SCIENTIFIC ABSTRACT KOGANOVSKIY, A.M. - KOGARKO, S.M.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000723620008-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 19, 2001
• Sequence Number: 8
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

NL' V
rbialitati" autoustle o6ntrol of the ferrie-ohlorMs coagulAnt
based on.36 Oxid.o-reduotion potentWo Ukrekbimosbwe 20 n*96s
693-100 154* Om 813),
le Institut obehahey i neorganichaskoy khIvii AWaxii nauk
usm,
.(Water-Purifia'ation)(76rric thloride)(Automatic control)

V-4
AID P 2626
Subject USBRMedicine
Card 1/1' - Pub. 37 -3/22
Authors
Kullokiy,.L. A.., Kogenovokly, A. N., Rovinskaya, T. N.
Title t Effect of sodium Silicate on a purification of,water
by coagulation r
Periodical Gig.1 san., 8JP 12-15, AS 1955

Abstract Various tests for purifyingand decolorizing the
water by different ohemiols.are denorlbod..-It is
.
demonstrated thO.t ferric chloride is a better
d6c6lorizing-agent and,& better activator of
flocculation:04anTsodium silicate. The'addition of
the latteir to ilater.is-Usrefdre not recom"ded.
-
Tables. 4 zvfse-p .193T 19530

Institution Institute qf General and Inorganic Chemistry'sUad,
of Sci., Ukr. SSR
Submitted n 18,'..1954

-,@ - . m - , "i
- an-maw rIffirlill s

Iz- MORIaliEN't i- -n -, - ,

73-1--22/26
AUTHOR: Kullokiyo L. A01,10amnovskiy A. M., Makhorin
Kaliniychuk To m Clio mov 9, __V Itz and Dikolenko ToI
TITLE-.' Production of AftivO Anthracite Suitable for the Purifi-
cation of Waste Waters,of the ArLiline-Dye Industry,
(Poluchen.17e Akt;ivirovamogo Antwat sita . Prigodnogo Dlya
Ochi.stki Stocbnykh Vo4.Aaainok:@,a.socb.noi Prom7ablennosti.)
PMODICALi Ukminskiy. Dimicheskiy Zhumal, 1957, Vol- 239 Molq'
ppe
ABSTMOTV-TAbomt ry-a'hd- d1ot- plant investigations on the
0
activation Of %Zracite-by water vapour and'a mdxture of
combustion' 3mftots Sf carburetted benzene with water
vapours -at, 00 - 950 @ 0 are described* It was found that
vhe-. -cj-x-a-- lity-Vt - obtained-- adeorbents depended - on@ the
thracite. The activatea ajithraoite- contained
Mont @, of Vie. -an
150.-: 200 mg/g phenol and up to 300 mg/g methylene* The
activati6n,of anthracite gives an absorbent with,a.phenol
content of 123 - 165 mg1g and a methylene content of 120-
Th' Be
-130 mg/96 Activated coal KAM is produced.. , 0 U, fuln4ss,
of the a6tivatdd anthracite for sorption purification
Of Waste vatdrs;of - tbe -aniline-dye industry is evaluatido,
The kilu :ror the activation of anthracite ia-illustrated,
000
and d - Abed The properties of activated anthracite
Cara 1/2
_;P MIR,

73-2-19/22
AUTHORS;Xoganovskiy A'.I(.1 Rovinskaya T'.X. and Taranp kjr.
TITLE: lation of ihiosulfate and sulphide in aqx;eous so3.uiionB
on aeration in the presence of pyrolusite. (Okisleniye
-tiosullfata i sulffida, v vodnykh rastvorakh pri aerataii
v prisutstvii pirolyuzita),.
PERIODICALt nUkrainskiy Xhimicheskiy Zhurnal" (Mcrainian Journal
of C6601stry), - V01.23, 00,21 Marc=prilf 1957,
pp-.256-265 MSSR).
ABSTRACT: Thiosulphate is one of the strongest oxidation inhibit-
ors for'sulphate solutions". it-oxidises on pyrolusite
simultaneously with the sulphite; in the absence of pyro-
lusiteno oxidation,of the thiosulphate by.air-oxygou
occurs. The catalytic oxidation of dilute solutions of
,UL
5
lphitey thiosulphate and sulphide and their mixtures
with the aid of air-oxygen is of paramount importance for
the aniline-dye and oil industries (waste waters)'- A
detailed kavestigation, of the kinetics of the reaction
showed that in the presence of pyrolusite and 30-35
minute-aeration quantitative oxidation of thiomlphate
solutions is achieved (at concentrations not etceedi
QuA 1/3 50,M9-equ'#/*1)'. - Oxidation proceeds at a greater ratenfn
an acid medium and at a slower rate in alkaline media

73-2-19/22
Oxidation of thiosulfate and sulphids in aq-qeous solutions
on aeration in.the presence of pyrolusite 0 (Cont.)
(PH 11 12)t (Di ams 1-3)', -In both media the reaction
is of the firEft o r'. Onli 30% of sulphur passes into
the sulphatel.'the remainder being found in the form of
polythionates. The quantity of thiosulphate oxidisirg @up
to the poisoning.of',the pyrolusite is independent of the
initial conoentration of the, solution is constant/unit
weight for the same.,catalyst.. --Faster oxidation of sul-,
jhides by aeration in the presenoe of pyrolusite occurs..
he main produce is thiosulphatep 'sulphate and a small
quantity.of polythionates'i The.oxidation of a mixture-of
sulphateg thiosulphate and sulphide is more intensive
than the'oxidation of the separate components because'of
the interaction of these substances amongst themselves a2A
with the reaction.produati, The aeration of the solutions
on p@Tolusite can be utilised for the purification of
sulphur-oontaminated effluents of chemical plants'produc-
ing organic chemicals'., - Experiments were carried out in.a
30 mm diameter glass column-*filled with p rolus@te gran-
2/3 ules (480 g) previously activated with 5FIE onto
Card yo4f
this 20O.ml thiosulphate solution was poured and air vas
P

