SCIENTIFIC ABSTRACT KOLKOVSKI, P.G. - KOLLAR, K.

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CIA-RDP86-00513R000723830002-6
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S
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100
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November 2, 2016
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September 18, 2001
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December 31, 1967
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SCIENTIFIC ABSTRACT
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I . I KOMKOVSKI, P.; ALEKSIYLV* T. (Bolgariya) Comparative evaluation of the methods for determining total protein it. the blood sertim. Lab. delo, 7 no,12.-&7 D 161. (BLOOD PROTEINS) (MM 14. 11) 777= KOLKWKI, Ludvik, mgr in%., Machivability and the production efficieno7 and costs. Machanik 35 no.,9.-480-483 162. 1. Politechnika Slaskap Gliwice. 124-58-9-10510 Translation, from: Referativnyy zhurnal, Mekhanika, 1958, Nr 9, p 154 (USSR) AUTHOR: Kolkunov TITLE: Low-cost Construction of Wide-span Buildings (Ekonomichnaya konstruktsiya boll sheproletnykh zdaniy) PERIODICAL: Sb. tr. Mosk. inzh. -stroit. in-ta, 1957, Nr 27, pp 30-46 ABSTRACT: A brief descriptionidesign calculation, and analysis of the Card 1/2 stressed state of three -dimenp ional, thin-walled, reinforced- concrete, three-span roof-support structures. The roofing above the central span (3Z m) consists of a prismatic shell which com- prises plane ribbed reinforced-concrete panels 5. 5 x 4. 0 m; the roofing above the side spans (3 m) consists of composite flat slabs reinforced.by ribs. The calculation is performed accord- ing to V. Z. Vlasov' s method and by stipulating a number of hypotheses of the engineering theory of shells; this leads to the necessity for the solution of a system of six differential equa- tions. The coefficients of,the equations are obtained. The system of equations- is solVed by means of an expansion of.the desired functions in a trigonometric series. The solution of the example is carried through to a numerical solution, and 124-58-9-10510 Low-cost Construction of Wide-span Building stress distribution curves are plotted therefor, A possible procedure for the erection of such a structure is described. A. D. Pospelov 1. Structures--Design 2. Structures--Costs Card 2/2 )I . KOLKUWVq_Lv,. I Designing thin-walled hyperbolic cooling towers. Ifauch.dokl. vyo.uhkol7; atrol. no,2:25-35 159. (MIRA 13:4) 1. Relcomandovana kafedroy stroitellnoy makhaniki Moskovskogo inzhenorno-strottel9nogo inatituta imeni V.V.KVbyehova. (Elastic Platag and shells) (Gooling towers) 1 Z3 a,,~thor deduces the ge -I er. a -I J- z ed v:.,riat4-3n~:1 B~:,--nov-Ga, ~r- 0 f e s -71 gard, 16/1 1a Imam-'s M. V.11. dots., red.; slavovich;PASTUSHIKHRI, SAMSONOVA, S.S., telchn. red. (Fundamentals of the design of elastic shells] Osnovy ras- chota uprugikh obolochek. Movkvaq Vynshaia shkolap 1963. 277 p. (MIRA 16:12) (Elastic plates and shells) 11 KOMMUOV, V.A.; WHI. L.B.: MDIK. A.P. Singularities of acme Fayoman diagms. Zhur.ekspA toore fiz. 38 no-3:877-43% Mr 160* 1 (HIM 13 -- 7) 1 (Collisions (Nuclear pbysics)) 0 EDLMIOV, V.A.; 0101, L.B.; RUDIX, A.P.; SUMMY, V.V. Position *of the nearest singularities of the 7WI-acattering amplitude. Zhurj eksy. i teor. fiz- 39 no.2:340-344. Ag 16o. (MIRA 13:9) (Field theory) (Scattering (Physics)) KOLKULTOV, V,A9 . I Position of #a singulatitles of some Feyuman diagramg.-- Mar. eksp. i teor. fizi 40 no.2:678483 F 1610* (MIRA 31-17), (Field theory) -- I .- --- - '. - - - - .- - -5/056/61/041/006/026/b54 Covariant deduction of the B102/B138 )2, CY In the case of high electron energies (kp~,kq, (kp '~k' this relation changes into the WeizeAcker-Williams formula 013B 0 + (kq)l Ps y LO dO W,-- -qs- the subscript B B r-e-f -er s -.tc W~izsgcker-Williams, a ~~__dph' The authors thank I. Yu. Kobzarev$ I. Ya. Pomeranchuk and I. M. Shmushkevich for discussions. Reference is made to the following papers: 1. Ya. Pomeranthuki I. M. Smushkevich, Nucl., Phys. Vo 4521' 1961; A. M. 12 Badalyanp Ya. A. Smorodinskiy,,ZhETF, _~O 32, 1961; A. Badalyan. ZhETF5 41t 13151 19614 There are 2 figures and 6 references: 4 Soviet and 2 non-Soviet. The two referencee to English-language publications read' as follows. G. F. Chewr F. E. Low..Phys. Rev. 1640, 1959; R. Dalitz, D. Yennie, Phys. Rev. jO5, 1598# 1957- SUBMITTED: April 26, ig6i Card. 3/j S/056/62/043/004/042/061 B125/BI,86 Kolkunov, V. A. TITLE: Calcul.ating the invariant phase volume of N particles PERIODMU: Zhurnal eksperimentallnoy i teoreticheakoy fiziki, v- 43, no. 400), 1962, 1448-1455 TEXT: The invariant phase volume forN pax:ticle's- is derived in the form of the onefold contour integral N (7), d: *1, (z) 11 ~,H"' (zV,), 442iQ4 W~ere mj/14. Substituting half the sum of the Hankel functions H( 1) and H(2) for the Bessel function J,, it follows that; 1 Card 1/4 (2n2i 8A "') ~' H" I(z) fj H" TN I S/056/62/043/004/042/061 .Calculating the invariant phase ... B1 25/B186 .The paths of integration are shown in Fig- 3. The integral (a) can be solved only by a series expanzion. In the non-relativistic case, mi > -Zm holds for all particles, and integration yields the multi- dimensional series ON = (2g)3(N-10 QW-A I 1~01V-6)12(fljf~) X cc C 04) XOMIC k) F%"' ... C (MN) XMNM (10). X 2 r ((3N - 3)12+nk+ m, m,T M-0 XO X/I 2 2pk I Its domain convergence is the hypercube. -1< xk