CIA Reading Room cia-rdp86-00513r001134710006-8: SCIENTIFIC ABSTRACT MISIC, V. - MISIK, V.

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"APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8 :. i .'i :/"-}' '"- i .' ~ Exte~mlo? do probl~me tie la torsion Corn � - � '~ Dans c~ article 0n [~en,e l'ext~sion du probl~me de la torsion dr.s barrcs i section variable. E ~quatlons de Lam~ t3),. on ddduit lea ~,.m~, .............. tibs!!~. (4}/'{,j. ct les ~quadoa~ 'de Cbnto~. - -.. :~ -c.-:-.---~'T-7:m'.-:'~,-~:- que Ia' d6f6rmMion a u~; earact6re incom~re~bk~. Le ' ' '. ' - p?bl6me gdndralis6 de la torsion est rtdult . d un probl'~me do t~ e N t ' , ' , . /p e ~mann, enutdisan,le~fonmfles. ' I d iteration (12} et ~la) 'Rts, ,~ ,te I au eAPPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000CTA-RDP86-00513R001134710006-8,~CKSICU, M.So. East Maropean AccessionsVol. 5, ~,~o. 9APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8" "APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8 " . '11 :: ~: ' � 'w ~.s ..... � -i - � - - - - - . ~ -. .- x,:,~,:.:.~'~;';';'';"':"?'"'::.- ............. ' :"~"'';, .... '"" -'".-. - ' ' � . .. -; ' '. ' ':'" '';'. -" .... ":'.-'-" ' ' ";;'.' ' ' '' '-' ~'- -,~,.~,'.'-' : -' "'~.'~.~~J~-;?;, ::,!~-~G:k~-:;v,_A ;. ,'.,- '. ?~+. ~'...":;2..': .-..'.~ .;:- :-:,~ ..':. :-. ': ;~:::,-: ';~;t..'_-_.' .: r. '7 -~Z:-':;' '..' 2.'~-.~ ~' .~:: '"'-;/-2 .~.~;k~ZZ~?~ ~ � ~-'~.~a~;~.x. '..i*':-;x ~ ;:..':-.-'--" _-. '-:------- --- .-.-.-'..- - - � :-- ' - ----- -:. '~-. '-,,-.-: .....APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8" "APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8:,~]!:~:.:,: ;!~ ,.:,,: ~ ~ ~-,~ ,:: ;:. ~,~; ,: ? .,' � ,:-: .: .--~*-.::t,,~_.:~,~;~ ~J~l~":'fF.~,,f;4.~_: - -~ '-'~ ' ""�~' [i't~ , ' " � , , ..APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8" "APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8 ,;1~._~ .. ! ~ : :,.. .... , ~ .:.. ?~~ ~ __:_~ ................ ............. ~ ~. ~ ~. ~ ~ .~-,~'~ .... ~:.-~ ....APPROVED FOR RELEASE: 0611412000 C1'A-RDP86-00513R001134710006-8" "APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8; -'1 _: ''. -- - .~ :,.!; :!i'...�."l. ' i'~ _ - i :,' .:..'-'~ ':': ",. ~' . ":'; ~' ~,.-i':.'-"'- ':...'~': ;-: i',";'?.i~ ." -'.':'-. . .-,.,-. ., : ~.~,..� : --; . ...�,-� .:. . .......:..~ . .. : .� .� , , � . , . .. .. . .,.. .,, ..; . . ,..,. . .~ . ,., .... ~,...,~,..,-.,.-,.~_.f ,: ._. �. ... .. ,,~... ....: ~ . .. ._. ......... , ...... ,......APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8" "APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8.,t / .~-J'!~;i6r~ ;,~7~:~:~:-:~!' ;': :'"'?:"::.: , : :-i;.~ ~" ~ '~'~ ~:' ":~;':~ ~ -~-~ -.~. z.~.~'~::, '.~' .' :- . ,: '7:'~W .APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000C1'A-RDP86-00513R001134710006-8'~epresemtat�on of the -~lmst�c-equiltbr~ur~ equabio~ by means ofqmatern/on-monogeneous function~..SO:AprilM�nthlYI958Index of East European Accessions (EEAI) LC. Vol. 7, no. 4,APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8On the Boussinesq snd Hertz dynm..~ic ?roble~. In C-er,~n. P. ~69.~%.,th]y list of Eastern European Accessi. o.~ I,:de~ (~..