SCIENTIFIC ABSTRACT KRZHIZHANOVSKAYA, G.V. - KRZYCKI, Z.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000826920017-6
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 99
• Document Creation Date: November 2, 2016
• Document Release Date: April 3, 2001
• Sequence Number: 17
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

SHAR V, Ivan Aleksandrovich, akadenik; OZEROV, T.N., red.; UZHIZHA-
NOVSXATA,,G.V.; ZUBRILINA, Z.P., takhn.red.
(Operation of hydraulic land-improvement systems] Xkspluatataiia
gidromellorativufth sistem, Izd.2., Ispr. i dop. Koskva, Goo,
isd-vo sallkhoz.lit-ry, 1959. 576 p. (MIRA 1238)
(Irrigation) (Drainage)

red.; FRQKOFIUVA,
IIOGOVSKIY# Tadeush Timofeyevioh;.qMIZ4A_Nq A
L.N., takhn.red,
[Practical work in the mechanization. organization, and execution
of hydraulic engineering operational Praktikum po makhanizatall,
organizateii i proizvodstvu gidrotakhnLoheskikh robot. Moskva#
Gos.izd-vo sellkhoz.lit-ry, 1960. 282 p. (KID 1319)
(Hydraulic engineering--Study and teaching)

KALABUGIN, Aleksondr Takoylevichp prof.; K;RA&W, Sergey Iustinovicht
doteent; rRZH ZUROYSLAU, G.T., red.; 0010TA, Z.D., tekhn.reds
EAgricultural water supply pnd 1" improvement] Sel'skokho-
zielptvannoe vodoswbshonld i molloratelia. 10.2., perer. I dop.
Moskva# Gos.And-vo sellkhos.lit-ry, 1960. 342 p.
(Water supply, Rural) (MIRA 14d)

XRZHIZH"OVSKIY. G.M.
Study, think, work and be daringi Zaan.alla 35 no.4:4-5 Ap 160.
(MIRA 13:p*
(Irxhizhanavskil, Glob Paksimillanovich)
Mucation of children)

KRZHIZHANOVSKIY, G.M.
Planning and standardizing. Standartizataiia 29 no.8:20-21 165.

FEREFELKINA, M.D.,, nauchMy notrodnik; GUBINA, R.S.,, napchW aotrudnik;
Prinimali uchastiyes SHULESHXOt I.S., kand.tekhn.nauk;
_41ZHOM K.Z.; DOROGOT, Te.V.; LITICHEISKIY,
_R9 Kly N.V.
Effect of certain factors-on the oharacteriotice of nonwoven
fabrics manufactured t7 the-knit-and-stitch method. Takat.
prom. 22 no.12AS-52 D 162. OaRk 161l)
1, Nauchno-looledovatellekly-Inatitut takatillnoy promyehlen-
nosti Leningradskolo soveta-marodnogo khozyaystva tfor
Perepelkina, Gubina). 2. Naeh&llnlk pryadillnogo sektora
spetnialinogo konstruktorskop Ivwo tekstillnoy promWahlennood
Ladngradakogo soveta narodnogo-khotyaystyl (for Shuleahko).
3. GlavW insh. tokatillnoy fabrikilm. Nogina (for Irzhl-
zhanovskly). 4, Stara~ly Inzh, spetWallnogo kono%rWctorskogo
b7uro trikotashrqkh mashin Ceningradela:~go, soveta narodnogo
khozyaystva (for Utic~pvekly).
(Nonwoven fabrics)

BERNSHTEYNp M.Kh.1 YABKOv Ya.M.; ZAYONCIIKOVSXIY, A.D..; KRZHIZHAIIOVSKIT 9,00;
Z114YATIN, K.K.j EnNSHTEYN, Ye.5.1 BARKOVA., L.Vo; PROKURAT, ".-.I
VTOROV, G.N.
Artificial.leather with a nomoven base. Kozh.-obuv.prcm. 5 no.4i
18-21 Ap 163. (MIRA 160)
(Leather, Artificial)

BOBIN, K.P,; GMASIMOT, N.S.; GOLUBAT, S.G.; DIMIDOT, P.G.; DAMILUMO# M.P.;
177MSMIN, N.M,; ZJMSKIT, R.I.; KAWMIKOV, K.A.; KONCHAYV# B.I.;
KORCM, A,I.; KRZHIZHANOVSKIT, P.I.; XULAKOV, G.M.; PCLOSUICHIN, M.N.;
ROTDM, M.Ta.j MNTBffMff#-T.-r.-;-MMUSMN. B.V.; SMUROVO A*No;
TAWOV-.WAKOVg, Na.; TOKASHU, A.I.
Semen Thaillavloh Kallaev-, obituaz7. Pozh. dolo 4 no-5t29 NT 15B.
(Kallasy, Semen Vasillavich, 1904-1958) (MIRA 11:5)

AUTHOR: Krzhizhanovokiy, R.Ye. 32-8-17/61
TITLE: Perfection of the Method for Simultaneous Determination of th*
Heat Conductivity and the Current Conductivity of Various Types
of Steel (Usovershonetvoyaniye metoda odnovremennogo opredeleniya
teploprovodnosti I elektroproyodnosti staley).
PERIODICAL: Zavodskaya Laboratoriyap 1957t Vol. 23, Nr Ot pp. 925-927 (USSR)
ABSTRACT: In the Central Institute for Steam Boilers and Turbines (no place
given) a new apparatus was constructed according to the Kolraueh
method which permits the simultaneous determination of the thermal
and current conductivity of heat-resistant steel alloys (?band 6).
The two values are determined on the basis of an investigation of
the temperature distribution and of the potential of the sample
which is included in the circuit. The initial formula Is;
a dv)3 t;~d2t _ a(t _ t ) a 0. where 3 signifies the surface
(N-
dx2 8 op
of the cut of the sample, t - the temperature of the sphere,
a - coefficient of heat varfEtions on the surface of the sample.
The solution of this equation yields the characteristio of the
Card 1/2 newly constructed apparatus which was recently perfected. The

Perfection of the Method for Simultaneous Determination of the 32-8-17/61-
Heat Conductivity and the Current Conductivity of Various Typea of Steel.
principal scheme of this apparatus is given. The process of
determination takes 2 hours. The construction of the apparatus
is adapted to the determination of the ), and a values of cylindri-
cal samples (loo mm, in length and 4-6 mm J) or tubes of the cam*
dimensions. Cast steel of type A IT was here used as sample.
ASSOCIATION: Central Institute for Steam Boilers and Turbines (Tsentralonyy
kotloturbinnyy inatitut).
AVAILABLE: Library of Congress
Card 2/2

17't'r-CL
KRZEIZEMOVSKTY, R. Ye... Motor Tech Scl (diso) -- "Mathcxia and results of
Investigating the thermal conductivity, electrical conAmetivity, and Tpmntz
constant of rofractory alloya". Wacow, 1958, 12 pp (Min Eligher Educ USM,
Moscow order of Lanin Power Tnat), 150 coPien (KL,No I~ 1959, 119)

111sho
r
Beat conductirity of sustonits steel, Bus rgoma shinostroonis
no.11144-46 1 158. (MIRA 11ill)
(Anstonito)

AUTHOR: Krzhizhanovskiy, R.Ye., En6ineer. 96-1-12/31
TITLE: The Dependence of'We Thermal Conductivity of Certain Heat-
resisting Alloys on Their Condition and Heat Treatment.
(Zavisimost' teploprovodnonti nekotorykh zharoprochnykh
s.plavov ot sostoyaniya i tormicheskoy obrabotki)
PERIODICAL: Teploenergetika, 1958, Vol-5, No-1, PP. 44 - 48 (USSR).
ABSTRACT: The experimental equipment, illustrated in Fig.1,
employed Kohlrausch's riiethod, which is bac-ed on the investi-
gation of the distribution of temperature ai)d potential in a
snecimen carrying electric current. The formulae used in the
calculations are given. The sample viac a cylinder, 5 mm dia.
and 100 rm long; measurements were reade on a length of ?0 mm.
The specimen was in an evacuated protective cylinder, provided
with heaters.
The accuracy of determination of electrical conductivity is
better than 1%. The scatter of data on thermal conductivity
,-,jas usually 1 - 2%, and did not exceed 3%. The correction for
lateral beat exchani.e did not exceed 3 - 51jo' of the axial heat
flow throueb. the specimen. The investigations were, for
different alloys, made under the came conditions. Table 1
gives experimental data for a number of steels and alloys.
Cardl/4 Test8 were made on alloys qlT, Dt4-606 and W-572. The analyses

