SCIENTIFIC ABSTRACT VESELOVSKIY, V.I. - VESELOVSKIY, V.S.

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SCIENTIFIC ABSTRACT
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50) SOV/76-33-2-10/'4r, AUTHORIS: Ifoi3ova, K. 1. , Rakov, A. A., , Veselovokiy, V. 1. ,T--rTLE: A Study of the Electrochemical Behavior of Ozone on the Platinum Electrode by the Method of Cathodic Polarography (Izu- cheniye claktrokhimichonkogo povedeniya ozona na platinovom elektrode metodom katodnoy polyarografii) PERIODICAL: Zhurnal fizichesko khimiif 19599 Vol 33, Nr 2, 1 ' PP 349 - 3',6 ABSTRACT: Experimental material concerning the cathodic reduction of ozone on the rotating platinum electrode in sulfuric acid solutions at 25, 0. -30, -50 and -700C was the basis for thorough investi.gations on the mechanism of the electrode reaction in the region of high anode potentials (analogous to the experiments in reference 3). The apparatus used was previously described (Ref 4). The rate of rotation of the platinum electrode was about 3000 rpm in all experiments. The stationary potential was determined as a function of the temperature at constant ozone concentration in,10 nH SO (Table 1) 2 4 and as a function of the ozone concentration at 250C Mard 1/3 (Table 2). The polarogram curves (Fig 1) which were obtained A Study of the Mectroclemlcal Behavior of Ozone on thO SOV/7C-33-2-18/45 Platinum ElectrDde by the Y'c:thod of Cathodic PolaroUraphy in 10 n H SO saturated with 20a ozone and at 250C indicate 2 't a value of T1/2' 1.30 volt for the ozone reduction, rhile the reverse curve slhoi7s a half-wave of T1/2"1-55 volt for the ozone reduction. The size of the limiting current is directly proportional to the ozone concentration in the solutionp no that the methol of cathode polarography with the rotating I't electrode c~tn ba uned for a quantitative deter- mination of ozone in solutions and in the gaseous phane. At lower temperatures (-30 and -700) two polarogram waves appear for the ozone reduction (Fi.-s 3,4), which is explained in terms of a two-stage reduction reaction (0 3+ e 03; 0- + H + __~k 0 + OH). It is assumed, on the basis of the 3 2 formation of surface oxygen compounds on platinum, that the following reaction mechanism takes place: FtO+2 OH --). PtOE01 ads+H20; PtOC03 ads +2H++2 e- -+ PtO+H 20. Card 2/3 . A Siudy of the Electrochemical Behavior of Ozone on the SOV/76-33-2-16/45 Platinum Electrode by the M1'e-thod of Cathodic Polarography There are 4 figures, 6 tablesp and 7 references, 5 of which are Soviet. ASSOCIATION: Fiziko-khimicheskiy institut im. L. Ya. Karpova..Moskva (11hysical-Chemical Institute imeni L. Ya. Karpov, Moccoly) SUDITITTED: JulY 10, 1957 Card 3/3 84629 S/076 ,/60/034/010/009/022 BO15/BO64 AUTHORS: Shub, D. M.,Tyurikov, G. S.j and V - ____ 0 " - TITLE: Photo- and Radiation-chemical?Decomposition Of HYdrogen Peroxide in the Presence of Iron Oxide "_~60, Vol. 34, No. 10, PERIODICAL Zhurnal fizicheskoy khimii, 1 pp. 2245-2253 TEXT: The application of semiconductor materials as heterogeneous sensitizers in the transformation of radiation energy into chemical energy is of special importance for the utilization of nuclear radiation to initiate radiation-chemical reactions. in continuation of previous in- vestigations, the results are given of the photo- and radiation-chemical decomposition of concentrated H202 solutions with suspended Fe20,. A nPK -2 (PRK-2) quartz lamp served as light source, while Co60 with an activity of 81) Curies was used as I-radiation source; the experiments were carried out in an apparatus warranting a stabilization of temperature, good mixing of the solution, and regular irradiation. The experimental Card 1/3 V 8h629 Photo- and Radiation-chemical Decomposition of S/076~60/034/010/009/022 Hydrogen Peroxide in the Presence of Iron Oxide BO15/BO64 results obtainel show that the catalytic effect of Fe20 3 upon the H202 decomposition due to light irradiation, as well as the V-rays is strongly increased. This means that a chain reaction sets in on the surface of Fe 203 which is due to an energy transfer causing an excitation of the particles of the Fe 203surface, and that the chain reaction of the H202 decomposi:- tion is passed on into the liquid, The high photo- and radiation-chemical activity of Felo can only be lue to the effect of a heterogeneous 2 3 sensitization 'which depends on the electronic state of the semiconductor) The active centers on the Fe2c3 surface which cause the chain reaction are the same in the thermal H202 decomposition and in the decomposition due to radiation. A temperature increase accelerates in both cases the rate of decomposition. Since no particular difference was observed between the effect of the ultraviolet light and the I-radiation, the reaction mechanism is assumed to be the same in both cases. Apparently, the higher energy (approximately 1.25 Mev) of the y-quanta is transformed into a Card 2/3 84629 Photo- and Radiation-chemical Decomposition of S/076/60,/034/010/009/022 