Feb. 28, 1933. 1,899,758 K. w. JARVIS AMPL-IFYI‘NG SYSTEM Filed July 17. 1926 Fig. 2. INVENTOR WITNESSES I Ken/76777 W Jafv/s. ' ATTORNEY Patented Feb. 28, 1933 > ' 1,899,758 UNITED STATES PATENT OFFICE KENNETH W. JARVIS, OF vCINCINNATI, OHIO, ASSIGNOR TO WESTINGHOUSE ELECTRIC &7 > » MANUFACTURING COMPANY, A CORPORATION OF PENNSYLVANIA ' AMPLIFYING SYSTEM Application ?led July 17, 1926. Serial No. 123,211. My invention relates to amplifying sys 10 methods. 15 Fig. 4 is a diagram of the same circuit as tems, and it has particular reference to sys of Figure 2, illustrating the application tems employing thermionic tubes, either as that of a preferred form of my invention thereto. audio or as radio-frequency ampli?ers. In all views, like elements are similarly One object of'my invention is to provide numbered. ' means for preventing, in thermionic tubes Referring speci?cally to Figure 1,,a ther and the circuits associated therewith, the mionic tube 1 having a ?lament 2, a grid 3 parasitic, ultrahigh-frequency oscillations and a plate 4, is provided with an input cir-v which tend to occur under certain conditions. cuit comprising a portion 5 of an inductor 6, Another object of my invention is to pro— located between a connection 7 leading to th vide means for the prevention of parasitic grid 3, and a connection 8 leading to the ?la oscillations in ampli?er circuits that have al ment 2. The inductor 6 is shunted by a con reac y been partially neutralized by known denser 9 for the purpose of tuning. 55 60 7 to the input circuit, is an inductor A still further object of my invention is to 11,Coupled which may be a source of signal fre 05, provide means for the prevention of para quencies, either radio or audio. sitic oscillations at frequencies above those The tube 1 is provided with an output cir to which the circuits associated with an am cuit connected between the plate 4; and the pli?er system are normally tuned. 2, comprising an ‘inductor 12 and a Numerous attempts have been made to de ?lament source of plate potential 13. 7 70 vise circuits' which would prevent oscilla An inductor 14 coupled to the output cir tions from spontaneously starting in circuits cuit inductor 12, enables variations in the associated with thermionic-tube ampli?ers, output current to be'impressed on the input especially when such circuits are being used of a succeeding ampli?er stage. 251 in the ampli?cation of high-frequency sig circuit A source of potential 15 for the ?lament 75 nals. , is provided, as is also a potential source 16 None of the systems known to the prior for the proper biasing of the grid 3. Con art have proved entirely successful, there be nected between the plate 4: and an end 17 of ing always a tendency for the tubes to oscil so late at ultra-high, parasitic frequencies, no’ the input inductor 5 remote from the grid connection, is a small condenser 18, which, 80 matter how carefully the circuits have been taken in conjunction with a portion 19 of neutralized against oscillation at the fre the inductor lying between the ?lament con quencies lyipg in the normal tuning range nection 7 and the end 17, provides means for thereof. 35 According to my invention, I provide neutralizing the tube 1 against oscillating at ‘any frequency determined by the setting of 85 means, in the nature of reverse~feed~back the tuning condenser 9. coils, which are so arranged that all tendency The circuit thus far described and illus of an amplifier circuit to oscillate at para trated is the now well known'“Rice” circuit, sitic frequencies is nulli?ed. v shown in the United States patent to Rice, In order that a complete understanding of No. 1,334,118, to which referenceshould be 90 my invention may be had, the following de— scription should be read in connection with In the patent referred to, a-statement is the accompanying drawing. made that, in order to obtain perfect neu in the drawing, Figure 1 is a. diagram of 45 a well-known type of neutralized ampli?er tralization, it is necessary that unity coupling be had between the two portions of the input 95 made. circuit, Fig. 2 is a diagram of the same circuit as 50 ' inductor. . ' F ' . This statement, according to my experi that of Fig. 1, in a different form, ments, is not necessarily true if the fre Fig. 3 is a diagram of the same circuit, the quencies determined by the setting of the tun- ‘ tuning condenser being omitted, ing condenser be the only frequencies con > 1,899,758 2 back at parasitic frequencies are approxi— sidered. For suoh'frequencies, it is not even neutralized. necessary that the filament connection be mately Usually, in practice, the separate induc made at the exact center of the input induc tors 5 and 19 form parts of single inductor, tor, nor is it necessary for the two portions shown as the inductor 6 in Figure 1., It is accordingly obvious that the total inductive at all. in fact, the circui may be arranged effect of the ‘iJ‘WO reverse-feedback inductors as shown in w be effectively of such ind .ctor to be , inductive relation comp .nsatcd i 1 ingcondenser, on the tuned circuit cor.=..prisinry inductor 6 - . 9 is substantially Zero, and. 75 insuch event, separate portions of and condenser not decrease the signal intensity. ‘ the input inductor are coupled suf?ciently does My invention is capable of use in connec» ' ‘ effect of the tuning through resonatin tion with many differ rig types of circuit, and’ condenser. , if the circuit of Fig. 2 is nov:r considered 15 is not to be considered restricted to use with illustrated in 1. in relation to ultra-high freouencies above theBycircuit my invention, ll. arn enabled to con those determined by the tunii g condenser, it truct an ainpliz'i er having either one or a plu is obvious _. t the tuning condenser 9 offers 80 .. >2) rality of stages, ivi'a complete assurance‘ substantially Zero impedance to these fre that none oft-he stages Win oscillatespon quencies. fig. 2 may, accordingly, be re ' ieously ultra-high parasitic frequencies. drawn as in Figure 3, with. the tuning con denser elii hated, and the two portions of the inductor in parallel with respect to the .y invention