SCIENTIFIC ABSTRACT VYALKIN, A. - VYALOV, O.S.

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• Collection: Scientific Abstracts
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• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

. Y")ZIT1,117r, 4
TYALKIlf, A., kand. ,ekon. tauk,
Rnlarge automotive transportation arxits. Art. transp. 36 no.1:30
jrft 158, (MMA 11:1)
(Transportation, Automotive)

,:- VYALXINt-~I-.---
Xa!l for the heroine of Brestp Raiva Abakumova. Med.sestrp 19 no.]-Is
Wi-43 N 160. WM 1311l)
(ABAKUMOVA9 RAISA IVANOVNA)

VYALKI:,t V.p polkcvnik; i"".7iKOV, Ya., r.-,ayor to'chn. tlu&.by
CUckin- or orientation. Voen.veot. 39 no.5:S3 I-rf 160.
(A"!--:-. W-2)
(Antiaircraft guns)

Y/-J L, k c) ye, r,
USM/Chemical Technology - Chemical Products and Their Application. Fomentation
Industry, I__517
Abot Journal: Referat Zhur - Khimiya, No 19, 1956.. 63559
Author: Malltsev., P, MI. Zazirnaya, M. V., Velikaya, Ye.
Institution: None
I Title: Effects of Separation on Qualitative Composition of Beer Wort
Original
Periodical: Tr. Kievsk. tekbnol. in-ta, pishchevoy prom-sti, 1953, No 13, 101-105
Abstract: Studies of qualitative changes in turbid beer wort an 5-minute centri-
l'ugation in laboratory precipitation centrifuge at 2,000 RPM. The
indexes thus obtained are compared with those of clear wort (CW) col-
lected from outlet of filter-press after filtration of turbid liquor
that was concurrently subjected to separation. Residue of insolubles
in CW waa the same within 0.01-0-03 9/100 ml. Turbidity of separated
CW is almost 2 times less due to more complete removal of colloids both
prior to and after hop treatment of the wort. Color and pH of CW are
the same. Protein content and dextrin content of CW are practically
the same.
Card 1/1

vy"l!plKffll JI.P ;,apltanj voy!3rnyy letchik I;tr-;ogo kirissa
-- --------
f - .-A-
Ilignt, inetructrj:* ~nli atudent. -,/. j krj,. l.7
Jo 1o4. I (m i It; r! /)

VYALKOV, P.D.j, mashinist
We are wasting'i3and. Elek. i tepl. tiaga r-o.1:41 Ta 161.
(MIRA 14:3)
(Diesel locomotives)

VTA IZOVA, GqA*0 operatsiounaya sestra
AxabaPgo of experience. Mad.sestra 19 n0-8:37 Ag -160,
(KIRA 13:7)
1. Is otdoloniya parelivanlya krovi 1~rumensko7 oblnotnoy
bolluitay.
(BLOOD--COLLECTION AND PREURVATION)

VYALLO , A'* ~,
Combined cutting and press-working of shafts. Stan. i instr.
36 no. 12r23-26 V 165. (MIRA 19:1)

Tfaov., 'k. .,!.
Vyalov, A. M.
"Influenzal ir-fection Of the'Fodibugrova,,al region." First '!oscow
Order of Lenin Medical Tn-,t iloni I. ";. S-nhcnov. 'foscow, 195(.,
(Dl.nrortutlon for tho lJvj,.-cjo of In Mnellcnl
Knizhnaya leto2ist
No. 21, 1956, Noscow-