Hydrogen Peroxide in the Prenence of Iron Oxide BO15/BO64 lower energy (several ev) of the light quanta, thus, causing the same excitation of the semiconductox as the light rays, no that a princ:cpal analogy exists between the effect of light and nuclear radiation. fie author thanks the laboratory assistant L. G. Kazakova. There are 6 figures, 2 tables, and 11 referencest 9 Soviet, f-British and 1 French. ASSOCIATIONs Fiziko-khimicheskiy institut im. L. Ya. Karpova (Physico-chemical Institute imeni L. Ya. Karpov) SUBMITTEDi February 19, 1959 Card 3/3 7 4 6 010 AUTHORS-: TITLE: PERIODICAL: 3/020J60/132/04/38/064 B004/B0O7 Goohaliyev, 0. Z., Zalkind, To. ID# Veselovskiy !?he Potential of the Platinum Electradelin an Irradiate d Sulfuric Acid Solution- :Doklady Akademii nauk SSSR, 1960, Vol. 132, No- 4P 872-875 TEXT: In eazlier papers (Eefs. 1-4) the authors found that the potential of a Pt electrode in irradiated 0.8 N H 2so4 (irradiation dose 2.1015 ev/OJ.s'eo) assumes a value close to that of the potential of the 9 eleetrods. The present papef6 deals yith the results obtained by a more intensive irradiation (6.1.10 ev/oM-'.seo)o The experiments were carried out with a Cj)60 radiation source,* and the method is described in Refs. 2 and 3. Fig. I shows the dependence of the potential of the Pt electrode in oxygen-free 0.6 N H280 4 on the duration of irradiation. Also with this intensityo selectivity of the Pt electrode with respect to the reduaing radialytio products was observed. The potential assumes a value of between Card 113, The Potential of the Platinum Electrode in S/020J60/132/04/36/064 an Irradiated Sulfuric Acid Solution B004/BO07 10 and 20 mvV which remains aons tant up to a dose of 2.10 20 ev/om 3 and then rises up to 0.85 v (Fig. 1). For the oxidation of the reducing radiolytic products and the reduction of the oxidizing radiolytic productog occurring in the irradiated solutiong the authors derive equations for the currents I and I As the reaction constant k' is R 01' R considerably greater than k I because if the selectivity of the, Pt Ox electrode, the potential observed results. By the escape of R into the gaseous phase -the stoiohlDmetria ratio between the reducing and the oxidizing products is, however, disturbed, which leads to a positive shifting of the potential in the case of high doses. Fig. 2 shows the dependence of the depolarization current at 0-4 v on the duration of irradiation. The course of this curve is,explained as follows: Due to the selootivity of the Pt electrode, the oxidation of H at first pre- dominates. Aa a result of the escape of R into the gaseous phase, the reduction of R 202 is accelerated, the total current (I R - IR 0 ) decreases 2 2 20 3 and attaine negative values in the case of doses higher than 2.10 ev/om If the experivient is carried out in a vessel that is hermetically sealed and gompletely filled with the solution so that no gaseous phase is able Card 2/3 The Potential of the Platinum Electrode in an Irradiated Sulfuric Acid Solution 6/020/60/132/04/38/064 BO04/BOO7 to form and no bldrogen can escape, a potential of +20 mv quickly forms, which remains constant throughout the experiment (20 h)(Fig- 3)~ Because of the increasing concentration of the oxidizing products, the polariza- tion current quickly decreases (Fig- 4). The ionization of the H on the Pt electrode, which is formed by radiolysis, may therefore be carried out in the *&as of a steady potential only if the reduction of the cxidizing products taken place at the same rate (e,g., on a second electrode which is selective for these products). At the same time, a current will flow through the outer circuit. There are 4 figures and 7 references- 6 Soviet and I English. ASSOCIATION:. Flziko-khimioheakiy inetitut im. L. Ya. Karpova (P!jYsico-__ chemical Institute imeni L. Ya. Karpov) PRESENTED: February 26p 19609 by A. N. Frumkin; Academician SUBMITTED: February 25, 1960 Card 3/3 I /---r ,S71-1600 B/020/60/133/03/10/013 B004/BO56 82275 AUTHORSi Lazorenko-Manevichq R. M., Aladzhalova, N. A., -Te-selovskiyl-v. 1. TITLEi Electrochemical and Photoelectrochemical Processes on p- and. n-Type, Germanium in the Region 3f Cathodic Polarization PERIODICALt DoUady Akademii nauk SSSR, 1960, Vol. 133, No- 3, pp. 620 - 623 TEXTs The authors investigated the action of illumination on the separation of hydrogen on germani~Afte experiments were carried out - 21.0 ohm.cm) and n-type Ge with samples of p-type Ge resistivityt 0.5 (1.1 and 22.9 chm'.cm) in IN KOH and IN H 2 so 4* The electrode surface was etched with CP--4 (8R-4) or a mixture of KNO 3 + HF. All experiments were carried out in a hydrogen atmosphere. Illumination was carried out by means of a 300 W lamp through a 10 cm thick water layer. The light -1 2 intensity on the electrode surface was about 10 cal/cm .sec. Fig. I Card 1/3 A41,00, Electrochemical and Photoelectrochemical Processes 3/020/60/133/03/10/013 on p- and n-Type Germanium in the Region of B004/BO56 82275 Cathodic Polarization