SCIENTIFIC ABSTRACT PUZEY, I. M. - PUZHAY, Z.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001343710018-3
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: December 30, 2016
• Document Release Date: June 19, 2000
• Sequence Number: 18
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

AUTHORS:
Molotilov, B. V., SOV/48-22-.lo-16/23
PUE2y,
Rad1kov, A. I.
TITLE: On.Volumetrical Magnetostriction in Iron-Nickel-
Molybdenum-Alloys (Ob"yemnaya magnitostriktsiya:spl&vov
zhelezo-nikel-molibden)
PERIODICAL: Izvestiya Akademii nauk SSSR. Seriya fizicheakaya,
1958, Vol 22, Mr lo, pp 1251 - 1253 (USSR)
ABSTRACT: A description of various devices used for the
following work is to be found-in reference 1. Special:
attention has been paid to the observation of iso-
thermic conditions during the tests. The adiabatic
process of maenetisation is known to hinder any
adequate measuring of magnetostriction, chiefly
~oviing to the magnetacaloric effect. Nickel has a ne-
gative volumetrical mag-retostriction, so that its
derivative 'dA/&o is negative too. Thus some amount
of nickel should be found on the descending branch
of.the Bethe curve..(Bete). Any reduction of the
intermolecular distance should increase the Curie
Card 1/3 (Kyuri) point, especially if.the average value of

~On Volumetrical Magnetostriction in Iron-Nickel- SO'1/48-22-lo-16/23
Molybdenum-Alloys
the variable integralis thereby increasing. That
corclusion.is corroborated by the measures of the
displacement of the Curie point with pressure (Ref
Iron has a positive isotheric volumetric magneto-
striction, so.that iron should be found on the
branch of the'Bethe curve. After such a
coordination some alloys changed.the index of volumetrical
magnetostriction (alloy 86) or magnetostriction
becameneutral (alloys 88, 89, 90). Obviously those
alloys should be found in the maximum area of the
Bethe curve. Alloys involvinE a (modified) index
in connection with~thermal work should be found
near the zero lines of the linear magnetostriction
(Ref 1). Molybdenum-permalloy lies away from those
lines. Its inder of volumetrical magnetostriction
remains unchanged. Furthermore the magnetostriction
scarcely chan.-es its magnitude in passing from the
tempered to the annealed state. There are 3 figures,
1 table,*and 5 references,,2 of which are Soviet.
Card 2/3

AUTMI SOV/2o-120,4-22/67
T11TL5j The, Temperature Stabiltzation of the Magnetic Propertiee
of Permalloy (Temperaturnoys, stabilizatsiya mWitnykh
evoyetv pormlloya)
PWRTODTM:~ Voklady Akedemil nauk 33311~ 1958s Volo 120# Hr 4P PP9760-770

ABnRACT-1 lk* present paper Investigaten tbo exact temperature de-
pendence of the qiora of the maeotio anisotropy of the
780 % Us, 179~ %,Fog 308 99 Me* A alnglecryete~ bred
fres the melt served as a s"Plos the simple was of exact
spherical skspe andwas gamseled for 4600 hours at tempora-
or tron 555 to 300 beforebeing investigdod.1he first.,
magnetle anisotropy has a normal temperature
oonstant of
.
in tue case or other "tales within the range:~~
Pendenoe lp:
of from 440 530 and acres Is*, the absolute value of
o
thIg eanotgnt inereaseg w1th decreasing temperatures From
Wto 55e the temperature dependence is *anomalous", i.e.
the Gonstant becomes smaller with decreasing temperature and
Card 1/3 charges Its sign withln the temperature interval of from

30V 20 - 12 04
The T e. m p e va t i. r eja f c) r. u I
494 to rh r e k j,' n,--. e a In p. apparently doEs not lean
to --iui I ibritmi The inventigation of polycrystrilline
.4~o,.ved that viFneto,--triction in the
0 -6
st~ato ul-tuined.bf qv-:~Yiehin- berinni ut 600 1-
alvi in the annt?aled state + 5t9*10' Final thermal treat-
ment ;-,It lo,-. temnarawrez3 con.",isted in rapid cooling do-in
eturting Vrom 'Pile CorlvtAnt of I-otrcny clAc-ined there-
b i f, h t 1,
'Y tomperaturt -'Oj e r, pose
of --,tabilizing p.--z-7.L.-i'llity the material imuit ~e c:onveyel
into a state "anomalouu" t-~mneratu--e devendence of t-e
ont,w" ma;~-netio snl-~otrov.
o on i3 f , es tire dpm
_y ich compensat
Nut
--wt tp- -~neo i~xeroi~ed b,7 ruagtir-tistviction. The correctlielos
of this conclu-11or was t,,cted or, the basis of two eamn-les
another alloy
of standard molybdenum-permallor 19 NS and
~-ihlch is- described. A st3bilizing treatment as described
above reduces the ternnerature-se-c-itivity o;. neripeabilitv
considerably, especially zithin the range of low teuiperatureo.
The here de-sor-1 bed ~ method of -tabillv-tion is effic .Ou s
~Ic I
0
nithin, the temperattire range of from -1960 to +100 Stabiliza--
tion car-, probably be still further improved. There are 3
Card 2/3 rieurei, I table, and 5 ref er,- rice -3, 5 of which are Soviet.

TI T.
rj
3.3 r.
pi; M- v
1119;
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r. ILI :1
Am
14

V,
PHASE I BOOK EXPLOITATION SOV15526
Vsesoyuznoye 3oveshchanlye po magnitnoy strukture ferromagnetikovo
Krasnoyarsk, 19~8,
Magnitnaya struktura ferromagnetikov; materialy Vsesoyuznogo
sove3hohanlya, 10 - 16 Iyunya 1958 g., Krasnoyarsk (Magnetic
Structure of FerromaZnetie Substances; Materials of the All-Union
Conference on the Magnetic Structure of Ferromagnetic Substances,
Held in Krasnoyarsk 10 - 16 June, 1958) Novosibirsk, Izd-vo
Sibirskogo otd. AN SSSR, 1960. 249 p. Errata slip Inserted.
1,500 copies printed.
Sponsoring Agency: Akademiya nauk SSSR. Institut fiziki Sibirskogo
otdeleniya. Komisslya po magnetizmu pri Institute fiziki metallov
MiN.
Resp. Ed.: L. V.,Kirenskiy, Doctor of Physical and Mathematical
Sciences; Ed.:, R. L. Dudnik; Tech. Ed.: A. F~ Mazurova.
PURPOSE: This eollection of articles is intended for researchers in
forromagnotinm and for metal scientists.
Card 1/11

Magnetic Structure (Cont.) SOV/5526
COVL-tIAGE: The collection contains 38 scientific articles presented
at the All-Union Conference on the Magnetic Structure of Ferro-
mignctie Substances, held in Krasnoyarsk :In June 1958. The ra--
terial contains data on the magnetic structure of ferromagnetic
materials and on the dynamics of the structure in relation to
:r-agnotic field c*.=_nZcs, elastic stresses, and temperature. Ac-
cording to the roreword the study of ferrw..agnetic materials had
a succeanful beginning In the Soviet Union in the 1930's, was
subsequently discontinued for many years$ and was resumed in the
1950's. No personalities are mentioned. References accompany
individual articles.
TABLE OF CONTRITS:
Foreword
3
Shur, Ya. S. (Institut fiziki metallov IN SSSR Institute of
Physics of Metals, AS USSR, Sverdlovsk). On the Magnetic
Structure of Ferromagnetic Substances 5
Card 2 1

?-'npnatic Structu~c-a (Cont. SO-T/5526
rbservation of the Domain Structure and tY.4 --1-rkh;,u-r,
1117

,dichev, A. e... -and M. K. Sav,.
M M -~hcnko [Institute of Physica,
Branch AS USSR, Fr-3.,noyank]. IMP:h-anini. Barkhausen

-t In Mkinocr-,rota1% of Tr~-rsform..~r Ste-F'l 151

'I Z~yl
V. M. LutosNcln, ani A. I. Midlklov
I
e
r
Rp
l S
I
nv-srch
; "
nstituLe
entra
ci
ntific
t L
;-il" y]. Sttzdy of tbA Dynarat,:z of tt~c-
Domnln StMeLure in an Ultra3onlc Field 5 51
K i rr, r, k i y, L. V. A. L Drokin,, and V. S. Chnrkarihln
[Inztitute of Phy~;Ics, Siberian Brarich AS USSR, Tzo~a-hers
In,,~titute, Kraznoyarzkl. Effect bf Ultrasound on RaC-
nc-.tic Properties of Ferror.Lignetic Substances at Various
Temperatures 165
Cherkashin V. S. (Institute of Physics, Siberian Branch
AS USSR X Rapidly Changing Stresses
rasnoyarsk]. Effect or
Card 8/11