__!njpV~ - BAGNOVA, M.D.; BULYCMV, G.V.; BYLOV,, I.S..- G'.-TKIN, A.G.;
K& OVA, F.S.; FUSIMLIA, H.N.; YUSHUVICH, L.B.
Comparative evaauation of health conditions in workers employed in
producing synthetic fatty acids ana higher fataty alcohols. Dig. i
san. 26 no.4:15-21 AP 161. (MIFLA 15: 5)
1. 1z klinichoskogo otdola Moskovskogo nauchno-isoledovatellskogo
Inatituta gigiyeny imeni F..F.Erismana 14ininterstva zdravookhrananiya
RSFSR.
(CIUVICAL INDUSTRIES-HYGIENIC ASPLCTS)
(ACIDS, FATTY-PHYSIOLOGICAL EF~TCT) (ALCONOLS-411YSIOLOGI CAL EWECT)

'MAI'M fASMO) 'MMM, 'At'DO) MMUMNSU)'T OZ.-) W$VM$,)
BYIDV,, I.S.; DEMIN, A,G.; MEL"MOVA, S%MMUU,'I.S.
Changes In the bealth of vorkars engaged in the production d
synthetic fatty acids. Uch.zap. Mosk.nauch.-issl. Anst. san.
I gig. no.9:30-54 1~62 (MM 161ll)

BAGNOVA,: M.D.; VASIL'YEV,A.S.; FUSILKINA, N.N.; YUSHKEVICHo
L.B.; BULYCHEV, G.V.j BYLOVp I.S.; GE21KIllp A.G.j WIDKOIA #Loll.;
ZHIGULINA, L.A.
Early changes in the state of health of workers in the cumene
process of phenol and acetone production. Ucho zap* Moskonauch.-
issl. inst.san. i gig. no.9tl3-16 161 (MIRA 16:11)
111~

EXCERPTA MICA See 8 Vol 12/10 Netirology Oct 59
5022. LESIONS OF THE HYPOTHALAMIC REGION DUE TO INFLUENZA
(Russian text) - Vya I ov A. M. - ZH. NEVROPAT. I PSIKHIAT. 1959, 59/3
(261-264)
In the clinical picture of hypothalamic lesions, 2 groups of symptoms are distin-
guished, according to the functions of the hypothalamus. The following.2 groups of
*symptoms characterize the diencephalic syndrome: (a) AStnenla. adynamia, sudden
occurrence of dyapnoea-. either retardation or acceleration of respiration. change
In the ratio between length of inspiration and that of expiration; vasomotor lability;
disturbed oculo-cardiac, pharyngeal and epigastric reflexes. atd. finally, &change
In blood pressure. (b) On the other hand, the following symptoms are also reported -
auorexts and bulimia; oltgodipsta and polydipsta; subfebrile and subnormal body temp-
eratures: asymmetry of skin temperature; disturbed non-conditioned thermo-reffulat-
oryrenex(Tcherbak); and sleep disturbances, Inparticular, it is to be remarked that
subfebrile temperature, It not accompanied by other signs of hypothalamic disturb-
ance, cannot be attributed to damage to the tegmentum In the region of the 3rd ven-
tricle. Oen*rally, this Indicates disturbances in other parts of the thermoregulatory
system. (L.8)
:7, lap.
31
(
;
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1777777T7-7~'~7-
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M019 t GO I
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VTALOVhAB'-78 6oo
OROMOV, n. ~r-l IrMT!
2. USSR (0600)
Experimental Flnnt of "Glavtsinksvinets" (Main Admin. of
Zinc and lead Industry) "The Separation of Zinc Sulphate
Solutions from Iron", Tevet. Ret. 14. No 7, JulY 1939
9AWReport U-1506, 4 Oct. 1951.

A --LIX a, 11 10 -A-1-L-WW-C( X
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forpl#"Is -I,
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Pulwadw of idsc twat@ solutions 4 estrutifid Im.