~.I) LC %~1. ~J, J?o. 11~'~ove,%er 1959 -Uno!.APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8AUTHORTITLE;~5/~o~6 6m the Propagation of the Seconde-r~' and Primary Disturbances of the Total Fieldp~ODIG~ Stuff ~ Cereet~i de Mee~e~ Apllcat~, 1~, No, 3, PP. 65~-613 ~e author establishes In t~e ~ttcle the e.~umtions of the non-relativistic therm~, rheom~etic ~d ~vitation~ field, c~led the "Tot~Field". ~e fo]~o~ing factors ~e considered fo~ the Total Fie!d= the electricfield E, the msetic field H, the electric lng=orion D, th% m~etic inductionB, the lo&~ densl~ ~ , the 9rop~gation s~eed of the light in vacu~ c, co,coted~ the ~uatio~ of the m~elll~ electrom~etlc field (1~), the c~ent d~-slty J (1.~), ~d the e~ations ~ the ~heologie ~ield (~.5). ~e theologico~ M. Ee~e~ (~), E~S. ~vlin (~)~ J~L. ~ic~en (3), B~D~ Cotter (~), ~.G.royal (5), ~d S. Z~emBa (6) e~ be t~en into conslde~ation ~lth ~eg~d to therelatio~ between stresses ~d defo~ations~ ~e author then ex~lnes them~etl~ ph~omena of theologic line~ity without the coefflozents of the ~tion t~e~ ~eSe 9h~omena ~e either pure visco~ ~tic or D~e 91~toviscous.Card 1/3APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-885~o33 ~/oo876o/'ooo/oo3/oo~/oo7 A~aS/k026On the Propagation of the Secondary and Primary Dls%urbances of the Total FieldAn e. rt. ension of thcs-, relations within the total field can also be accomplishedon the basis of some studies by W. Roll (?) and R.S~ Rivlln (2) and (4). Theauthor recapitulates the general theologic expressions: the relations Detweenstresses and deformations (1~8), the relations cz' an isotropi� linear theologicfield (1.10), the equations of convection corresponding to the T thermal fielU(1.13), the equations of' the total f'ield (1~i9), and the lmpu!setheorem (1.20).In order to explain the interaction of the tbermal and magnetic theologic field,the author tries to establish symmetric relatlon.~ instead of the equations of thetotal field. For this purpose he transcribes them in the form of (2ol) and final-ly deduces the symmetric equations of the ternar[ ir~teraction of the three equa-tions show symmetrically the interaction of the three forms of the =otal field.Considering a deviation o[' the ~al,zes of the seconda,'-y field in relation to astationarM field, and the expression (3.!) being a component of r. he spectral de-composition of the value of th~ primary end secondary field, the author dcduc~successively the characteristic cone of the secondary disturbance of the totalfleld. Introducing the equation which gives the speed o~ th~ AlfvSn wows, heobtains the solution of the linearized e~u~tion (3~43) and the ~elat. ion of fro-.quenoles (3.~.6). Considering then a homo.~enoum magneti= field H,Card ~/3APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8On the P~oP&g&ti�n of the Secon~ ~ Prim~ D~stur~ce~ of the ~ot~ Field studies the c~e o~ pl~e ~ves, ~eviving the ~u~tlons%he ~%~%ion~ ~ z, h~ i~ {~ 1~) ~e spee~ of w&ves ~n the t~forme~ ~ the infinite conddotivity ...... ize~ e~ui~ib~ . ~- -~,+wor ~eO ~tu~e ~,.