N 33574
11140
J44.
S/194/61/000/012/069/097
14 1 &P D273/D303
AUTHORS: Puzey, I. M.,.Lutoshkin, V. M. and,Radlkov, A. I.
TITLE: 1nvestigating the dynamics of domain structure in ul-
trasonic fields
PERIODICAL: Referativnyy zhurnal Avtomatika i radioelektronika,-
no 12, 1961t 1~,, abLtract..12E8a_(V. ab. 'Magnitn.,.
st;uktura ferromagnetikovl.-Novosibirskt Sib. otd.,
AN SSSRt 1960t 1515-164)~
TEXT: The influence ofultrasonic~s on ferromagnetics leads to a
relaxation change of domain structures, accompanied by a change of
modulus of elasticity and also of velocity of the ultrasound., At
relaxation times and large,periods of ultrasonic waves, the domain
structure does not have any influence on the velocity of the ultra-
sound. In the case of application of a strong magnetic field, the
domain structure is destroyed and the velocity of the ultrasound
changes, relative.to,the sampleg to a zero field. There takes place
a dispersion of velocity.The passage of ultrasonic pulses through
Card 1/3
Magll~e_

33574
3/194/61/000/012/069/09":
Investigating the dynamics ... D273/D303
tostriction). Disperaion-curves are drawn for nickel, iron and
transformer steel, with measurements not of absolute value of velc-.
city, but of its change on the application of a magnetiefield.
There is an increase in velocity with one in frequency inthe range
.16 Kc/s to.3 - 4 Mc/s. For nickel, hardened steel and iron, Our_!,S_S!
are obtained of the dependence of the damping constants of ultra'.-
sound on the value of the magnetic field at frequencies of 100
Kc/s and 1 Mcls with a maximum daniping.at the beginning of the
curve. Maximum damping and minimum velocity in weak fields are ex-
plained by the increased permeability of the submagnetic state
There is obtained the frequency dependence of the damping cons;ant
for iron (at a frequency .of 180 Kc/s there is a maximum) and for
transformer steel (absorption spectrum). 11 figures. 13 referen.-
.Ces. Z-Abstractor's note: Complete translation.-7
Card 3/3

S/120/60/000/01/030/051
OVE391
AUTHORS: Puzey, I.M. and Sabinin, A.
TITLE: lQj:c~trma~i~et Vfor Physico-chemical Studies
PERIODICAL: Pribory i tekhnika 3ksperimenta, 1960, Nr.1,
pp 104 - log (USSR),
ABSTRACT: In 1950-1955 the authors designed and,constructed,two
laboratory-type electromagnets (Refs, 6,7). The first
of them is shown schematically.in Figure 1. All its
parts, except the wrought pole-pieces, were made of cast
armco iron. The yoke of this electromagnet was a section
of a tube in which two conical (53 0 cone angle) cores
were mounted. The maximum diameter of the poles was
150 mm and the maximum gap between them was go mm, To
produce a uniform field between'the pole-pieces the latter,
were slightly recessed, as suggested by Rose (Ref 8).
The electromagnet weighed about 1 500 kg. Figure 2 shows
the magnetic fields obtainable with this electromagnet
as a function of the number of ampere-turns. For a 17 mm.
gap and a pole-plece diameter of 30 mm the field was
about 32 000 Oe at the gap centre and for a 30 mm gap and
Cardl/3

S/120/60/000/01/030/051
EJOI/E391
Electromagnets for Physico-chemical Stu les,
a pole-plece diaibeter of 50 mm the field was about
23 000 Oe. When a 50 mm gap, recessed at the centre to
54 mm, was employed with pole-pieces of 78 mm, diameter
the field at the gap centre was about 14 000 Oe; all
the three field values just quoted were obtained with
3
8o x 10 ampere-turns. The second (improved) electro.-
,magnet is shownschematically in Figure.4 and its photo-
graph is reproduced in Figure 6. This electromqgnet
weighed 3 500 kg. The cores were again In-thia fdrm of
truncated cones with the cone angle of 830; the'largest
and smallest diameters of the cones were 530 and 230 nun
and their height was 170 mm, (Figure 5). The "legs" and
the pole-piece5 of the electromagnet were made of wrought
iron purer than armco iron. Figure 7 shows the magnetic'
fields in air Saps obtainable with the second electromagnet.
By adjusting the position of the "legs" highly uniform
fields could be obtained (from 10 000 Oe for a gap of
120 130 mm and a pole--piece diameter greater than 200 M)
Card2/3

5/12o/6o/ooo/ol/030/051
EJ014E391
Electromagnets for Physico-chemical Stu le
In a small gap (5-6 trun) and with pole-pioces of 10 mm
diameter, fields up to 50 000 Oe could be obtained. All
these values were obtained with 180-200 x 10 -7 ampere-turns.
The total power which had to be supplied to the second
electromagnet amounted to 10 -, 18 kW. Both the first and
the second electromagnets were mounted so that they could
easily be rotated about a vettical axis passing through
the centre of the gap. The second electromagnet was found
to be satisfactory in laboratory investigations,:such as
studies of anisotropy, etc. Acknowledgments are made to
P.G. Sabinin and M.M. Suchkova for the.design work
connected with the electromagnets and tolI.P. Bardin
(deceased) for his help.in construction. There are
figures, 1 table and 12 references, 5 of which are
Soviet, 4 English, 2 German and 1 French.
ASSOCIATION- Tsentrallnyy nauclino.-issledovatellskiy,institut
chernoy metallurgil (Central Scientific-research Institute
for Ferrous Metallurgy,
SUBMI'ITED: December 22, 1958
Card'x Pz

.-SI/0-58/61/000/Oli/ol8/025
A058/Aioi
AUTHOR: Puzey, I. M.
TITLE. Investigation of the magnetic anisotropy energy of nickel
PERIODICAL: Referativnyy zhurnal, Fizika, no. 11, 1961, 241, abstract 11E517
Sb tr. Tsentr.-n.-i. in-t chernoy metallurgii" 1960, no. 23, 139-
14q)
TEXT: 'The temperature dependence of the anisotropy, constants K, of a-
single crystal composed of 99.92% Ni, 0.035% Co, 0.008% Fe, 0.02% Cu, 0 *009% S,
0.03% C and 0.001% P and having a specific weight of 8.926 g/cm at 200C was
studied by the mechanical moment method in the range from -252.8 0to +271.80C.
It was e*tablished that at I-252.80C in a field H - 11,250 oerstnds K - -403.4
104 erg/cm3, while for extrapolation to H -40 KI w-105.36 . 10 er;~c,3. With
increasing temperature the curve of Ki.versus T decreases monotonously ino
absolute magnitude, and at high temperatures changes sign; K 0 at 217 C
Above this temperature up to +2720C the value of K is small 300 erg/cm3).
Thus, the possibility of a change In sign of KI, WLch was,*prediated by S. V,
Vonsovskiy (Zh. eksperim. I teor. fiz., 1938, no. 8, 1104) was substantiated
Card 1/2

'n'7--
1~

2P,556
8/137/61/000/009/038/087
A-1-60,/A101
AUTHORS: I.m., Molotilov, B.V.
TITIE:- Magnetostriction of nickel-iron-molyWenum alloys
PERIODICAL- Referativnyy zhurnal. Metallurgiya, no. 9 51, 11, abstract 9Zh64,
C'Sb. tr., Tsentr. n.-i.- in~t chernoy metallurgii", 1960, no. 2_3,
15Q 160).
TFM: The magnetostriation of'Ni-Fe-Vio alloys is Investigated as a func-
tion of ordering and temperature. The measurement of magnatostriction was car-
ried out by the bridge method. Tensometers we~ra cormected 'Ln.all.four arm4; of
the bridge (two of -them working,two fox, :!ompensation.). The working t-ensometers
wer glued onto different sidesof the apsaimen. The magne"ostrijtion -was mea-
sured in the electromagnet iffiff -L(IFS-1) in fields tip to 17,000 oersteds. Both
polycrystalline and monocrystalline.speci-mans of alloys obtained in va"vm frj,.)m
the'melt were investigated. It, was-established that the crdering leada to the
displacement of the zero line (~,- 0) towards th-s NI aidex but no more than 1%.
The magnetostriction constants of four single zrys-tals having compositions clcse
to the zero values of magnetostriction are cited. In the ca3e Of single Q1-ya-.alr,
Card 1/2