73-2-19/92
Oxidation ofzthiosulfate and sulphide in Aqueous solutions,
on aeration in thepresenoe of Molusite, (Cont,o)
bubbled through at a velocity of 127 lAour'.- H01 or
alkali was added to.achieve changes in pH. The relation
of time of practically complete breakdown of thiosul hate
during the aeration-of the solutions is tabulateC $a"ble'
if. Table 2 gives the dependence of the composition of,
th; oxidation products of thiosulphate on the pH of. the
solution'. The effect of poisoning of the pyrolusite on
the composition of the oxidation products is shown in
Table 4.
There are 3 diagrams, 9 tables and 15 referencesp-4 of'
which are Slavic2.
ASSOCIATION: Institute of General and norganio Chemistryt
Academy of Sciences, Mcrainer (Institut Obshchey i
Neorganncheskoy Shimli AN Will)-&
SUMMED: June 19t 1956's
AVAILABLE: Library of Congress
Clard 3/3

-tK o C A N 6P 5 K
- - L@ . . $ ILTOZMMO
ZU116% i doktor tokhnoAauk, OtTs"do; XA
E 74-130 (61111.@ '.II
- -*# .
XOGANOVSKIT, ON,
rods; ma om.
7 ,kmndiwd.n&*" **ed.:
I aln-i
kand V" 0; SMZOTA, O.T-. ova,
WXnIXU; 'Tidli TURMSMt T.I.-- "hyshiuk T.11-tokhAoreds
Elu
Eswdtary piotection of witer vMllss ind industrial savage paWl"tioul
Saatorna okhorona vodolvWshoh i,ochystka pronrolovykh stichafth vodo
41Y. lyd-vo Akad.nauk M=,- 1939. 162 ps (MIRA 22s?)
1, Akademiya nauk VMg 91yov, Rada po "Yabs"in,produkt- syl am

%14(0)
AUTHORS: Kullsklyp L, A., Koganovskiyj A. M., SOV/64-58-8-13/19
Rybehinakiy, M.tTf

TITLE: A Counterourrent Adsorber With a Two-Stage Suspended Layer
(Protivotochnyy adsorber s dvukh"yarusnym vzveshennym sloyem)
PERIODICAL: Khimicheakaya-prom ahlerinost', 1958, Irr 8,
Pp 498 - 499 (USSR@
ABSTRACT: The use of suspended adeorbente in the purification of in-
dustrial waste waters has a number of advantages, but also
one drawback in comparison to fixed adsarption1ayers: the
adsorption volume actually used is much smaller (Ref i). As
a result of previous investigations (Ref 2) an adsorber was
designed (Fi@), @- in which@the suspended adsorbent is contained
in two vessels sennrated from one another. The'w'ater which
is to be purificethrou .Sh them in nuccession while the ad-,
aorbant.automatically flows (counter to:the water) from one@
vessel Into the other. The two vessels constitut e an organic.
glass column of 2.2m height. The top vessel is larger than the
Card 1/2 bottom one. Water 'Containing about 100 mg/1 phenol4as

A, Countercurrent Adcorber With a.Two-Stage Suspended SOV/64-5S-6-13/19.
Layer
conducted through tho apparatus at a rate of 240 IN
i.e. a linear speed of 6.6 mm per necond.-A table with
comparative data proves that the use of a two-stage-column
results in a lower adsorbent (active coal) consumption '
than would be the case with a simple column. There are I
figure, I table and 2 Sovipt roferences.
ASSOCIATION;* Institut obahchey i neorganicheskoy khimii AN USSR (Institute
of:General andInorganic Chemistry AS UkrSSR)
Card 2/2
clh4
ONN

50)
ATJTHORSs
TITLEs
Xullskiyj L, A#p K6ganovekiZg A* h SOV/64-59-4-12A7
Kalinlyahuk, Ye.*- M61enkoq Ye. Is
Regeneration of Activated Coal After Adsorption Purification
of Waste Waters in-- the Aniline Dyestuff Industry
(Regenerateiya aktivirovannogo uglya posle adsorbtsionnoy
ochiatki otokov anilino-krasoohnoy promyshlennosti)
Dimiaheskays, pr omyshlennostfp 1959P Or 49 py 46-49 (USSR)
The regeneration of activated coal (AC) which may be used.for
purifying 'waste waters-in aniline dyestuff factori so is.most
suitably carried out by thermal-destructive regeneration. The-
first experiments of a simple annealing of the (AG) Of the type
.K&D at.6oo-m0p without or with limited,air admission have
shown'(Tablde 'I # 2) that.already af ter having repeated the, treat-
ment for 3 - 4..times nearly complete deactivation.of the (ACY
occurs. Purtber investigations were carried out in superheated
-steam current with KLD and a relatively inert anthraxite (AN)
which was produced according to tbe method IOM AN _'UkrSSR
(Ref.9). Regeneration was carried out in the laboratory ina
retorte (previously heated up to 7500) in steam current at
PERIODICALs
ABSTRACTs
Card 1/2

Regeneration of Activated Coal After Adsorption 307/164-59-4-12/27@
Purification of Waste Waters in the Aniline Westuff Industry
7500 for 20.zinutes. The different substances correspondiranto
the above mentioned waste waters were adsorbed ` in. - (AC d
(Ali) In differlnt'test series# and (AC) and (AN) worel'theAl
regeneratedo'E#erimento (table 3) have shown that oxi heating
.the KAD-in steam ourreat at 700-7500 for 20-40 minutes (41) for@-
60 minutes) &@complete rigenoration without a decrease in the
adsorption properties.may be-obtained. The steam consumption Is
0. 9 @ I g1g for KAD andl. 2 jIg for(AN)-at a mean carbon con.
sumption of 54%.Jor the purpose of obtaining high quality of
small@carbon consumption$ the,t*erature
must rise slowly In the begIMdng of the regeneration process*
The different composition of waste waters of aniline facto-
ries hardly influences the quality.of the regenerated coal.Por
the'purpose of checking laboratory experimentsj two semi-'
industrial experiments wire made in cooperation with Ke Yeo
.Makhorin and V.X& Chertov. For these experiments a mixture of
.steam and carburetor gas-,combustion products was used. The
results obtained ire given (Table 4). There are 2 figures,
4 tables# and 9 references, 8 of which are Soviet.
Card 2/2

OMMTOV, T.Me; YAMWRIN, X* Ye.; MNOVSKIT A.M.
Combining processes for the production and regeneragtion of
activated anthracites XhIs6prose uo,.7:635-637 O-N (f590
MIRA 13:5)
(Carbon, Activated) @(Anthracits)
M V! W, -11 VZO

