SCIENTIFIC ABSTRACT KHAYKOV. A.Z. - KHAYLOV, M.S.

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CIA-RDP86-00513R000721920010-9
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December 31, 1967
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SCIENTIFIC ABSTRACT
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UUTKOV. A.Z. ...................... Self-oacillatore under large circuit losses. Radiotekhniim 12' no.1158-62 A 157- (KLRA 10:3) (Oscillators, Electron-tube) AUTHORt FLAiKOV,A.Z. PA - 2018 TITLE: An Autogenerator in the Case of strong Fading of the Oscillation Circuit. (Avtogenerator pri boljgih zatuhanijah kontura. Russian) PERIODICAL: Radiotekhnika, Vol 12, Xr 1, pp 63-72 (U.S.S.R Receiveds 2 /1957 Reviewe~z) 3 / 1957 ABSTRACT: The present work investigates the influence exercised by the con- plete fading of the oscillation circuit on the frequency and the form of self- oscillation and on the energetic correlations in the autogenerator. At first the equations for self-oscillations are soughtl only a single-osoillation oir- cuit autogenerator with inductive back-coupling is investigated. A graph shows the equivalent echeme of such an autogenerator at high frequencies. The system of differentW equations is set up from which the final formula is derived. When studying the energetic dependences in the autogenerator it is of essential importance to know the shape of self-oscillations. Such a shape was obtained b,, RA (his article publ. in R 9, Vol 1, 1954). The linear method cannot be used for energetical computations because it is too cumbersome. The equation takea the form of a differential equation in each of the domains. Difficulties arise when combining equations that correspond to different domains. A complicted system of transcendental equations iB obtained. The next chapter deals with the shape of self-oscillations and it is proved that the mains voltage and its first de- rivatedwith respect to time and correspondingly also the required time function y and 14 (where t is the eigentime of the system) change continually with time on the occasion of transition from one domain to another. A diagram shows the CARD 1 / 2 PA - 2018 An Autogenerator in the Case of strong Fading of the Oscillation Circuit. function y in the case of different lengths of lj(total fading of oscillation circuit in consideration of load). In the last chapter the energy correlations are investigatedg and equations together with the corresponding diagrams are set up. The exact solution of the equaticne for the autogenerator accordi-ng to domains shows that frequency and shape of a lf--oscillations depend on the complete fading of 'rhe oscillation circuit. IfYis increased, the frequency and the amplitude of the first overtone diminish and the aMDlitude of higher overtones increase. The efficiency curves under load and th-e curves of the general degree of efficiency of the generator attain their maxima at cettain values ofal. ASSOCIATION: PR13SENTED BYt SU13MITTED: AVAILABLE: Not given Library of Congress CARD 2 / 2 S/1279 4 94 61/000/004/037/052 13 3 D266 302 AUTHOR: Khaykov, A.Z. TITLE: On the external loading of klystrons PERIODICAL: Referativnyy zhurnal. Avtomatika i radioelektronika, no. 4, 1961, 17, abstract 4 G108 (Tr. uchebn. in-tov svyazi. M-vo svyazi SSSR, 1960, no. 1, 73-84) TEXT: The amplification of a klystron can be given as a function of complex.frequency. 