28556
S/1 37/~ I.Ar-OIX 9/0.38/0 B7
Magnetostricti,= of n1okel-iron-molybienum alloys AY-ACIA101
the displacement of the zero line alao takes place. Tha of the zero
lines 'AJOO = 0 and )6111 = 0or, tne phaae gi-Fe-Mo triangle mad!4 it poss-41ble t-)
make the tk-region more precise. All alloys the compoalzions of which lie in
that region have physical constants such as mo favor the obialnlng of a high
permeability. Despitle the low value of magnetostriction of the alloys invest!-
gated,(r4lo-6), It was possible to investIgate itz'timperature dependence. For
poly- and mono-crystallina apsoimnne ma~nat-.xitricilon dgereaues merv)tjnously -a3
the temDerature increases.
A. Ruzakov
[Abstracter's note: Complete translation
'Card 2/2

S/126/60/009/02/020/033
AUTHOR: Puzey. 10M. E062/E335
TITLE: Special Features of.\the Temperature Dependence of the
Maxnetic Anizotrop Nnergy of Fe-Al Alloys
PERIODICAL: Fizika metallov i metallovedeniye, 1960, Vol 9, Nr 2,
pp 279-282 (USSR)
ABSTRACT: The author had previously pointed out (Refs 1,2) certain
anomalies (e.g. maxima, revevals of slope and of Sign) in
the -temperature dependence of the magnetic anisotropf?ffy(Ni,
Fe, Co) alloys near their magnetically isotropic condition,
The temperature variation (from -196 to 400 OC) of the
anisotropy constant is now reported for the case of both
annealed and quenched samples of Fe-Al alloys (7*4 to
16910 Al). Peculiar features are observed and explained in
terms of the ordering process and also of the difference
between the magnetic moments of Fe atoms surrounded by
8 Fe atoms and those surrounded by 4 Al and 11 Fe atoms.
There are 6 figures and 12 references,6 of which are Soviet,
1 German, I French and 4 English.'
ASSOCIATION: Institut pretsizionnykh splavov TsNIICh]61 (Institutj,~~
Precision Alloys, TsNIICbbl)
SUBMIWED: 7__j_u_1Y6, 1959
Cardl/1

S/126/60/009/02/025/035
E073/E335
AUTHOR: Puzey' I.M.
TITLE: Features -&-f-the Temperature Dependence of the Energy of the
Magnetic Anisotropy~~f Crystals in the Neighbourhood of
the Magnetically Isotropic State
PERIODICAL: Fizika metallov i metallovedeniya, 1960, Vol 9, Nr 2,
pp 302 - 303 (USSR)
ABSTRACT: In earlier work (Refs 1 2) the author found that in the
neighbourhood of the magnetically isotropic state single
crystals of binary Fe-Ni, NI-Co, Fe-Co alloys and also
molybdenum permalloy, within a certain temperature range,
a temperature dependence was observed for the constant of
magnetic anisotropy which is similar to that observed by
.Bozort for MnBi and Mn 2Sb (Ref 3). This can be explained
as follows. According to S.V. Vonsovskiy and Ya.S. Shur
(Ref 4), in addition to the energy and natural anisotropy
U it is necessary to take into consideration the
0
elastic one plus the magnetic elastic energywhich is
determined by the following expression in cubic crystals:
Cardl/4

6663h
s/i26/6o/oo9/02/025/033
E
Features of the Temperature DependenceOWW Energy of the Magnetic
Anisotropy of Crystals in the Neighbourhood of the Magnetically
'Isotropic State
9 2 2
U - (C X C X1 0 2C 44% )f(S S
1 4 11 100 12 0
where Ciii C 129 C 44 are elasticity moduli and
are magnetostriction constants. If X
100 Ill 100
and X are small, the temperature characteristic of
ill
the anisotropy energy is determined by the behaviour of the
energy of the natural anisotropy U in the same way
0
as for molybdenum permalloy (Ref 1), where changes in the
near range order of:the solid solution bring about
radical changes in the temperature dependence.. In
particular, there will be a change in the sine of the
constant and a reversal of the temperature dependence,
formation of a maximum although the elastic properties and
Card2/4

66634
S/126/60/009/02/025/053
E?7~4E3jg
Features of the Temperature Dependence 6 e ergy of the
Anisotropy of Crystals in the Neighbourhood of the Magnetic,~,L~.,-"
Isotropic State
the magnetostriction change little. Areverse temperature
dependence, a maximum or minimum can also be due to other
causes, particularly in the case of large values of X
100
and X U can be of the order of 1 000 erg/cm' and
differs in sine from that of U whereby the total
energy U +-U may equal zero for a certain concentration#
0
It is assumed that Uo/ 07 Ul> 0 and U 0 + Ul > 0
if the dependence of U and U an the temperature
is the usual one but ~Ou 0/dtj >. JdUl/dt then the
temperature characteristics of U + U will be reverse.
0
ones, i.e, the anis-otropy,energy will decrease with
increasing temperature- A reverse temperature dependence
and a change in sine are possible also for some other
Card3/4

68634
s/126/6o/oog/02/025/033
E?7j4Z3jR
Features of the Temperature Dependence o e ergy of the Magnetic
Anisotropy of Crystals in the Neighbourhood of the Magnetically
Isotropic State
relations between U and U and their derivatives,
0
The elastic plus the magneto-elastic energy have a strong
influence on the temperature of the anisotropy energy in
such alloys as Fe-Co, NI-Co and others, which have.a high
magnetostriction.,
There are 4 Soviet references,
ASSOCIATION: Inst:Ltut pretsizionnykh sp~avo.v".TzN1IChM AInstitute of
Prue-IsiLon Alloys, TsNI1C1-x1-1)
SUBMITTED: March 5, 1959, initially,
Slon.
May 18, 1959, after revi
Card 4/4

S/028/60/000/010/014/020
BO13/BO63
AUTHORS% Gabrielyan, D. I., Klevitskaya, G. Z., Puzey, I. M.
TITLE: Magnetically Soft Precision Alloys
PERIODICAL: Standartizatsiya,.1960, No. 10, PP- 48-51
TEXT: This is a report on a stands rd worked out at the Tsentrallnyy
nauchno-issledovatellskiy institut chernoy metallurgii (Central.Scienti.lfic
Research Tnstitute of Ferrous Metallurgy) for magnetically soft precision
alloys, which classifies precision alloys into five groups: 1) 45H (45N)lq
and 50 H (50N)%with increased permeabili y1land high magnetic saturation;
2) 50~in(5(Yli-P),%q65~ln(65NP)~'434~ii4mn(34NKMP),Ilsand 47HMi1(47NMP)'tha-.,e a.
_,a.1 or magnetic texture;
h1ph maximum porm9abillty and a crystallographic
3) 50HXG(52!!~hS X613 HC(12~~,dand 42 K(42110)111have an Inorelped
permeability and a ~.Jgh electrical renistan"~'e-,- 4) 79H14(Z2.11-01'"JI16
(80NKhS),%'678H(78N),%"76HY,A(161ff.LD),1460 Vi~-J(eoNiLh)~74HMA474NMD),10and
-4 9NMA iihave a high permeability in weak fields; 5) 50 KO(50KPI Vhas
7
9 PmThmj
the highest saturation induction. 45N, 50N, 50NP, 65NPi 50NKhS, 79NM,
8ONKhS, and 50KF are well-known standardized alloys, which are produced
Card 1/3

Magnetically Soft Precision Alloys S/028/60/000/010/014/020
B013/Bo63
in a great variety and in large quantities. Table I compares technical
data of the alloys specified in the above standard with foreign alloys.
It may be seen that only the alloys 50N and,50NP have poorer magnetic
properties than the Western alloys 5000HZ and Hypernic. The alloys
50NKhS and 8ONKhS, developed at the Institut pretsizionnykh splavov
TsNIIChermet (Institute for Precision Alloirs of TsNIlChermet) are
unmatched. The alloys 47NMP, 34VKMP, 38NS, 42NS, 78N, 76NKhD, BONKh.
and 74NMD, whose production has been started right now) will not be
standardized and are produced according to technical specifications. The
standard described here is based on various technical specifications,
FOr-75572-50 (GUST 5572-50), abundant material made available by
manufacturers, results of research work done at the Institnte, for, Pr.eoision
Alloys, and many data from foreign publications. Magnetically soft materials
are characterized by many parameters of which the standard considers the
original and the maximum permeability, the coercive force, saturation
induction, and, in some cases, the "orthogonality" of the hysteresi.5 loop,
Furthermore, the standard specifies the dimensions, tolerances, and the
surface state of the metal, taking into account the possibilities of the
manufacturer's equipment. The static magnetic characteristics of these
Card 2/3