shows the typical steady curves 0 - 4) after 10 - 15 h of cathodic polarization and durve 5 for not previously polarized p-type germanium. The inflection of the polarization curves of p-type germanium at high amperages is explained by the inhibition of electron diffusion, which does not occur vith n-type Go, because the latter has a high electron con- centration in the conduction band. Fig. 2 a shows the change with time in the overvoltage-I after switching on 10 ma/cm 2. The occurring maximum of 'I depends on the pretreatment of the electrode. In germanium coated with a thick oxide layer (1000 - 2000 A), no maximum ofiZ occurs. The drop of the I-ourve after the maximum is explained by an increase in the rate of the generation of electrons on the germanium surface, which is caused by the absorption.of hydrogen. During illumination of p-type Ge a rapid drop ofiZ occurs due to a photoeffect. Besides, it was observed that in the presence ol'7 hydrogen this drop occurred already in the region of diffusion inhibition, which is explained by photodesorption of H. Fig. 3 shows the potential course in germanium,?(t), without an external current source during illumination and in the dark. In the case of p-type Ge the Card 2/3 kr Electrochemical and Photoelectrochemical Processes 5/020 60/133 03/10/013 YB V2 2 15; on p- and n-Type Germanium in the Region of B004 B056 Cathodic Polarization photoeffect vanishes after a short cathodic polarizationg and in n-type Ge it is intensified. Short anodic polarization no longer reduces the potential to the initial value. The authors draw the conclusion that the adsorption of hydrogen on the germanium surface increases its negative charge aue to the formation of acceptor levels in the forbidden band. Molecular hydrogen does not produce this effect. The illumination of polarized p-type Ge influences the rate of gas separation in an alkaline solution (Fig. 4). Photodesorption occurst Under the action of light the adsorbed hydrogen dissolves in the electrolyte. There are thereforetwo steady states: a dark state and a light state, where the latter differs from the former by the lower probability of gas-bubble formation and the higher content of dissolved hydrogen in the electrolyte% There are 4 figures and 11 referencess 4 Soviet, 5 American, I British, and I German. ASSOCIATIONs Fiziko-khimicheekby institut im. L. Ya. Karpova (Physico- chemical Institute im. L. Ya. Karpov) PRESENTEDs )larch 10, 1960, by A. N. Frumkin, Academician SUBMITTED: Harch 1, ig6o Card 3/3 Ar 82525 S/U20/60/133/04/29/031 Boo4/Bo56 AUTHORS: Yak.eyleva, A. A., Borisova, T. I., Veseloyakiy, V. 1. TITLE; Tho Effect of Light Upon an Anode-polarized Germanium Eloctrode A PERIODICAL: Dolclady Akademii nauk SSSR, 1960, Vol. 133, No. 4, pp. 889 - 89a TEXT: It was the aim of the authors to investigate the effect of illumination upon the structure of the interface between germanium and electrolyte as well as upon the anodic dissolution of germanium. The method employed. permitted illumination of the electrodes through the solution as well as of the dry side of the electrodes. (The electrode formed the bottom of a cylindrical Teflon vessel.) The experiments were carried out with monocrystalline n-type germanium of different resistivi- ties in 0.1 N XaOH in a nitrogen atmosphere. The Ge electrodes were etched with CP-4 (SR-4). Illumination was carried out by means of an incandescent lamp within the range of 0.4 - 0.7,,w, partly with a constant current, and partly with constant voltage, It follows from Fig. 1 that Card 113 82525, The Effect of Light Upon an Anode-polarized S/020/60/133/04/29/031 Germanium Electrode B004/B056 the system was aensitive to light within the entire region of polariza- tion. The potential barrier Is removed by illumination, and the poten- tial drops within the saturation region to the constant value of 0.5 v. Above the breakdown potential this effect stops. In the initial part of the polarization curve, the rate of the anodic reaction is not limited by the concentration of minQrity carriers (Fig. 2). The last-mentioned author derived equation (1);: 1 = k 9xp(-,&yF/RT).9xp(--aAHF/RT) for this region in an earlier paper (Ref. 7); here,,Ay denotes the potential chango in the volume charge of the somiconductor,,dH the potential change in the ionic double layer. 11or A!p, there further exists the dependence (2) on carrier concentratiom on the surface: 0 surf = C Yolumeexp (-ne,WRT). All factors influeacing the surface concentration of electrons and holes must therefore also influence and the total potential difference 6_T- Fig. 3 shows Ailight and A tight a, function of the intensity of illumination. 6ilight increases proportional to the absorbed light quanta. AT14ght rises exponentially in the initial part of polarization, and tends toward a limit with a saturation current. Card 213 82525 The Effect of Light Upon an Anode-polarized 5/0?