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00 which are tint orutrollmd by *4kiWg 18 dtOW, 4T 4 "Stilt

00 A V covig. Za nr ZUO, 14(h Is INS iddrd to oxidise the Fe

pH coativi is occewary for the owvm of the new method.
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r A 4 1 ~ , I -, - I , ~ - 11 - - - - --. . I - ~ . .1 - , ~ . - ~ %.~ r4 - -,!,! 4 , . W9.
t ~
p-- - m M ORM

BABIKOV, V.V.; VYALOV, G.11.; INDREASH, G.
(Calculation of the electric system of extraction of an
ion beam from a classical cyclotron] K raschotu olektriche-
skoi sistenV vyvoda ionnogo puchka'v klassicheskom taiklo-
trone. Dubna, Ob"edinannyi in-t iadernykh inslodovanii,
1963. 14 P. (MRA 17 s li

VYAI,OVI__g-.-Nt--
One method for computing the shape of a magnet for a given field.
Zhur,tekh.fiz. 32 no.3:287-293 Mr 162. (KIRA l5s4)
(14%nets) (Magneltio fields)

VYAIDV --G.N,- -
.
[Two-dimensional problem of a vagnetic field formed in tbe
- gap
of a symmetric magnet] Ploskaia zadacha formirovaniia. mWitnogo
poliA v zazore simmetrichnogo *magnita. Dubna,, ObIledinenr*ri in-t
ladernykh issl. 1961. 34 pe .(MIRA 15:1) ' +
(Magnetic fields) (Nagnets)

VYALOV G.H.; FIKS, M.M.
Acceleration of particles of variable charce in P- ;:vtLential. electric,
field. IAd. fiz. 2 no.1!117-136 JI 165.
(MIRA 1818)
.1. Ob"yedinennyy institut yadernykhAualodovaniy.

VYALOV.-G.N.
Some problems concerning the regulation of a magnetic field by x9ans
of a currant. Zhur, tekh, fiso 32 no.114361-1370 N 162.
(MIRA 15sll)
(Magnetic fields)
1---

w 0 mi MR W afflam 9 R me m mm W.".

llc~, I , . '.., . . , 1, ~ , " --; to ., ..
. . r . . . , , reo
1 11 M, ~Ir, - . :1
I I 1 -1
~f

VTALOV' G.N.
Anomalous magnetic moment of nucleons, Zhur. eksp. I teor, fig.
31 no.4:62o.624 0 156. (MLRA 9:12)
1. Yizicheekiy institut imeni P. N.Iebedeva Akademii nauk SSSR.
(Midlear moment$) (Nualsonu)

h?215
5/057j62/032/011/007/014
B104/B102
AUTHOR: Vyalov, G. N.
TITLE: Some problems arising in the formation of a magnetic field
by a current
PERIODICAL: Zhurnal tekhnicheskoy fixiki, v- 32, no- 11, 1962, 1361-1370
TEXT: The build-up of a given magnetic field by a plane current in a
multi-layer magnet is investigated. Three cases are considered:
~1) no interface (homogeneous magnet), (2) magnet with one interface and
3) with two interfaces. The current is calidulated from the magnetic
field produced by itself. The problem leads-to the solution of a two-
dimensional Fredholm integral equation of'the first kind. The V~
arbitrariness in the definition of the intensity of magnetization U is
avoided by considering only a plane current:
(1-7)
P'=0' (1.8),
M (r) M. (r) -_W~= M(r) - k, M. M, = 0. (1-9)
Card 1/4

0/057j62/032/011/007/014
Some problems a,rising in the ... 1$104/B102
where it is required that M(Xvyvz) at infinity should vanish with the
current. The solution of the system
rot If (r) = 4np,
div H (r)
W H (r) grad (r),' (1-4)
-5)
900
is sought in the form r) 096) + 90), where is determined from
. rot h (r) = 0,
div h (r) = OM grad a (r) -i-l It - gnid it (r) 4n div M (r).
Lengthy calculation leads to
A (P, q) (1'.26)
(P, q, a, 27t a P, q1 ON P q 0)]
7-)
Card 2/4