96-1-12/31
The Dependence of the Thermal Conductivity of Cert4in Heat-
reuisting Alloys on Their Condition and Heat Treatment.
of these and the other alloys lnvesti6uted are given in Table 2.
The results of tests on alloy qlT are given in FiC.2A and
those on 3L4-606 in Fig. 2B. The influence of aeeinZ on the
thermal and electrical conductivity of the alloy was studied
on specimens of steel 3~~-5?2 held at about 700 OC for
4 000 hours; the results obtained are given in Fig. 3. The
alloy has the least thermal conductivity in the initial
hardened condition because most of the alloying elements are
present in the form of solid solution; a photomicrogra8h is
in Fig. 4a. If the metal is aged for 500 hours at 700 C,
there is a fairly marked increase in thermal conductivity,
accompanied by a change in microstructure, as show& in Fig. 4b.
When the specimen was held for 2 000 hours at ?00 C. the
thermal conductivity fell somewhat conVared with the value
after 1 000 hours. Increase in the tire to 4 000 hours causes
a further increase in thermal conductivity.
The influence of heat-breatrent on tLe thermal and electrical
conductivities of nickel-base alloys, and particularly steel
D.+G-07, via', then considered. The effect of the hardening
uord-'al/4temperature on the thermal and electrical conductivities was

96-1-12/31
The Dependence of the Thermal Conductivity of Certain Heat-resisting
Alloys on Their Condition and Heat Treatment.
examined. At a temperature of 550 - r50O OC, alrost all speci-
mens of W-60? have a minimum electrical conductivity. F~g-5
shows graphically that ~f the steel is hardened at 1 000 C and
then maintained at ?00 C for 2 hours, the thermal and elec-
trical conductivities scarcely change.
Further results of tests made on samplea subjected to compli-
cated heat cycles followed by long periods at high temperatures
are given in Fig. 6. The influence of the ageing temperature
on the properties of the alloy is given in Fig. ? and is seen
to have more influence on the thermal than on the electrical
conductivity.
Allog N-43?, which is also nickel-based, was maintained at
550 C or periods of up to 2 000 hours; the resultant elec-
trical and thermal conductivities are shown graphically in
Fig.8-
It is concluded that for steels 9JlT, 30-606 agd W-572, the
state and low-temperature heat-trt,-atment (340 C, 000 hours)
have no appreciable influence on the thermal conductivity of
18/8 tyBe steels. On the other hand, holding hardened steel
at 700 C affects its thermal conductivity. In the case of
Card 3/4

96-1-12/31
The Dependence of the Thermal Conductivity of Certain Heat-resisting
Alloys on Their Condition and Heat Treatment.
alloy -D%A-607 and Wr437, soaking at 700 - 8500C has little
influence on the conductivity. The mechanism of ageing is not
the same in 18/8 type alloys and in nickel-base alloys; there-
fore, the influence of soakinE on the thermal conductivity is
different. There are 8 figures.
ASSOCIATION: TsKTI
AVAILABLE: Librar7 of UonEress.
Uard 4/4

AUTHOR; Krzhizhanovskiy, Ro Ye. 57,1-27/30
TITLE: On the Lorentz Constant for Steels (0 postoyannoy Lorentsa d1ya sta-
ley).
PERIODICAL: Zhurnal Tekhntcheskoy FIzIlcis 1958~ Vol. 28) Nr 1. ppe 202-~206 (USSR),
ABSTRACT: The irriestigation, of the influence of temperat,,ireo and of the struce
ture of steels and allo". on the quantity L (Constancy of the ratio
L -1/6T according to the Wiedemann-Franz-Lorentz Rule) was carried
out on a plant working according to the improved Kohlrausch method*
In order to achieve more genoral and more complete results not only
the own but also all other reliable data on beat and electric conduco
tivity of other scientists were used. The dependence L a f (t, strueo
ture) was determined according to the.X and G - f (t, structure)-cur-
veso The complicated character of the complex influences of the ad-
mixtures on the conductivity of steel was taken into consideration
and the data availtible were iised in different ways. The results of
the utilization of experimental data are given for three steel groups
(carbon steelo, chrome steels, and chrome-nickel. alloy3). iurthermores
it is demonstrated that the investieation carried out by Powell
(reference 1) (that heat treatment causes equal change of heat and
Card 1/2 electric conductivity) Is nat correct, The Irriestigation carried out

On the Lorentz Constant for Stehli. 57-1,-27/30
here FToved the contrary. The results of these investigations are gia
von. The following is stated conclusivel~i: 1) The Lorentz Constant
L for steeLs in a quant1ty depending on the temperature and the 3truc-
ture of the 3teel. In this connection the deppndonce varies with the
different steel groups, 2) The quantity L depends on the structure
of the alloy and represents a function of its heat treatment# The
work was carried o-A in the TsKTI In the laboratory of professorj doco
tor of technical sciences S30 Kutajoladze.
There are 3 figiires, and 5 referenceso I of wliich is Slavic,
SUBMITTED: January 25, 1957-
AVAIIABLE: Library of Congrei;e.
Card 2/2

5/114/60/000/010/007/007
E194/E484
AUTHORs Krzhizhanovskiyj R.Ye., Engineer
TITLE: Methods of Calculating the Thermal Conductivity of
Various Classes of Steel
PERIODICAL: Energomashinostroyeniye, 196o, No.10, PP-37-39
TEXTi There are a number of meth d for calculating the
thermal conductivity of carbon.steels,7d:veloped by various authors
on the basis of experimental data. The calculations usually
necessitate experimental determination of the relationships
between the electrical conductivity of steels and temperature.
However, for a number of Important classes of steels there is no
way of assessinS the coefficient of thermal conductivity. The
material obtained from work at the Central Boiler-Turbine
Institute, which is described in this article, fills the gap to
some extent by providing a unified method of treating the most
reliable experimental data to determine the coefficient of thermal
conductivity of carbon, low alloy and chromium steels and also
steels of the austenitic class including chrome-nickel steels.
Thermal conductivity coefficients were also calculated for a number
of grades of steel of various classes. Thermal conductivity of
Card 1/05

s/114/60/000/010/007/007
E194/E484
Methods of Calculating the Thermal Conductivity of Various
Classes oX Steel
steels is influenced by composition, temperature and structure.
The influence of alloying elements is best assessed in relation tc
their content by volume in the metal. Accordingly, the methods
of calculating the thermal conductivity coefficient given inthe
article are all related to the voiumetric composition of the
steels and to temperature. The method has been chocked against a
large amount of reliable experimental data. The tontent by
volume of alloying substance is calculated by the formula
V gi AFe (1)
Ai
V - the total content by volume of admixtures,
gi - the content by weight of the particular element in the steel,
A - atomic weight.
The atomic weight ratios AFe/Ai -for the various elements usually
contained in steel are given in Table 1. The method of
calculating the thermal conductivity of carbon steels is valid for
Card 2/5