GABRIELYAN, D.I.; KLEVITSKAYA, G-Z-; PUZAY, I,K-

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17847
S/133/61/000/008/016/025
.240'9
A054/A12q
Or"
IHORS: Puzey, I.M., Pluchek, B.Ya.; Suvorov, V.A.
TITLE: High-perm6lable iron-aluminum alloys of, 1012 (Yu12) and ~O 12K (YU12K)
grades
PERIODICAL: S tal no. 8, 1961, 742- 744
TEXT: The application of iron-aluminum a]5r)ys as magnetic and structural
materials is discuesed it Refereme I (A.M. Samarin, Elektrichestvo, no. 7, 1960).
A Soviet alloy prepared by B.G. Livshits, N.G. Lakhman and X.V. Emmil [Ref. 4.i
Trudy TsNIlChM,(Transactions of the TrsNI1ChM), v. 23, 1~60, 1941 contains 14 - I I
359 Al and some additions of molybdenum and me-rganese. This alloy displays high
magrietio propertiez after hardening from 6GAOC in water. A new Soviet Iron-alu-
minun aJ_11oy was also developed with a high permeability and ordered structure,
containing vnly 12% aluminum and 88% iron. The test metal was molten in an in-
du:,,tlcn vaojum furnace (magnesite crucible) from armco iron and AS-000 (AV-000)
type aluminum. Pouring into sheet bara took place in argon atmosphere. After
J131cw heating to 1,OOOOC the sheet was rolled to 2.5 mm thickness without. any in-
ter.mediate hhaating, next the st-rips were heated t,,j 6000C and rolled to 0.35 mm
Carl 1/5

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S/133/61/000/008/016/025
Hig~., permeable ircri-alumin-am alloys of.... A054/A12q
1with s=oth edgea). OH~ magnetic tezrs were carried out on toroidal samPles
with an internal diam-r--ter of 20 trip. and an ext'ernal diameter of 30 mm. ' Fi_zure 2
showe, t~ie dsperidence of m5ximum magnet-ic permeability and coercitive force of Vie
10
al5zy on !',a aluminum oontent aft-:~r annealing In vacuum a:t 1,100 and 1,2500"
0 1 DOC for 3 h. Min'mum Coer-
I h with -:.o llng to 60010 at a 100,-~C/h rate and the 301.
citAve force arel a very steep peak. of maximum permeability were obtained with a
'12-',% aluminum content. The pe--k is narrow and is caused by the sharp decline of
the curve of dependence of anisotropy constants on the. alloy's composition. The
study of the rellationship between -maximum Dermeability of the 12-% aluminum alloy
and 1-hour amiealing shows that pe-rmeability Increases with the rise In tempera-
Annsaling temperature, OC ... 1, 000 11200 1,250
fmax, 10:3 gauez/oerated ..... 18 72 128
The atudy of specific. elsotric resist-ance of ircn-aluminum alloys with.12 - 13%,
a"'Iminum ccntent; depending on fttierzmal treatment showed that minimum electric re-
sl stan_,e, was f o1jPd in- all, -13 --1 &f ter hardening in water. When bardenIng In oil, re-
sistartae Is. a little higiner. Long-term annealing increases the electric resist-
ance o2 ecrtaining ltess than 11.5% aluminum. Upon increasing the aluminum
ccritent, electriz resi-stance rapidly decreases. Alloys with a 12-% aluminum
bard 2/5

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S/133/61/000/008/016/025
Highpermeable Iron-aluminum alloys of.... AO54/A129
tent, after being cooled to 2000C at a 5VC/h rate and subsequently in furnace,
have a apoolf1c electric resistance of 1.07 ohm - mm2lm. Tests were also carried
out with alloys containing 2% cobalt ben4den 86% Iron and 12% aluminum. The ta-
ble shows that the binary Yu12 and tortint-,tj Yu12K alloys could be obtained with
ordered magnetic properties, approximat.ing, those of the high-ni ckel- containing
permalloys. The Yu12 and Yu12K alloys have a higher electric resistance2 (above 1
ohm - mm2/m) and a lower specific gravity (6.8 g./cm3) than those containing nick..;
e1. They have also a high resistance to corrosion and plastic deformation after
annealing, and are, moreover, isotropic. Compared with the 50" (50N), 50HXC
(50NKhs) and 3814C (38NS) nickel-alloy'S the iron-aluminum alloys display a steeper
permeability curve and are magnetized in fields of a much lower voltage. The
watt-losses are lower in the new alloys due to their high electric resistance.
,They are suitable for transformer cores working at high frequencies, for magnetic
amplifier cores, stators, runners and whenever a high chemical resistance is re-
qul.red. There are 4 figures, 1 table 'and 5 references: 2 Soviet-bloc and 3
non-Soviet-bloc. The references to the English-language publications read an
follows: J.F Nachman, J.W. Buehler, Journal of Applied Physics, 1954, v. 25,
no. 3, 307, ~.F. Nachman, J.W. Buehler, Electrical Manufacturing, 1956, no. 11;
M. Hansen, B. Anderno, Constitution Diagram of Binary Alloys, N.Y., 1958.
ASSOCIATION: TsNTIChM
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S/14, 6/61/011/004/004/o23
Z073/X535
AUTHOR. -zey. I. M.,
TITLE: Dependence of the 2nergy of Magnetic Anisotropy of
Invar on the Temperature and the Field
PERIODICAL: Fizika metallov i metallovedeniye, 1961, Vol.11. No.4.
pp-525-528
TEXT: Invar has a number of anomalous physical, properties: a
large magnetostriction, a low coefficient of thermal expansion. a
high susceptibility of the paraprocess, a flat temperature
dependence of the saturation and a possible "latent" antiferro-
magnetism. R. M. Bozorth (Ref.3) determined the constant of the
magnetic anisotropy of invar at room temperature but no data are
given in the literature on the temperature and field dependence of
this constant. The author determined the anisotropy constant of
invar (monocrystalline sphere of 10.720 + 0.0005 mm diameter) in
the temperature range from the hydrogen iemperature up to 3200C in
fields between 6000 and 23 000 Oe. The temperature dependence of
the anisotropy constant, measured in a field of 10 3000 Oe, 3for invar
containing 36% Ni, rest Fe in plotted in Fig.1 (10 erg/cm Va.
temperature, 00. The curve is similar to the corresponding curve
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Dependence of the tnergy of S/l26/6i/OijL/Oo4/oo4/023
2073/9535
for Ni, i.e. a sharp rise at low temperatures and a change in the
sign at +1000C. The dependence of the anisotropy constant on the
field,;trength at varioustemperatures is plotted in Fit,21
K, er cm-3 v9. H, Oe (curve 1: -252-70C, curve 2: -195 ,
curve 3: +19.10C, curve 4: +81.20C, curve 5: +114.20C, curve 6:
+263.70C, curve 7: +175 50C). For both positive and negative-values,
the constant increases ;ith increasing field intensity. In the
temperature range 70 to 1200C changes in the field strength leads
to a change in the sign of theconstant. The absolute increase in
the anisotropy constant with increasing temperature on increasing
the field strength from 6000 to 22000 Oe becomes less pronounced as
the Curie point in approached but the relative change in the constent
decreases rapidly. Thus, at the liquid hydro gen,temperature it in
7.7%; at the nitrogen temperature it is 8.2%; at room temperatureit
is 50% and at,81.20C it in almost 100". According to data obtained
earlier by the author of this paper (Ref.4),the change in the constant
of nickel for the here investigated field range was 3.8% and at room
temperat ure this magnitude equals 9%. According to L. V. Kirenskiy.
R. S. Nosova and N. V. Reshetnikova (Ref.10). the value of 9%
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E073/E535
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u
?0

