ÇÀÊÀÇÀÒÜ

ÂÎÏÐÎÑÛ ÀÒÎÌÍÎÉ ÍÀÓÊÈ È ÒÅÕÍÈÊÈ
Ñåðèÿ "Òåîðåòè÷åñêàÿ è ïðèêëàäíàÿ ôèçèêà"

Ãîä: 2010 2009 2008 2007 2006 2005
Âûïóñê: 1-2-3 1-2-3 1-2-3 1-2-3 1 1-2-3

 

 

2010 ã.
BÛÏÓCÊ 3

ÀÍÍÎÒÀÖÈÈ:

ÓÄÊ 533.7
ÌÈÊÐOCÊOÏÈ×ECÊAß ÝËEÊÒÐOÍÍO-OÏÒÈ×ECÊAß ÐEÃÈCÒÐAÖÈß ÏÐOÖECCA ÂÛÁÐOCA ×ACÒÈÖ CO CÂOÁOÄÍOÉ ÏOÂEÐÕÍOCÒÈ ÓÄAÐÍO-ÍAÃÐÓÆEÍÍOÃO CÂÈÍÖA / Í. Â. Íeâìeðæèöêèé, A. Ë. Ìèõaéëoâ, Â. A. Ðaeâcêèé, Â. C. Cacèê, Þ. Ì. Ìaêaðoâ, E. A. Coòcêoâ, C. A. Aáaêóìoâ, A. Â. Ðóäíeâ, Â. Â. Áóðöeâ, C. A. Ëoáacòoâ, A. A. Íèêóëèí, E. Ä. Ceíüêoâcêèé, O. Ë. Êðèâoíoc, A. A. Ïoëoâíèêoâ, O. Í. Aïðeëêoâ // C. 3
ÐÔßÖ-ÂÍÈÈÝÔ, ã. Ñàðîâ

Ïðeäcòaâëeíû ðeçóëüòaòû ìèêðocêoïè÷ecêoé ýëeêòðoíío-oïòè÷ecêoé ðeãècòðaöèè ïðoöecca âûáðoca ÷acòèö co câoáoäíoé ïoâeðõíocòè óäaðío-íaãðóæeííoão câèíöa, èìeþùeé ðaçíóþ còeïeíü øeðoõoâaòocòè, ïocëe âûõoäa ía ïoâeðõíocòü óäaðíoé âoëíû c äaâëeíèeì ~15 ÃÏa. Ðeãècòðaöèÿ ïðoöecca ocóùecòâëÿëacü âèäeocúeìêoé ÷eðeç cècòeìó c oòíocèòeëüío áoëüøèì êoýôôèöèeíòoì oïòè÷ecêoão óâeëè÷eíèÿ. Äëÿ ïoäcâeòêè ïðoöecca ècïoëüçoâaëcÿ êoðoòêèé (4 íc) ëaçeðíûé èìïóëüc. Çaðeãècòðèðoâaíû ÷acòèöû câèíöa ðaçìeðoì oò 3 ìêì è ïocòðoeí èõ cïeêòð.

MICROSCOPIC ELECTRON-OPTICAL RECORDING OF PARTICLE EJECTA FROM FREE SURFACE OF SHOCK-LOADED LEAD / N. V. Nevmerzhitsky, A. L. Mikhailov, V. A. Raevsky, V. S. Sasik, Yu. M. Makarov, E. A. Sotskov, S. A. Abakumov, A. V. Rudnev, V. V. Burtsev, S. A. Lobastov, A. A. Nikulin, E. D. Senkovsky, O. L. Krivonos, A. A. Polovnikov, O. N. Aprelkov // P. 3

The authors present results of microscopic electron-optical recording of particle ejecta from free surface of shock-loaded lead, where the free surface has different roughness levels (Rz80, Rz20, Rz5), after shock wave arrival to the surface at pressure of ~15 GPa. The process was recorded by video camera through a system with relatively high optical magnification coefficient. Short laser pulse (4 ns) was used for illumination of the process. Lead particles with sizes of 3 µm and more were recorded, and their spectrum was depicted.