S/114/60/000/010/007/007
E194/E484
Methods of Calculating the Thermal Conductivity of Various
Classes of Steel
annealed steel with alloying component contents by volume of
0.2 to 7% over the temperature range 5 to 5000C. For calculating
the relation between the coefficient of thermal conductivity, the
composition and the temperature, the following equation is valid:
X = K(6-35 - + 28. kcal (2)
100 m h -C
The values of the coefficient X which depend on the quantity of
admixtures of the steel are given in Table 2 for values of V
between 0.2 and 7%. Calculated values of thermal conductivity
coefficients as function of temperature and amount of alloying
agent for carbon steels are given In Table 3, the method in
accurate to within 5 to 7%. The thermal conductivity of low
alloy steels can be calculated by means of the equation:
(2.56 - 0.29V) (6.35 - t + 28.8 kcal (3)
100
Card 3/5

s/114/60/000/010/007/007
E194/E484
Methods of Calculating the Thermal Conductivity of Various Classes
of Steel
Values of the thermal conductivity coefficients of low alloy
steels as a function of temperature and composition are given in
Table 4 whilst Fig.2 compares calculated and experimental data;
it can be seen that the method is accurate to within about 10%.
The method is valid for annealed chromium steel, it is assumed
that the total content of carbon, manganese and silicon is about
2% by volume. The relationship between the thermal conductivity
of chromium steels and the volumetric content of chromium and the
temperature is given in Table 5 whilst the graph of Fig-3
compares experimental and calculated results for certain chromium
steels. The accuracy of the method is 10 to 15%. Austenitic
steels are based on an edge-centred structure of gamma iron which
is of high electrical and thermal conductivity. Therefore, even
quite large changes in the amount of alloy components have little
influence on the thermal conductivity of austenitic steels.
Accordingly, Eq.(4) is recommended for all high alloy steels of
austenitic structure and, over the temperature range 50 to 901*C-
its accuracy is 10 to 15%. The thermal conductivity of a number
Card 4/5

s/ll4/6o/ooo/olo/oo7/Oo7
E194/E484
Methods of Calculating the Thermal Conductivity of Various Classes
of Steel
of other grades of steel of various classes is then considered and
coefficients of thermal conductivity are given in Table 6. The
conductivities given here are appreciably lower than those given
in some other handbooks and tables which are in error. Recently
determined thermal conductivities for steel grade R-2 are given in
Table 7 and it will be seen that agreement between theory and
experiment is good. Because of recently developed experimental
methods, it is now possible to determine the thermal conductivity
of steel to within 3% but this is relatively complicated and
laborious and the method of calculation described in this article
should be used where an accuracy of 5 to 15% suffices.
There are 3 figures, 7 tables and 10 references: 8 Soviet and
2 English.
Card 5/5

DMIZWOVBKTYI R.- E.-
"Influence of Thermal Treatment on Therman and
Electrical Conductivities of Heat Resistant Alloys."
Report submitted for the Conference on Heat and Mans Transfer,
Minsk,.BSSR, june ig6i.

22538
glob IVSS S/o96/6i/&oo/oo6/oo5/oo6
E193/E183
AUTHOR.- Krzhizhanovskiy, R.Ye., Candidate of Technical Sciences
TITLE. Investigation of the thermal and electrical
conductivities of some titanium-base alloys
PERIODICALs Teploonergettka, 1961, No.6, pp- 56-6l
TEXTs The high strength/weight ratio and excellent corrosion
resistance of T1 and TI-base alloys make these materials eminently
suitable for many industrial applications, including those in the
power generating industry. However, in order fully to realize the
possibilities offered by these alloys it is often necessary to know
their heat and/or electrical conductivities, and since data on
these properties of the Ti-base alloys are scarce, the present
investigation was undertaken. The chemical analysis of the alloys
studied is given in Table Iq 'where the column headings are as
follows. I - number of the specimen; 2 - alloying elements, wt.%;
3 - remaining components. The measurements were carried out in
vacuum with the aid of equipment described by the present author in
a previous paper (Ref.4; present journal, 1958, No.1). The 50-950
OC temperature range was covered by experiments spaced at intervals
of 50 OC. The results are tabulated and also reproduced graphically
Card 1/6

22538
s/o96/61/ooo/oo6/oo5/oo6
Investigation of the thermal and ..... E193/E183
in a manner designed to show the effect of various alloying
additions on the thermal and electrical conductivitie 15 X and a
respectively) of titanium. Thus, Fig.la shown a (*h'_iCm-l' left-
hand scale) and X (cal/cm sec OC, right-hand scale) plotted
against the temperature (00 for specimens 11 2, 18 and 21 (see the
insert for the legend), whereby the effect of Al additions is
illustrated. The effect of Mo and V is illustrated in the same
manner in Fig.16, and that of Zr in Fig.10. Similar graphs in
Fig.2 show the effect of Sn (Figs. 2a and 6) and Zr (Fig.20).
It should be noted here tVt the scCle of o in these graphs
varies, being a, a x 10 , a x 10- in Fig.1 a, 6, and 8, and
a x 10-4, a, and o x 10 in Fig. 2 a. 6, And Q , respectively.
Analysis of the results obtained showed that at any given
temperature, X, a, and L = VoT (where T is the absolute
temperature) are functions of the total alloying additions content,
expressed in vol.%. It was shown also that since the value of L
at any temperature is constant and equal 3.3 x 10-8 v2/oC2, the
thermal conductivity of Ti-base alloys whose electrical conduc-
tivity is known can be calculated from the formula
Card 2/6 X = L OT x 0.239 = 7.9 x 10- 9 aT cal/cm.sec.*C.

22538
s/oq6/61/000/006/Oo5/Oo6
Investigation of the thermal and .... E193/E183
It was concluded that, in applications in which thermal
conductivity is of pnramount importance, Ti-base alloys containing
zirconium or aluminium should be used..
There are 3 figures, 4 tables And 7 refeeences: 3 Soviet and
4 non-Soviet. The English language references read as follows:
Ref.2: L. Silverman, J.metals, N.J.S., 631, 1953.
Pef.3: E.G. Loewen. Trans'. ASYE 78, No-3, 1.956.
Ref.5: J. Lunsford, N.J. Grant. 1XIet. Progr., 10s No.3% 1956.
ASSOCIATION; Tsentralfnyy kotloturb.'nnyy institut
(Central Boiler. and Turbine Institute)
Card 3/6

S/121ti/611011/005/010/015
EO/VV35
AUTHOR? Krzhizhanovskly, R.Ye.
TITLE:~ Investigatton of the Influftice of Agnijiq on tho
Thermal Conductivity of the Alloy `) - )"A (E1607A)
PERIODICAL, Fizilto metallov I. metallovedenty.e, 19W
Vol., 11, No. 5, pp. 741 -- 740
TPXr-. The eteel E1607A is prone to precipi-tat.Lon--hardenlug;
during ageing an intereDetalltte pha~6-~- is ~*Jected~ Formation
of a dispers,;~ phase is slow at 6000- 700 C., Ahe operating
temperature for this alloy is 700 C but depending on the
conditions of operation of the gas turbin,45. it. may operate at
lower temperntures.of the order of' 500 - 600 0C. The
elef-trical--resistance method was applied for ctitablishing the
existence, under c.ert-%in cond0ions of heating or heat-
treatment, of a particular structure. the K-statei In
nichrome-base alloys the K-stat-e njay occur in the tempetature
range 1100 .. 700 (2C. In earliir -work (Ref. 5 Tpploenergetika,
1958. No. .1) the author has ihown that In A nTimbeT of cases
Card 1/.10

sh26/6i/oil/005/010/0.15
Investigation of E073/9335
structural changea in attels have A gr#3ater Influence on the
heat conductivity than ort the eje< f r j(- cutidur tivit y. Th or e -
fore, it was proposed to tit ilt4-e *I lo tnoasuz onjint of the
heat conductivity for studying structurd) phArjumena. According
to earlier work of the author (Ref. 7 - Zh, xtkh.fiz_ 1959,.
28, No.. 1k) and that of A.S. Pradvoditelev (IRef, 6 - Zh. exp. I
teor. fiz-, 1934, No. 8) the mechanism of heat condmtivity Is
not the some an that of eltcltrical conductivitv. Atoms which
are extraneous with respezt to iron and ditorti~avs in the
crystal lattice increase the scattering of electrons and
reduce the eltctric;al conductivity and the heat transfer.
Since the 2nfluenc-e of these taclor-A on 'the -1~cal:ter of the
elastic oatillations of atoms Is less,:tht (4f-t Of the latter
on heat-transfer will increase. In high-alloy steels and
alloys, the electron and phonon parta of the total heat-
conductivity are of the same order of magnitude. Thus any
change in the internal structure of the alloys restilting in
an Increase ordecrease of the electron srattr-ring will
also affect the electric conductivity and the olectron heeit
Card 2/10