/

0
0 l

S/126/6i/oll/005/005/015
E073/E535
AUTHOR: Puzey,,I. M.
TITLEz ,Dependence of the Energy of Magnetic Anisotropy of
iron-Nickel Crystals on the Temperature
PERIODICAL: Fizika metallov i metallovedeniye, 1961, Vol-11, No.5,
pp. 686-692
TEXT;*, The aim Iof the work was to investigaLe systematlically
the temperature dependence of the anisotropy constant of iron-
nickel alloys.in the y-phnse.range and also the influence of
heat treatment on this dependence. This is considered particular-
ly important since the heat treatment influences the structure
of the y solid solutions within a wide range of nickel concentra-
tions. The experiments were made.on single.crystal spheres of , 1 1
7 to 11 mm diameter produced from the melts Specimens 1,2,3,and.
12 contained 100, 88.4, 85.5 and 35.0 at.% Ni (for these the
k(T) curves are not given in the paper). Specimens 4,5,8,9,10 and
11 contained 82.5, 76.7, 70-5, 65.5, 52.4 and 43.8 at~% Ni,
respectively. In earlier work (Ref.l: Izv.AN SSSRI, ser.fiz.,
1952., 16, No-5, 549) in which specimens 1-11 were investigated at
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'Dependence of the Energy of S/126/61/011/005/005/015
E073/E535
room temperature, the dependence of.the constant on the composi-
tion as regards Ni Fe showed an asymmetry in the ordered state.,
Therefore, the autAor considered it of interest to get more
accurate information for specimens with compositions approaching
Ni Fe. For this purpose specimens 5-7 were again chemically
an2lysed after the tests (the results were practically the
:ame as
before). Furthermore, the orientation of the crystal axes a
Measured with an accuracy of In addition to high tempera-
ture annealing, the specimens were subjected to the following two
types of heat treatments 1) Heating to 600*C followed by cooling
to 3009C for 15-20 days (this is referred to as "annealing");
2) heating to 700% and quenching-in water (quenching9.. The
invar specimen was annealed at 1000*C in vacuo in a quartz
ampoule and was then cooled in air together with the ampoule. For
determining the anisotropy constant, the mechanical moment was
measured which acts at various temperatures on the single crystal
in the plane (100) for 24 orientations of the magnetic field.
differing by steps of 15*, From the obtained results the fourth
harmonic was determined and the anisotropy constant calculated.
The-accuracy of measuring.the angle was 7.5 min, the accuracy of
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2 9 641
Dependence of the Energy of S/126/61/011/005/005/015
E073/E535
measuring the mechanical moment was 0.2%. Since 24 moments wer
measured, the accuracy of determining the anisotropy constant i:
almost fi-.rp +-inloq AR biwh as it would be if a single reading was.
used. T h e t o r q u e was measured in a magnetic f ield of
10 000 Oci for nickel at low temperatures a field in excess
of 17 000 Oe was applied and the results were extrapolated for an
infinitely strong field by a method described in earlier work of
this author. The temperature was determined by means of a
platinum resistance thermocouple.with anaccuracy of 0.1% The
temperature dependence of the constant of the anisotropy energy
(K), was measured on face-centredaingle crystals in the tempera_
ture range -252.8 to +250*C. At the edge sections of the y-phase
a strong temperature dependence was detected at low temperatures
and an inversion of the sign at high temperatures. In the neigh-
bourbood of the zero values of the constant, corresponding to the
composition approaching Ni Fe, an "anomaly" was observed in the
liquench+ed" specimens, i.e.3a non-monotonous character .of the.
temperature dependence. This "anomaly" teased after the specimens
had been transformed into the ordered state by annealing, as a
result of which there is a strong increase in the anisotropy energy,
asymmetrical with respect to N! 3Fe. at all temperatures.
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Dependence of the Energy of S/JL26/61/oljLT()95/005/OJL5
E073/E535
Smoluchowski (Ref.14~- J, phys,et rad,, 1991, 12V 389) expresses
the view that the asymmetry is caused by the influence of the
exchange energy on the process of ordering. Since this energy
increases with increasing Fe content, the ordering energy in the
alloys will be asymmetrical relative to the Ni 3Fe composition,
which leads to an asymmetry in the phase curve of order-disorder
transformation. Apparently this is the cause of asymmetry of
the temperature dependence of the anisotropy constant. There are
8 figures, I table and 14 referencess 8 Soviet and 6 non-Soviet.
The references to English-language publications read,as followst
Bozorth.,,R.M. Rev. Mod. Phys~. 1953, 25. 42; Dillinger, J.,
Bozorth, R. Physics, 1935, 6, 279; Bradley, A.J., Jay,A.H.,
Teilor, A. Phil. Mag. 1937, 23, 155~~ 545,,
ASSOCIATION: Institut pretsizionnykh splavov TsNIIChM
(Instituteof Precision Alloys TsNIIChM)
SUBMITTED3 August 12, 1960
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E073/E335
AUTHOR: Elliz e y 1-1
TITLE: Influence of Cu, Si, Cr and Mo on the magnetic aniso-
tropy and the saturation induction of N11-Fe,single
crystals
PERIODICAL: Fizika metallov I motallovedeniye, v. 12, no. 3,
1961, 453 - 455
TEXT-, The single crystals -were prepared and investigated as
described in an earlier paper by the author (Ref. I - AN SSSR,
ser. fiz., 1952, 16, no- 5, 540)--- All the data gaven relate to
specimens that have been water-quenched from 600 C. A part of
the phase diagram of the Ni-Fe-Cu system is plotted in Fig. I
the dashed 1.1nes represent the lines of constant saturation
induction, based on results published by 0. Anvers and
H. Neuman (Ref.*2 - Wiss. Ver8ffentl. a.d. Sivnens Werke, 1935,
14, no. 2, 93); the arrows indicate the magnitude and sig~n of
the anisotropy constant. Due to the limited solubility of Cu
(5-50,'U') , single crystals containing up to 5% Cu only were
prepared. By utilizing data of the anisotropy energy for Ni.-Fe
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S/126/61/012/003/017/021
Influence of E073/E335
alloys and by carrying out a linear extrapolation for the range
of 30,'
0 changes in the content of Ni and Fe, a zero anisotropy
line was plotted, which is approximately parallel to a constant
Ni content line.. Similardata for the system 3Ni-Fe-113are
plotted In Fig. 2 (composition, at.%; 2 x 10 erg/cm',- 8 kgausa)i
the lines of constant induction are plotted from data obtained
both by the author and by Bozorth. The lines of zero anisotropy
are based on data entered as arrows and on data obtained for
Ni-Fe alloys. The lines of constant Induction and zero ariLso-
tropy form small angles with the base line (Ni side) and are
inclined In opposite directions. The position Is similar for
Ni-Fe-Cr alloys; in alloys with Cr the induction and isotropy
lines are somewhat steeper than in alloys with Mo. Fig 4 shows
a similar diagram for the system Ni-Fe-Si (contents, All
the alloys with Cr which were investigated had a negative
anisotropy constant. The isotropy compositions are to the right
of these and the isotropy line should be inclining towa--ds the
Fe corner of the diagram. It was of interest to note that with
increasing content of Si the anisotropy constant K increases.
Ca rd 2.1'~4,

S/126/61/012/003/017/021
Influence of .... E073/E335
Thus, for a content of 11.6 at.*,O' Si and 70.9 at.% nickel
K = -6-23 x 104 erg/cm3 , i.e. higher than for Ni, although the
saturation induction of such an alloy,is BS = 5 300 gauss, i,.e.
towor tlinri for Nt. The results show that from the point of view
of iogr nattirntion Induction, Lhe Allaying elomeritn onij fie
grotiped In the following sequonce: Cul SI; Crj Mo. For these
four elements the saturation-induction gradient along the line
of a constant NI:Fe ratio of 2-7 is 150, 550, 600 and 900
gauss/at.0", respectively. The ratio of these gradients is
'0
1:3-7:4.o:6.0 at room temperature. In.the case of binary alloys
of Ni with the same elements, the ratio of the gradient is
1.-.4:4.4:5.5 (low temperatures) (Ref. 4 - C. Sadron, Ann. de
Phys., 1932, 17, 371; Ref. 5 - V. Marian, Ann. de Phys., 1937,
7, 459). Thus, the ratio of the gradient remains approximately
equal. For binary Ni-base alloys with Cu, Zn ' Al, Si, Sb and
Mo, the change in the saturation was explained by E.C. Stoner
(Ref. 6 - Phil. Mag., 1933, 15, 1018) and N.F. Mott, H. Jones
(Ref. 7 -.Theory of the Properties of Metals and Alloys, Oxford,
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S/126/61/012/003/017/021
Influence of .... E073/E335
1936). According to them the electrons of the outer shells
of the admixture atoms become transferred into the 3d-shell of
tile. Ni atoms due to the more satisfactory arrangement of their
energy states, and.compensat*e each magnetic moment by I Bohr
magneton. As has been shown in earlier work of the author and
N.S. Akulov, in Ni-base binary alloys (Ni-Cu, Ni-Mo, Ni-Sn) the
anisotropy.constant decreases with the composition in the same
ratio as saturation. As a result, the curves of the saturation-
dependence of the anisotropy constant are similar. From this,
the conclusion is drawn that charges of Cu, Sn and Mo ions have
no specificInfluence on the anisotropy constant and that their
effect manifests itself through electron concentration and, in
final analysis, through the average magnetic moment of the N!
atoms, since -the Cu, Sn and Mo atoms have no magnetic moment. Oil
transition from the Cu region to the Cr and Mo region, the
negative anisotropy decreases appreciably. The line of isotropy
is always more inclined to the base line at the Ni corner of
the diagram. The Ni:Fe content ratio along the anisotropy line
increases. Forturnary alloys and concentrations of Cu, Cr and
(-~,ard

