Lorusso v. Ultra-Hi T. V. Manufacturing Corp.

168 F. Supp. 626, 119 U.S.P.Q. (BNA) 373, 1958 U.S. Dist. LEXIS 3329
District Court, D. Massachusetts·Decided October 31, 1958·No. Civ. A. No. 55-589·Published

Opinion

FRANCIS J. W. FORD, District Judge.

This is an action for infringement of the Lorusso patent No. 2,572,166 and the Lorusso reissue patent No. Re. 23,960 for an antenna system for television. Claim 3, which is the same in both the original and reissue patents, is the only claim in issue. It reads as follows:

“3. An antenna for the reception of signals of frequencies associated with television broadcasting comprising a dipole element providing a continuous conductor bent to form two opposed V-shaped structures, each in a plane, one end of an arm of each V being connected to a corresponding terminal of a transmission line and with the ends of the other arms of the V’s being conductively connected together, with the varied spacing between the arms of each structure serving to broaden the band width and to keep the characteristic center impedance of a 300 ohm transmission line, and with the length of said element corresponding to a one-half wave length of a frequency at the lower end of a channel range which is to be accommodated, in combination with a straight director spaced from the arms of said V’s which are connected to the transmission line, with said director cut to a length which is not more than one-third the over-all length of said dipole element, so that the said director improves the sensitivity of said ele[627]*627merit at said director’s resonant frequency, while leaving at least two-thirds of said element exposed that cannot be nullified by said director when said element is operating at a frequency other than the frequency to which said director is cut.”

Antennas are an important part of the apparatus for transmitting or receiving television and radio broadcasts. An electric current flowing in the transmitting antenna sets up electromagnetic waves which travel through space at the speed of light. These waves passing over a receiving antenna generate in it a flow of electric current corresponding to that in the transmitting antenna. The receiving antenna is electrically connected to the radio or television receiver. The picture or sound is thus transmitted from the source to the receiving set by means of these waves.

The present patent is particularly concerned with an antenna for use in connection with the ordinary television receiving set. There are several characteristics which are desirable in such an antenna. It should be unidirectional, i. e., it should be strongly affected by signals only from one direction. Thus it can be pointed in the direction of the transmitting station and receive its signals at maximum strength and will not be affected by reflected signals approaching from other directions which would impair the quality of the picture received by causing so-called “ghosts.”

To obtain a maximum transfer of energy from the antenna to the receiver, the impedance of the antenna should match that of the receiver and the line connecting them. Since the ordinary television set is built with an impedance of 300 ohms and the standard connecting line has a 300 ohm impedance charaesteristic, it is desirable to have an antenna with a 300 ohm impedance.

Broad band reception is also sought for in television antennas. Two sections of frequencies in the electromagnetic spectrum have been assigned to television transmission. The low frequency range, from 40 to 90 megacycles, includes channels 2 through 6, and the high frequency range, from 170 to 215 megacycles, includes channels 7 through 13. The best antenna from this standpoint is one which would function equally well at all of these frequencies.

One of the earliest forms of antenna was the so-called simple dipole which consists of two arms of a conductive material extending laterally away from the upper end of the transmission line connecting them to the set. It was found that such an antenna would operate well for a given frequency when cut to an over-all length of approximately one-half the wave length of that frequency and would receive signals strongly from one direction only. However, such an antenna worked well only within the narrow range of frequencies for which it was cut. It produced good results only over a frequency range wide enough to cover a single television channel. When it was operated at other frequencies its performance was much less efficient. To get good reception on two separated channels, it was necessary to use two separate dipoles, one cut to each of the desired channels. These could be connected with a matching stub arrangement such that one was inoperative when the set was tuned to the other or each could have its own separate transmission line to a switching device near the set so that one or the other could be connected to the set as desired.

Several improvements on the simple dipole antenna were admittedly well known before Lorusso devised his particular structure. One of these was the so-called folded dipole, which had a second strip of conductive material parallel to the arms of the simple dipole and at a relatively short distance from them these parallel sections being electrically connected at the ends so as to form a single structure. This antenna would give fairly good reception over a range equal to four television channels. Its particular advantage, however, was that, at least when operated at the frequency [628]*628for which it was cut, it had an impedance of about 300 ohms and hence very suitably matched the impedance of the standard television receiver. It was also well known in 1949 that the band width of the folded dipole could be broadened by moving the parallel legs farther apart, thus increasing the cross-sectional area between the legs. However, there was a serious corresponding disadvantage in that when the legs were moved apart, the 300 ohm impedance was rapidly lost.

Another well-known development was the use of parasitic elements. The simple or folded dipole electrically connected to the receiving set is known as the driven element. Other strips of conducting material (really additional dipoles), placed in front of or behind the driven element but not electrically connected to the receiving set, are known as parasitic elements. When these are placed in front of the driven element, i. e. in the direction from which the signals are coming, they receive energy from the radio signal and re-radiate it in the direction opposite to that from which the signal was received. When they are placed at a proper distance from the driven element so that the re-radiated signal is in phase with the current produced in the driven element, that current is reinforced. Such elements are known as directors. They are usually cut slightly shorter than the driven element. A reflector is a similar parasitic element usually cut slightly longer than the driven element which receives the radio signal and re-radiates toward the driven element to additionally reinforce the signal received by the driven element. These parasitic elements also serve to increase the directivity of the antenna. A combination of a driven element, either a simple or a folded dipole, with one or more parasitic elements, is called an array.

With this background in mind, the Lorusso antenna can now be described. It is an array consisting of a dipole, a conventional reflector, and one or more directors. The dipole is a modification of the folded dipole having what he calls a bat wing shape. (Actually it has no resemblance to the shape of a bat’s wing.) This bat wing is made up of two V-shaped structures, one end of an arm of each V being connected to a terminal of the transmission line with the ends of the other arms being joined conductively.

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Lorusso v. Ultra-Hi T. V. Manufacturing Corp., 168 F. Supp. 626, 119 U.S.P.Q. (BNA) 373, 1958 U.S. Dist. LEXIS 3329 (D. Mass. 1958).

168 F. Supp. 626 (Lorusso v. Ultra-Hi T. V. Manufacturing Corp.) — published by Counsel Stack Legal Research, free access to 12M+ legal documents.