S/126/6i/oil/005/010/015
Investigation of .... E073/E335
conductivity. A change in the structure of the alloy will
also inevitably affect the propagation of elastic waves,
bringing about a change in the ratio of the electron and
phonon heat conductivity and tiorelative change in the total
heat conductivity can be many times as high as the changes
in the electric conductivity. Therefore . the structura.]
changes in the alloy can be investigated by moasuring simul-
taneously the electric and heat conductivities. The
experiments were made with cylindrical spec4mens, 5 mm in
diameter and 100 mm longin a vacuum of 10 mm 11g. In this
paper the author deals with the structural changes which take
place as a result of holding the alloy spritimens at 600, 700,
750 and 800 OC for periods of up to 2 000 hours. The
experiments also encompassed the ntudy of the influ. enke of
heat-treatment. prior to ageing on the propertles. OU-stalled
table in given on th 0 Sarious heat-treatmenOt -hich were
tried. Ageing at 600 C took place aft 9r quetithing, followed
by multi-stage heat-treatM6jjtL, At 600 C Iwo prozeases may
occur. disintegration of the solid solution with rejection
Card 3/10
_j J

S/126/6i/oil/005/010/015
-Investigation of E073/E335
of a finally-disperse intermetallIto phait.. % regrrupinx of
atomm i..ot formation of the K-stato. If the apec2wen -its aged
aLt,%.,L quei)ching, both processc-a may occur simultaneously.
However, the processes of formation anl destruction of the
K-state can be separated by preliminary heat-treatmont, aimed
at rejection of a second phase from the solid solution. The
possibility of the formation of the R-fitate in the alloy is
indicated by the S-shape of the dependence of the electrical
conductivity on i.emperature for moist of the investigated
specimens. The minimum electrical c8nductivity was obtained
for the temperature range 500 - 600 C. To determine the
relation between these two processes and their Influence on
the ageing behaviour of the alloy at. 6oo 0c, ~wo differing
heat-treatmenta were used:D heating at 1 100 C for 5 hours,
followed by quenching in water (ageing times 48 - 2 000 0hours
at 6oo 0);2)1 100 OC - 5 hours, water-quenching + 1000 C -
2 hours, + 900 OC - I hour, + 800 OC - 2 hours, + 750 OC -
20 hours. + 650 0 - 48 hours (ageing at 600 0C for 500-2000
hours). The second mentioned heat-treatment was intended
Card 4/10

S/126/61/011/005/010/015
Investigation of .... E073/9335
to ensure preliminary rejection of a second phase from the
solid solution. The resulting changes in the temperature
and electrical conductivity and the value L (=X/&T , T
being the absolute temperature) are plotted in Fig. 1 for three
differing temperatures of determination of the coatficients of
heat and electrical conductivities (h, cal/cm sea C,
(r x 10-4 XIOM-1 , a, 108 V2 /a2 versus ageing time '~', lira
(Russian text at the origin of the coordinate system means
"initial state"). CAbstractor's note; both the figure caption
and the text specifically mention the quantity L the plot
itself only shown values of #,, a- and M.
It can be seen that the heat conductivity/and the electrical
conductivity 0, decrease even after 46 hours h 8Iding at
6oo OC. It can also be seati that agejLng at 600 C effects a
considerable change in the ratio of the heat-to-elertrical
conductivity (L) which is attributed to the fact that the
structural transformations have a stronger effect on the heat
Card 5/1.0

,S/126/6i/oll/005/010/015
Investigation of , ... E073/E335
conductivity than they have on the electrical conductivity.
Preliminary rejection of the second phase did not have any
appreciable effect on the heat and electrical conductivity or
on their interrelation. This leads to the conclusion that the
influence of the algaing time and the thortnal and electrical
conductivity plotted in Fig. lJs mainly conditioned by the
low-tomperat'ure process in the solid solution, which ha3 a
greater effect on the thermal conductivity. Experiments at
other ageing temperatures also showed that the thermal
conductivity was more sensitive to structural changos than
the electrical conductivity and therefor* in the further part
of the work only the results of thermal conductivity are given.
The character of the dependence of the thermal and electrical
conductivity f8r ageing at 700 OC was basically the same as for
ageing at 600 C. However, the influence of preliminary high-
temperature heat- reatment in more marked. Fig. 2 shows the
results obtained tor specimens aged for durations from the
"initial state" to 2 000 hours for the following heat-treatmentes
Card 6/io

S/126/61/011/005/010/015
Investigation of E073/9335
1) agoing after holding at 1 100 OC for 5 hours and water-
quenching; 0
2) &going after holding at 1 100 C fog 5 hours and water-
quenching followed by holding at 1 000 C for 2 hours and
cooling in airl
3) ag8ing after a heat-treatment consisting of holding it
1 100 C for 5 hours, water-quorahing, holding at 1 000 C
for 2 h8urs plus holding at 900 C for I h8ur plus holding
at 800 C for 2 hours plus holding at 750 C for 20 hours.
During the initial period of ageing, the greatest distortior
of the atomic lattice, obtained as a result of the fine
diapers* rejections, occurred for the first mentioned heat-
treatment. However, with Increasing &going 'time.. these
distortions are rapidly removed. JudSing from the fact
that the preliminary heat-treatment reduces :the minimum of
the curves expressing the dependence of X on the &going
time lt~, it may be that a sharp change in the heat
conductivity during ageing after quenching in duo to the
more intensive rejections and coagulations of tho particles
Card 7/10

Investigation of
S/,126/6i/oli/005/01,0/015
9073/Z335
of the second phases Fig. 3 shows the influence of the
ageing temperature on the heat conductivity for a test
temperature of 600 *C. In this case, all the specimens
had th8 same preliminary heat-treatmentt is*. holding &t0
1 100 C for 5 hours, water-quenching, holding at 1 000
for two hours, cooling in air. The obtained results confirm
the earlier expressed view that,in a number of cases the
heat-conductivity is more sensitive to structural cb~anges
than the electrical conductivity and that low-temporature
processes hove the greatest effect on the conductivity of
the alloy. There are 3 figures, 1 table and 8 Soviet
references*
AOSOCIATIONt Tmentrallnyy kotlovturbinnyy Institut lawU
I'10 Polnunova (Central Boiler-turbine
Institute latent I'l. Polsunov)
IUBMITTZDs August 22l ig6o
Card 8/10

S/862/62/001/000/oo6/oiLa
E202/r.492
AUTHORs LrO$,Xhj-qq" *kAy R.Te
TlrLEs Certain regularities in the behaviour-of thermal
conductivity of metals and alloys
SOURCEs Tsplo- i massoperenon. t.1: Toplofizich*skiyo
kharakteriatiki materialov I metody ikh oprodelonlya.
Ed. by A.V.Lykov and B.M,Smollskiy. Minsk, 1zd-v6
AN BSSR, 1962, 113-125
TEXT% The *ffect-of t*mperaturs, crystallographic structure and
presence of admixtures on the behaviour of thermal conductivity k,
of non magnetic and-magnetic metals and alloys with particular
reference to iron and its common alloys in studied over the
temperature ranges above room temperature. The main made of
investigation in based on determining the exact value ofthe
index m in a formula relating electron thermal conductivity Xg
to the absolute. temperature viz
Xe a kT
and plottinj Xe as a function of temperature for the metals and
alloys Investigated. Extending similar arguments to the phonon
Card 1/2

Cortain regularities
s/862/62/00l/ooo/oo6/oi2,,
E202/E492
component of X i.e. Xph, the author discusses the relation
Xph U bT + f
in which b is a constant and f a quantity Icharac'terizing the'
scattering of phonons on the admixtures. Lattice deformation*
are considered to b@ equivalent in this respect to the admixtures.
Electrical resistivities a are also plotted as functions of T
and compared with X plots. The effect of duration of thermal
treatment on A and a are also studied. It is concluded that,
contrary to general belief, X plots are more sensitive in revealing
the structural changes occurring within the metals than the
metallographic observations and resistivity measurements.
There are 4 figures and 1 table.
ASSOCIATIONt Teentralinyy kotloturbinnyy,inatitut im. Polzunova,
g. Leningrad (Central Boiler and Turbine Instittkta
imeni Polzunov, Leningrad)
Card 2/2