S/126/61/012/003/017/021
,.Influence of .... E073/E335
Mo between 0 and 2.5% this ratio changes, respectively,
between 206 2.9, 2.6 - 4.6 and 2.6 - 4.8. Assuming that
even in ternary alloys the charges of Cu, Cr and Mo ions have
no appreciable influence on the anisotropy constant, at least
-when present in small concentration, the conclusion can be drawn
that in ternary alloys with Cu, Cr and Mo magnetic neutralization
primarily of the N! component will occur since the range of
.negative anisotropy narrows toan increasing extent on tran-
sition from Cu to Mo (in binary Ni-Fe alloys the range of
negative anisotropy energy extends between 100 and 72-50% Ni).
Si alloys behave differently. The isotropy line Is inclined
towards the Fe side of the diagram and the negative anisotropy
is greater than in Cu-containing alloys. This is explained by
the fact that the heat of formation of a solid solution of Si
in Fe is 20 kcal/g.atom, that of Si in Ni being 37 kcal/g.atom.
This.1s apparently why in Ni atoms which are adjacent to Si
atoms, transition of the electrons into the 3d-shell is
energeticallyless favourable, as a result of which the range of
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Influence of .... E073/E335
negative anis tropy becomes wider. The conclusions could be
0 1
checked by measuring partial magnetic moments in alloys by
neutron-,diffraction methods but such data have not been published.
There,are 4 figures and 10 references: 4 Soviet-bloc and
6 non-Soviet-bloc. TheEnglish-language references are quoted
i. nthe text. ~bstracterf 9, note:, this is a complete translationd
ASSOCIATION: TsNIIChM im. I.P. Bardin
SUBMITTED: December 13, 1960
FAbstracter's note: this isa completetranslation
Card 6/~

3/04#6'10,~1025/012/015/022
DI 17/B104
AUTHORs' Puz*y, I. M.
TITLEs Crystal and magn etoelao tic eneray of anisotropy and its
dependence on temperature in iron-nickel sonoorystals
PERIODICALs Akademiya nauk 33SR. Izvestiya. Seriya fizichookayat v. 25,
no, 12, 1494 1497
TEXT* The course of temperature of the anisotropy constant. of a series of
Monocrystale in the high-temperature range, and the physical cause of sign
alteration of the anisotropy constant in the nickel and invar range were
studied. Spherical monocrystal samples grown from the melt by slow
cooling were first investigated. The method of investigation is described
in previous works. The @"plea war* quenched after annealing at high
temperatures. Two sections, to which the sign of the anisotrolreonotant
changes, were found to exist in the face-centered phase of Fe-Ki alloys.
The first section starts with pure nickel and includes alloys with a nickel
content of up to 85%i the tomperature of isotropy rising with decreasing
nickel content, The second section comprises compositions with a 30 to,
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31606
3/048/61/025/012/015/022
Crystal And magnetoolastie ... B117/B104
55-60% nickel content. On the first section, the negative anisotropy
constant becomes positivet and 'an the second, the positive change into a
negative one. It was assumed that this alteration of signs was caused by
the magnetoelastic component of the energy of anisotropyq 'Thereforet the
following was investigated on monocrystals of Fe-Xi alloyss (1) moduli of
elasticity and their dependence on the temperature and on the fieldt (2)
magnetostriction parameters and their dependence on the temperature and on
the field. The following monocrystale were investigatedi.(I) 100% of Ni,
.0% of Fe; (2) 76% of Ni, 24% of Fe; (3) 80% of Ni, 20% of fog (4) 36% of
Ni, 64% of Fe. In summary, the following was founds In the range of
comDositions showing a high nickel content, pagnetoelastic energy is posi-
tive; it is negative from the side of invarl the total energy of anisotro-
py is negative in the range of nickel, and positive in the range of invar.
The moduli of elasticity change relatively slightly with temperature.
Magnetostriction changes linearly. Since magnetoelastic energy is a
square function of the magnetostriction constants, it will decrease con-
siderably more slowly than the crystal energy. This leads to an alteration
of the signs of the anisotropy constant at high temperatures since the
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0

S/776/62/000/025/06;~NZ5:
AUTHOR:
ze M.
TITLE: The temperature of the magnetic -anisotropy energy 0~_;'
single crystals of Iron-Nickel alloys.
SOURCE:. Moscow. TsentralInyy naiichno-issledovatell'skiy institut chernoyl, v
metallurgii. Sbornik trudov. no.25. Moscow, 1962. Pretsizio=yye
s plavy. pp. 5 3 - 7 0.
xperimental ii -a,continuation of the u#
TEXT: The present e avestirration is a
a , -or
earlier study of the energy of magnetic anisotropy.of.Fe'-Ni single crystals a~_
C. I room,
temperature (AN SSSR, IZV.,.'L; ser- fiz., no.16, 1952,,549). The present workinves-
tirfates the temperature (T) dependence of the anisotropy constant-of the re-Ni
alloys and the effect of heat treatment on that dependence. The.specimens w re in
the shape of a single-crystal sphere, 7 to 11 mm diam f: 0.0005 mm. The cremical
comuosition of the specimens is tabulated. Chemical analyses were made be4pre
and after the tests to detect any changez~ therein. The orientation of the crystallo-
graphic axes was determined by the.magnetic method with an accuracy. of ':E 1
The HTs are specified in detail. The magnetic -anisotropy constant was meals, red
by means of the mechanical moment that acts in the single crystal in the plane. (100).....,
Card 1/3
I T II I I

The temperature dependence of the magnetic- S/7761621,000/025/003 25.
for Z4 positions of the magnetic field (MF)" i.- e., at 150 intervals.- The values of
the mechanical moments were used to determine the fourth harmonic and therefrom.
to calculate the anisotropy constant. Measurements made with increasing, and. de-
creasing T showed that there was no hysteresis attributable to thermal inertia, at
least at the slow heating and cooling rates employed. The field utilized has 10,000'
except that a field of 17,000 4 was used for the Ni at low T. The results of the
measur~ements are detailed in a 3-page table and are illustrated in 11 graphs..,~The
anisotropy constant of Ni grows very steeply with decreasing T. Upon addition of
Fe and quenching,the steepness of the curve decreases with the approach to the
isotropic alloy, whereupon it steepens again'up to the invar alloys, in which it.
attainsthe same value as for Ni. In the ordered state the T dependence. remains
great, even in the region of the, stoichio metric composition; it is greater for alloys
with 74.3 at-To Ni and 70.5% Ni than for the alloy with 75jo Ni. The sign reversal of
the anisotropy constant, which is characteristic of Ni at high T., is not observed up
to 3000, even in an alloy with 88.4 at-7o Ni. Inasmuch as at such concentrations no
long-range order is observed, we are dealing here apparently with transformations
of the short-range type. In t*.-e alloy with 85.5 at-5) Ni the anneal and quench
curves diverae considerably more.' At a temperature of 9_580j ordering processes-
are observed in the alloy, and the quench curve takes a steep turn toward an
approach to the anneal curve. All of thisoccurs within 30 min, the time of heating:',.-.-.",.
Card 2/3
F I