ÓÄÊ 621.039; 519.224.2
AÍAËÈÒÈ×ECÊÈE AÏÏÐOÊCÈÌAÖÈÈ ÄËß ÐAC×EÒO ÐAÇÌEÐO CËÓ×AÉÍÛÕ ÂÛÁOÐOÊ C ÄEÔEÊÒAÌÈ ÏÐÈ Ó×EÒE È ÊOÍÒÐOËE ßÄEÐÍÛÕ ÌAÒEÐÈAËO / A. Ì. Çëoáèí // C. 7
ÐÔßÖ-ÂÍÈÈÝÔ, ã. Ñàðîâ

Ïðè ïðoâeðêe âûïoëíeíèÿ íoðìaòèâíûõ òðeáoâaíèé ê cècòeìe ó÷eòa è êoíòðoëÿ ßÌ ýêcïëóaòèðóþùeé oðãaíèçaöèè øèðoêo ïðèìeíÿþòcÿ âûáoðo÷íûe ïoäòâeðæäaþùèe èçìeðeíèÿ ßÌ, oáúeì êoòoðûõ äoëæeí áûòü çaïëaíèðoâaí ïðè ïoäãoòoâêe è âûïoëíeíèè êoíòðoëüíûõ ïðoâeðoê è ôèçè÷ecêèõ èíâeíòaðèçaöèé.  oáùeì cëó÷ae ðaçìeðû cëó÷aéíoé âûáoðêè oïðeäeëÿþòcÿ ÷ècëeííûìè ðac÷eòaìè c ècïoëüçoâaíèeì êoìïüþòeðíûõ ïðoãðaìì (íaïðèìeð, ïðoãðaììû SpotCheck). Äëÿ ðac÷eòoâ ðaçìeðoâ âûáoðoê â êoíêðeòíûõ çoíaõ áaëaíca ßÌ óäoáío ècïoëüçoâaòü aíaëèòè÷ecêèe aïïðoêcèìaöèè.  íacòoÿùee âðeìÿ ía ïðaêòèêe øèðoêo ïðèìeíÿeòcÿ èçâecòíoe aíaëèòè÷ecêoe âûðaæeíèe, çaâècÿùee oò äoâeðèòeëüíoé âeðoÿòíocòè Ð0  è «íeäoïócòèìoão ÷ècëa äeôeêòoâ» D0. Ê coæaëeíèþ, ècïoëüçóeìaÿ ôoðìóëa cïðaâeäëèâa òoëüêo äëÿ áeçäeôeêòíûõ âûáoðoê. Oäíaêo ïðè ïðoâeäeíèè âûáoðo÷íûõ ïðoâeðoê cðeäè oòoáðaííûõ ýëeìeíòoâ ìoãóò áûòü oáíaðóæeíû è äeôeêòû, ïðè÷eì äeécòâóþùèe íoðìaòèâíûe êðèòeðèè â ýòèõ ócëoâèÿõ ìoãóò è íe íaðóøaòücÿ.
 ïðeäëaãaeìoé ðaáoòe ía ocíoâaíèè ìeòoäa oöeíêè ãèïoòeç ïoëó÷eíû äâe ïðèáëèæeííûe ôoðìóëû, ïoçâoëÿþùèe c ïoìoùüþ êaëüêóëÿòoða âû÷ècëÿòü ðaçìeðû cëó÷aéíûõ âûáoðoê, íeoáõoäèìûe äëÿ ïoäòâeðæäeíèÿ âûïoëíeíèÿ íoðìaòèâíûõ òðeáoâaíèé, â øèðoêoì äèaïaçoíe ðaçìeðoâ cècòeì ïðè íaëè÷èè oäíoão èëè äâóõ äeôeêòoâ â âûáoðêe è c äocòaòo÷ío õoðoøeé òo÷íocòüþ.

ANALYTICAL APPROXIMATIONS FOR CALCULATING RANDOM SAMPLING SIZES WITH DEFECTS FOR NUCLEAR MATERIALS CONTROL AND ACCOUNTING / A. M. Zlobin // P. 7

When conducting inspection of fulfillment of the normative requirements to Nuclear Materials Control and Accounting System (NM C&A) of the Operating Organization it is using random NM Confirmatory Measurements, volume of them must be planned in the frame of the preparing and conducting control inspections and physical inventories.
In general random sampling sizes are calculating by using computer codes (for example, Spotcheck). For calculating random sampling sizes in the Material Balance Area (MBA) it is convenient to use analytical approximations. At present it is often employed well-known analytical formula for calculating random sampling sizes, depending on the probability Ð0 and «inadmissible» defects number D0. Unfortunately this formula is correct only for the random samples without defects. Nevertheless in the frame of the sampling inspections defects may be found out without violating normative NM C&A criterions.
In the present paper two approximate formulas for calculating random sampling sizes with one or two defects are obtained on the base of estimating statistical hypotheses. The formulas allow finding sampling sizes necessary for testing fulfillment of the normative NM C&A criterions with calculator only, without using computer codes, in a wide range of the system sizes and with a high accuracy.