~+,. electric con~C-of the ~ .... d ~ (~.20)~ '[r_e = ...... '~-~ b~ (%.22), the t~n shape ~o~ a con~t~ d~sitY ~avit~lon~, ~ostati~, m~et�~tat~c' pce,s~e' of the ~b~e~ ~C~fe~ ch~a~t-e~ .lnce the~ ~d viscoel~tic ~iel~. the no~e~ities of h ~e respec '- , ' 1% ~glish, 3 Soviet, 1 order of H. ~ere ~e 2 fl~es ~d ~1 referen~eS~ ~de~tifi~d.APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8AUTHORS: ~i~icu, ~{., and Dinc~, Fl. / ,zooozoo /�o,xoo D255/D304TITLE:Dynamic bending of girders with viscoelastic proper-ties. I.PERIODICAL: Studii Bi cercet~ri de mecanicg aplicat~, no. 2, 1961, 239 - 254TEXT: The authors establish the equations of the transverse vibra-tions of a straight girder which has linear viscoelastic proper-ties depending on an arbitrary number of parameters. A series ofusual schemes in the theory of viscoelasticity are considered tobe the physical schemes of the properties of the viscoelastic ma-terial. These schemes were first considered by L. Boltzmann andlater described, under the designation of Voigt and Naxwell models.In this paper, the authors do not consider the plastic Pheno~ena;the general theory of motion, however, is established for anAlfrey-type model of generally linear oscillation. Since no creep-Card 1/6APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8 /00 /61/000/00 /001/008 D235/D304Dynamic bending of girders ...� . ' terfer, a ~axwell model is conE~idered i~ot~es~P~~-lng phenomena ~n ' of freauencies of 5 - Pcations regarding the vibratzons ~ the transversal oscilla-determining the differential equation oftiens of straight beams, the authors consider a straight b~am of Llength, referred to an orthogonal system of Oxyz axes, the Oz axiscoinciding with the non-distorted axis of the girder, while the Ox axis is directed in such a way that the system of coo~~din~tos be deduced Th q � ~z should be a straight system, e e uations of ~otion from the theological theory of continuous med~a. If ~,~ ) is the normal stress on the transversal section at a z distz~ce from the axis, the following hypothesis may be admitted: a) t~ ~teri~l distort~ according to a general theological s~he~e$ bi The P and Q operators are purely differential; c) Pn and qn are constant coef- ficients; d) The transverse dimensions of the girder are reduced in ratio with the length L, so that the current hypothesis in the theory of thin girders may be accepted. These hypotheses lead to the equation of transversal vibrztions:Card 2/6APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8Dyn.~.~i cbonding of girders~/co~/e~/c~/co2/~o!/ooe _ Z $c~ ~ (~.~) (1.5) section, u the t~e:~.sversalin ~:hich is the inertia r. oncnt of theover-l] .... sp .... ~e.n .... or -o~ the length ~ity, f(zt ~) ~ ~ the g~uchy problem =or ~hclength uui~y. The complete co_u~zu,, ~'consists in determiuing thetr~svers~l vibra~ions of the girderssolution of the differential c%u~tionwithin the bo~dary conditions~ ,,,~',. (% t): ~'~,~'" (o, ~): o, (~.~) ( ~. 7 )~ ~'" (% t) = ~)i'~" (o, t) = o,caraAPPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8 ~/ooe/e~/ooo/oo~/��z/��s o2~5/D5o�Dynamic bend~.ng of girders �..and the initial con~ ~o.~s ~O ~0 ~ ~ to h~.ve the sh~ge ofOonsi~e~in~ the (~.~ ( ~l(Z) ~ Tl(t),bein~ the funo%ions to be ~e~e~mine~, the authors , ~ ..