P1
1/776/62/000/025/0(
AUTHORS: Puzey,. I. M., -R~ad'kov, A. 1. 1
TITLE: Investigation of the dispersion of ulty'asound in ferromagnetic subjOance i."_
SOURCE: Moscow. Ts entrall nyy nauchno -is sledovatell jkiy ins titut che rno
y
metallurgii. Sbornik trudbv. no. 25. Moscqw,'1962. Pretsizionilky,
e
splavy. pp. 71-85.
TEXT: This experimental investigation deals with.tKe profound effect thatthe-
interrelationship between elasticand magnetic phenomena exerts on the passap of-
ultrasonic (US) waves through fe-rromagnetics. : US, affects primarily the domain
structure in a manner analogous to a magnetic field, so that there is a displacement
of the boundaries between domains. This displacement remains reversible with
small amplitudes. The present investigation deals with the dynamics of the action
of US on the domain structure, which -,because of the absence, of any effect a~ialogous'
to the skin effect of the magnetic field, -, is considerably more.deeply peneiratting for
the US field than for the magnetic field. The action of the US on the-domain structure
leads to its relaxational change, a concomitant A E effect, andi hence, an alteration
of the speed of propagation of the US. When" the relaxation time is appreciably
greater than the period of the US waves, the domain structure will not exert a subm
Card 113

Investigation of the dispersion of ultrasound S/776/62/000/025/0041025
stantial effect on the rate of propagation of the Us waves, that is, in that event, the
material will behave as though it were nonferromagnetic. The same occurs if a,
strong magnetic field is superimposed on a breakdown of the domain structure.-,
Details of the making of the rods (e'lectrolytic Ni. 000, Armco Fe, Mo Permalloy',
and transformer steel with 416 Si) is detailed. The US tests were made at frequen-:
cies from tens of IWps to several mcps in the presence of various MP (up to
10,000 4). The HTof the specimens is identified. -A block diagram of the testing
equipment is shown, and typical oscillograms, depicting the interference pattern
under "in-phase" and "counterphasell conditions, are shown. , In all of the materials
investigated a velocity minimum and a damping maximum of the, US waves was
observed in the initial region of the fields which, apparently, corresponds to a
magnetization of 30-5016 of the saturation value. This effect is attributed to a more
ready mobility of the domain boundariesupon the imposition of a magnetic field.
When the field eliminates their resistance to motion, the permeability of the
material increases sharply. This occurs, in all ferrom agnetics. A decrease of the
speed of US in Ni in the region of strong fields is attributed to the appearance of
macroscopic circular Foucault currents. This hypothesis is discussed in some
detail. As expected, there is a damping maximum at a certain critical frequency..
which in Fe appears at 180 kcps and in Permalloy at 20 kcps- Another critical.-:.,.
frequency is found for the maximum of magnetic lo5ses in a variable magnetic field
HT: Abbreviation for heat treatment.
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Investigation of the dispersion of ultrasound S/77616Z/000/025/00 0 2,5
This frequency must coincide with the critical frequency of the damping of the US
waves, since both of them. are a result of the relaxation4i ~-haracteristics of tle'-
displacement of the domain boundaries, regardless of the nature of the force i tider.
ent occurs. a
the effect of which this displacem A gre t di %fficulty encountered ~s
the complexity of the sp Iectrum of proper frequencies of the rods employed in.01 .e
h
experiments, the mathematical theory for w ich does not admit any exact expkession..
es,
This difficulty was overcome by measuring not the absoliLte speed of the US w;%v
but its changes with the imposition of a magnetic field aVvarious fr~equencies,~Pla pro-~,
ce'dure which afforded a possible determination of the dispersion curves. Th
eld at
absolute speed is then determined by adding the speed in a magnetic.fi
basic frequency of a rod and the speed produced by the effect of the given ma etic...
field. Other difficulties occurred with the broadening of the resonance lines, -
-ethod. There are 15 figures an 11
which reduced the resolving power of the m
-language Soviet, I German, and 2 English-language).
references (8 Russian
.,Card 3/3
I .T I I

HU

0
1
0

PUZEYP I.M.
Magnetic anisotropy in single crystals of iron-cobalt-nickel
alloys.. Fiz. met. i metalloved. 16 no.2:179-183 Ag ,63.
(MIRA 16:8)
1. Institut pretsizionnykh splawov TSentrallnogo nauchno-issle-
dovatel'skogo instituta, chernoy metallurgii.
(Metal crystals-MagAetic properties.)
(Anisotropy)

ACGESSION NRt AA01.1770 S/0181/64/006/001/0294/0296
AUTHORS3 Hiryasovs No Z.; Puzey' 1. 1-1.
TITLEi Study of induced magnetic anisotropy in Ni-Zn-Cr ferrite containing GoO
SOURCE: Fizika tverdogo tela, v. 6, no. 1, 1964,, 294-296
TOPIC TAGS: Ni-Zn-Cr ferrite, CoO inclusion, induced magnetic anisotropy, magnetic
anisotropy, uniaxial anisotropy, anisoLropy constant
ABSTRACT: The influence 'of temperatur e on the constant (K of induced uniaicial
anisotropy and on the spontaneous magnetization (Is) of a Srrite was studied.
bq.)eriments were conducted on Ni-Zn-Cr ferrite in the temperature range of -196 to
300G. FieM dependence of K was investigated in the interval of 3-21 kiloersteds
-196, 20, 90, and 200G. he magnitude order of Ku and its linear relation to
agreed with the theory of directed orderinZ.. The work was conducted in order
to verify previously obtained results., Anisotropy was studied by the method of
turning moments, and the specimen under investigation was,a sphere 10.7350 + 0-0005
mm in diameter,-magnetized for 5 hours at 300C in the field of an electroma7gnet.
It was determined that (with the drop of terq)erature) the value of Ku increased
Card 1/2

AMMION NR: AP4011770
within the range of 102-104
.1..3., This magnitude of KU agreed with theiheory
of directed ordering, The differential dK/dT reached a maximum near 00-1' and'dropped
t ero OOK& It was further determined that below 50C the relation between KU and.,,
is linear. A slight deviation froni this relation at higher temperatures was
caused by an additional magnetization along the field. A series of experiments
on another specimen showed that with sufficiently high fields Ku increased directly.
with Whe 1"ield intensity. Orig. art. has: 3 orraphs and 2 formulas.
ASSOCIATION: Fizicheskiy fakultet W'M fin. M. V. Lomonosova (k1hysics Departmant
MOU); In-t pretsisionnyokh splavov Tsg!IChM (Institute of Precise Alloys TSMIChm)
SUBMITTED: 17Jun63 DATE AcQ: 14Feb64 FAIGL: 00
SUB CODEs PH - NO PEF SOV: 005 GTMR: 005-
Card 2/2

ACCE10,S11ON NR: AP4028437 s/blsi/64/bo6/W4/nooA1o3,
~AUTIHORS: Somonovskaya# S. V.; Umanskiy, Ya. S.; Puzey, L M.1 Granoviklyp Too Be.
TITLE: Investigating*tho phonon spectrum of nickel by diffuse scattering of
x rays
SOURCE: Fizilca-tverdogo telas v.- 6j no. 4P 1964 1100,4103
TOPIC TAGS: phonon, nickel, diffuse scattoring,'x ray, elastic wave, sound
,:velocity, elastic constant, forromagnetic property, multiphonon scatterirg."
';goniometer RXSO, ionizer URS 50 IM, counter MST 17.
,ABSTRACT: The authors determined the dependence of frequency on the wave vector
'';for lontitudinal and t s propagated along~the symmetry directions-
01 1]. , fan verse waves
~1110 .9 01, and 111 at room temperature. The initial segments of the disper-
~.sion curvos permit approxijmte determination of the voldeity of sound. The
velocities thus obtained agree with average values detorm nod ultrasonicallLy with-
t /cm2)
;.in 7% or less. The computed values of the elastic con5t:~hts (in dynes
-12
2.45*10 for c11, 1.6-10-12 for c32, and 1.3-4,10-12 for c44--are in good aigree-_]
1:ment with data from the literature. The dispersion in Ni is found to be much
L
caecr-7