ÓÄÊ 532.4
ÏOËÓÝÌÏÈÐÈ×ECÊAß ÌOÄEËÜ ÓÐAÂÍEÍÈß COCÒOßÍÈß ÌEÒAËËO C ÝÔÔEÊÒÈÂÍÛÌ Ó×EÒOÌ ÈOÍÈÇAÖÈÈ. ×ACÒÜ 1. OÏÈCAÍÈE ÌOÄEËÈ / Ä. Ã. Ãoðäeeâ, Ë. Ô. Ãóäaðeíêo, A. A. Êaÿêèí, Â. Ã. Êóäeëüêèí // C. 19
ÐÔßÖ-ÂÍÈÈÝÔ, ã. Ñàðîâ

Oïècaía ïoëóýìïèðè÷ecêaÿ ìoäeëü óðaâíeíèÿ cocòoÿíèÿ, oðèeíòèðoâaííaÿ ía oïècaíèe òeðìoäèíaìè÷ecêèõ câoécòâ ìeòaëëoâ â øèðoêoé oáëacòè cocòoÿíèé.  cocòaâëÿþùèõ äëÿ ó÷eòa âêëaäa â äaâëeíèe è ýíeðãèþ òeðìè÷ecêè âoçáóæäeííûõ ýëeêòðoíoâ ýôôeêòèâío ó÷èòûâaeòcÿ âëèÿíèe ía ïoâeäeíèe òeðìoäèíaìè÷ecêèõ ôóíêöèé cíÿòèÿ âûðoæäeíèÿ ýëeêòðoííoão ãaça è èoíèçaöèè. Âêëaä aòoìoâ ïðè íèçêèõ òeìïeðaòóðaõ oïècûâaeòcÿ ìoäeëüþ Äeáaÿ. C óâeëè÷eíèeì òeìïeðaòóðû ðeaëèçoâaí ïeðeõoä ê ìoäeëè èäeaëüíoão oäíoaòoìíoão ãaça.

SEMI-EMPIRICAL MODEL FOR EQUATION OF STATE OF METALS WITH EFFECTIVE CONSIDERATION OF IONIZATION. PART 1. MODEL DESCRIPTION / D. G. Gordeev, L. F. Gudarenko, A. A. Kayakin,V. G. Kudelkin // P. 19

Described here is a semi-empirical model of equation of state for metal thermodynamic properties description in a wide range of states. The effect on the character of thermodynamic functions of electronic gas and ionization degeneracy minimization is taken into proper consideration in components taking into account the contribution to pressure and energy of thermally excited electrons. Debye model describes atom contribution at low temperatures. The transition to the model of ideal monatomic gas is realized as temperature grows.

ÓÄÊ 532.4
ÏOËÓÝÌÏÈÐÈ×ECÊAß ÌOÄEËÜ ÓÐAÂÍEÍÈß COCÒOßÍÈß ÌEÒAËËO C ÝÔÔEÊÒÈÂÍÛÌ Ó×EÒOÌ ÈOÍÈÇAÖÈÈ. ×ACÒÜ 2. ÓÐAÂÍEÍÈE COCÒOßÍÈß AËÞÌÈÍÈß / Ä. Ã. Ãoðäeeâ, Ë. Ô. Ãóäaðeíêo, A. A. Êaÿêèí, Â. Ã. Êóäeëüêèí // C. 26
ÐÔßÖ-ÂÍÈÈÝÔ, ã. Ñàðîâ

Ïðeäcòaâëeíû ðeçóëüòaòû ðac÷eòoâ ïo óðaâíeíèþ cocòoÿíèÿ Al, ðaçðaáoòaííoìó c ècïoëüçoâaíèeì ìoäeëè, oïècaííoé â ÷acòè 1 (cì. íacò. âûï., c. 19–25). Ía ïðèìeðe oïècaíèÿ ðaçðaáoòaííûì óðaâíeíèeì cocòoÿíèÿ ýêcïeðèìeíòaëüíûõ è ðac÷eòíûõ äaííûõ, õaðaêòeðèçóþùèõ òeðìoäèíaìè÷ecêèe câoécòâa ýòoão ìeòaëëa, ïðoäeìoícòðèðoâaía oáëacòü ïðèìeíèìocòè ìoäeëè. Ïðeäcòaâëeíû òaêæe ðeçóëüòaòû cðaâíeíèÿ ðac÷eòoâ ïo ðaçðaáoòaííoìó óðaâíeíèþ cocòoÿíèÿ c ðac÷eòaìè ïo äðóãèì ìoäeëÿì: Òoìaca–Ôeðìè c ïoïðaâêaìè Êèðæíèöa–Êaëèòêèía; Òoìaca–Ôeðìè–Äèðaêa; Òoìaca–Ôeðìè–Äèðaêa–Âaéçeêeða, Caõa è äð.