1he poles and zeroes of this function com- pletely determine the properties of the klystron. Thee xternal loading changes the number and position of the zeroes and poles of the amplification function. The analysis is carried out with the aid of these poles and zeroes for various external loads. It is shown that non-periodical loading can change the effective attenu- ation of each resonator, and frequency characteristics analogous to those of cascade amplifiers can be obtained, but with an increased frequency band. It is possible to increase the bandwidth by employ- Card 1/2 7 S/194 61/000/004/037/052 On the external loading of klystrons D266 302 ing a resonant external load, but the obtained frequency character- istic differs from the usual characteristic of a cascade amplifier. It is suggested that by allowing a certain mismatch in the input line larger amplification can be achieved in the same frequency band, The best solution is to employ coupled circuits only in the last stage and choose appropriately the parameters of the other resonators. Under these circumstances an output power can be ob- tained which is close to the nominal in the given bandwidth. CAb- stracter's note: Complete translation-7 Card 2/2 4ol3o VIC 621017100310051005 'C" Khaykov, A.Z., Mcmbcr of tlho Socicty (see lo~ 12 i I.L-LIII - on a multiloo- Outl'ut C;.-Ct!4-,L- OIE' a frequency 0--c--illator TLITODICAL: Ra(14oteihni!,~a, v. 17, no. 0, 19162, 32-42 The design of the outpv-t circuit of a hi-Ih-z---rcc-': U ..Cncy 05C2.11ator i sconsidered, a syst-em of coiploC.. circi.Ats -.~-C: (:crived whi ch - c alcti, at C:-: this i)-,Iri)o--C- F 0 -L T- Cuit parameters by me"ansuof given parameteirs or- Ghebyshcv's charac- 'Cleristic .The inhluence of wnlincar operatin[~ conditiono of rpo-vmr- ful oscillators'on the Ere qucncy--,-L-;!7.z:rccier--1st ics is Co7as4dercd.. in calciuIrting. the energy, relationships, the author proceeelo from an equ3-vhl.-tnt circuit, shoTm schematicallt. The problem o-,'-' obtain-IlIg optimal frequency chr-racteristics' of t'ic output circuit, ir. solved ...in ti-io stages: The linear problev. a-ad :'he effect of t1he nonlincar ara made and design for-L processes., Simplifying assumptions -rLilas 0 ard G/ S/1061621 017/00u 0051005 ir cuit, D409/D303. On a Multiloop output. C n tcr-mv, o' -ven para- it par=eters. .1 are obtained for the circu Dyshcv-' requency charactei~i-stil~.- These -POXTAUias =0 -of 'C-Circuits ,eters- - Chel -'01:~tueen t A -, - d termini:hg the COUP Ing *i'. use or e o- thc "en a- ctcristic impedance , nd the chara (;0'P the b and-, 1) a s s i s. d c t c r, a i ha cffect Of 0* '--c'' ' " I '- I L. -- '-C ai-ions on the Krequenicy characteriutics '--nn C, 9f a tiYDc oscillator, w1hich made it poss"'01 U,-,C Z. lDcl a.-A!" e-thod (Pc-.L. 2: G in c,',LcU].,'t in~ r -1c I .Col l-LIS40TIS: The obtanin.cd nolutioar a -.,::c - ~tl)t,t circui,* of t-1-1, oscillator so ~!~c to o1 ers 0-~-' the ou L .L . 1, 4n cv.ency cl-Iftracteristic (in the ]-;nc ar dl-lcby,--hcv'- ch~iractcrintic for ,I,,iy numiber o-.': on-tors). Them-- sol%L""Ons Can 1)n a!-"O 1~flc~! for C n - 1.7 relationships, such aS the denev-eencc 0-:7 i*n-'2 of~ Circuits, on the cone~ition that tije tor rcmaiiis unchanc."Col. Thcrcbll? :'!.t. fov"I~. ti- ;'ncrcat~cs sharply, caril;,,'~rCd to thr~t 0'!~ oir',' .'Lln7l Ircuits- io --*-17crr-'z's'-(*. to -a the woz-.1-cr of- cow?lccll C. I,- po"! Cal.-:~ 2/3 On a multilo S/103/62/017/00'-/CC,.5/r,0.5 OP Output circuit D409/D301 If the iTifjuencc of TIOnlincar opcratin,, calletion- '11c" characceristic3, ohowcd that in tllc c' on t-.,,~ . . Sn"otcli, to excess-voltagc conditions, of -k " .7 the freqticncy 0,,jaj.