-0/60/133/04/29/031 Germanium Electrode BOO4/BO56 Table 1 gives the quantum yield X for various intensities of the absorbed radiation in the case of a saturation potential. Table 2 shows thevalues of K for two inten5ities. K has a maximum in the saturation range. The results obtained b illuminating the dry side of the electrode are shown in Fig. 4, namely Xilight as a function of 1/1, the reciprocal value of the thickness of the electrode, 61 light grows linearly with 1/1. No differences between the two kinds of illumination could be found. Also in the illumination of the dry aide of the electrode, a potential drop occurred with olectrade thicknesses that were a multiple of the diffusion leng-~h of the minority carriers. There are 4 figures, 2 tables, and 7 references: 2 Soviet, 4 American, and 1 German. ASSOCIATION: Fiziko-khimicheakiy institut im. L. Ya. Karpova (Physicochemical Institute im, L. Ya. Karpov) PRESENTED: 11arch 18, 1960 by A. N. Frumkin, Academician SUBMITTED: March 18, 196o Card 313 33122 51-Li 5-o o 8/638161/001/000/053/056 *' 3 roe) B125/BIO4 AUTHORS: Shub, D. M.9 Tyurikov, G. S., Veselovskiy, V. I. ---------- TITLE: Heterogeneous sensitization of radiochemical processes on the semiconductor - solvent interface SOURCE: Tashkentskaya konferentaiya po mirnomy ispolizovaniyu atomnoy energii. Tashkent, 1959. Trudy. v. 1. Tashkent, 1961s 370-377 TEXT: Data on the radio-electrochemical process in Cc 60 gamma irradiation (activity --s20,OOO g-equ. Ra) Of a Cu'CU20 electrode in a 0.1 KOH solution are presented. The action of the optical radiation of a 500-watt bulb under the same conditions is compared. The eyetem Cu-CU20-KOH solution was irradiated. after 3-hr saturation with nitrogen. The radi.o-olectro- chemical effect was first determined only from the change of the electrode potential undor the simultaneous action of cathode current and radiation from,&V, a VO.- V T at I a const for potentials between 0-770 v and 0.200 v. The potential was shifted toward more positive values by irradiation. V0 and V T denote the electrode potential during and after irradiation, Card 1/4 333-22 8/63"W151/001/000/053/056 Beterogeneous sensitizatioil ... B1257BI04 respectively. Visible light and gamma rays apparently give rise to similar excitation processes in the semiconductor, with the absolute values of I&Vc under gamma irradiation being higher than with visible light. Fig. Z.,shows the typical dependence of potential change on the duration of irradiation for an initial potential of 0.200 v. Fox the other initial potentials examined) the curve shape wan similar, but the absolute values of A_Vc were lower. The potential jump at the beginning and the following slow approach of the potential to the steady state are due to the excita- tion of the semiconductor and to the electrochemical oxidation, respectively. The compon&nts (OHI 02) appearing in the radiolysis of water speed up the electrochemical reaction. The experimental results available so far are not sufficient to back the assumption of a specific mechanism for the radio-electrochemioal process on the CU*CU20 electrode. They suffice, however, for the following hypothesis: Due to the action of radiationp Clu.20 can be oxidized to Cu(OH)2 . hydrogen peroxide may also be produced Isy a sensitized reaction involving the oxygen which is always present in C112P. The radio-electrochemical process on the Cu-Cu20 electrode is of interest also for heterogeneous radiation sensitizztion. Card 2/4 Heterogeneous sensitization 33122 S16 38/61 /001 /000/0i5~1056* B125/B104 A noticeable sensitization,.however, is only possible in the case of a sufficiently large acting surface of the sensitizer. According to data available on the dampi-A'g of luminescence (see also Veselovskiy V. I., Miller N. B. # Shub D. K. Sbornik rabot po radistnionnoy khimii, It., AN SSSFO 49, 19551 Shub D. M-s Tyurikov 0. S,p Yeaelovskiy V. I., Trudy I Vaesoyuznoeo ooveshchaniya po radiatsionnoy khimii, M., AN SSSR, 161t 1958), the energy bf excitation of a semiconductor by electrons can.be transferred to the solution componente. A participation of excit4d electrona of the semiconductor with more than 3.0 ev in the reaction, and an excitation of radio-chemical processen by the energy absorbed and converted by the semiconductor are possible. The rate of disintegration under the action of irradiation is considerably increased by the presence of an Fe 203suspension. In a microheterogeneous system, the suspension Fe203-H 202solution is not substantially changed by radiation, and, therefore, tho rate of hydrogen peroxide decomposition does not change either. The heterogeneous process depends on the electron state of the semiconductor, and the active surface centers determining the reaction are of ihe same nature during decomposition due to heat and irradiation. The Card 3/4 33122 S/638/61/001/000/053/056 Hetbr,ogeneous vensitization ... B1257BI04 experimental data fit the said hypothesis and are indicative of the possible excitation of-lieterogeneous sensitization processes. There are 5 figures, I table, and 8 references: 7 Soviet and I non-Soviet. ASSOCIATION: N.