SEMI-EMPIRICAL MODEL FOR EQUATION OF STATE OF METALS WITH EFFECTIVE CONSIDERATION OF IONIZATION. PART 2. ALUMINUM EQUATION OF STATE / D. G. Gordeev, L. F. Gudarenko, A. A. Kayakin, V. G. Kudelkin // P. 26

Given here are Al equation of state computation results using the model from Part 1 (see p. 19–25 of the present publication). The range of applicability of the model is shown by the example of experimental and calculated data describing thermodynamic properties of this metal using the equation of state. Equation of state results are compared with other models results: Thomas-Fermi with Kirzhnits–Kalitkin corrections; Thomas–Fermi–Dirac; Thomas–Fermi–Dirac–Weizacker, Saha, etc.

ÓÄÊ 532.542.4
ÏEÐEÊÐÛÒÈE ÄÂÓÕ ÏAÐAËËEËÜÍÛÕ ÇOÍ ÒÓÐÁÓËEÍÒÍOÃO ÏEÐEÌEØÈÂAÍÈß, ÂÛÇÂAÍÍÛÕ CÄÂÈÃOÂOÉ ÍEÓCÒOÉ×ÈÂOCÒÜÞ / Â. Ì. Êòèòoðoâ, O. Ã. Cèíüêoâa, Ã. C. Ôèðcoâa, Þ. Â. ßíèëêèí // C. 35
ÐÔßÖ-ÂÍÈÈÝÔ, ã. Ñàðîâ

Ðaccìoòðeí ïðoöecc ïeðeêðûòèÿ äâóõ ïaðaëëeëüíûõ cèììeòðè÷íûõ ÇÒÏ, oáðaçoâaííûõ ðaçìûòèeì òaíãeíöèaëüíûõ ðaçðûâoâ. Oïðeäeëeía cêoðocòü ðocòa oáúeäèíeííoé çoíû ïeðeìeøèâaíèÿ äo âûõoäa ðaçâèòèÿ çoíû ía aâòoìoäeëüíûé ðeæèì. Ðac÷eòû ïðoâeäeíû êaê â äâóìeðíoé, òaê è â òðeõìeðíoé ïocòaíoâêe ìeòoäoì ïðÿìoão ÷ècëeííoão ìoäeëèðoâaíèÿ óðaâíeíèé ãèäðoäèíaìèêè áeç âÿçêocòè c ècïoëüçoâaíèeì ïðoãðaìì ÝÃAÊ (2D) è ÒÐÝÊ (3D). Ïoêaçaío, ÷òo oáúeäèíeííaÿ ÇÒÏ ðacòeò ìeäëeííee, ÷eì â aâòoìoäeëüíoì cëó÷ae, è äëÿ âûõoäa ee ðocòa ía aâòoìoäeëüíûé ðeæèì òðeáóeòcÿ âðeìÿ, çaìeòío áoëüøee, ÷eì ðaccìoòðeííoe â ðac÷eòaõ.

OVERLAP OF TWO PARALLEL ZONES OF TURBULENT MIXING MADE DUE BY KELVIN – HELMHOLTZ INSTABILITY / V. M. Ktitorov, O. G. Sin'kova, G. S. Firsova, Yu. V. Yanilkin // P. 35

We consider overlap of two turbulent mixing zones; each of them was made by widening of tangential break due to Kelvin – Helmholtz instability. We calculated speed of growth of the united mixing zone using direct numerical modeling. The calculations were performed using the following numerical codes: EGAK in 2D-simulation and TREK in 3D-simulation. We proved that the speed of growth of the unified mixing zone is lower than one in a self-similar case. We proved as well that value of time interval, which is necessary for settling the self-similar regiment is much more than time value that we had in the calculations.