-Ljcc c charigos, cOMPLIred to the characteristic C culnl-rd in - i-W-l .ation. These chan&cs nmount to a 1-educ "-; C, L-on 411 tuir-illa! MLLX5m,! of Cho-by-shev's chara'-`cteristic, and a zl.1trro':-"* r.- o.-"': ane. pass. There are 12 figures. ASSCCIATION: Nauclino-telhn4cheskoyc ob-shchestvo rad-4ote',1111i, i i 7 clektrosvy,-zi im. A.-. Popova (Sciept-f-4C -111d '~ecil- nical Society of Radio Engineering and 7", cctric-l L C man, unic at ions imelli- A.S. 'L'o-)ov) 3AUBMITTED: Card 3/3. Jazraary 13, 1962 r~~p S~;_KUKK, K.I., otv, red.; KOKORIN, Tu.I., InT --!~ -1 red. [Power amplifiers using multicavity klystronal Moshchxqe usiliteli na mnogorezonatornykh klistronp-kh. Moskva? Tzd- vo "Sviazt," 1964. -167 P. (MIRA 17-13.) AG I q 'AC I Fj ri "4r a 1 y-- vo -fe "I C~ c Tr. tinhahn. in-tov -%vvami. M-vo sv-va 3L.iR- vv- 1q. 196A. 18- 2S -4.r. Fl a:- I ACCESSION NR: AP404'2893 S/0108/64/019/007/004Z/0051 AUTHOR: Kha ~L._ZjActive member) . IxtML TITLE: Power relations in a high-power broadband kl- ystron amplifier SOURCE: Radiotekhnika, v. 19, no. 7. 19,64. 42-51 TOPIC; TAGS: amplifier, klystron amplifier, broadband klystron amplifier ABSTRACT: A theoretical investigation of the power relations in a klystron is reported. The beam perveance, accelerating voltage, output -resonator charac- teristic impedance, output-gap transit anglejand ather parameters determining the klystron design are studied. It is assumed that the current exciting the output gap is independent of the frequency and that the excitation power ensures the beat possible bunching of the electron beam. Formulas describing the effect of the klystron parameters and load parameters on the klystron electron efficiency are developcd. - They are useful in binding the klystron power for a specified frequency bandwidth. On the oth6r hand, klystron parameters ensuring a maximum efficie.ncy ca'n be determined for a specified klystron-amplifier power and bandwidth. The Cord 1/Z I L; N R. H I &H ~.M A Si R 7 -ACC NP, WOK EXPIDITAT1011 UR KhoLykav, Arnn Zalmanovich High-power multicavity tron ampl1f1e;6dchchnyye usiliteli na mnogorezonatornykh klistronakh) Moscow, Jzd-vo "Svyaz 1,,11 T964. 0167 p. illus -, biblio. Errata slip inserted. 4,300 copies printed. TOPIC TAGS: klystron, SO amplifier, circuit theory, band pass amplifier, amplifier deGign, resonator, cavity resonator, resonant cavity, amplifying equlymnt,, oacilla- tion PURPOSE A11D COVERAGE: This book is intended f,:.r scientific workers and engineers con-, cerned with oupcrhigh frequencies, and for students in universities specializing in this subject. It aims to present the basic problems a,;sociated with the general theon of floating-drift klystrons operating as high-power amplifiers of superhigh frequency' oscillations. The text contains material on the theory of multicavity klystron am- plifiers, on the analysis and synthesis of Mystron amplAfier circuits, on the energy dependence in klystrons during videband tuning, and on the relationship between ef- ficiency, power, and pass band of an amplifier. It also includes material on the cou- struction of moplifiers with Chebyshev-type frequency characteristics, of the maximal1y f lat type or with linear lphace chamcteria tics The author thanka Prof. G.A. ZeytIe" F~rof N.S. BeschastqM, and Docent I.N. Fomichey for their valuable advice cacerrAn.