-i. fiziko-khimicheakiy inatitut im. L. Ya. Karpova (Scientific Physicochemical Research Institute imeni L. Ya. Karpov) Fig..2. Dependence of the potential change Of a Cu'Cu20 electrode on the duration,of irradiation. Legend: (1) gamma radiation; (2) optical radiatioui. (3 radiation; (4) time, min. Card 4/4 7 , gi 7A i -.104 4010 OIDA 1h 1016 of-Ioxidat on-and 'L. TITLE't; witici -of. aid 0 rogen'-gas'.0A a, P !k. num 2 Ong.-, S '.i-,~-.-~--~i:'-;, Q4 .4- A, -- - -19,61"t .22564264'____- L-1 isid 4's-kay" M I" iiji.,*. Aio 10 PIRIODIVAL": -kh -~z M el~~&-_,Me 0 :20abi f --The 46sb:i~i 'if fictivo, i~:rate aut4drs, Of ------- 2 _d n- gas: on - a-, plat hum Mat ioiv,'_ a dati okf,;~ Ov're nd a stion"- o h t iToxy y roge electrode-, . bas , od __ on gts- -cO.nsUMptit- -confron 4tion is.,made with data ft k found earlier by polarography (Ref. 11: _K I. Rozenta- if I; - Veselovskiyj Zh. fiz. khimii, 31, 1555, 1732, 1957). Fig. I shows the experimental arrangement. The electrode to be tested is placed in the central part A, and the auxiliary platinum electrode B is situated in the lateral ramifications along with the reference electrode C (Pd sheet saturated with H2). The electrode to be tested consisted of a platinum net wrapped around a glass tube which was caused to rotate at 700 rpm by a magnetic field. A was filled with electrolyte (1 N H 2so 4; 1 N HC1 04 or 1 N KOH) -shich was Card 1/4 A-,/ 28287 S/07 61/035/010/004/015 Kinetics of the! electrochemical ... B101 YB110 saturated with the respective gas mixture (H 2 :N 2 - 2 ; 1j 02 : N2 = I . 2; H2 : 02 - 2 : 1) at atmoupheric pressure and 200C. For the preparation of gas mixtures and electrolytes, see Ref. 11. After the desired potential was attained by polarization, the gas volume that entered reaction within 30 min or I hr -was determined by the level of the liquid in the burette D at the beginning and end of the experiment. The rate &j(cm3/hr) of the eloctrochemical reaction was measured as a function of the potential f. The following was found: N&J.2 in 1 11 H2SO4amounted to ~1 CM3/hr 'letween 0.15 and 0.8 v. On a passivated anode (0-9-1.4 v), co still wa.3 50-3VY* of the maximum rate, and thus was higher than had H2 been found in Ref. 11 by polarography. The oxidation of H2 on a passivated electrode was assumed to take place by interaction with chemosorbed 02 vdiich was either set free electrochemically or entered from the gaseous phase (in case of oxyhydrogen gas). (2)4j 02 max was twice as high In acid solu- tionB as in alkaline oneE. The values based on gas consumption agreed With those based on current consumption. (3) The rate of reaction of oxyhydro Card 2/4 28287 S/07 61/035/010/004/015 Kinetics of the electrochemical ... BIOIYB110 gas depended on the electrode,potential, on the type of anion, and on the pH of the solution. In case of a steady potential (V - 0) 1 the "combUBtiOril rate.of oxyhydrogen gas in 1 X H2S04 0.6-0.8 v) approaches the maximum rate, end is almost twice that in I N HC10V and three times that in 1 N KOH (,~ 11C104and IKOH - 1.6 v). The assumption that H2 ionization and 02 reduction in oxyhydrogen gas take place independently of each other is valid with restrictions (for KOH, and in part also for HC'04)' *n general, these processes exert a reciprocal influencet and gi~ve rise to either.an increase of the rate (with H2solt, ) o.r to an in"aibition of H2 ionization (with HCIO4). 0. A. Petrov assist.ed In the work. There are, 7figures and,16 references: 9 Soviet and 7 non-Soviet. The two most recent references to Engl I eh- language publications read as follows: M. J. Joncicht 11. Hackerman, J. Phys. Chem-p Ut 674, 19531 J. M. Kolthoff, J. Jordan, J. Amer. Chem. 80c- ]At 570 and 4801, 1952. SUBMITTED:- February 111 1960 TBUSOVI GA.; AIdZHALOVA, N.A.; VESELOVSK.I.Y, V.I. SepLration of hydrogen iootopes on a panadium cathode, DokloAN SSS11 138 no.6:1385-2388 .16 161. (KMA, U.- 6) 1*. fisiko-khWobaskiy institut imo L.la~Karpovae Predstavleno akedemikom A.N.Frw*lnym. (Nydrogen--TAotopes) BORISOVA,, T.I.; VF,8BL01r:JKTYp.VI, Eleotrocbemical and photoelectrosAamical be&--vlor of the silicon electrode in acid and alkaline solutions. Zbur. fiz. kbim. I'll no.60246-1254 Jre'62 (MIRA L Fiziko-khimicheskiy- Institut imeni Kailova, ~btikva. MAZITOV, Ti.A.; ROZENTAL-110 K.f.; VE'l-novsKlyp V.I. lonLzation of cxygen at a three-phase baarxh--y in alkaline solutions. Zhur. fiz. khim. 38 no.2:449-455 F 164. (M1 W. 17: 1, Fiziko-khimicheckiy institut iment Kamovae ___m MAZITOV, Yu.A,j RMENTALI, K,I,.,* MEWV5Y11Y,,~ Y,I, (HOSCOV) Ionization of oxygen at a three-phase boundary in alka2ine oolutions. Zhur. fit. khim. 38 n3.3t697-701 Mr '64. (MIRA 17-.7) 1. Fiziko-khimiches'Uy institut imeni L.Ya, Karpova. MAZITOV, Y%,A.; ROZENTALl j K.l.j VE,%M:uV3KlYi V.1. Oxywen ionizaticn on a sil"fer -'--trade In alkaline solution, Elektrokhlmlia I n0.1-.36-410 J- 165. (MIRA 1815) 1. Nituchno-issladavatel'skly fiziko-khimicheskly institut Im. L.Ya. Karpt)va, Moskva. all It alka LL. Cam L 4 9 4,6- 7 - -esTs IT -al et j:: O--M--J 0-a- krhyatca a --kiv ins Ya 'Karp*v I A 0 C r f,:Fi I--i -I-! r-! z.1 t. 7~kj, sm- cc tRin f the rural nonagri cultural geography 0 Czv. Vaes. geogo Several fca-t;UrOa of '~he Vologda ITOVInc6v (MIRA 1831) Populated localities of _0 t 6,4 ot,va 1)6 no.6z488-494, 11 MAZITOVJ, Yu.A.; RDZENTALI, K.I.; ~T_S !qXj_y~~. (Moscow) Anodic formation and cathodic removal of oxides on palladium. Zhur. fiz. khim, 38 no.1:151-155 'Ja'64. (MIRA 17:2) 1. Fiziko-khimicheskiy institut imeni L.Ya. Karpova. ,AOOES SION NR: AP4011448 SWO-076/64/038/001/0151/0155 ~AUTHORS; Mazitov, Yu. 