ÓÄÊ 534.222.2:531.3:536.424
ÔAÇOÂÛE ÏÐEÂÐAÙEÍÈß Â ÓÄAÐÍO CÆAÒÛÕ ÕËOÐÈCÒOÌ ÊAËÈÈ È α-ÊÂAÐÖE C ÒO×ÊÈ ÇÐEÍÈß ÐEÍÒÃEÍOÂCÊOÉ ÊÐÈCÒAËËOÃÐAÔÈÈ / Ë. A. Eãoðoâ, Â. Â. Ìoõoâa // C. 39
ÐÔßÖ-ÂÍÈÈÝÔ, ã. Ñàðîâ

Ècïoëüçóþòcÿ ðeçóëüòaòû ðeãècòðaöèè ðeíòãeíoäèôðaêöèoííûõ êaðòèí óäaðío cæaòûõ oáðaçöoâ õëoðècòoão êaëèÿ è α-êâaðöa äëÿ oöeíêè âoçìoæíoão ôèçè÷ecêoão cocòoÿíèÿ âeùecòâa â oáëacòè cocóùecòâoâaíèÿ ôaç è âëèÿíèÿ âðeìeíè ðeëaêcaöèoííoão ïðoöecca ía ïoëoæeíèe ýêcïeðèìeíòaëüíûõ òo÷eê aäèaáaòû Ãþãoíèo â ýòoé oáëacòè. Ýêcïeðèìeíòaëüíûe ðeçóëüòaòû coãëacóþòcÿ c èíòeðïðeòaöèeé, â êoòoðoé cocòoÿíèe âeùecòâa ía ïeðeõoäíoé êðèâoé, coeäèíÿþùeé aäèaáaòû Ãþãoíèo ècõoäíoé ôaçû è ôaçû âûcoêoão äaâëeíèÿ, ìoæío ïðeäcòaâèòü êaê cocòoÿíèe âeùecòâa c íeçaâeðøeííûì ðeëaêcaöèoííûì ïðoöeccoì. Còeïeíü íeçaâeðøeííocòè oïðeäeëÿeòcÿ oòíoøeíèeì âðeìeíè ïðeáûâaíèÿ âeùecòâa ía óäaðíoì ôðoíòe ê ïoëíoìó âðeìeíè ïðoòeêaíèÿ ðeëaêcaöèoííoão ïðoöecca.

PHASE TRANSFORMATIONS IN SHOCK COMPRESSED POTASSIUM CHLORIDE AND α-QUARTZ FROM THE POINT OF VIEW OF X-RAY CRYSTALLOGRAPHY / L. A. Egorov, V. V. Mohova // P. 39

In the report results of registration x-ray diffraction pictures of shock compressed potassium chloride and α-quartz samples for an estimation of possible physical condition of substance in field of coexistence of phases and time influence relaxation process on position of experimental points of Hugoniot curve in this area are used. Experimental results will be co-ordinated with interpretation in which on the transitive curve connecting curves Hugoniot of an initial phase and a phase of a high pressure, it is possible to present a substance condition as a condition with not finished relaxation process. Incompleteness degree is defined by the relation of time of stay of substance on shock front by full time relaxation process.

ÓÄÊ 546.799.4
ÔAÇOÂÛE ÏÐEÂÐAÙEÍÈß ÏËÓÒOÍÈß È ÊÈÍEÒÈÊA EÃO ÂÇAÈÌOÄEÉCÒÂÈß C ÂOÄOÐOÄOÌ / Ï. Ã. Áeðeæêo, A. A. Êóçíeöoâ // C. 42
ÐÔßÖ-ÂÍÈÈÝÔ, ã. Ñàðîâ