~ the solution or the mathematical problems; Prof. 8.A. ZusmanaysgyL on whose advice a Card ACC NRi nwriber of problem were examIned; B.S. Zabalkanskiljor his great help in preparing the manuscript; T.L. Tarasqva and A.V 't Challkow for carrying out the calculations cc the "Minsk-l" ccWp-u16ir; and_V.I. 61-0-voyev for'precessivg the calculation results. TABLE OF COMENM (abridged]: Forevorcl Ch. I. Passage of a signal through a kJystron amplifier 5 Ch. II. Analysis of k1yetron. ciavity circuits 13 Ch. III. Analysis of a klystron amplifier circuit -- 48 Ch. W. Frequency characterlotica of a klystron amplifier -- 76 Ch. V. Characteristics of a klptrca output circuit -- 111 Appendix. Determination of klystran cavity parawters by the given yaremetere of the Chebyshey ebaraoterlatic -- 147 Bibliograrby -- 16* 80 CODE: 091 SM DAT91 070at6k/ 01M WW: 009/ OTO MW: 052 Card 2/2 ACC N.R. ikk'00330'16 SOURCE CODE: UR/0108/66/0211 AUTHOR: Khaykov, A. Z.. (Active member) ORG: Scientific Technical Society of Radio Technology and Communication& im. A# So Ponov (Na,.;chno-tekhnicheskoye obahchestvo radiotekhniki i olektroovyazi) TI~I,:-,: Enerey relationships in a.klystron amplifier with extended interaction in the output circuit SOURCE: Radiotekhaika,-v. 21, no. ioj 1966, 37-44 TCPIC TAGS: klystron, electronic A3STIRACT; Large si&nal operation of a two-cavity extended interaction klystron is studied in'order to determine the conditions for maximum operational efficiency. T,-.e klystron efficiency is determined by analyzing motion equations for electrons in the gaps of the two cavities at the klystron output. The use of extended inter- action in the klystron output circuit gives a maximum klystron efficiency of 66-55 at a phase shift of 1200 between potentials of the first and second resonators. This! is a 241", increase in efficiency over that for a single -interaction klystron. efficiency is obtained for a minimum value (1200) of the electron beem angle in the space between the centers of the two gaps. The value of the =aXi-mn efficiency'decreases as the distance between the gaps is increased. Orig. art. A-las: 9 fi6ares and 10 formulas. -ST UB CODE: 091 SUBM DAM: 03jul65/ ORIG REF: 001/ O-ni REF. 003 Card 1/1 UDC: 621.385.624 KRISANOVp A,F,j KHATKOV, L,L, Redealp of alactropmmatic distributors. Fatallurg 8 no.gv- 32-33 Ag 163. (lm 161161 1. Nikopol'61,iy yuzhnotrubnyy zavod. I KUYXIDY.9,-, J44 -podpolkovnik. . , ,Inzh. I-, = Bleatrolytic capacitora. Voon, gvlax, 16 no.2t38-43 r 158, (Condensers (Xleatrioit7)) (MIRA 1113) P1117YA10'-~1i),1V 137-58-5-9484 Translation from: Referativnyy zhurnal, Metallurgiya, 1958, Nr 5, p 96 (TISSR) AUTHORS: Golubev, T. M. , Khaykov Sakharov, G.A., Danilov, L. 1. , Shamets, Korchemnyy, M. I. TITLE: Reductions and Pressures Employed in Rolling on a Medium- gage Sheet Mill (Rezhim obzhatiy i usiliya pri prokatke na sred- nelistovorn stane) PERIODICAL: Sb. tr. Kuznetskogo mezhobl. pravl. Nauchno-tekhn. o-va chernoy metallurgii, 1956, Vol 1, pp 79-95 ABSTRACT: The results of an investigation of reduction (RE) schedules on a 2150 2-stand three-high Lauta mill with 850/560/850 mm rolls are presented. Analysis of the temperature of rolling (R) and the pressures and actual RE schedules in the R of 1150-1800 mrn wide sheets of St. 3, St. 4. 65G, IKhl8N9T and SKhL4 steels from slabs 80-Z20 mm wide established that actual R schedules do not reveal any differentiation in RF, with width of sheet as en- visaged in the technical instructions. Differentiation of actual RE in accordance with the grades of steed being rolled is ob- served to be correct. R of sheet of ShKhl5 and 65G steels is done Card 1/2 in accordance with the technical instructions, while Nrs 3 and 4 137-58-5-9484 Reductions and Pressures Employed (cont. steels are rolled by more intensive and lKhl8N9T and SKhL steels by less intensive regimes. When billets