'A. (Moscow); Roazental't X. 1. (Moscow); Veselovsk (Mosoow) ;'TITLE: Anodio formation and oathodio removal of oxides on palladium Zhurnal Xiz. kh1m, v. 38, no. 1, 1964p 151-155 ,,TOPIO TAGS: anodic palladium oxidation, cathodic palladium reduction iABSTRLOT: The soarcity of work on the anodic behavior of Pd prompted. .'-'this study. The authors investigated the formation and reduction-of., :,palladium oxides in 10.6 N KOH at different temperatures by plotting .Ahe curve of cathode charge after prior polarization of the electrode ot. ~ 1.Vith different potentials. It has been found that begl=lng with 1.05 v anode potential, the '-Id surface becomes coated with a divalent Pd oxide, or at the potential of oxygen liberation with two differenV.- ,oxides. It is supposed that the second is a perokide. Th6 rate of ;oxide decomposition rises with the temperaturp, and the'stabIlity :of the first oxide is greater than of the second. IIt was found that 'the slope of the Tafel equation for cathodic reduction of both oxides :Card ~ 1/2 AGOBSSION n APA*11448 iis 55 mv. The formation of an overvoltage resulting from the re- -iduotion of the second oxide has been observed and It Is attributed ~to ooncentrated ;,olarization in the oxide layer, OrIg. art, havi ..13 Figures ASSOOIATION:.PJ.z:lko-kh:Lmloheak:ly institut Im. L. Ya. Karpova! (physloo-chemioal.lustitute) SUB OODE: OR DATE JLCQ: l4Peb64 lNot: .00, SUMaTTED: 17Apr63 NR UP. SOV:- 001 OTM* OU 2/2 VESEIDVSKIY, V.I.; BORISOIIA, T.I.; YAKOVLEVA# A.A.; IZIDIROV, S.O. - . ...... wSom Specific Features of the Double Ia7er Structure and Electrode Process on Elemental and Oxide Semiconductors Go, Sip hg~O# Ta '2050 Tj02*v* Report presented at the 14th mating CITCE, Intl. Comm* of glectrochanical TherrWynamice and Kinetiesp Moscowp 19-25 Aug 63. Karpoy ftpico-Clamical Xnetitute,, Moscow# U.S.S.R. ROZENTALI K.I.; VESEIDVSKIY, V.I.; *Inimai uchastiye: FEIROV, G.A. Wscow) Kinetics of the electrochemical oxidation and reduction of ff2Q2 and oxyhydrogen on an Au electrode in N H2S04 solution. Zhurefiz.khim. 35 no.11:21+81-2486 N 161. (MIM 14:12) le inatitut, imeni L.Ya. Karpova. Hydrogen) Oxygen) ~Orldsttlon-reduction reaction) 8/844 62/000/000/028/129 D244YD307 ''AUTHOR: Veselovskiy, V. Io TITLE: Radiation-electrochemical processes in aqueous solutions SOURCE: Trudy Ii Vaesoyuznogo soveshchaniya po radiatsionnoy khi- mii. Ed. ~y L. 6. Polak. Moscowt I.,,,d-vo AN SSISRt 19629 171-175 TEXT: The appearance and evolution of stationary radiation-electro- chemical processes is described. The process of changing the elec- trode potentials was carried out in aqueoas H 280 , under the action of r rays, using gold and platinum electrodes. He Pt electrode po- t6ntial drops from about 0.9 v to.0.05. v '(stationary potential) af- ter 30 hours and that of the Au electrode increases slowly from about 0.7 v to 0.9 v (stationary potential). The fall of the Ft electrode potential to a value near that of the hydrogen electrode -is explained by the selectivity of the Pt electrode in respect to the radiolysis products of water (H and H2). stationary potentials --of a metal electrode reached under the action of radiation of a Card 1/3 5/844/~2/00/000/028/129 Radiation-electrochemical' 1)244/,V,)07 givQn intensity* are iven by 0 t q)0 k fox [Ox] Ox red + RT 1n Tstat 2. 2dF k;ed ~edj 0 and 0 are-the values of stationary potential for the where YOX red oxidizing and reducing components respectively and the k 6X and kred are resdectively the rate constants for the-electrochei,,tical oxida- tion and reduction processes. The total ionization flow in,the Pt electrode in an.uninsulated system increases with the radiation do- . 