Ìoæeò ëè ôaçoâoe ïðeâðaùeíèe â íeëeãèðoâaííoì ïëóòoíèè âëèÿòü ía cêoðocòü eão âçaèìoäeécòâèÿ c âoäoðoäoì? Çäecü èìeeòcÿ â âèäó âëèÿíèe ôaçoâoão ïðeâðaùeíèÿ ía êèíeòèêó ðeaêöèè, aíaëoãè÷íoe âëèÿíèþ, oïècûâaeìoìó ýôôeêòoì Õeäâaëëa (Hedvall effect). ×acòè÷íûé oòâeò ía ýòoò âoïðoc ìû íaøëè â ðaáoòe Ä. Ô. Áoóýðcoêca (D. F. Bowersox. Report LA-5515-MS, 1974). Ïo äaííûì èç ýòoé ðaáoòû, ïðè âçaèìoäeécòâèè Pu c D2 íaáëþäaeòcÿ áëèçocòü ìaêcèìóìoâ çía÷eíèé êoícòaíò cêoðocòè ïðè 125 è 210 °C ê çía÷eíèÿì òo÷eê ïeðeõoäa α–ß- è ß–γ-ïðeâðaùeíèé Pu. Ïðè âçaèìoäeécòâèè â èíòeðâaëe òeìïeðaòóð 335–605 °C âëèÿíèe ôaçoâûõ ïðeâðaùeíèé Pu ía cêoðocòü ðeaêöèè âûðaæeío ìeíee oò÷eòëèâo. Çäecü oòìe÷eío ëèøü òoëüêo oäío coâïaäeíèe ìaêcèìóìa êoícòaíòû cêoðocòè ïðè 460 °C c òeìïeðaòóðoé δ–δ‛-ïðeâðaùeíèÿ Pu.

PHASE TRANSFORMATIONS OF PLUTONIUM AND  KINETICS OF ITS INTERACTION WITH HYDROGEN / P. G. Berezhko, A. A. Kuznetsov // P. 42

We are trying to answer the next question: can a phase transformation in a coupon of bulk unalloyed plutonium activated preliminary by means of heat treatment in vacuum influence upon the rate of reaction between plutonium with hydrogen gas? It means here an influence of the phase transformation on the reaction kinetics that is similar to the influence described by Hedvall effect. We have found a partial answer to this question in Bowersox‛s work (D. F. Bowersox, LASL Report LA-5515-MS, 1974). According to this report, in the reaction between Pu and D2 the proximities of the maxima of rate constants at 125 and 210 °C to the α–ß and ß–γ transition points of Pu are observed accordingly. In the temperature range 335–605 °C the influence of Pu phase transformations on the reaction rate is expressed less distinctly. Just one coincidence of the rate constant maximum
at 460 with δ–δ‛ transformation point is marked in this temperature range.

ÓÄÊ 531.51
ÍOÂÛÉ ÂÇÃËßÄ ÍA ÏÐÈÍÖÈÏ ÝÊÂÈÂAËEÍÒÍOCÒÈ Â OÁÙEÉ ÒEOÐÈÈ OÒÍOCÈÒEËÜÍOCÒÈ / Ì. Â. Ãoðáaòeíêo, Ò. Ì. Ãoðáaòeíêo // C. 46
ÐÔßÖ-ÂÍÈÈÝÔ, ã. Ñàðîâ

Aíaëèçèðóþòcÿ èçâecòíûe èç ëèòeðaòóðû ïÿòü òðaêòoâoê ïðèíöèïa ýêâèâaëeíòíocòè â oáùeé òeoðèè oòíocèòeëüíocòè ía ïðeäìeò èõ coãëacoâaííocòè c óðaâíeíèÿìè oáùeé òeoðèè oòíocèòeëüíocòè. Oêaçûâaeòcÿ, ÷òo coãëacoâaííocòü èìeeò ìecòo ïo oòíoøeíèþ êo âceì òðaêòoâêaì, ça ècêëþ÷eíèeì òoé èç íèõ, â êoòoðoé òðaeêòoðèÿ cïèíoâoé ïðoáíoé ÷acòèöû oòoæäecòâëÿeòcÿ c ãeoäeçè÷ecêoé. Çaâècèìocòü òðaeêòoðèè äâèæeíèÿ ïðoáíoé ÷acòèöû oò íaëè÷èÿ cïèía è òeì caìûì oò âíóòðeííeé còðóêòóðû ÷acòèöû ìoæeò èçìeíèòü cóùecòâóþùèe ïðeäcòaâëeíèÿ o õaðaêòeðe äâèæeíèÿ ïðoáíûõ ÷acòèö âáëèçè cèíãóëÿðíocòeé ãðaâèòaöèoííoão ïoëÿ.

NEW APPROACH TO THE EQUIVALENCE PRINCIPLE IN GENERAL RELATIVITY / M. V. Gorbatenko, T. M. Gorbatenko // P. 46

There are five treatments for the Equivalence Principle in General Relativity. We analyse the treatments to clarify they are consistent one to other or not. It’s find out that a consistency exists for all treatments exclude that in with a trajectory of a probe particle identifies with geodesic line. A dependency of a world path of a probe particles vs an existence of particle spin can change exist views about a character of moving of particles near singularities of gravitational field.

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