NULISKIY, -L,A.;,,XOMOVSKU#,,. 1@6; GOMOVSKIY. I.T.; MWCUM, X.A,;
DEYMBLILV As &-'oty.red.; NUSNIK, N.I., tekhred.
loo. profit;
EPhysicochemical foundation* of water purifioation throv6
cosplation) Pislk6-khimlcbeW@ ognovy cohletki Yody kongm-
liatsisle lievs Isd-.vo Akad,neuk uss, 196o. 107 P.
(KIRA 13M
1. Daystvitalinyy chlen Akmdesii nauk Ukrainskoy SSR (for Dm-
A
(Water-ftriflostion)
AM

IN RIO RM,
P", M4
Me

1-4

KULISM
L.A.- KIDGaIOVSM
A.M.; BREVCHRIKU
II
A
.
.
,
,
,
VI

ChemIcal problems linvol-nd In the pratection of bodlea of vi*
+ -
IP
d
an
Impro7ecan
)f Uno quailt7 of water* L
Ar. khlm. zhure
n o12 11
243 -1246 164 (MIRA 1W)
- @

Vt

"N ug
UAR
a iz--am
Bailin -,mm"m

..-I
4 @- R, @ m Ir
-- 1. "linumul-RM-1-0- -R@

9(2)9 25(lo5) SOV/28-59-10-4/36@,
AUTHORS: Valeeyan, ShOGt and Koganskiyj S.De
Of Parametric Series for Electric Exe-
orkin
TITLE:
outive so
PERIODICAL: Standartizataiya 1959v. Nr 109 pp 17-19 (USSR)-
ABSTRACT: In.,th'O- cu@:rrint seven years, production in machine-.
bitilding.and.metal-Working industry will be doubled.
In.-this@,oonneotioni construction of normal machines
and devices acquires a great importance The,1959--
1960-.Plazi provides for compilation of w;rk.."Parqmet--.
rio:Seriew.,of.Zleotria Executive Devices,fdr Regulaom
tion and Distance Control of Technical Processes
(Oiltput.Pb~ramet.ers)";:.:~it,is to be worked out by-tho
,Speoial~06natruotion-Bureau.of Standardization ind'
Normalization TpNII_of@Oomplex Automation'(SKB -st,
TeNIM), Bleotrio executive mechanisms are power.'
designs incorporated into the systems of automatic '.
regulation-and remote control over-production ptooes-
sea The constant speed executive devices are it
'Card 1/3 present.manufactured according to their output @ara-
.-vac

SOV/28-59-10-4/36
Working Out of Parametri-c-.Seriee for Electric Executive Devices
their output parameters (see Table on P18).. The
project of SKBSN provides only for a parametric
series for torque, time of one turn, and for the
number of turns of the output device depending on the
type of executive mechanism. However, these stana-
arda'are.not sufficient for a correct evaluation of,
the full volume of work when constructing executive
devices, This part of the project needs to be oom-.
Working .,parametric series for elec-
pleted.
trio executive devices will permit a decrease in
their diversity and variety, and speed up the pro-
cess of computing constructions of new electric
executive devices.@ There is 1 table.
Card 3/3

S/119/60/000/009/008/008
B012/BO58
AUTHORS: jfalesyan, Sh. G.t Kogans kiy, S. D.
,TITLE: @Rational,Kinsmatlo,Diagrams of Electric Switching Crank
Gears
PERIODICAL: Priborostroyenlyeo 1960f Nc. 91 pp'. 30-31
@TEXT: Work concerning.the selection of a rational kinematic diagrasibr
the series of electric switching mechanisms of the orank-gear type is
conducted at present at the--SKB "Aytomatika". (SKB "Automation") at
@A/kirovokan. A short summary of the results &chi_9`ve_&__s_o7ar is given in the
/present, paper. The electric ewitching crank gear consists of an-electric
.motor, a gear, and an additional device. The guarantee of self-looking
and greatest efficiency is one of the principal conditions for thegearo
It is pointed out that all the electric switch mechanisms manufactured'
at home'and abroad can be subdivided Into two groups according to their
kinematic characteristic#. These are described here in short. In the first
group (Fig. 1)9 power transmission to the crank at the exit takes place
with the aid of two.worm gears. The two varianto possible for manual drive
Card 1/2
B, NMI-
I--@MMIK

Rational rinsmatio.Diagrame'of Electric 8/119/60/000/009/068/068
Switching Crank Gears B012/BO58
are shown (Figs, Is, and 1b) and.desoribed. A worm gear (Fig, 2) is MUM-
cient for a short response time (1-60 seconds). In the second group#
power transmission from motor to crank takes place with the aid of some
pairs-of spur gears (Fig. 3)o It is pointed out that It is appropriate.
to combine 'the positive properties or both groups. Such a construction
is shown in Fig, 4- Power transmission for the.latter takes place with
the aid of some pairs of spur gears.and a worm gear at the exit. This
variant Is highly efficient and corresponds to the self-looking conditione6
A further varlant.of a switching mechanism with a manual drive is shown
In Fig. 5. This drive is built in the form of a "differential", and in
combined, v1th a device for limiting thi maximum load (Fig. 5a). The con-
shown In Fig. Wisdesoribed as being most promising. A plane-,
tary gear with two Internal tooth, combined with a two-sided overrunning
clutch, is used here. There.ars 5 figurss@
Card 2/2

NOGARSOIJ, 13.
L*19-Yange gas
Ist In blast burners eVIO.Ving external sjjcl,,.
PrPx,,. 7 no.6t33.34 162,
Using a ceramic.grld
-in -forges with gas heating
(jU Ibid. 134
RA l7s6)

XOGAMON B M
@@ . 0
DesIgn of a ps
-fll'ed b9a.rth. Ga..
prom' 10 U098:2" 165.
(KRA 18:9)