~.,,~, . . ,- (2.5) On ~he ~asis o~ ~he ~reen ~nn~ion ~ ~he Broom~ieh integral ~he g~hors ~hen ~edn~e ~he rel~ion o~ ~(~)Card ~/6APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000CTA-RDP86-00513R001134710006-8Dynamic bending of girdoz'~ /ooe/6 /ooo/oo /ooz/ooeD235/D30/~in which Tl(t) and T2(t) are expressed by(2.28)(2.27)(2.28) /tara 5/6APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000C1'A-RDP86-00513R001134710006-8 /008/61/000/002/001/008D255/D30~Dynamic bending of girders ...Tl(t) represents the solution of tke differential equations for '~' s w~ile T2 for the given initialthe homogeneous initial condz~lon --conditions. T2 is completely determined by the initial c.onditions,,..~ m bT t>e disturbing ~-~uction. There are I figUre, I table .... ~ ~ ~ -- _ _ . i ...... d 22 non-Soviet-bloc. ~ne fourand ~� ~references: z bovle~-u~uu ~ most recent references to ~.g!isk-language publications read as follows: P.S. Berry and S.C. Hunter, The propagation of dynamic stresses in viscoelastic rods, J. ~ech. Phys. Solids, ~, 72-95, 1956; H. Ko!ski~ The propagation of stress in visoe!astic solids, Applied 51echanics Review, II, 9, 465 - 68, 1958'; E.H. Lee, ~.d J.A. ~orrison, A comparison of propagation of longitudinal waves in rods of viscoelastic materials, J. Po!y. Sci., 19, 93 - !!0, 1956; J.A. ~ � . ~ave orooagation in rods of Voigt materia ~~m terials wlth three pare~ezer models, Quar~.~ud visco- . - -. . App!. ~.iath., 1�, 153 -'%96, 1956.SUBSiITTED: December 21, 1960Card 6/6APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000C1'A-RDP86-00513R001134710006-8 M,; DINCA, Fl,bars with viscous elastic properties, 8tudii cerc me� apl 12 no.4:899-9~ '6t.APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000C1'A-RDP86-00513R001134710006-8APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000C1'A-RDP86-00513R001134710006-8~ T~ODOSIU~ O.The ~.~ symmetrical problem an~ plane problem of the elasticitytheory for the nozhcmogenecus isot=opic ~odies. OcanmicarileAR 12 no.8=921-927 Ag '62.1. Comunicare prezentata de academician E. CsrafolieAPPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000CTA-RDP86-00513R001134710006-8MISIO[~, M. Rheolo~� structurea. '62.Stud~ cerc mec13APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8F~OO~/ 6Z/O '~ 3/O06/O0 ~ /O08AO65/Ai26AUTHOR:TITLE: Rheologic structureP~MIODICAL: Studii ~i cercet~ri de ~c~lc~ aplica~, v. 13, no. 6, ~962, [,357 Being a continuation of ~ a~ticle 'published in Rede de M~c~niQueAp9liQu~e, no. 4, ~962, 7~3 - 749, this a~tlcle descries the elements of ~hetenso~ densities ~d of the emte~io~ forms. The elements of ~e ~, ~, ... ~[=~]~ ... ~[~] .pace, have me o~,ete~ of nonlinea~ operators whi~ applie~ to so~ co- ~ oont~ava~ian~ elements, de~em~ine ~he invasions in p ~ ~. ~e ~o~ isolation of ~he elements of ~hese sp~ces in the expression of the ~esDec~ive in~apiants, should be b~o~h~ into co~esDondenee wi%h'thei~ type of st~C%u~ and their operator c~racter. For %his purpose, ~e au~or amines ~e followf~ supplgmenta=y indications In comparison with the inflnl'~si- mat ~eory: the [g (Vn)] space; the [3~]-vectori~l sp~ce; the ope=~tor dices; ~e n-vectors; the operative KPonecker symbols; ~d the ~nsor densi-APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8MISI�U~ M, Theory of viscoelasticity with couple stresses and reductions to two-dimensional problems. Pt, 2e Rev mec appl 8 no. 6:921-952 ~63.APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8Rheolo~f.