S/057/62/032/011/007/014
Some problems arising in the ... B104/B102
P. 1. 00 P. q. 00 (1-27).
where the n quantities:-. d(S) are 'determined from the system of'n linear
algebraic equations
This expression is discussed for the three special cases mentioned
above, and it is shown that the value Mo(xvyjajA) of the density of
magnetization required for the production of a given field in a
homogeneous magnet is important. a is the distance to the midplane
z - 0.. If Mo(xjy*a9A) is known as an analytic function it becomes
possible to arrive at the exact expression for the equivalent
Card 3/4

5/057/62/032/011/007/014
Some problems arising in the ... B104/B1O2
magnetization when account is taken of the effect of the interfaces for . .
infinitely thin current layers (6 --*0) situated very near the interface.
The corrections for finite thickness A of the current layers and for
the finite distance d of the current from the interfaces can be obtained
by successive approximations. V
SUBMITTED:
May 3, 1961
Card 4/4

50), 180) SOV/32-25-4-55/71
AUTHORS: Kvyatkovmkaya, G, V., Vyalov, 11. 11.
TITLE: Attachment ti the 1111eichert" Microscope for Auttomatically
Shil'ting Ground So~,tionu (Pri3pouobloniye k mikrookopu
JReykhort" dlya avtomatichoskogo paredvizhenlya shlifov)
PERIODICAL: Za,.-cdi3 aya Laboratori;,al 1959~ Vol 25, Nr 4,
~
=R)
P 495
ABSTRACTs An apparatus was developed which renders it possible to
shift automatically grcund sections under the microscope
no fl-at 1200 fiolda, i.o# a Dample ourfaco of 15Y 65 MM
'
may ~o viowod successively. Th
e apparatus (Fig) is mounted
.rith the stape of the microscope and consists basically of
a small device operated by an electric motor. The shifting
of the ground Fection is done by means of two pairs of
viorm t-hreads transmittine the rotation of the electric
motor via a cog wheel. As soon as the section has shifted
by 15 mm a lengthwise shift by 0.8 mm follows, etc. The
apparatus desaribed has already been used for five years
in the metallographic laboratory of the Kuznetsk MetallurCi-
Card 1/2 cal Kombinat. There is- 1 figure.

Attachment to the "Heichert" Microscope. for Automatically SOY/32-25-4-55/71
Shifting Grouni Sr;;:,tio!*,a
ASSOCIATION: KuzretF3k!y netalluri;1--~liesklLy kombinat (Kuznetsk lletallur-
gical K=binat )
Card 2/2

15-57-12-17264
Translation from: Referativnyy zhurnal, Geologiya, 1957, Nr 12,
p 81 (USSR)
AUTHOR: YYajov 0 S.
TITLE: Rrief Survey of Facies and Depositional Characteristics
of Sedimen.ts in Western Regions of Ukrainian SSR
(Korotkiy oglyad fatsiy i umov utvorennya osadkiv y
zakhidnikh oblastyakh UkrSSR--in Ukrainian)
PERIODICAL: Nauk. zap. L'vivs'k. prirodozn. muzeyu, AN URSR, 1955,
Vol 4, pp 5-19
ABSTRACT: Bibliographic entry
Card 1/1

15-57-12-16794
Translation from: Referativnyy zhurnal, Geologiya, 1957, Ur 12,
p 15 (USSR)
AUTHOR: Vyalov, 0. S.
TITLE: The Paleogene of the Southern Shore of the Kara-
Bogaz-Gol (Paleogen yuzhnogo poberezhlya Kara-Bogaz-
Gola)
PERIODICAL: Tr. In-ta geol. AN TurkmSSR, 1956,Vol 1) pp 163-171
ABSTRACT: A brief description of the Paleogene razrez (section)
in the region of the southern shore of the Kara-Bogaz-
Gol is given on the basis of work done in 1938. 1) A
variegatel marl formation, 34 m thick, rests on Danian
limestones. White marls predoMinate,in the lower
part, red spotted marls in the middle part, and var'L-
egated marls with layerg at-caldareous clays in the
upper part. Fossils have not beenjound in the for-
mation. 2) Next occurs a white marl formation, 23 m
Card 1/2