21 sage to about 0.1 ev/ml x*10 and then decreases to a value below zero. The cros3ing of the zero line indidates that considerable ionization of H202 takes place. The ionization current in the i't electrode in an .insulated system reaches the 'maximum value rapidly Card 2/3 8/844/62/000/000/028/129 Radiation-electrochemical ... D244/D307 and then falls slowly to a value slightly above zero. For the Au/Pt electrodes acting separately and selectively to oxidizing aqd reduc- ing components the current remains constant (about 6 mka/cm~) inde- finitely. The power yield in the processes does not exceed 2 3~4 of the absorbed radiation energy. There ari 3 figures. ASSOCIATION: Fiziko-khimicheskly institut Im. L. Ya. Kar~ova (Phy- sico-Chemical Institute im; Ya. Karpov) Card 3/3 8/84 62/000/OOU/030/129 D244YD307 AUTHURj: Gochaliyev, G. Z.j Zalkind, Ts. I. and Veaelovskiy, V. I. VITLE: The radiation electrochemical processes in oxygen-bearing aqueous solutiona of sulphuric acid SOURCE: Trudy 11 V8euoyuznogo-ooveshchaniya po radiatsionnoy khi- mii. Ed. by L. 6. Polak. i-iosc.owg Izd-vo AN 8SORt 1962t 183-187 TEXTz The authors investigated radiation-chemical processes in 02-c ontaining solutions to obtain additioYial data on the interme- diate reaction-products. The experimentB ivere conducted at 10 OC + 1,0C with a rotating Pt electrode and a dropping Hg electrode i-m-_ mer8ed in 0.005 H 11260 + 0.5 N Hu 2so4 containing 02# '2he irradia- tion dosage was 4 x 1016 ev/mlouec. On irradiation there appear two waves in the polarization curve for the',Pt electrode, occurring at 0.76 and 1.06 v, corresponding to the oxidation of H 0 formed 2 2 Card 1/3 The radiation ... J/844/62/000/000/030/129 1)244/D307 during irradia-,ion, and Q'tV value of the li6iting current at the reducing potentialij of U is increaued. Pif ty minute8 after the, be- ginning of irradiation, 9tutionary currents are established, cor- responding to the oxidation of H202, After the end of irradiation, curreAt decreakiec in both cases, which it; accribed to the disap- pearance of intermediate reaction products cEipabl2 of being oxi- dized at the sa-.ie potentiul~ as H202 and reduced at the reduction potential of 0. at the,Pt electrode. For the dropping Hg electrode. ,there are also two polarization waves, the first of which corres- ponds to the reduction of 02 to H202 through the intermediate stage of H02 formation, and the second corresponding to the reduction of H202 to H20. An increase in the current during irradiation takes place both at the reduction potentials of 02 and at that of H2020 .For the Pt electrodeq the current decreases at the reduction poten- tials of 02 after the irradiation is cut offs The 8tationary con- Card 2/3 8/84 62/000/000/030/129 The radiation D244YD307 centration of If202obtained during the irradiation.wae calculatedo With decreasing concentration of H 0 (1,64 to 1.18 n x 10- 3) the 2 2 10-4 concentration of the intermediate products falls from 3.4 x to 1.6 x 10-4 N. 'ehere are 5 figur*es and 1 table. ABSOCIATIONs kiy instiXut ime L. Ya Karpova (.Phy- Pizik6-khimiches aico-Chemical Institute im. L. Ya. Kar;ov) Card 3/3 S/844/62/000/OOU/031/129 D244/D307 AUTHORS: Shub, D. M., B-31okopytov, V. Po and Veselovskiy V. I. TITLE: Investigation of radiation-chemical processes using semi- conductor electrodes SOURCE: Trady II Vfjeso:yuznogo. soveShchaniya po radiataionnoy khi- mi-' . B'd. by L. 6. j?olak. Hoscow, Izd-vo AN SGSR, 1962, 188-192 TEXT: The system Cu - Cu20/KOH solution was investigated to de- tormine whether semiconductor ulectrodee,tranaform the aboorbed energy of irradiation into electronic excitation energy, as is cur- rently believed. The solution (0.1 N KOH) containing the (;u-Cu2 0- 60 electrode wao irradiated with rray's from a Co source with an ac- tivity of about 20,000 g-eq4iv. Ra, and with visible light (500 W lamp). Under the irradiationj a uhift of the CU-CU20-electrode po- tential (in the region of 0.2 - 0.7 v) in the positive direction, _yas ob8ervedo A reverse effect was observed in the region of 0.8 - Card 112 3/844/62/000/'000/031/12"] Inveutigation of radiatiori-'... D244/D307 6 1-7 V. Detailed analysis 6f the results in tl ie region of 0.2 - 0.7 v allowed that irradiation'promoted an electrochemical reaction on the electrode 8.urface, which led to the oxidation of Uu20. Reduc- tion of the products of -Vlle oxidizing reaction and return of the electrode to its original state lakes place by means of cathodic polarization. The oxidation reaction occur8 as a reoult of absorp- kaon of the irradiation unargy by Ua 0. The results are interest- ing from the point of view of the Mcidation of the posoibility of reaching a otationaty potential difference uriier the influence of ionizing radiation, since the Cu-Cu20 electrode then assumes a sufficiently high and stable anodic potential. There are 4 fi- gures. ASSOCIATION: Fiziko-khimicheskiy.institut im. L. Ya. Karpova (Phy- sico-Chemical Institute imq L. Ya, Karpov) Card 2/2 3/844/62/000/000/032,/129 D244/D307 AUTHORS: Killer, He Be, Veselovskiy, V. 1. and Borotyntoev, V, A TITLE: Investigation of the mechanism of radiation-electrochemi- cal processes in aqueouu solutions of uranium salts SOURCE: Vrudy II Veesoyuznogo.soveshchaniya po radiatBionnoy khi- mii. Ed. by. L. S. Polak. Moscow, Izd-vo AN SSSR9 1962, 193-198 TEXT: Soluticna of hexavalent U and mixtures of U VI and UIV were investigated to elucidate the mechanism of radiation-electrochemical conversions, using Pt, Au and lig electrodes. The muthod used was that described. previously (Collection:.De~atviye ioniziruyushchikh izlucheniy na nL;organicheskiye i organicheskiye sistemy, Izd-vo AN SSSR, 1958, P. 93 (The action of ionizing radiation on organic and inorganic systems.)).