� a~uatuze~.APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000CZA-RDP86-00513R001134710006-8International Symposium o,~ the Applications of the Theoryof ~cttons L~ ContL~um Kechm~cs, Septe~Eer1~3, ~ T~Ilat. grunt cere mec apl 15 no.1:26~-265APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8 MISlCU, H....... ~ee~'~~ ' vlscoelaticity with couple st~esa~ and some ~d~%l;n~ to tw~_di~e%~n~,proble'~- Pt. 2. p~evme� appl 9 no. 1~3-~ '~.APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000C1'A-RDP86-00513R001134710006-8A ger~*-.r.altz~t:,-on of Cos~erat c'l',ati~n~ el' the ~.:otlon ofdefor~abl~ bo:ite~ (,~ith Int~:rnal degree, s of fr~.edo.~). Re*~mec appl I{o,~ 9 n0.6:1351-1359 '64.1. Institute o!' Applied ~.~chantcs of the I{~n~ Academy,Buch~es~. Su~t~d November 1, 196~.APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8 � ~ ~,/e5/o~.o/oo~/~-o85~''~~r~,�,,r~ sotmc~- CODE: Ru/uu.,.w~,-- - ~,I A CC Nih AP60183~8 ' ~ ,5'ORG: Center of the Meohanios of Solids, Academy of the Socf~If~t Rel~bli� of Ru?_____~ ,SO~: ~m ~~ ~s sciences ~c~es. ~e~e de mec~e a~H~ee, v. 10, ..' TO~C TA~: Ma~lo soll~ el~O s~cmce, no~omo~ne~s s~e, meo~c~ a~sa ' e~a~cns o~ e~ium a~ &~/ved on ~e basis of meoh~c~ work ea~Eshed ~e~sly, wMck ~[ows ~e ~i&~a~oa of bo~ consWa~ed ~6 cent~s~me~ic o~e. ~us, It M ~ssible ~C: 539,APPROVED FOR RELEASE: 06/14/2000 CIA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8ACC NR~ ~g60183Z$ elements. Acco~dln~ ~o tho present e~dysis, ~ch mo~ls a~e c~ac~riz~d by a m~ s~esses ~d ~a~en~ o~ ~o~tLons, or ~een c~p[e-st~esses out ce~t~o-~me~' ~e pr~a[atio~ of ~uen~ be~een ..... tro-[c ~es ~th ..... ~[.~ ~ are ~so Such effec~ are presen~ ~_~u ,~_~ D~[c su=face effecm o~ de~ed. Orig. ~.~: 106 fo~ ~d 4 fi~res. S~ CODE: 20/ S~M D.&~: 07J~65/ O~G ~F: 006/ O~!/2 7J/_.APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000C1'A-RDP86-00513R001134710006-8,~eory of asymmetric pI~stic ~d v~scoel~st~c pla~t~c'~o..~.?~.Rev mec ~ppl ~ ~o. 3~-~9~ '6~.APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8$tudi� cer� mat l~ n0o3:46~7,33 '63.APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8SO: ~onthly List of East European Accessions,Uncl.L.C.Vo!.2, No.!i, Nov. 1955-APPROVED FOR RELEASE: 06/14/2000 CTA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8increased importance"ol. il, no. ';2, a~c. 1955So. ~ast %k-opean Acc,:ssb~ns L~st'%1. 5, i;o. 9 :.ie~:te:r,!:,,r 1056APPROVED FOR RELEASE: 06/14/2000 ClA-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000C1'A-RDP86-00513R001134710006-8MISI~.UJIOZ, AIXADII~$ZGleboznawstwo o~olne. Wyd. 2. ~,~rszawa, pan,~two'.ve ',..')~wn. P~inteze ~ kesn~,1956. ~00 p. (General science of the soil. 2d ed.) DA Not inMonthl, g List of East European Accessions (EEAL) LC, Vol. 6, No. ~, Au~ 195~. Uncl.APPROVED FOR RELEASE: 06/14/2000 C1'A-RDP86-00513R001134710006-8""APPROVED FOR RELEASE: 06/14/2000C1'A-RDP86-00513R001134710006-8 mercury ~ons ~ the levelrabbit ~.o~ se~ ~n acute ~