34681
S/129/62/000/002/010/014
E073/9335
AUTHOR: Krzhig-bo iovskiy_,_.R.Ye.. , Candidate of Technical
Sciences
TITLE: Influence of heat-treatment on the thermal
conductivity and electrical conductivity of the
steel 15X12BMT (4A802)(l5Khl2VMF (EI802))
PERIODICAL. Metallovedeniye i termicheskaya obrabotka metallov,
no4 2, 1962, 48 - 49
TEXT: The steel E1802, which was developed by the laboratory
of the author, is intended for rotorlo~ discs and blades of turbines
operating at temperatures up to 580 * The chemical composition
is: 0.16% C, 0.21% Si, 0.63% Mn, 11.81% Cr, 0.42% Ni, 1.03% W,
0.59% Mo, 0.24y. v, 0.014% S and 0.01% P. The work described was
devoted to investigating the influence of the quenching and
tempering tempegatures and the duration of ageing of this steel
at 550 and 600 C on the thermal conductivity X the
electrical conductivity w and the quantity a X/oT
where T is the absolute temperature. A change in a indicates
Card 1/2

S/l29/62/OOo/Oo2/oio/oi4
Influence of heat-treatment E073/9335
that the state of the solid solution influences the background
part of the heat-conductivity. X and a' were determined on
the same specimens. It was found that the quenching and
tempering temperatures did not affect the thermal and electrical
conductivity. Tempering after quenching increases the thermal
conductivity by 3 - 13% and the electrical conductivity by
0 - 10%. Both the thermal and electric:l sonductivities
increase appreciably aft8r soaking at 6 0 C for 1 000 hours.
However, soaking at 550 C for the same length of time does
not bring about a change in the thermal and electrical con-
ductivities. Microstructural analysis proves that holding ag
550 OC does not change the structure, whilat holding at 600 C
leads to appreciable separation of carbides and their coagulation
followed by redistribution of the alloying elements between the
solid solution and the carbide phase. Thus, it is concluded
that the thermal conductivity of the steel EI802 depend a
to a greater extent on the structure than the electrical
conductivity. There are 3 figures and 2 Soviet-bloc references-
ASSOCIATION& TsKTI im. -Polzunova
Card 2/2

Sow regular features of the behavior of the heat conduction
of metals and alloys. Teplo- i maoeoper. 11 n5-125 '62.
(MMA 16 t 1)
1. TSentrallrqy kotloturbinnyy institut in. Polzunova, Ieningrad.
(Metals-Thermal properties)
(Alloys-Thermal proportion)

- __
I- . __ _-.-I....
"The possIbility of an anomalous relation of thermal conductivities of
insulating materials and their volume weights."
report submitted for 2nd All-Union Conf on Heat & Mass Transfer,, Minsk,
4-12 May 1904.
Polzunov Boiler & Turbine Inst.

YJMIZIIAIICYVSKIY, R,Ye.; SIMMA, H.P.
Determining the heat conductivity of liquid-mtal coolants by the
longitudinal heat flux method. Inah.-fiz. ztn=. 7 no.8:75-80 Ag 164.
11 (MIRA 17:10)
1. TSentrallnyy kotloturbinnyy Inatitut im. 1.I. Polzunova, Leningrad,

ACCESSION M AP4044417
8/0170/64/=/m/m5/0060 t
AUTHORSt Krzhizhanovskiyt R. Ye.1 Sudorova, N. P.
...........
TITLEt Determination of heat conduction of liquid metal heat conductors by the
method or longitudinal heat flo-Y
:SOURCEt Inzhenerno-fixicheakiy zhurnal, no. 0, 1964, 75-80
TOPIC TAGSs heatflowp heat conduction, thermal gradient, liquid metal
.ABSTRACTs Work was performed to datermine.the feasibility of the method of longi-
;tudinal heat flow as a means of-determining the coefficients or heat conduction for
.liquid metal conductors. An electric heater attached to a container holding liquid
'Metal wan used to promote heat flow. Heat losses -from the collar and lateral sur-
faces were eliminated by means of sectional heaters and innulation. Heat lose
magnitude was determined by means of thermocouples. Expressions were developed
quantifying longitudinal heat Ions for the sample. The differential equation for
heat conduction was derivedt boundary conditions were evaluated, and an expression
for heat conduction coefficient extracted from the resulting solution. Another
expression for the conduction coefficient was developed for heat exchange with the
ambient environment* Aoouracy of measurement by the method described was found to
,Card 1/2

~ACCESSION NRt AP4044417
;be about 2%. A schematic diagram of the experimental apparatus used was ahownt as
was a plot or the temperature dependence of heat conduction coefficient for thrle
.selected liquid metal alloys, Orig. art. heat 20 equations and 2 riguress
1ASSOCIATION# Teentralln
yNy kotloturbinny*y institut in* Is Is Polsunove, (Central i
~Steam Turbine Institute)
:BUBMITTE;Di 27NOT63 ENChl 00
;SUB CODki TD NO RU SOVI 001 004
Card 2/2-

ACCESSION NR: AP4042465 S/0294/64/002/003/0392/0396
AUTHORt KrzhLzh4novskLy, R. Ye,
TITLEs Thermophy~icsl properties of titanium and its heat
conductivity when alloyed with tin and aluminum
SOURCEi Toplofiniks vy*sokikh temperstur., v. 2, no. 3, 1964,
392-396
TOPIC TACS: Soviet coinmercial grade titanium, titanium thermo-
physical property, titanium tin alloy property, titanium aluminum
alloy property, titanium heat conductivity
ABSTRACT: The thermophysical properties of Soviet commercial-grade
titanium, 99.6Z pure tLtaniumj and of a titanium alloy with up to
20 wt% tin or up to approximately 8 wtZ Al have been Investi-
gated. All measurements were carried out in a vacuum of 10-4_10-5=H8;
measurement error was 2-3% for thermal conductivity coefficient X,
land about 1% for electric resistivity o. The temperature diffusivity
:coefficient a and magnitude L a A/cT, which characterize# the role
of electron conductivity in a metal, were calculated from experimental
ard
;C 1,/3

ACCESSION NRt AP4042465
data based on A. p, heat cap&city,and specific weight. The absolute
values of X obtained were closest to those obtained by G. Lowen for
RC55 titanium (99.64% TO and those cited by Us W. Kirby and C. Sykes
for 75A titanium (99.75Z TO. The temperature dependence of X for
titanium was found to be almost constant, L,*., about 18 w/m-deg C,
and increasing at higher temperatures. Additions of tin or aluminum
cause X to drop sharply to about 8.3 w/m-dag C for Ti - 20% Al and
Ti - 7.5% Sn alloys. Increasing the amount of an alloying element
causes a simultaneous increase in the temperature diffusivity, which
at high temperatures (.800C) tends to equalize X for various alloys
(Ti-7.5% Sn which has a small temperature diffusivity coefficient).
Similar behavior is also observed for p. The data on Ti-Sn and TL-Al
alloys show the possibility of the existence of titanium-bass alloys
with very low values of X which can be utilized for heat exchange
equipment and parts subjected to high thermal stresses, or for struc-
tures utilizing the good heat-insulating properties of titanium in
combination with high strength. Origs arts hast 4 figures.
Card. .2 / 3.

