SCIENTIFIC ABSTRACT APIN, A.Y. - APLYAK, I.V.
Document Type:
Collection:
Document Number (FOIA) /ESDN (CREST):
CIA-RDP86-00513R000101820019-9
Release Decision:
RIF
Original Classification:
S
Document Page Count:
100
Document Creation Date:
December 30, 2016
Document Release Date:
June 19, 2000
Sequence Number:
19
Case Number:
Publication Date:
December 31, 1967
Content Type:
SCIENCEAB
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ACCESSION NR: AT4002169
formulug 4 figur" &M I table.
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APIA*,$ _~.Yj,~*,(Foskva); VGSKOBOr-.'lKC.V, !.Y. (Moskva); SCISWA, G.S.
11 - kNoskva)
CourBo of tho reaction In a detonation wave of mixed explosives.
P1ffF no.5t 115-117 S-0 t63. (MIRA 16t11)
YAKOVIYVA , G. S.; APIN, A~. _Y&.; KURBANGALINA, R. Kh. I STESIK, L. N.
Detonation velocity of liquid hydronitric acid. Dokl, AN
SSSR 156 no. It152-153 MY 164. (FIRA 17:5)
1. Institut khimichaskoy fiziki AN SSSR, Predstavleno
akademikom V. N, Kondratlyevym.
FEPEKINP V.I.; DYMOVA, T.N.; LXBEDEY, Yu.A,j AFIN, A.Ya.
H"t of formtlon of wAgnestus hydride. Zhur. fis. kh1m. 38
no.4tlO24-1026 Ap 164. (MIRA l7t6)
1. Akademiya nauk SSSR, Institut khImicheskoy flzikl.
i LA t i
M AP4030M
8/002o/a/1561001/0152/0153
AUnM Yaboyleve.), 0" Be; A
PLAA. Ap tangalinap Rq Kh.; Steelk, L. V.
TITLE: The rate of detonation of liquid hydrazoic acid
B=Cz: M SWR& Doklady*j ve 156j no* 1# 1964# 152-153
:TOPIC TAGSt bydrazoia &aid,, explosive# detonatiou# detonation ratep liquid
hydrazoic acid
;ABSTRACTs HN Is not used In practice as an explosive,, nevertheless.. it is of
!interest to ditermine its detonation characteristics in the liquid state* Measure-
meat of the detonation characteristics are frequently used in the studies of tho
hi pressures (hundreds of thousabdo of atmos-
equation of the state of gazes at 911
-pheres)',and at high teVeraturee (several thousand degrees)* In treating experi-
mental data one is involved vith multicomponeat systems since the majokty of
1,explosives consist of at least four types of atomse Consequently,, the explosio--'
products contain several types of moleculeso In this respect HNI differs frAwrobly!
i-from other explosives because one might expect that products of detonation of
-liquid HN All consist primarily of molecular nitrogen and hydrogen* The rates
3
ACCESSIM NR: AP4035M
of detonation vere recorded by the optical methods The resulto of the" me"xirv-
Monte am as follovs:
concentration of diametetof rate of detonation Noe of
HR.,,, wt % gap ms
char M/sec esperimen
-0SI ftI4
j -IV 31)
90 7-4 1 7
440-25 2
80 n 7060-11
~rlg. rrEg has: table an I figure,
ASSOCLWION i Institut Ithi-4 chaskoy fiziki Akadomij nauk MR (LIsti" of
Chemical PIW*Ias,, Aaa4esW of SoLences SWR)
susavm: 3ODu63. SHOL: 00
so CWst YP NO MW owl 002 1 002
L L11 L i L 1
L 2M." W(mVM(01W(J)1ZAWA(c) RPL- WWIJWIJWDIFM
ACU93 Mki APS026032 UK/0403/65/000/001/CI09/0111
AUMORI Parfenov, A. K. (Wacow); ~Ritlj A. Va. (Moscow)
TITL9t Low-velocity, de on a powdered explosives
~n& t I~
SOURCEt Mauchno-tekhmicheskiye problemy Soreniya i vzryva, no. 1,*19650 109-111
TOPIC TACSs explosive, detonation theory, weak detonator, strong detonator,
detonation velocityo detonation
ABSTRAC"I't Previous studies have mhown that the detonation velocity D in liquid- 1
and solid-explosive charges depeuds mainly on the power of the detonator. This
dependence was stuidlea using the high-speed photogrNhic camera IM-2. Sherpa
(5-40 um in diameter d and 50-4W us lonj) of.1KRU, tatryl, and h"toganwere
detonated with a week and a strong diatons. _r
tot. x GTA-Naci (som) squib
(d - 20 me, dmnsiW p - 1.0 &/". and D a 2000 st/see) was used as the weak distoostoft
i the saw siss squib of compacted tratyl (p - 1.62 &/cc, D - 6900 Wase) was used
as the troing detonator# The charge diameter dependence curves of the distouatiou
veloc14 (D vs. d) show that In all comes where the charges are detainated with
the weak detonator. then Is a certain charge dismater range within which low-
velocity Jotonation is stable, Its low-velocity detonation increased five 1200 to:
IBDD.-Zloo &/see the charge dimater increased. to the case of tstryl, the
CWd "I/)_ _- - I , . . 11 - I . - i
L 2111-6i
ACCESSION NRt APS026032
velocity also depends on the site of its particles, The upper limit of
which low-velocity detonation is stable varies with the explosive (%30 MM 1%)k
trotyl, %17 mm for hazogen, aud N20 = for tatryl with a partic-lo site of ~'LO-1.6 no.
The low-velocity detonation regime which is developed in totryl and hezogen
charges changes suddenly to a normal velocity reglain after a distance of about
2-4d of the char&*. In trotyl charges, the low-velocity detonation changes
slowly to a normal regime. In the explosive charges detonatnd with the strong
detonator, a stable normal velocity detonation regime to established at a short
distance from the initiation point and in the came of trotyl end hexagen, the
detonation propagates with an approximately constant velocity over the d tango
studied. In the cooo* of te'tryl, a stable detonation was observed only in charges
of a cftt-&W dUwotoor. Thus, In trotyl and hexogen charges, depending on the detonator
used, stable low-velocity or normal-volotity detonation regims are established In
a certain rangs of diameter*; andlin the case of totryl. a stable detonation
regime is established only In charges of a certain diameter regardless of the
detonator used, To explain the lov-volocity detonation Initiated by & weak
detonator, It to suggested that the amount of heat liberated during Initiation by
a weak detonator Is not sufficient to maintain tha combustioa Inside the charge
particles and so the combustion propagates on their surface. Oris. art. hani
3 figures and 1 formula. (PS)
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