is, tlierefoh, of importance in 85 I ,. ‘ion with the present trend‘ toward ub'e tuned radio-frequency amplifiers grid and filament of the tube. I in which parasitic oscillations practically lit is obvious teat, under certain condi always tend to be set up. tions, the circrit saoivn in Figure 3 is cap~ Although I have illustrated and'de'scribed able of oscillatin very high frequencies but single speci?c form of my invention, 25 determined by he l reactance of‘ the it will be obvious to those skilled in the art ~ jne grid-filament that many modi?cations thereof are possi inductors 5 and 19, 35 capacity of the tube, necessary feedlbacl: ble. My invention is accordingly not to be using supplied both by the plate grid ca limited except insofar as is necessitated by pacity inside the tube, the neutralizing the prior art or by the appended claims. condenser itself. l claim as my invention: , V 1. In thermionic-tube amplifier, ineans ‘With unit] co iling between the inductors 5 and 19, the induc t ve reactance of the two ‘for preventing self-oscillation including a 1 effective grid induc capacity between certain of the elements of 40 , be reduced to Zero, said tube, and independent nieans providing preventing potential, changes on the grid additional coupling between said elements, caused by variations in the output current. said coupling being inductive in character, in practice, however, such unity coupling is whereby the spontaneous generation of para substantially impossible ofattaininent, and sitic oscillations at ultra‘ high frequencies is 1.9.5 the circuit will accordingly oscillate at very high frequencies, as before explained. prevented. ‘ v _ 2. In a circuit comprising a thermionic In order to 1; ‘ever vparasitic‘ oscillations, l tube, means for preventing self-oscillations in said circuit, such means comprising; ca I. have discovered that it is necessary to com 45 pensate the lacl: of unity coupling; int-he cir pacitive coupling between certain of the ele 1.19 means, including cuit under consid zion by introducing into ments of the said tube, each portionor ' gut'inductor a ?n}: ap~ a plurality of inverse-feedback inductors, proximately equal opposite to set up for increasing the range of frequencies over by the feed-back oupsng ins-Thfrequencies. which the circuit is prevented from oscillat» 1.1.5 lieferr rig spec-i . 1g. 4, this is a diagrammatic view _. a pr'ferrel form of my invention as aoplied to lent to that ill at ‘ ' circuit equiva ' *. 2. ~ inc‘. 7 . ' 3. in a circuit comprising a thermionic tube having an input circuit and an output circuit, capacitive coupling means between ilate circuit of said circuits for preventing self oscillation, al c; the therinionic .e a plurality of and, independent inductive coupling means ‘ reverse-f ed-bac; ., 2 23, the also between said circuits for the prevention inductor 12 being; 1 I. to the grid-lila of parasitic oscillation at ultra-high fre nient portion 5 of ' motor 6, and the quencies. In combination, a thermionic tube hav other inductr .: coitipled to the plate .c-* r The di~ ing a ?lanient a plate and grid, an input 1.5-‘ ircuit comprising an inductor associated ' luctors, with said and filament, incans capaci ‘ of each inductor and 1e amount of coupl" ,, coupling said plate to said input cir to the corresponding portion of the inductor tively cuit for too prevention of oscillations over c ial s set up 6 are so chosen tha; the potent the tuning range, and additional independ- 129 across each portion of theinductor 6 serially 1 to- 111? /. 60 rectiono ‘ i p 1 1,899,768 ent means comprising a plurality of induc tors connected to said plate and coupled to said input inductor for the prevention of parasitic oscillations. 5. In combination, a thermionic tube hav ing a ?lament, a grid and a plate, an input circuit comprising an inductor associated with said tube, means comprising a con 10 denser and a portion of said inductor for neutralizing the effect on said input circuit of variations in potential of said plate, and additional means connected {to said plate and inductively coupled to said input cir 15 cuit, for preventing the tube and associated circuits from oscillating spontaneously at parasitic frequencies. 6. In combination, a thermionic tube having a ?lament, a grid and a plate, an in ductor connected between said grid and ?la ment, a second inductor connected between said plate and ?lament for the prevention of self-oscillations over a given tuning range, said connection including a con 25 30 denser, and additional inductors connected to said plate and coupled to said ?rst men tioned inductors for the prevention of para sitic oscillations outside of the tuning range. 7. In combination, a thermionic tube hav ing a plate and a grid, an input circuit for said tube comprising an inductor, one end of said inductor being connected to said grid and the other end of said inductor being con nected to said plate through a condenser, means for inductively coupling said plate 35 to said input circuit, said means being so arranged that the total inductive effect on said input circuit is zero at frequencies cor responding to desired signals, but is not zero 40 nals. at frequencies above those of desired sig 8. In combination, a thermionic tube, having a ?lament, a grid and a plate, a 45 thermionic tube provided with an input in ductor having a plurality of sections which are effectively in parallel at very high fre-' quencies, and means comprising a plurality of inductors connected to said plate and so coupled to said input inductor that parasitic oscillations are prevented from being spon taneously generated. a 9. In an inherently oscillatory thermionic tube ampli?er, feed-back means for prevent ing self oscillation over the range of fre quencies for which said ampli?er is designed ' and additional feed-back means for prevent ing self-oscillation at frequencies above said range, one of said feedback means being ca pacitive and the other inductive in character. In testimony whereof, I have hereunto sub 60 scribed my name this 28th day of June, 1926. KENNETH W. JARVIS. .65
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