IiACCESSION NR: AP/~028437

ACCESSION XR: AP402338 7 S/0048/64./028/003/0440/0443
AIUUIOR-. Puzoy, I.M.; Goman'kov, V.I.; Loshmanov, A.A.
TITIZ: Neutron diffraction determination of atomic magnetic moments in iron-nickal;
alloyn containing Me, S1 and Cu CRoport, Symposium, on- Ferromagnatisc and Forroalec-, i_.i
tricity hold in Loningrad 30 May to 5 June 10617
SOURCE: AN SSSR. Izvestiya. Seriya fizicheskaya, v.23,no.3, 1964, 440-443
TOPIC TAGS: neutron diffraction, atomic magnetic moments, permalloy, impure para-
alloy, Mo pormalloy, Si permalloy, Cu permalloy
ABSTRACT: The magnetic moments of Fe and ~i in alloys of the permalloy type Con-'
taining up to several percent Mo, Si or Cu were determined by the diffuse ncutron.~
scattering method of C.G.Shull and M.K.Wilkinson (Phys.Rev.,97,305,1955). The mea-.
surements were undertalien because of the interesting fact that both Fe and Ki have
larger magnetic moments in iheir Alloys than in the pure metals, and because there
is evidence (I.M.Puzey., Fizika metallov I metallovodeniya,12,No.3,453,1961) that
1..*,o and Si differently affect the magnetic moments of Fe and Ni In these alloys. Thei
apparatus has been described elsewhere (V.1.Goman'kov, D.F.Litvin, A.A.Loshmanov,
Cardill

ACCESSION NR: AP4023387
and B.G.Lyashchenlco, Fizikametallov i metallovedeniy,14,26,1962). The alloys were
propared from electrolytic metals, wcre~forged Into bars, and quenched from 7000C
in water to obviate ordering. Correction--was made'for the effect of multiple magne.-!_'.
tic Bragg scattering. This correction war%.9valuated by extrapolating measurements
on four samples of the,,swao,composition'but different size to zero 4ampl6 size. The':-
measurements were performed4t 770C. The results are shown in the table below,
which gives the decrease in,,the magnetic momenU of Fe and Hi,-.in Bohr magnetons
It can be seen that Si affects Fe more'strongly than does Mol~~
per percent admixture.
Fe N1
Ito .01 ~1.07
Si .03 ".03
Cu .00 o3
and Mo affects Ni moro.strongly than does Sli. Ueasurements with colder neutrons..,
will be required to elucidate the mechani sm of this effect. to In conclusion, the
authors thank B.G.Lyas~chenlio, D.F.Litvin and A.V.Doroshanko for assistance in the"I.
work." Orig.art.has; 219igures 2tables.
2,/0 2L
Card

ACC Nilt AP'
6035723 SOURCE CODE: UR/0413/66/ooo/o1q/oo85/OO
~,MXTOR: Puzey, !. M. trenko, E. D.
Pe
ORG~ none
1ITLE. I-ron-cobalt-nickel base magnetic alloy, Class 40, No. 1806698 (announced by
the Central Scientific Research Institute of Ferrous Metallurgy im. 1. P. Bardin
(Tsentrainyy nauchno-issledovatellskiy institut chernoy metallurgii))
SOUIRC7: izobreteniya, promyshlennyye obraztsy, tovarnyye znaki, no. 19, 1966, 85
TOKC TAGS: magnetic alloy, iron cobalt nickel alloy, mol bdenwm containing alloy
4V
'3STRACT: T,-.-s author C' ba~
ertificate introducesan iro -c
-nickel base magnet c
i alloy.. To combine the increased values of magnetic and electric properties in order
to obtain rectangular hysteresis loops or a .linear dependence of induction on the
eld intensity in the range of 0 to 10,000 gs, the alloy has the I llowing chemical
L 10
co=os4.'.ion in i'j: 0.03 max carbon, 0.3 max silicon, 0.3-0.6 manganese,
27.5-31 .0 iron, 24-27 cobalt, 4-6 molybdenum, remainder nickel.
SU .3 CODE: l1/ SbBM DATE: 2lJul65/
Card uDc: 669-018-5:0'69-15124125-194
1 7 T_ 7r

ord
L 50989~65 ------ --- ---- - --------
AOCESSION NR-. AP5011460
IL
all cases id Gd; theAndicated limits are.bas6d on tested:films so:that, the actua
tages:corresponding to changes. An behavior ~may- be- dif f erent.): The films
percen,

S/058/63/000/003/()87/104:
Wa-~eguide modes in open waveguideletruoture
A059/A101
'

i'-
- on the area S, an inf inite number
2) quasi-
possible; cylindrical structures
:
4
i of non-overlapping circles of finite radius can'be placed; the Laplacian opera-
.
1 .
tor spectrum can be partly discrete;* the existence of WM waves is not excluded
y never form a complete system.- :3) -Tolosed structures all that
but the quasi
.':. do not belong to the fiiist two lasses; the Laplacian operatorapectrum is
0
discrete and WM waves -form the complete system, in the general oasis only for
A.,~. TM-type fields. The characteristics of-symTetrical band structureswere in-.
vestigated by variation methods. It was shown that the WM waves can propagate
both in olosed and in open .(quasi-cylindrical).structures of this kind. The
lie!
agrams of the dependences of the.critical.wavelengths on.the dimensions of't.

calculation are confirmed ex
al
structures are given.. The dataof-the.theoret-o
re.
The are 18 references.
perimentally.

V# -oil d'enburg

~.
[Abstraoters'noter'-Complete t ati6
ransl
,
U-4% ~4

Card 2/2
.

ADRIANOV. P.K.; ANDRIANOV, S.K. ; BENEZIKOV, B.S.; GOWVKO, V.G. (Holovko,
V.H.1; I)OBROVOL'SKIY. A.V. [Doborovollslkyi, A.V.]; DOVGAL', M.P.
[Dovhall, M.F.], YELIZAROV, Y.D. ClElizarov, V.D.1; Z.HIZDRINSKIY,
Y.M. [Zhyzdryn91)W1, V.M.]; ZYN141GORODSKrY, O.M. EZvenigorodelkyi.
0.M.1- ZAYCHMIED, R.M. [Zaichenlro, R.M.1; IVANAENKO. Ye.l. CIvanenko.
13.1.1; KOMAR, A.M.; KGSIYANOV, O.K.; XAZAKOV, 0.1.; KOGIMO. S.K.;
KLIMENKO, T.A.; KIRIYAKOV, O.P.; XALISHUK. 0.L.-, LELICHENKO. M.T.;
LEB3DICH, M.V.; MIKRAYWV, V.0. ERZkhailov. V.0.1; MOROZ. I.1.:
HO311GHIL' , Y.Yu. [Moshchill, V.rU-J; IMPOCZ1RHY, P.S. [Neporozhnii.
P.S.]- IWDATNIY, S.M. (Nazdatnyi, S.M.]; NOVIKOV, V.I.; POMNOT.
S.K. ~Polevoi, S.K.]; PERAHREST, M.S.; PtJZIK,-O.ye. [Puzik, 0.3.1;
RADIN K.S.: SLIVINSKIY. 0.1. [Slivinsilwi-I O.f.-T-,-'-5TAkSIAVSXIY,
A.I. tStanialavalkyi, A.I.1; USPXNSKIY. V.P. [UsDenolkyt. V.P.1;
KHORKHOT, O.Ya.; XHILYUK, F.P.; TSAPENKO, M.P.; SHVRrS. V.I.;
MALICMSKIY, V. [Nallchovs1kyi, V.],.red.-, ZELNNKOVA, Ye. Delen-
kova, R.], tekhn.red,
.[The Ukraine builds] Ukraine budute. 1yiv, Derzh.vyd-vo lit-ry
z budivrqtstva, i ark-hit. 9 1957. 221 P. (KIRA 11:5)
(Ukraine--Constluction industry)

USSR/General Biology - Cytology. B-2
Abs Jbur Ref Zhur - Biol., No 8, 1958, 33302
Author Puzhaka, Kh. Ya.
Inst
Title Nerve Regulation of Cell Division Processed,.
(0 nervnykh regulyntsiyakh.protsessoV deleniya kletok).
OrIg Pub Zinatnisko rakatu kraji Mips med. inrt.,.Sb*
nauchn. rabot. Rizhsk. mede in-4, 1956, No 6.2 75-83
Abstract A st was-conducted on mitotic activity (Mk) on the
udy
epithelial. cornea of,mice and -rats by hypodermic.injec-
tion of substances which stimulate,(ephedrine'), excite
(pilocarpine) and depress (atro pine) the sp~theitc
mediator of the cell cholinreactive systemse When rats
are injected with 2-5 M9 of elliedrine per k(; wei0it
there is a decrease of M& in 15 minutes, which attains
a minimum. 2 hours after the injection; the MA then
starts to increase anO 6 hours after the injection
Card 1/2

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