The Paleogene of the Southern Shore (Cont.)
15-57-12-16794
thick, which is divided into three members on color and lithology.
3) A brown (fish) horizon, 23 m thick, consists of shaly marly clay
and thinly platy argillaceous marl, with thin layers of "gilyaba"
(a bleaching cl%) in the lower part (the lower boundary of the
horizon is place at the first appearance of-lalayer of gilyaba).
Larfe quantities of small fish scales are present in the sequence..
4) formation of green calcareous clay, 20 m thick roduces pla'~y
rubble; the calcareous content decreases upward., 5J ~ formation of
green clays and sands, approximately 50 m thickoccurs next in the
section. The number and thickness of sand layers reach their
greatest values in the middle part of the unit. 6) A formation of
green platy clays, approximately 100 m thick, contains small fish
scales and, in the upper part, indeterminate pelecypod imprints.
In addition, the author compares the Kizyl-Kup razrez (section) with
other regions and gives a table showing the comparison of the
sections.
Card 2/2 V. A. Levitskaya

TYALOV, 0~,So, a)-ademik.
A comparative study of the Paleogene In Central Asia, the Caucasus
and the Crimea. Dokl. AN SSSR 110 no.4:631-633 0 156,
(MLAA 10:1)
1. Mmdemlya nauk USSR.
(Geology, Stratigraphlo)
.8

V 4 14L-Vij 4~1, &J (
SUBJECT USSR / PHYSICS CARD 1 / 2 PA - 1781
AUTHOR VJALOVOG.N.
TITLE jhe Anoma, ous Magnetic Moment of Nucleons.
PERIODICAL urn.eksp.i teor.fie,~lffasc-4t620-624 (1956)
Issued: I / 1957
In the present work the anomalous magnetic moment of nucleons is computed in
consideration of their excited states and on the basis of the semi-phenomeno-
logical theory of the interaction between piona and nucleons (I.E.TAN11 et al,
iurn.eksp.i toor.fis,,L6,649, 1954). All quantities are given with FEYNMANIS
denotatione.
At first the rather voluminous LAGRANGIAN of the system of nucleons and mesons
in the alootromagnatio.system for the symmetric pseudoscalar meson theory with
mixad.pseudoscalar and pseudovectorial coupling of the meson field with the
nucleon field is given. By variation 6f,the LAGRANGIAN with respect to I and
in the case of the validity of the addLitional condition B 0, equations
for the'waVe functions T and-B& are obtained. These eqk*"i~_ns :re trans-
formed and solved by FEYNMANIS method with the help of the inverse operator
(L-') Kap* - There follows the'e7mputation of the matrix elements: Here the
contrf9u,tion made by the diagrams represented by a drawing to the anomalous
me,onetic moment of the nucleons in computed. Because of the great singularity
of the inverse operator K v the matrix elements diverge considerably (di-
vergenoe of the fourth order). This divergence is eliminated by the introduc-

V
Zurn.eksp.i teor.fis,51,fa.se-4,620-62.4 (1956) CARD 2 / 2 PA - 1781
tion of FEYNWIS cut-off factors. In order to simplify computations, cutting-
off is not carried out within the entire matrix element at one and the same
time but separately in each summand.
Numerical resultst discussion: The numerical result for the anomalous magnetic
moment 6.4.,. depends on the sign of the constant g of the pseudovectorial oou-
pling. When using the values g 2.Oy2j g 2. 0,131 a - 21 M m+2t25
1 1 '~& I E - 1,61
one finds for g > 0 and A ev M for the anomalous magnetic moment of the pro-
ton and neutron 6 ep - 115 01 6eH 3 0 respectively. With an increasing
the absolute values of 6 and 6,~t,, inoreasop on which ocoasion their re-
~41 P
lation remains approximately unchanged. Thus it is possible, by a suitable se-
lection of the out-off parameter A , to attain quite good agreement between
theory and experiment. Approximately the same conclusions were arrived at by
A.KANAZAWA and 11.5UGAWARIj Prog.Theor.Phys.lill 231 (1954), but the author
describes his own computations as being more consistent and more acturate.
Thus, the additional interaction between nucleons and the electromagnetic
field (constant E ) was not taken into account by the above cited work. The
contribution made by this additional interaction towards the anomalous magnetic
moment is of the same order as other types of interaction and must therefore be
taken into account.
INSTITUTION: Physical Institute "P.N.LEBEDEV" of the Academy of Science in the
USSR.

