of rotation and the fundamental frequency (critical speed) of the pedestal/support system. In a hard-bearing machine, the frequency of rotation must be less than % the fundamental frequency of the pedestal/support system, rather than twice the fundamental frequency as in a soft-bearing machine.

The plaintiff contends and this Court agrees that until 1960 few found the hard-bearing method commercially useful. Practitioners before 1960 thought it desirable to increase rotational speeds in order to generate larger more precisely measurable forces but wanted to avoid rotational frequencies of sufficient magnitude that distortions due to resonance occurred. Many practitioners introduced damping into their measuring devices in order to suppress resonance as they reduced the difference between the speed of rotation and the fundamental frequency of the measuring system. Mr. Federa, in his work which led to the 511 patent, determined that damping which was intended to eliminate errors due to resonance actually introduced other errors in measurement, especially in locating the radial position where a counterweight should be placed.

II.

There is no dispute in this case concerning the basic principles of patent law. In an infringement suit, the plaintiff must prove that it is the owner of a valid patent and that the defendant’s device is included within the claims of the patent. The validity of a patent is determined from an examination of the newness, utility, and non-obviousness of the invention described in the patent claims. This examination requires information concerning the state of the art in the field the patent will be practiced and is initially undertaken by the Patent Office. The Patent Office relies on the inventor to present information to establish that the claimed invention meets the prerequisites of patentability. If the Patent Office finds the prerequisites present, a patent is issued and that patent is afforded a presumption of validity, 35 U.S.C. § 282. See, e.g., Reinke Mfg. Co., Inc. v. Sidney Mfg. Corp., 594 F.2d 644, 646 (8th Cir.1979); Pro-Col Corp. v. Commissioner of Patents,

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Bluebook (online)
570 F. Supp. 810, 1982 U.S. Dist. LEXIS 10213, Counsel Stack Legal Research, https://law.counselstack.com/opinion/carl-schenck-ag-v-nortron-corp-tnmd-1982.