;ACCESSION NRS AP4042465
ASSOCIATION: Teentral**/ kotloturbLnny*y InstLtut Lm. 1, 1,
Polzunova (Central Scientific Research Design and Plsnninj Boiler
And Turbine Institute)
SUBMITTED: l5Apr64 ATD PRESSt 3070 ENCL: 00
SUB CODEs MHjTD NO REP SOV# 001 OTHER: 006
'Card 3/3

F71
7~1!w
I
a
kit:ii
i ; r ci 2 / 3

: ---- UR/0294/66 03W/63~!~
ACC NRt AP6021212 SOURCE CODE 1004 011~~
AUTHOR: Kmhizhanovskiy.-R. Y .;_Chudnovskaya, I. I.
1 ORG: Central Boiler and Turbine Institute im. 1. 1. Polzunov (Tsentrallnyy kotlo-
i
1 turbinnyy institut)
TITLE: Investigation of thermal insulatioAropertiea of kaolin fiber
P I
SOURCE: Teplofizika vysokikh temperatur, v. 4, no. 3, 1966, 355-359
TOPIC TAGS: kaolin, high temperature Insulation, radiative beat transfer, convective
heat transfer, insulating materialhea~ 0,dndvc-k;v;~1Y
ABSTRACT: The thermophysical properties of kaolin fibers were studied at temperature
up to 16000C in an oxidizing atmosphere to determine this material's insulating pro-
perties at high temperatures. The tests were conducted in an Insulated chamber in .
which a cylindrical sample was tested both in oxidizing atmosphere and in vacuum. The
tests were performed on the same sample, since the packing density of fibers proved t
influence the experimental results. The sample was heated by means of electrical con
duction in the platinum-rhodium thread on the axis of the sample. To reduce thermal
gradient, an auxiliary michrome wire heater was also used. This test rig was capable
of measuring thermal conductivity coefficient in the range from 0.005 to 1.0 W/degree
-meter. The testing procedure of various samples Is recorded and the coefficients of
thermal and temperature conductivity plotted for several packing demnities. It was
Car UDC: 536.2,08
. ~d 1J.2_

V r-
1
I ACC NRi AP6021212
found that the thermal conductivity of the kaolin fiber has a minimum at about 160
/M3 density in an oxidizing atmosphere and at about 140 kg/M3 in vacuum, in the tem-'
perature range of 400 to 6000C, The existence of the minimum In the coefficient of
thermal conductivity is ascribed to radiative heat transfer in addition to convective
transfer. Orig. art. has: 4 figures.
SUB CODE: 20/ SLMM DATE: Olrsb65/ ORIG REF: 004

Card 2/2 fV

!.A.; G101,1101PUIL)TO EX.; LOGO;
N.D. 1, SHOK011011A , BOG.
P: oportles of the dunt of rotary iA Irm and waye of using 1t.
rrudy lUzhpliproteementa no.4'40-54 63.
(MIRA 17:11)

~r, C,f
n'j,31Z 46
(MIRA -'8.'5)

77

'1 1.1 tt,,P,, of oilrates and nitritas in theM
U S S R ' Po, 'I
.. tj~ f.
11:11t .Ming meat. It. llictiki- r"Ild 11 1
krOdOvivAl 1, Aru,l. ('Aeoi- 9, 4( 7- V 191
I
C.A. 49. 4NvNs. H. I" fl-i~ (p

p Z i,~
Category : USSR/Electronics - Gas Discharge andfau-11IBeharge Instr,,=entj H-7
Abs Jour : Ref Zhur - Fizlka, NO 1,-1957~ No 1721
Author :Tsigelka, I., Chernyy, L., Gusa, V., KrzhiziL, I., Uuinar, I.
Title :Mechanics of Are Discharge at 11igh essure In Stream of an Air
Circuit Breaker
Orig Pub :-Zh. tekhn. fiziki, 1956, 26, No 3, 499-5o4
Abstract No abstract
Card

KRZHOVINA, Frantishek [Krovim, F.)
Standardization in tho Czechoslovak Socialist Republic.
Standartizataiia 29 no,7143-45 JI 165, (MIRA issn)
1. Prodsedatell Upravlerdya po Btandartizateli I imereniyam
Chokhoolovatakoy Sotaialiatichookoy Roopubliki.

KOGU TA, 1, S.; H.; FZRW-GA, D.
Fat emboliam In liver steatosis. Zdray, vfjtstn. 31, no.5/6:100-104
165.
1. Interna klinika medicinske fakultate v Ljubljani (predstojnik:
pror. dr. S. Mahkota) i Patolosko-wmtomski institut medie4nsku
fakultete v Ljubljani (predstojn1k: prof. dr. F. HrIbar),

--- F ~7'T --r-- -::- -- -
.4 ~ i,_ 04 1 : I t , .
"A ,, I .- I t !.,, ~ Pr 1, 1. 11
I Lj,iblj-,~n~i. ., .1-1,
J~Itxla.ll p. 5 . Vol. ~~, -~:). ll~, *,n-,-j. 1',r2l
. .
SC: "ontirdy List of E,st European Acccs!Aons, V,-)l. 2, B, Libr-ry of Cor-,reoz;
kigu-1t, Y/153, Uncl.

fO*AVUU4 Wd Cats,
49, A. 341-344),-In thn
WA* ot A, ~waian yield I Oft Alv Ip")-
Inationt Od yitLU per ho~tjixe ejual t, 0Q,.m OA,iinq fiwn -Ai,i
can ho ol4ziw~4 with mo~4vfiit* kAl rerl-jittinvL'i C44 inA* fr~jn
Of me4:4% should bavs hlt% fftdin# value, vi &z.- " 't 'f h, h
Prtitela 'Loattat (-40-4) and their MW vnk;itard w-A'('41

GRGUAEVIG, Matko, dr.1 KRZIIARp Borin, dr.
Sarcoma of the uterus. Lijecn. vjeon. 83 no.3:239-21+8 161.
1. Iz Oinakoloske klinike Hadicinakog fakulteta. u Zagrebu.
(UT&M VEOPLAS14S statist.) (SARCOMA statist.)

Y L:(,O 6 LAVIA
Dr Hihovil DEXARIS, Dr Boris nd Dr Zivko KULCAR, Gynecologic
Clinic of Medical racl,lty (Ginckoloska klinika Yedicinskog fakulteta)
n:A State Institute of Health (Republicki zavod za taBLILe zdravlja),
2 a -ireb .
113tatun of Uterine Cancer In the National Republic of Croatia.'
Zagreb, klj~ctj~~ki V Tjk, Vol 84, No 8, Aug 1962; pp 765-771.
jjs
Ab~jtra.~,t jLnglish stm=ry trodified": The authors' cl1nIc Lospitalizos
50% of all patients with cervical and 25% of those with uterine cnqus
cancer In Croatia; exiviustIve stati3tical data indicate that diAgnuatic
and therapeutic results have not Wproved in the last 10 years And
detection It still lower than, e.g., in Slovenia. Epidmlclo~Ac
Vattern3 are intereating for postible etiologic studies; there Is still
a shorLage of gynecologists and poor organizational plannfiz and rccc;rld
keeping for maus 6creeningi remedial me4sures are propo3r.-I. '-'11 x
diagrams, 5 YUgOSIAV, 1 Polish and I US reference.

A06IIA101
AUTHORP.;' Krzuk, J., Zuber, A.
TITr.F- A scintillator for the recording of slow neutrons
PFIUODICAL-. Referativnyy zhurnal, Fizika, no. 10, 1962, 12, abstract 1OB8()
("Pier,itsze krajovie sympoz. zastosowaft izotop~)w techn., Ro&u, 8
12 czer., 196 )011 . Warazava, 1961, no. 121, - Polish, su=,artes in
Russian and English)
TF--.(T: Described is it scintillator for the recording of slow ncutron5,
,i;Kich has been obtained by sintering natural B 203 with ZnS(Ag) at 64oOc. The
efficiency of 10 and 24 cm2 scintillatorn with respect to slow neutrons, fast
neutrons, and gamma quanta amotAnts to 10, 0.1., and -10-4%, respectively.
[Ab3tracter's note: Complete tranalationi
Card 1/1

" 1, "T"Ir'. , ~, if
Freq.-Oinp rachineo.
1". 310. (Loiz-, Poland) Vol. 8, no. 12, Dec. ).'-)57
E~;: -Ont.
, ly Index of Mst European Acceislon (.-; ~:Al) ':,' Vol - 7, No. 5, 1958

F. , PUL;Kl, J. M11.1,USKI, R.
RntAlr of locomotive wheel aFXregates by welding.
P. 275. (PRZIMAD KOLF.JWY MECHANICZ11Y) (Warazawap Poland) Vol. 9, no. 9, Seot. 19
SO: Yonthly Index of Fast Wropean Accession (EFAI) L.G, Vol. 7, No. 5, 1958