!. -. @,@ li - p ) -7

137-1958-1-532@
Translation- from: Referativnyy zhurnal,,Metallurgiya, 1958; Nr 1,p85 (USSR)'@'.
AUTHOR: Koganzon, Sh. M.
TITLE- Standardization and Mechanization of the Recasting of Type Metal
(K. voprosu o normalizatsii i mekhanizateii,pereplavki tipograf-
skikh splavov)
PERIODICAL: Sb, n. -i- in-t poligr.. prom-sti. 1956, Vol 4. pp
95'-103
ABSTRACT: A process manual on the preparation and recasting of type
metal for the printshops of the Ukraine has been developed. The
manual presents a table of grades of type metal, their composition,
in accordance with, GOST (All-Union Standards), and temperature
conditions for recasting. Chemicals to be used in cleaning type
metals of impurities and methods of modifying them in accordance
..with analytical findings are recommended. while measures to re-
auc,e casting waste and other losses ofmetal are indicated.
G.S.
10 Tn* mUl-RoaasUng 2., Type noUl-Pnparation
Card 1/1

85-57712-6/2@
AUTHOR; Umzon, Ts.$ Leaders Model-airplane Builder's Team of.
KhTZ cUldrenis Mlib
TITLE: -Model Airplane Builders of the XhTZ (Aviamodeliety Kh*T'Z)
PERIODICAL: Xr7l ya rodiny.. 1957,.Nr 12., p 6 (USSR)
ABSTRACT: 'A photograph shows two model-airplane builders,, members
of the Children"b-Club of the Xharlkovskiy traktornyy zavod
(Kharskov Traotor.,Plant)o
ASSOCIATIONi Kharikovskiy traktornyy zavod (Khar1kov Tractor Plant)
AVAILABLE: Library of Congress
Card 1/1 1. Photograph

-@j
@ Al"i
@3646
-A
i: 4
.1,006/005/026
B1040201f'
4
VTITLE-
"a 33''
0
0
ku 831C V 1,37 no. 61 1961p 1331-13
'P.
-A
4
N
MA.", a, Ove -a me'dium 'may @bb- de' iinat'
TEXT A -Aesoiipti that
I of
3 ed
'In some a proxlmd@j6-@@'" id. ExpAnsion;and compre esion of
n r
4W
@tfii bubblea`.-are eaorilo6d,, -It4. amics.' :The
At UM
1 equations of hydrodyn
;@'beginAn of 'a if6i
n 4 i,@49,eenti ally on the existence of' 'etrange
e size'of w As
"'t'-pa @eticled ;6`- Iiqui4, th hioh,
@_3 _5' i'n n@clel-are,
cm1w In 'th4,_'m6dsl: VIdo*.-a6' _r tion, cavitat o
naide a
takon to, and to be distributed unif ormly, over.
;.',the entire volu Ahe lnxiol4estble -liquid. with denaityL Qo'@ Cavitation -
bubbles will b t P, o
f rme4 he,,Uquid only -if the pressure U below
. I -I -.. @'-- " 111 or
,_Pressure p, a iuiO4 @O romaN.-Oone'tant, in, the'bubbles with expan-
Dion and.Mprees on, @.b` thi? i@ft i -radial moti
The' 6n.-of 41.1 bubbles obeys,
@,the same as doeoAfie- iotion.'oejk;,@., single spherical cavity with, ccnetant@
ard

S/oiq6i 11 W006/005/ 020
Model, of a cavitating iqA&.-
B.1.04/B201
.,4
interndi ressure-in-,an inx n f '--,4oluii. of Ahe incompressible liquid.
p
-for each individual bubble$
OR 3 dR P
W + T (W)
g'l
Pe
zr
time -F i -and p. :is- the pressure-of'-the
Where R de@
iuth0r: iii-i"' al@l Uid.
uqa A'-i modq@ that miztures of vapor afid'liq
it
-14tter can thqn be des'-
are a hom .ogeneous'.- midi '*it@@;,AL-,iean di4sity., The
Cribed: by
b
rom -!,th s,e two :0-"4" Vio I.. .....
_,@tosiaf@- -e,.t'b derive -the function
q atii6#ii,
2
f(Q) A'W* i '�r
h with the continuity iquation and
p
the equation of onsdrva&6&@;,b i:momeh tei a 'closed @sjsteme
tum,"constitu Of
@,equationz. 'The free energy. F,oan be -def ined- as- f ollows V
IR
F (4)
P.,Rs + (T), S-
V,Card 2@'
T@
7-1

9-2A46
-s/02
61/137/006/005/020
Model 'of -.a ca@ita,ting liquid B 201
%

It is easy on the,b'asia of@,this system,'to generalize the model taking
aocount-of the surface tension@t viscosityt and change of pressure 'in,the
-bubbles.
The linear J*, Steady, iotion, of wliquid. throuSh a tube With local'
narrbwines *is f inal17 .@dealt, withe' If thb. arose section in a 'zone of khis
-tube is larger@than,a,givon minimum cross a th t

' the pressure in
ectiQn 8 a
mi
n
zone will drop to 'below.p rb
: Equations
d
,
dU dP
PU

S ZIN M - QOU40, t(6)
U
Q

Pe
P

@
TOTR17-ROD,

R, V
da dR
OA 3 MR is
j+uR7U7UF- -
p.
hold f or, such.* neo Here$ u-denotes the flow velocity, and q is the
liquid consumpti 0*11 Theae.equations have,been numerically integrated
for

Card 3/5 ,
.

23846
f
/61/137/006/005/020
S/020
Model of a oavitatingliquid B104/B201.
the case of@ the cross' se6ti6tit,_i@ing:ii :NnQtion of x, thus
S 2
(x) k x k,. as Uen-fotind that, beiginning from the initial value
0
R , the bubbles ittain-a. det6imi d @ maximum size j and.subsequently:become

'
-
0
smaller.. The bubble rig': fur
th4iiore 0- display a
tendehey toward a steady
growth. This_-@cojrresponds to the case of a supersonic flow through a nozzle .,

