SCIENTIFIC ABSTRACT AFANASYEV, Y.F. -

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CIA-RDP86-00513R000100420001-3
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RIF
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S
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100
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November 2, 2016
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June 5, 2000
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1
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December 31, 1967
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SCIENCEAB
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ACCE.5310N 1111: AP4043519- !uravneniyakh matematicheBkoy fiziki. Matem. ab. vol. 14 (56)t Vy*p. 1-2, 1944) a Fredholm type of integral equation was derived for 1). Illustrative examples were ;worked out for specific cases of given pressure profiles. Orig. art. hast 25 formulas and 3 figures. ASSOCIATION: Institut mekhaniki AN SSSR (Institute of Mechanical AN SSSR) SUBMITTEDt 3ijun63 ENCLi 00 SUB CODEs ME NO REF SOVIL 005 OTHM 1 002 'Card--: 3/3 AFANASSYEV, Ye.F. (Moskva) , Impact of a body against a thin plate lying on the surface of a compressed liquid. Prikl, mat. i mekh. 28 no.5:868-879 S-0 164. (MIRA 17:11) t 15689-65 E',VT(1)/EWFW/F-1S(k A (h A01CESSION NE: AP4049573 'AFFT: ~;/02 58/64/004AW0650/0658 AUTHOR: Afantislyev, Ye. F. (Ijoscow) TITLE: Effect of a weak shock vave on a body lying on the boundary dividing two media %t SOURCE: 1n7.henerTq*Y zhurnal, v. 4, no. ;, 1964', 650-658 TOPIC TAGS: shock wave, diffrzaction study, ecmpressible fluid, displacernent reacticn ABSTRACT: The author studies the plans diffracti.on problem of the effect of a shock wave on a boJ.- w"Lth rectangular sect-ion on, the botLrldary dividing two media of the imcompressible fluid tv~,e 0 he finds the fDrces Fjkt) and F,(t,' actirw- on '-he q nz! -:~, !aw r-v-~ti 7 < Lnf) boid~, respA)c- 44 vely, ~c not rautually Influence tne press~jr~- fiel(is Jr, ~.ham. He fi-rst studies two aux-i-liary probiemB: A) on di-ffracLl,:~L of tiit, urave p = F(t-y-h) with respect Card l/ ;2 71 L 15689-65 ACCESSION NR: AP404957) to a rectangular wedge (x 0, y -h) ir. fluil' I ari-i J`splaced in the direction of the Oy axis at "he rote V(t); and B) on -!Ie n -11 a rigid heIf-stl-n-ir (X 0, y < 0) aceordirng tc tll.e -,e ACe Y E) d w; !nmalresvibIle f"Uij 'I. f 'i rf~ -n _r "ne (D A, 'n, a wrij V 61., L_ A T 1,-., Ninstitut mekhaniki AN- S SS Ins' 'itu Le J' Mechanics, AN SSSR) ST-'B~UTT-SD: 24Dec63 ENCL: 00 SUB COM M W REF SOV a 004 GTHERs WD -Card AFANASIYEV, Ye,F. (Mcs~va) Action of a weak shock wave on an cbvlacl~~- 4 164. W-7RA 17:13-0) 1. Institut mekhaniki AN SSSR. AFANASIYET,, Ye.F. (Moskva) Effect of a waak shock wave on a body located on the boundary of separation of two media. Inzh. zhur. 4 no-48650-658 164 (MIRA 1W) L 58292-65 r-R-r-(j)#ijP ACCESSION NR: AP5019h77 M % A J-. - ru-JL UR/OD40/64/028/005/0W/0879 le. F. AUTHOR: E!~IBI yev Tl= : Body striking a thin plate.1ying in the surface of a-c-o-ppressible fluid ,50L~RCE: Prtkiadnaya matematika i mekhanika, v. ?F, no. 1~, 1964, 868-879 ,TOPIC TAGS: flat plate model, fluid surface, compressible fluid , differe"tial 'equation ABSTRACT: The plane problem of a body of finite width striking a thin plate lying on the surrace of a compressible fluid is discusapd. The problem ii set up and for some initisl time inLervdl reduced to the aolu- of an integral differenti&1 equation in which the integral term has I If f erence liornpl vi ?,h a seini- f int tp in, rereeni, in the variables, Tile ~uL~,c- ~. )( Une equation in given -n lte F-~,rm- ~f The exist- ence of the Sojutiou .1a proved. Tli- p~,-eF, !tz tn-n .4olyed for &n-v given tIML., Simplo fomulas are gi-ron for calcuiftttiij~ t~:Ik -leformation of the Card 112 L 5"2 2-65 fACCESSION KR.f AP5019477---- 0 plate a-nd the velocity of the body after strtking the plate. The effect of the pla plate on a body Fitriking a fluid i.-3 ann' v7P,1 F, ~irf fig-ures, 97 foMilaS. kSS(~- : fiLT ~ ON. none .1M'T7FD- ? ~~'tq r~- 71, IDE ME V - Card _2/2 ACC N~ ' AR6033808 SOURCE CODE: UR /0l24/66/000/067/V096M2l_- a AUTHOR: Afanaslyev.-Ye. F. TITLE: Action of shoelk waves on an obstacle SOURCE: Ref. zh. Mekhanika, Abs. 7VI59 REF SOURCE: Tr. 5th Sessit Uch. soveta po narodnokhoz. ispolIz. vzryva. Frunte, Ilim, TOPIC TAGS: shock wave, shock wave interaction, Helmholtz equation, Fredholm equation, Dirac delta function ABSTRACT: The problem of the interaction of an absolutely hard moving plate of finite width with a plane shock wave in a linearly elastic medium is solved in an acoustic approximation. The disturbance pressure satisfies the wave equation and the boundary condition on the plate. By means of the Laplace transform with respect to time the problem is reduced to a solution of the Helmholtz equation with the Neumann condition in the half-plane. The solution of the Helmholtz equation is represented in the integral form by means of the MacDonald function. The Im unknown function participating in the solution of the He holtz; equation is found from the condition of the continuity of pressure outsid. the plate which results in Card 1/ 2 ACC MR' AR6033808 the solution of a Fredholm integral equation of the second kind. The Fredholm equation is solved by the method of successive approximations. The expression derived for the pressure drop value on the plate includes terms of the incident, reflected and diffraction waves. Curves of pressure distribution on a fixed plate of finite width are given for a step wave as function of the time elapsed since the collision. The speed of plate displacement Is determined for the initial movement of time with the action of a stepwise impulse and an impulse having the intensity of the Dirac -function. A. G. Gorshkov. [Translation of abstract) SUB CODE: 20 2/2 L-2784-66 SWT(l)/KWP(M)/FC5(k)/KV1A(l) ACCESSION KRs AP5021524~ UR/0258/65/005/004/0612/0622 534*26 Y A'JT110Rs Afanaslyev, Ye. F9 Moscow) TIT19i One problem In shock wave diffraction t SOURCEs InzhenerWy zhurnall v, 5, no. 4, 19659 612-622 TOPIC TAGS: shock wavep wave diffraction, shock wave diffraction, shock wave interaction ABSTRACT: Using linear approximation., the plane problem of shock wave interaction! (including diffraction and vave effects) with a shape shown in Fig. I on the Enclosure is considered. Assuming an arbitrary wave and pressure profile pl P(x#y,,t), the solutions to case la and 1b (see Fig, I on the Enalosure) are aesumd as 'PV (X, 0, 0. P-P.(X,Y.t) (Y>0'-1