1317"I'EL-MHRZYNSKA, fladz!eja; PHUSO J Iga, JANUKWICZ-LOPENIZ, Italina;
KPZYZANCUSKA, Olga; FLYNKI CZ, Henryk
cce SZ
liadjonctive I(Aine, (1-131) esta in dwarflam syndromes. Frdokr.
Pol. 14 no.6:597-602 N.-D 063.
1. Przychodnia FndokrynoIogIc%na I Oddzial Endokrynologil
Dzieciecej I KlIniki Ghorob Dzieci Akademil Modycznej w Gdansku
(Kierownik: prof. dr K. Erecinski) i Zaklad Fizyki Lekarskiej
Akademli Medyc,.noj w Cdansku (Kiorownik: prof. dr J, Adamczewnki).

r
'PUVIOd Ul glulld ;VVJ(nft Put luldLund ;wull,
.uiw )a tionmuiruo3 mn joi aminaw 101111ifilloddo wilivid 4)pso,,
PUT Ruldwtkd 31ji3ap) NUMUM J6 2141140111 -A%%UwlhV -.bd-I "41 lo
nuvid jofvw )a iuatuelnbl 441 10 U01idIJ393P Put "I-nimnoi in(tm
wnqnA ul v)uvld sulclLund aiii3als ul Alljodej I'-Illvivul 'Alslau,
)a tunIvIntun3if Isniva $a A3u#i3ljia 041 so U94112,11tusnau 1111414
aftioli pus Vuldlund '1143#14-0jP" IWU14ww 10 vutNINOS INA114-I.
-inuild aftlolf Pug Sulduawl paulqujW 10 a3flunpu j4j ,I vjujud
*wluwtd XV-04 :nil-%Na vnotJVA Ul 11SAMIll JJd V'wg- lun)JnPUA4 ju liva4l
.141 so -%vl m oxviuvAps Rvw SUIJLP wamp " $jno4 30 jjqtunu
,;ui cn SulPioij, 'w')Adww V 'u(ninim f%JJu,)N 19DW 841
dwnd Aoj wpiq anq paijazwId aww SUISHWON PUT S%v4 uaiol,nv
mvaus aqi n lainsiu4 inuvid oln3Ma 4SM11 Pug MUldiusid paujq
-ww jvqj tamp )Iqvillddi &1T WVW An 2UjJaAW JO luvjuj nwpvA
trnt[Ak 01 "JSJP AM jo billIVUN OU 'P%q tq 9UK4MWjj 3kilitipai joil
rj,"w w"sva put juia" jamod 4&134a la pwm lo *aAjn,) Allw(l
I'M I "Al 91 'all-tol till
19S#1 'p-s oM 'V441,111JAW -.4-1413=403JOU4 IAIRWPAI Ifivivild
-04 4 vlQJ 431 WWJO JAD)RuJtWP I ajaudmod oulwa, Muawlllalx-
'8`4194"0 W-fVWil-tl!A-
vi *lox A1441 pug olmom olvaeow pug 11,14mona 4j)"m v wilix
99* 119 199 10

so an I
Xrvytki 9 Melh*ds for the ft"evilion of Peak tA*4* in row"
PWA:;',
-Spnootty swairrAnla uctWw obclittvA w energelyee". tnergetyka
Nn 11-12, 1950. pp. 397-402, 7 figs.
Apecl* wilrking conditions In power prmrtkee finablilty of actu-
molattiiir Plerfric enerly reserves, and lack of unitomilti In ron-
mumidlis". tiot emly on certain days of the week :and periods of the
d.iv PiA yvar, but also jis lite result of uutors"n phrnomenat atui in-
flurtwr nf thmr ronditknm on the Increase In Investment exprndl-
111re Tbe t~ndpnry to keep Swak "do In th"It by building special
rwak Imil Istatitt conital of peak loads hy means of ptoper rrguls-
I-i of i woumt rx' Ormond.

T.
1134 Ili
Krzycki 8: Heat Pumps aead Their ImpartAtic, in PrActive,
,,11-ump-t cJeplne I lch z[124-"t1lC' (I)A 110
1,2 1951, pp. 0-12, 9 tip-, 2 L-b-s.
Thtrmal cycle 1h the heat Pump. Initial to
ding these, punips for general im!, F.1"IrLeLcy (Lit:jors tit tjv,,,t Jjj!j.;;
-- theore0cal and actual. Influence N ultimate 'CmPCvA"11!rt (it', !1w
effIciancy factor. Example at si, hesting InstalUtion iia,,(l o:i tli~,
work of heat pumps,'Heat-pumpis a& a mcana fit r"ls.g Oil, aezr,~r
nip%
of himt U01sallon In xmer staticuts. Deal application out licat pu,
for btaUAg iiiiiid abojng. lncrftnd in;trmt In the kitroduction of
hftt Pimps Into Mr~Uj use. PoissilbillUes"Of usIng heat pumps iii
pow 1~rptwe.

KRZYCKI, S.
CooUng of tuftoreneratore by hydroFene po 78*
ENERGEMA, MiniBterstwo Energetyki Stalinoicrod, Vol, 9., no, 2., Mar./Air.
1955.
SOURCEI East European Accessions List (BUL)s Library of Congress
Vol. 5s No. 7s July 1956.

KRZYCKII S.
KPZYCY,I, S. Trends in building switchbo&rds. p. 299.
Vol. 9, No. 6, Nov./Dec. 1',155
ENTMETYKA
TECHNOLOGY
Poland
Warazawa,
Soi East Europoon Accesnion, Vol. 5, Ho6 5, May 1956

~,4r, r PI ;i ri
rs an
ti r) 2 , 'v'a r /A!-. r

Englan-J's power industvi in light of the roto:t nf tl,,c, Untral 12ectricit~~
Authority. p.102 .
E r '-1-` 1 1-~Y K A .Val. Ils 'No. 21 Ilzr.Fcb. Ioland)
S'O: List of' East Surot~can Accessions (1,1AL) IC. Vol. 6, ,o. 10, vctober 9570' Uncl.

____KRZTCJfI,_O.tqf~a~, mgr. ins.
Development of the electric-power eyottim in the German Democratic
Republics Inergetyka Pol 14 no.2:51-54 160. OMAI 9:6)
(Germany, lastern -31lectric power)

KRZYCKI, Stefan, mgr inz.
Some indications for the development of the Czechoslovak power
system according to the next Fivo-Year Plant Energetyka Pol 14
no-10017-319 0 1160. (EMU 100)
(Czechoslovakia-Electric power)

KnycKIx_k"fanO ngr inz.
~i Development of olootric power plants in Great Britain. Emrgetyka Pal
13 no,,2156-57 F '61* (EW 10s!,)
(Great Britain-Ilectric-power plants)

- KRZYCKI,, St. Mgr Inz.
Power engineers in the German Democratic Republic are aearcWng for
locations for now p=ping power plants. Energetyka Pol 15 no.--Xl
JI 161. (EEAI 10-9/10)
(Electric power-planta)

UZYCKII Stefanp mgrot inz.
-----
Existiag international cooperation of power systems in European
countries, Hhergetyka Pol 15 no.12t366-370 D 161.
1. Czlonek Kolegium Redakcyjnego 'Energetykal.
(Electric power)

KRZYCKI, Stefan, mgr. ins.
.A-.- - - - --- .
Large pump power plants in Western Europe. Energetyka Pol 16
no.60uppl.sBiul Inetyt Energet 4 no.5/6sl8o-181 je 162.
E.-'-

KRZYCKI p Stafa -zp inz.
- - --- ... ... 0 1
The interconneoted sleatric power system of the Soviet Union.
inergetyka Pol 16 no,109298-304 0 162.

KRZYCKI.-Stefan.-mgr Inz.- ---- --- -- ----
Large generator BystemB im 'Iftitime $bew*l electric power plants of
thejU.S.S.R. Energetykapol lcrw;n,346-347 N 162.
'N -W
is--,
1.1 ~

KRZYCKII St.0 mgr ins.
The first Year of utilLization of the combined pover systems in Great
Britain and Francim. Inergetyka Pol 16 no.n:350 N 162.
i

EMIC 4acu"a-gr inns,
Effoot of sumor dayliSht tim on the. jUttening of the Polish
power system load o" mA tha advantages of its applicationa
Inergetyka, Pal 17 nooW01-aa Ap 163,

Ydizlclu, 3top laer inz.
Experiencei from heretofore P-ooperation of the electric power
ayata= of ths mamber countries of the Council for Mutual Economic
Azalstance, Knergetyka Pol 17 no.6:165~-168 Jo 163.