"Anomalous Magnetic Mothent of Nucleons," by 0. X. Vyalov, Phys-
ics Institute iieni P.'H. Lebedev, Academy of Sciences USSR,
Zhurnal Ekuerimentallnoy i Teoreticheskoy Fiziki, Vol 31, No
(10), Oct 5b, pp b20-624
"The anomalous magnetic moment is computed with account of excited
states with a spin of 3/2 and an Isotopic spin 3/2. Diverging expressions
,are obtained which can be regularized by means of Feynman multipliers.
"It is shown that a cutofffactor can be chosen to yield agreement
between theory and experiment." -- Author's abstract

tACCESSIC0 M: AP4036530
B/0089/64/016/005/0442/0444
1AUMOR: Vyalov, Go No
iTITLE: Coaputation of phaso relationships in a cyclotron
SOURCE: Atomnaya, energiya, v. 16p no. 51 1964, 442JM
TOPIC TAG84. cyclotron phase shift$ magnetic field droip cyclotron ion energyp
phase shift computation,, cyclotron
ABSTRACT: The equation for the phase shift in tho cyclotron conta-bis (in addition
to the universal constants) the final ion energy, the phase) and the amplitude
of the accelerating potential. The parameters of the cyclotron can easily be
computed if the magnetic fiv.14 changes parabolically along the radius) or
linearly as a function of the relative ion energy (in comparison with the final'
f energy). The author found it convenient,, in his analysia of nu=roun cases of
zutpetia drop., to approximatte the latter vith linear segmentas MeaBurements ahov
that the magmetic field of the cyclotroa of tba laboratory for Nuclear Reactions
''Of the Consolidated Inntitu-W for Nuclear Investigations can be closely approxi-
mate4 by threa atraight 31nese Origo arL. bas: 1 figure.. 22 equationno
A12

L 20285..66 WTM/EWTWO~- AT
1TCCESSIOR RRs AP5020260' UR/0367/65/002/001/0112
/0116
IAUTHQ,~Ss yzilov, 0. No; Fika, M. M.
MITIX-s On tha accoleration of particles with a variable charge in olootrostatio
field
SOMCCEi Yadornaya flzikat v. 2. no. 1, 1965o 112-116
TOPIC TAGSs electrontatio field, electrostatic acceleration, Ion beami beam
velocity
ABSTRAM Tho ponsibility of high-current acceleration of heaM Ions bj changing
the ion rhargewas-investigated analytically. The nonpotential characteristic of
the pfoduat ZB under the integral of the energy equation ia shown by
_Z (E dr),
ftle optimum potential required to impart the maxi:m= energy to the aooolerat-ing ion
ibeam with given energy W is calculated and is given by
diij'inte-n's-itj -i in -W
various mechanisma for us oases e multiple acceleration
ITC~Iiej