It:has therefor not n possible to,set up%a continuo.us solution at the
e bee
It has been found necessaryto
tube outlet for an arbit.rary-preasuret P2'
-jump-coinciding with the boundary of the region of
introduce a comprea.gion
-ndt ve --of --the .%ompr
davitation. -The,cooid ession jump are related to the
pressure as follows:
le. dS
POU; OAS:
-
-PA+
PX
P
a dx.
gi
'
relation" is obtained
Thie
by,integration.of the first equation of system
.
the' compression ohdak., The ex'pression at 'the
taking account of
(6)1
,
right-hand side.'expressbe the_6nergy lose arising,with cavitation. L. 1.
Card 4
5
:
/

aX* I -
ACCESSION NR.O.A?4030779 S/0020/64/135/004/0779/0762
AUTHOR.-.'Ko a r1k, oB SS
TITLE: One@dimensional nonstationary motion of a fluid with the.
formation and development of cavitation
SOURCE:* AN SSSRI.,Doklady*, v.'155, no. 1+j.1964, 779-782
TOPIC TAGS: fluid cavitation,,nonunifom fluid motion, hydromachanic4:
cavitation; fluid motion
ABSTRACT: The cavitation bubbles formed in@the vicinity of a
vibrator located in water appear, and almost completely disappear
during each vibration cycle. Theauthor discusses the formation
01' a cavitation region in a fluid in the vicinity of a nonuniformly
moving piston under the assumption.that the motion of the cavita-
ting fluid io'described by the system of equations previously
suggested by.the.author (DAN 137v no. 6, 1961). These equations
describe.the:.relationship between pressure, density, and the veloci
of the fluid, and the number and radii of the bubbles (per unit
-follows thatj under certain ausumptionss there in in
volume). It
Card 1 2

AUTPORs ..Kqprko L. SOV/7-591-5-8/14-
TITLEs The Distribution of Alkaline Elements and of Thallium in the
Granitoido of the Turgoyak Massif (Central Urel) -(Rasprodeleniye
shcholochnykh'alementov i talliya v granitoidakh Targoyakskogo
massiva .(Bredniy Ural))
PERIODICALt
ABSTRACT i
Card 1/2
Geokhimiya, 1959t Nr 5, pp 455 - 462 (USSR)
The Turgoyak massif was -not formed by magmatic differentiation,
but by the reaction of a melt the composition of which
corresponded to the leucooratic granite in the oenterl,with
gabbro-peridotitio rocks. The transition from leucocratic
granite over biotite granite to granodiorite is shown by the
integration analyses of thin sections.(Table 1) and.the in -
creasing iron content of biotitee and hornblendes (Table 2)..
The alkaline elements Li,'Na, K, Rb vere determined,'flame
photometrically under the supervision of D. I. Ivanov, Poch-
vennyy in@.t AN SSSR-(Soil Institute AS YSSR), and by V._I. Le-
bedev, Institut geokhimii i analiticheskoy khicii ims V*
Vernadakogo All SSSR (Institute of Geochemistry and-Analytioal.,
Chemistry imeni V. I. Vernadskiy AS USSR).,Tl was determined.@.@@
according to,--the method of N. T. Voskresenskaya (Ref 4)1 the-

Thq Distribution of Alkaline Elements and of Thallium SOV/7-59-5-8/14
in 'the Granitoide of the Turgoyak Mascif Wentral Ural)
author thanks her for her advice in this analysis*. The re-
sults are@given in table 1, and graphically represented in
figure 1. The contents of all elements determined increase
from.leucoaratio granite up to biotite granite and Are,re-
duoed in the case of the transition from biotite granite to
granodiorite. Only Li is an exceptio n in the last case. The al,.
kali.- were transported on in the formation of the maonif';
-thallium is enriched on the surface in consequence.of its
greater mobility: in the center the Rb/TI ratio is reduced in
the leucocratio granite from 180 to 70 in granodiorite. There
are I figure, 3 tablesp and 13 references, 10 of vhich are,
Soviet.
ASSOCIATION: Moskovskiy gosudarstvennyy universitet im. K. V. Lomonosova
(Moscow State University imeni U. V. Lomonosov)
SUBMITTEDs January 5, 1959
Card 2/2

i- .I- .- @

gim, okh@@-j
MIA,

IIIIASHKOp V.M.; K(*Ap
Incluo4na in the aPatite"'Of tbO Xhibirq and Lovozero Massifa.
Dokl. AN SSSR 166 n0011202-205 ja v66.
Is Institut g OCRA .1911)
eokbWl i analitichookoy-khimij im. V.1-Vernadakcqto
AN SSSR-, SubmittOd -TU3.y 20# 1965s,

KOOARKOj L.N.
Distr'batiOn Of flUOrLnf in rophll.. Vrtt,4S'Pf the Lovoswo razw1ral
Old
(Kol&.p r'sula)- ft.dddgiL PO-40M329 162, (XOU'26t?)
16 Vernad*,r Institute of OgODbwdstrjr and AnalyUORI,
AcadmW of Saiefteg VOSSSORS) moveow, Mmistry,,
Tundarp-41opholine syeat.)
(Lovosero

RTABCHIKOVO I.D.; KOGARKO, L.N.
-Effect of anion subs ution on the acidity of xagmatio meltse- -
Gookhimlia no.3005-311 Mr 063. (MIRA 160)
1. Institute of Geology of Ore Deposits, Petrology, Mineralogy
and Geochemistry and V.I.Vernadsky Institute of Geoohwdstry
and Analytical Chemletry, Acadsvq of Sciences of the U.S.S.R,j
Moscow.-'
(Anions) (Magma.-Anoyaia)