KRZYCKI, Stefan, mgr Ins.
of elsotric power demand in housoholds In
Great Britain. Lnergetyka Pol 17 noollt346-348 N f63.

!-. KRZYCKIp Stefan,, sp in*.
Cooperation of the eleatric power oyotcm of Denvarkp Fin3And,
Norvay, and Swodon. lhorgetyka Pbl 18 no.W20-122 Ap'64
.0

IM"!YCKI, Stafan, togr Jj,.z.
, - - - - ~ ~ - -.- --l- .- -., ". --. "
r
"Development proupout;j of , -.,rr ungincering" b T z ,
1r; A ;( L- I
...~ . j.12 .
Sorgluaz '.Iim)ro!:l. Review d ry Tcl
Yl nc.10:324 0163.

KRZYCKIS Stefany -Mgr inz.
Experiences in electric power engineering gathered during
the last winter. Energetyka Pol 17 no.8:243-245 Ag 163.

MYCKI., Stefan, mgr Inz.
Various indexes concerning power management during the
years 1956-1960. Energetyka Pol 18 no. 2: 53-56 F 164.

KRZYCKI, Stefan, mgr inz.
-1- . ~.-. X-.. -
Expected developmant, of electric power demand in countries of the
Organization of Economic Cooperation and Development, Energetyka
Pol no*6:178-180 Je 164,

Kill"'MI, Stsfan, mgr inz.
The periodical OHnergetyka and the development prospects
of Polish power engineering. Energetyka, Pol 18 no.12:360-
361 D 164,
1. Editorial Board of "Knorptyka," Votreaw.

KRZYCKI, Stefan, agr inz.
A conference on brow.1 coal in pover engineering. Energetfta Pol
19 no,301-92 Mr 165.
I. I ' i:

39Y15 6/111/136
S/Oc, Do
0
7/ 062/Aloi
AUTHOR: Krzycki, Z.
TITLE: A cross coupler with a ferrite filled aperture
PERIODICAL: Referativnyy zhurnal, F1z1ka, no. 6,1962, 22, abstract 6zh150
("Rozpr. Elektrotechn." 1961, v. 7, no. 3, 355 - 364, Polish; Rus-
sian and English summaries)
TEXT: The coupling coefficient of two crossed rectangular waveguides through
a coupling aperture filled with ferrite is calculated. The waveguides are in con-
tact through the broader walls. The value of the coupling is determined by the
non-diagonal component of the ferrite magnetic permeability tensor and attains a
maximum value at the ferromagnetic resonance. Using this dependence, the con-
sidered system may be applied for measuring the width of the ferrite resonance
line and the spectroscopic splitting factor. Discordance between calculated and
experimental data does not exceed 1%. Similar arrangements can also be applied
as a broad band selective element with a magnetically controlled coupling.
[Abstracter's note: Complete translation) V. X.
Card 1/1

0/194/62/000/002/082/096
D271/D301
AU THOR rurzycki , Z.
-:Z. -
TITLE: licuouring the resonance line width of ferrites in a
0
.Lerrite with diaphragm
PERIODICAL: Referativnyy zhurnal, Avtomatika i I-adioelektronika,
no. 2, 1962, abutract 2-7-148m (Bull. Acad Orlon. sci.
Se'r. sci. techn., v. 9, 1961, no. 2, 105-1i
TEXT: The problem is considered of two waveguides joined by a dia-
"~hragm with an aperture filled by ferrite magnetized by a trans-
verse magnetic field. The aperture can be represented as a pair of
dipoles; Electric and magnetic, excited by the field of the primary
waveguide. The aperture, in turn, excites the secondary waveguide.
Fields induced in the secondary waveguide are determined, assuming
that both wE.veguides are rectangular, with TE10 waves. If the pla-
nes of transverse cross-sections of both waveguides coincide, exci-
ted field is fully determined by the diagonal component of tL mag-
netic permeability tensor of the ferrite,p; if the secondary wave-
Card 1/2

S/19 62/000/002/082/096
Eeasur~ng the resonance ... D271YD301
guide is turned by 90 0 relatively to the primary waveguide, its
field is determined by the non-diagonal component of the tanuor k.
OLiall ferrite spheres were used in the experimental work; they were
placed in the aperture of the diaphragm, whose dimensions were con-
Siderably greater than tho8e of the spheres. In these conditiona,
only in the second case the excited field is proportional to the k +
component of the tensor; in the firut case '%Lhe waveguide is excited
through the diaphragm aperture and a reliable measurement of line
width. by means o'Lu is not dossible. Results obtained by this method
are in good agreement with those obtained by neasurements in a croes-
shap?d configuration and in a resonator. Effective values of the
Lande factor were also measured, Measurements were performed using
a otandard apparatus, at 9300 Mc/s. 6 references. (Polish Institute
of -.Iafjic Techinical Problems.) /-Abstracter's note: Complete tranala-
-n.
, -7
Card 2/2

24948
P/019/61/010/002/00.8/009
D253/D303
AUTHOR: Krzycki, Z.
TITLE: A wide band ferrite Isolator for the 3 cm frequency
band
iERIODICAL: Archiwum elektrotechniki, v.10, no. 2, 1961,
599-601
TEXT: This is a description of a ferrite wide band isolator type
IXL-1, designed from home market materials at the Magnetic Mater-
ials Laboratory of IPPT, PAN. Its operation is based on the effect
of the waveguide field displacement which is produced by a magnet-
ized ferrite plate. The principle of its operation is illustrated
in Fig. 2 which shows the simplified cross-section of the isolator
and the electric field distribution for dominant mode H10. The
curve El shows the electric field distribution of the incident
wave, propagating from generator to the load. E shows the field
of the reflected wave in the direction from the foad to the gener-
ator wave. In the plane of the absorbing plate, the incident wave
Card 1/3

24948
P/019/61/010/002/008/009
A wide band ferrite isolator... D253/D303
has a zero electric field and propagates, therefore, without atten-
uation. The electric field of the reflected wave has, however, a
value ne.r the maximum and is attenuated in the absorbing plate.
The position of the ferrite plate in the waveguide, its overall
dimensions and shape and the absorbing plate have been adjusted
experimentally. The technical data of thelsolator are as follows:
Frequency - 8600 to 9800 Mcls. Minimum pass attenuation 0.5 db.
Maximum pass attenuation 0.7 db. Maximum stop attenuation 35 db.
Minimum stop attenuation 25 db. WFS (VSWR) (from both ends) < 1.15-pr
Maximum average power 5 wi Maximum pulse power 1 kw. Waveguide
1 inch x 0.5 inch, length 80 mm, weight 0.8 kg. There are no diffi-
culties in changing the parameters according to the requirements
within the above ratio of the stop to pass attenuation. The iso-
lator was engineered from the nickel cadmium ferrite as designed
by the magnetic materials laboratory, IPPT PAN. The ferrite has
the following parameters: Saturation magnetization 4900 gauss. The
resonance line width in the 3 cm frequency band 1400 e. Spectro-
scopic diffraction coefficient 2.09,curie point 3000C. The type
IXL-l isolator has been designed to work primarily in small power
Card 2/3

24943
P/019/61/010/002/008/009
Awide band ferrite.'Inolator... D253-/D303
measurement circuits. It in nasumed, however, th-t becnuse of its
high curie point, the dissipation 1power could be considerably in.;.
creased without any detrimental chafigen in its propcrtic3 and with-
out any demage to the isolator itself. 'Aiere are 3 figures and 2
references: I Soviet-bloc atwl 'I non-Sovic t -bloc. - The reference to
the English-language publication reads as follows: S. Weigbaum.
11. Scidly A field displacement isolator, Jell Syatcm Techiiical
Journal, 1956, No. 4, 877-898.
SUBMITTM: November 23, 1960
Fig. 2 Legend: Simplified diagram
of isolator; A t1agnet; B Absorp-
tion plate; C Ferrite
Card 3/3
A
'N' C
_451