L 20985-66
'ACCESSION M AP5020260
schema described above are listed. For a constaiLt AW the mean- multiple scattering
angle at small angles is given by const .11,
JAW
no scattering cross section for the large angle aperture accelerator is given by
.07,0i7,' 2' 'Cosot, ~'A i'
'FV~- 7
01, --A 17
and the beam intensity by
-- oxp( dt P(0,).
qvg
-JV 2
It is shown that for all elements high intensity ion beams can be obtained with the
limiting energ:r jjf,, 0 125'AoZo/- "The authors express their gratitude to
corresponding member of the AN SSSR) G. N. Flerov, for his coittinuous Interest in
the work and to Professor M. 10 Podg2retakjZ for his valuable advice and evaluation
!of the problem." Orig. art. hass 13 formulas.. [Ohl
ASSOCIATIONs Oblyedinennyy institut yadernykh inaledovaniy (Joint ihatitute or
Nuclear Research
SUBMITMi 17jan65 ENCLs 00 30 CODE s NP
REP SM 002 OTHERt 003 ATD PRESS4Z
-1 Card 212.AV

VYALOV, G.N.
Calculation of phaEe relations in a cyclotron. At=.ene.rg.
16 no. 5:442-444 My 164. (MIRA 17:5)

S/05"0652/032/003/004/019
B125/BI02
AUTHOR:
Method of calculating the shape of a m3gnet from a given field
TITLE:
PERIODICAL: Zhurnal tekhnicheskoy fiziki, v- 32, no. 3, 1962, V37 - 293
TEXT: The author determines the shape of one-dimensionally magnetized
iron shims which produce a given z-component of the magnetic field in the
central plane of a magnet. With known magnetization 1,1(:r:~) (e. g., with
homogeneous magnetization of the iron along the z-axis) the lower boundary
of the iron shims applied to the plane z . z0 and changing the field
strength in the central plane by AH(x,y) is sought. Owing to the disturbing
effect of the pole boundaries the author first determines the shape of the
magnetic shims from the field produced by them, and then takes account of
the effect of the poles. From the scalar potential
00)
I-r- to I -It -#1I]
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Method of calculating B125/B102
the following integral equation is obtained for the z-component of the
pagnetic field bH - -grade in the central plane z 0:
ZH(x, y)= dx'dy'M (x", y)
r and -r denote points in the planes z Z andz z,, and 14(X,Y)
0 1 0
IMZ(X'$Y). The sought thickness A(x,y,z0 zo-Z 1(XIY) is much smaller than
;
he". distance z0from the central plane. For thin reason) the expression
under the integral sign_of (1,~) is expanded into a power series of
)/ 2- -('* -' ) + 2
41(xl,yl,z0 x_x_l + Y-Y z0 (2,3), and Ot5) is transformed to
(2tO CO
if dx'dyK (x x, y-Y, zo)f(x, A. z,, I)M(-e, A=
=gh(x, y)-i-Q(x, y, s),
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Method of calculating ... B125/B102
where is a small parameter: -!(Xgylzo) . ~If (XIYIZO, ~H(X,Y)
E'h(x-..Y)(2,5). From the linear integral equation for f (XIYYZ
n 0
M (X, Y, -0) dxdW. (~p) h (XI, y). (3,6) is obtained
(2r)2
0
fo'r-othe~Ahickpessi.o-fQthb-magnetized layer,' by the Fourier method. For the
one-dimensional case 141PI+IPS
(3,7) 'XZ(x, --.)=i fjdpevwo~~w~~ f dx~h(x)e-IP".
P
is obtained, in polar coordinates
(396),
and in the axisymmetrical case
(3,9)-
w 2a
52 AeXI
9DI (r, y, z0) I /dr' I dVj, ~p) h (r', V).
0 0 .0
f Ael--J, (kr) rdr'j, (X6 h (6.
2x
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3/057/62/032/003/004/019
Uethod of calculating ... B125/B102
The function n~(x,y,z 0), which cannot be represented in compact form with
z0),0 but with z0-:~ 0, can be analytically continued into the region z-.;,,O.
Thus, the final result SOI(x, zj I 1 1 7~) -1-1 (4,9)
24 (n - 1) 1 Ix -#- I (a -.-0)J4-1 Ix-f(a-
is obtained for the region 0 ez