0-k! - -1 - V. 1 11 1 ILI '10
0111 A a If r
"Old
PC 7'
Va. It. ret'dowirb. Dewy .4W.%04-"-V1k is, 19.8 to 5MA010 11. Is the ubk 1vhTS
00 1A, a(Va"). --mudift of detonatka in wi& tubes 'we" datematJon woo *bon from 13 to OU.&% it. ppor an
sismIr wf4h the sAijft-t of Imming pwm about ib" iutwr of tmuts. from 26 to &n if the revort" pmwv Was I*
00 the ws"fnmat. 'nkv*vtkut good sigi - I with tU @;@ caled. One this ~I=
00 AO*W th4t by ow 44 lator (14bro If nm&wts hy wwome 44 The VlAvsksl tbwy of detokwimo-,[ *0.0
be pow*& to Gle""to volits. that bisd Owk 0 Wfttw"M the Wow limit. the mamound v v w WASS
60d tim appm. a tknro the raw - Value AM now the Upper wom 0
for cbm. nwtiod that they wmkl mot detaute in umm *111
004 tubes. Thc.Kpp. comkttd of steel tubts 305 ma. Is in- dwammasurvdpowpourew"Alsom- vOlvesslawascalw,
tem 41 416m, awl 13 2 w We --A with a For"WAts.-
holum"W101"WW *Ttw,l:tqmolirtwwwinltgkrtatidn:t% WO StOkbion"uk-'be tkw 1mas "W 41 th*
god a MI 1, Omfif tv! wilAuxive, TW lobif t1inmi. on# 10 to 1"141- 11W awk wavv unto
%0@ w mmaias to 14 mookis" In tv"Wilm WRIF tm mimmme
tiou studimm. The uw of The *Wit tubes bk*reA*J The tWw 44 tbw strain pp, wbk,b44 about 0.1 WOW- FIRLI,
wy vi%-h t"kito., the "Why of rawtift 110, to 0
of H evorms. in If-mir w6u. am which detautift my k" 09 v reommea two w ths 000
be Obso ved, I* narrow ubm, Adomb" wings. courparew with tbir ;w
*Uuw t SMIN d
In In" bo
the pressure d the remcdom products. Colt. a
dewpoom wa*me
the ibcoy for sonad
also dgUmm" We"s (z
C.A. JS 031) mW WW
.41. 19011) *Pwvd th-t 10 11tilft case Ow Uvgu 41 Zm;@ft-
"Itudw- and lbs Ms. reaction thma at do
wd with
O"AUSKICAL Lnl*Atb" tLAIWICAt"
alits, *9 4.v, all
A A i I bi a a 0 1
_0 00 0 0-1111-411 0-1111 0 -69-0-0-0 0 0 OAR-1111 -6 6,
t w - - Wev
19 00-00 90,0*00 0 0 0.000 goo 90016AL MkAL -91-A

MR - IPT

fri PER

.
@: , t,@m ms - `--?j
- 1 - " -
fil I -Z,,F;, R, K - ,
, M 14-1
,R&

AUTHW- WARNOP-boXi-P PA,
TITLk; 1"D tigazion of frossureDus to Fuel-Oxygen Mixture Detonation by.-
tTt3
tholMetkod of,-tko "Pirow of.rivot",
(Isslodevantyi cblivieiiji @@iwtodoi 'otlotVashcaege sterskiWa pri -
detoa&tsii'i*idA~oi-k:Lslo'rediyki '_ Russian)
ARIODICAL fturnal-Tokkne, FIz*,,.1957t Vol 27, Nr 4o pp 033-Wo (U-CsoueRO r
Received. 5/195T, Reviewed 6/1957
ABdTWT In order to obtain new,dats. on the mount of pressure In
wave #a the oca"ien. of.tko detonation of gaseous explosion mixtures.
the method doyeloped by Hspkluss Be (PhiloTrus.Royed"op At 213) 437P
1914) was applied with, a few modifications and Improvements. The basis
of this methods the experimeaLal plastpthe pressure gang* aid tke so-
tked of calculation are described. The rise of the red as well as.the
mount of motion sonvoyed by.tho rod and the average pressure daring
the time the skeek wav* see& to *ever a distance which is twit* a long
as the thrown pivot areAstersised according to the maxims deviation
of the thrown pivot I in the souse of -the experiment. Reflosties * pressirs
was. investigated istbe ease of detonations of fael-oxygoa aixtureal,
methme-oxygen- an well as "tkans-
w7gon-mitrogen-aixtures, The experiments show that in the ease of a
detonationof fuel-oxygen nixtures a zoa* existo is-the detonation wav*
in which prissurw;is higher than the pressure in the ftige-point, of
Card 1/2 the explosion produstas Ths maxisam values of reflection prossue.im

AUTHORs Koga SOT/57-08-9-27/33
TITLEs Investigation of the Tube End Pressure in affon-statiaosa PLev
Combustion. (Issledovaniye davleniye v tortse truoy pri
nestatsionarnom byatrom gorenii)
/Vol 28,
PERIODICALs Zhurnal tekhnicheekoy fizikil 1958, Nr 9, pp. 2041-2045 (USSR)
ABSTRACTj This is an examination of the pressure versus time function
found at the.front of the tube in the case of a non-steady and
.
a fast combustion of a propane-air mixture. If the initial
sure P . I kg/cm 2 the maximum pressure at.the front of the tube-,
2
reaches P w 470 kg/cm . When the previously oompressed mixture
is ignited the maximum pressure developing at the front of the
tube considerably,exoeeds the reflection pressures obtained by
an explosion of the same power fuel mixed with oxygen, which
.may be the case when the shook wave is reflected in a non-steady
fast combustion of a power fuel-air mixture. There are 2 fig-
ures, I tablet and 3 references, 3 of whioh are Soviet.
ASSOCIATIONs Institut khimicheskoy fiziki AN I.888R) Moskva (Institute of
'
CwrW*/-2 Physics IS USSR"Moscow')
Chemical

AUTHOR.- Kogarko, So. SOV/57-28-9-31/33
-TITLEt
stonation of Air-Methane Mixtures and the Dethtiation Limits-
of Hydrooarbon-Air Mixtures in a Large Diameter Tube
(Dotonatsiya metano-vozdushnykh amesey i predely detonataii
uglevodorodo-vozduohnykh smesey v trube bol'shogo diametra)
vol. 28
PERIODICALs Zhurnal tekhnichaskoy fizikio 1958, Hr 9, pp. 2072-2093.(USSR)
ABSTRACTt In this paper the problem is approached of the relation between
the velocity of the chemioal reaction in a gae,mixture in a
detonation,wave and the heat lose in the reaotion.zone.on the
one'hand and the propagation velocity of the detonation wave
and the detonation concentration limits on the other. This
problem was first investigated in papers by research workers of
the laboratory.of combustion processes of the association men-
'
tioned at the bottom of this paper.
The experimental equipment.,
which was used in the experiments-is described. It was built in
the.course of the study.The experimental evidence leads to the
following conclusions: 1) Methane-air mixtures can be detonated
a tube with a large diameter (305
MM) in a wide range of methaw
L
,
concentratione.The limit concentrations at this diameter ares
Card 1/3 a) lower limit 6.:3%'of CH4 in airp b) upper limit 13-5% of CH4
0.

BOV/57-2R-9-31/33
Detonation cfAir- .Uethane Mixtures and the DetoZation IdMitO Of
Hydrooarbon-Air Mixtures in a Largo.Diametor Tube
in air. 2) It was found that a) methane-air mixtures do not
detonate in a narrow tube (20 mm) at an arbitrary methane con-
tent within the limit detonation concentrations. This does not
occur even if a strong shook wave is injected (which is pro-
duced by:the explosion.of the detonator cap Nr e in the mixture).
b) A-wave@propagating in a steady state in a wid'e'diameter.tube.
is destrojed when it pauses into a tube with a smaller diameter
containing the same mixture. This tube may be attached in
parallelor in series to the large diameter tube. 3) It was
substantiated experimentally that the limit detonation con-
centrations and the possibility-of a detonation in gas mixtures
with a-slow chemical reaction is dependent upon the tube di-
ameter. This phenomenon.is explained theoretically. 4) It is.
shown that the detonation limits of gasoline and of benzene-air
mixtures in a large diameter tube the limit concentrations are..
considerably widened in comparison to those determined for 20 mm
diameter tubes. A benzene-air mixture detonates under the pre-
vailing experimental conditions in a concentration range spec-..
.ified by, the composition coefficient a varying from.00 to 102'1..'@.
Card 213 There are 8 figures, 2 tables, and 16 references, 9 of which

SOT/57-28_9_31/33
Detonation of Air-methane Mixtures and the Detmstlon Ludts 'of
.Hydrooarbon-Air Mixtures in a Large Diameter Tube
Soviet*
ASSOCIATIONs Institut khimicheakoy fiziki AN SSSR Moskva (institute of
Card 3/3

AUTHORS:
TITLE:
PERIODICAL:
ABSTRACT;-
Card 1/3
Kosarko --S. U.Ijkobelkin, V. 1.
Relaxation Interaction Between Shook Waves and the Combustiun'@:
Zone (Belakeatsionnoye vzaimodeyetviye udarnykh voln s.soncy
goreniva)
Doklady Akademli nauk 88SR9 19581 Vol 12o, Nr 6,
-pp@ ,1-2Go,,--'1283 (USSR)
The paper,under review presents an investigation of the-in-
fluenow-of the-kinetics of,the oombustion-upon the structure
and the intensity_qf@a shook wave'when it passes through'.the
comb-ustic'.n. zone0 The relaxIatIion time.t (the perio'd-during
r
which no.noiioeablo! infl4ence is exerted upon the diffusion
currents an&lbe'@beat,ourrents in the reaction'sone .by the
reaction conditions suddenly modified by Ithe shook wave) 14-of
the'same order as the reaction period Z (lio-3.- jo-5 sec).,t@
is defined ae'the ratio of the width of the combustion zone
and the normal expansion velocity of the flame. DuringIr
the.tomperature,and the pressure within the reaction zone. In-,
crease. During the relaxation time-the excess momentumin'tho.

Relaxationruteraction Between Shook Waves and the SOV/2o-12o-6-3.2/59
Combustion Zone
reaction zone is transformed into &.shock wave propagating
forward-and backward from the reaction zone. Equations giving
the state in-the shook'wltve'are written down. The whole amount.
of heatliberated in the passage,of the shock waveis expended
for the increase of thelinternal energy of the gas In tho-
reaction zone. V b denotes',the' duration 'Of., the,paosage of the
shock wave through the combustion zone. if Z >/,rb the reaction
is not completed during.,the-passage of thewave through the
front of the.flame and only a certain proportion of the
chemias ILl energy which is expended for theAncrease of the,
momentum of the wave is Imported-to the wave.'If'r< the,
reaction is completed within the periodIr :. The total komentumil-
of the.ehook w'ave.after pasiing'the combustion zone io'combinod.
from the interest mbien'tuml and.the relaxation momentum I.
The maximum amplification''of the momentum of the Shook wave it
b may be termed momentum resonance. Finally a method for
Card 2/3 the.determination of the'index of refraction is presented.

@Relwcttion. zntertdtion@ "twoon Shook Waves and the BOT/2o-i2o-6-32
combustion Zone
There-is I figuree
..ASSOCIATION:-. Institut kbimioheekoy fiziki Akademii nauk SSSR (Inatituie of,
Chemical1by .sion, AS. USSR).
PRISENTEDi March 6p 1.958t by N. X. Semenov# lembero Academy of Solenceso.
USSR
SUBMITTEDt February 25v,1958
1. Shook waves--Analysis 2, Combustion-Anakysis 3. MthemLt!aa,
--Applicatims,
Card -3/3

5(4)t 10(7) SOY/20-122-6-25/49
AUTHORS: Kogarkop S i Skobelkin# Vs Ia, Kazakov, A. N.
TITLE: The Inieractlon'@Betveen Shook Waves and the Front of,a Flame
(Vae4modeystviii udarnykh voln a frontom plameni)
PERIODICAL: Doklady-Akademii nauk SSSRI 1958vVol 122, Nr 69 Pp 1046-1048
(USSR)
ABSTRACT,. The present paper Investigateethe intensification of shock
waves in their interaction with thefront -of a flame by
variation of the'normal combustion proceso in the shock wave.
The length of the shook wave is assumed to be sufficient.
in'ihe direction of the reaction zone. For the interaction
between such a shook wave and the.flame front the following
applies.. 1) The shock wave is transformed at the flame front
(like on the boundary dividing two media). In this-way a re-
fracted4nd a reflected wave are formed. The flame front can
.by approximation be -considered to be a contact-discontinuity.
The expreesioni-f6r the refraction coefficient are written'
down# 2) When passing through the flame front the shock wave
compresses the gas in the reaction zone, whereby temperature
'Card 113 ,rises. This temperature rise increases reaction velocity'.80

-sov/20-122-6-25/49
the Interaction Between Shock Waves and the Front of a name
that the propagation velocity of the flame is also increased.
This propagation,yelocity Increases v6ry.rapidly, and, there-
fore this process may be looked upon as a sort of explosion
in the gas current behind th -a shook wave; it causes the forma-
tion 'of 2 additi*onal (intensifying) o'hock-waves,'The shook
wave front movee'vith subsonic velobity in relation to the
disturbed gas, and,therefore. any kind of disturbance is.able
to catch up with'Ahis front in the current behind the' shook,
front, thus changing its structures The propagation velocity
of.the flame is not increased immedlately upon arrival of the
shook wave# but only after a certain relaxation time. The
'latter is of.the.same order of magnitude as the duration of.
reactioni A diagram schematically shows the intensification
of the shook wave when passing through the-flame'front. Rx-
preasions for shook front oalculation are given* The now pro-
.pagation velocity of the flame is calculated 'according to
the theory developed by Zolldovich.'The amplitude of the
intensifying.shook vaye,depends upon the amplitude of the
initial shook wave as well as on the kinetic'propertie,, 're-
,action velocityp calorific value, activation energy, etc. ) of-
Card 2/3 the fuel. The second diagram shows the amplitude of the inten-

- ------- ---
SOV/2o-122-6-25/49
The Interaotion.Between $book Waves and the Front of a Flame
sify#g shook wave-of oomprepsion in the reaction zone for
,2 differ4#t-p';OpggqL~tgn-yo;goities.-There are 2 figures and
5 Soviet,:rQfer$AQQGq
ASSOCIATIONt InstiAui khinioheskoy f*;ik* Akademii nauk SSSR
(Institute for Chemical Phypios-of the Aoademy of Sciences,
USSR)
PRESE.RTED: June 21 p, 1958ilpy Vk-' 9Kondiatlyev, Academician
SUBMITTED: June Ill 1956
Card 3/3
A
N
MZ
M.

0 0
10(2); 24@8) PHAPH I BOOK ZXK4.OITATZON POV/2541
e- Akademiya nauk SSSR. Enereatichaskiy institut.
Goreniye v turbulantaom potokel diskunsiya p& obshchamosXovskom seminare po
goreniyu pri energetichaskom institute AN SSSR (Coubgstion In 1W-bu2sat
Flow; a Discussion in the All-Moscov Be"r at the Paver Engineering
Institute, USSR Academy of Sciences) Mopecyll Izd-vo AN SSSRO 1959. 167 p.
Errata alip-inserted. 2,000 copies print/4d'o
Ed.: L. N. Khitrin, Corresponding Member., USPR Academy of Sciences; Edo. of
Publishing Houses. R. I. Kooykh and X. M. Knoroz; Tech..Zd.: P. S. Kashina.
PURPOSE: This collection is intended for renearch scientists in the fields
of thermodynamicsand fluid mechanics.
COVERAGE: The collection contAing six papers which present the results of
experimental and theoretical research on combustion p)wnamena under conditions
of-turbulent flow.

Combustion in Turbulent Plod (Cont.) SOV/2541
TABIZ OF COMENTSt
'Preface 3
Shchetinkov, U.S. On the Calculation of Fla;w Pzvpaption in A
Tarbulent Flow
49
This paper presents a theoretical study of flame propagation in a
turbulent flow based on a.model of turbulent combustion which assumes
homogeneous reactions within turbulent mol@s (modsi of microyolume
combustion). The meth9d of calculation pormits a qwwtitative numer-
ical analysis of the effects of various fuel-mixture and flow pers-
meters (initial temperaturet prejeure, velocity, turbulence, etc.) on
such combustion chareateristico as flaw veloqity,, wi#hlof combustion
zone, and stability of the flame ton4m, Vader conditions where the
microvolume-combustion modelis roalized., the calcul4ted results are
in reasonably good qualitative Agreewnt,wilp; expertmeA.

Combustion in Turbulent Flow (Cont.), JW/2541
V3Aooyj, K. P. Experiniental. lnva#ip@lon of the Combustion.Zone pf a TuXbule;t:
Fume (Supplement to le-So Shaba UuWlls Report)
This paper gives.datails of #e't*st ;etup qnd som @vsults of an experi-
mental study of the combugtion pqrM $A a #F@ujjp% The test method
was based on 4=11-lag measuraments of tha, ioniW m;mnt and the temp-
erature. Experimental data Ion the diOributiona of the tonlrwd current and
the temIperatu;e are given aA4 the W464ma OatiWO1@1 o@aractqrlstics of
these quantities are presented as functions of +Mmi dep@h pf @he combustion
zone and the flow velocity.
_k_axka-,__ @- On the Model for Combus#on, iq % TurbuUn@ Flow 58
On the basis of the Du&Aahler-Shobalkin, #
,Mthelis, thiq papap
considers the mechanism of the cop1bustjoij 'of A haxpgansous mixt4m
in turbulent motion in the cross section of a tube. Tba qtabilILT.-
ation, of the flaw tongue is achiavqd with the aid of A pilot -fla.w
The author questions the validity of the model of combustion proposed
by Shchetinkov In the first paper iq this coLlection.

SOV/24-59-2-2/30
AUTIHORS Basevio h V. Ya. Chgarko S. M. (Moscow)
TITLE: The Structure of Turbulent Rlames of Homogeneous and Hater-
ogeneous Mixtures (0@strukture turbuleritnogo plameni, gomo-
gennykh i geterogennykh smesey)
PERIODICAL: IzVesti7s, Akademii nauk 8138R Otdeleniye tekhnicheskikh
nauk, BnergetikaA avtomatika, 1459, Nr 2t PP 13-20 (USSR)
ABSTRACT: It is known that unreacted fuel can be detected in the
jet,of a turbulent flame, and-even in the products of com-
bustion. This supports existing pictures of the possible@
mechanism of turbulent flames forAnstance the surface
model (Refs 1. 2) but insufficient quantita'tive evidence
is at present available. The purpose of the paper is to
study the temperature and concentration of the fuel and@the
velocity of combustion in turbulent flames, thus pe=itting.
an approach to.the problem oftheir structure. Theappara-
tus (Fie 1) consists essentially of an air heater (1) a
tube (2) in,whieh the fuel-(benzene or kerosene) is 2.xed
with the air,@a combustion chamber (6) and a burner.(7);
the amount of vapour phase was measured by a special devioe
9-16), With this apparatus the completeness of combustion
of homogeneous mixtures was measured as a function of
Card 1/3 the length (L) of the combustion zone; I is defined by
it. 10N@*; R"-- IV4P

SOV/24-59-2-2/30
The Structure@of Turbulent 71ames of Homogeneous and Heterogeneous
Mixtures
the equation
0
where 0 is the initial concentration of benzene and C
0
,is the ooncentratio*u at agiven point. vIn heterogeneous
.mixtures, the completeness of combustion was studied in
relation to the dize of the drops of atomised fuel. It
is concluded that with homogeneous mixtures at 1 atmosphere
pr'essure and temperature 4, 12500 there is a change of fuel
concentration and a corresponding increase in the products
of combustion with a conversion time