-On irradiation the Pt electrode potential in IV a solution Containing U assumes a value about 2U mv lower than zero (w.r.t. the hydrogen,electrode). The effect is accompanied by Card 1/3 S/844/62/000/000/032/129 Investigation of the U244/1)307 IV .Vigdrous evolution of 11 2 resulting from the preuence of U which acts as an UH acceptor and prevents the recombination of H and OH, VI ~11 ' IV V In the preaence of U .ixnd U.- there is some formation of U by the VY IV V reduction of U and oxidation of U . The yield of U in solutions containing only U VI Was ab Iout 4.ions/100 ev, and in those containing both U VI and U IV' it.was 6 ions/100 ev. Stationary concentrations of V 1 U in the eolutionu were fawid to be In the ratio of - V7. *tudy of depolarization currents at a et electrode potential of 0.4 V, the electrode being illuierued in the uranyl solutions irradiated with 16 4 x 10 ev/'rql.f3E!C, showed that for a given dosage the lower concen- tration limit, cc-i-respunding to approximately complete capture of H by the uranyl ions, ic 5 x 10-2 N. 3tudy'of the formation of U VI and UV on the oxiaation of UIV solutions showed that for increasing Ca!rd 2/3 8/844 62/000/000/032/129 InVeBtIgUtiOn 01' the ... D244YD307 IV V -concentration 01, U the stationary concentration of U becomes greater. Radiation yields G(UV) were found to be 2.1, 1.5, 1.06~per IV 100 ev of absorbed radiation for 0.1, 0.2 and U.4 1-1 solutions of U respectively. Die stationary concentrations,of U V were 1.2 x 10-4 2.2 x 10-4 and 3 x 10-4 M for the same solutions. There are 5 fi- gures. ASSOCIATION: Piziko-khimicheskiy institut im. L. Ya. Karpova (Phy- sico-Cheinical Institute Ya. Karpov) Card 3/3 8/84 62/000/000/045/129 D287YI)307 AUTHORS: Shub, D. 1,1,, Belokopytov, V. P. and Veselovskiy, V. 1. TITLE: Investigations of the radiolytic ox-'ation of organi.c substances sensitized with semicQnductors JOURCE: Trudy II Vsesoyuznogo.soveshchaniya po radiatsipnnoy khi- mii. Ed. by L. S. Polak. Roacow, Izd vo AN ~68R,~1962, 269-273 TEXT: Possible methods were investigated for increasing the yield of products during the radiolysiu of organic substances, by using the system ZnO (suspension) - potassium oxalate (aqueouE; solution)."' The marked effect of heterogeneous uenaitization can only be ob- served when the active uurface of the 8'ensitizer is sufficiently iarge. ZnO ausponsiona in aqueous potassium oxalate were therefore used, being continuously agitated during irradiation (800 rpm). Oxygen or nitro,gen were led through the sol4tion (40 ml/min) and the reaction temperature kept constant at 200C. After irradiation the concentrationa of 'A' (", 0 and If 0 were determined and compared ,-iith 2 2 4 2 2 Card 1/3 j/434 4/62/000/000/04 5/129 Investigationu of the 1)287/P307 L data obtained fov solutiona,not containing AnO. The samples consis- ted of 50 ml of 5.U x 10-3' H K 2C204 solutiozi (containing 1 g ZnO). Investigations on, tile relationuhip between the decomposition of , K2C204 and tile time of irradiation showed, in the preoence of oxy- gen, that the rate of decomposition increased noticeably in the pre- sence of ZnO. The yieldo also increased (4.7 mol/100 ev as against 2.8 mol/100 ev in homogeneous'solutions) in the presence of ZnO but .no marked discrepancies in the yield of 11 202 could be recorded in the presence or absence of ihe suspension (2,4 and 2.2 respective- ly). The gaseous phase did not contain any C.0 2 and it is suggested that the 00 2 is absorbed by,the solution, increasing its pH. This increase could also be observed during irradiation for e.g. 5 hours. Decompo6ition yields were much higher when the experiments were carried out in a current of nitrogen; increased reaction rates were also recorded but no H 202 could be detected. A linear relat .ionship Card 2/3 8/844/62/000/000/045/129 Investigations of the D287/D307 exists between the decomposition of K2C204 and the quantity of 6nO in the solution when the solution ie irradiated for 20 min. The re- action 16 thas hetprogeneoue,,-Hoterogeneous sensitization processes payt therefore, conatitute one method for utilizing nuclear radia- tion more effectivqly in chemical reactions. There are 4 figures, ASSOCIATION: FiT'iko-khimioheskiy institut im, L. Ya. K)trpova (phy-: sico-Chemical In8titute im, L. Ya. Karpov) Card 3/3 IZIDINOVI 4.0.; BORISOVA, T.I.j VESELOVSKrz, V.I. Partl=Lar fiature6 ot the photoolectrochamical bekdor of the oiliom-alMi interface. Dokl.AN SM 3.45 no.3:598-6oi n 162. OM& 15 &7) l*--Fixiko-k1iWchsxkiy institut-lwu~ L.,YA.Karpova. Predstavlano akadomJJtom A.N.Frw*ivme (Sillcon) (Alkali) (Photochemistry) A.A.; BORISOVA., T.J., VESELOV'jKIY,, Mo MOVUVA State of germani= electrode surface in the prozess of anodic solution. Dotl.Alf 3WR 145 no*2073-376 JI 162* (MM 15:7) 1, Fisiko-khimichaskiy institut imeni L,TaAarpova. Predstavleno akademikom A.N.Frumkigym. (Germardvm~--Zlectric properties) 42168 3/07 62/036/011/018/021 B101XIBO AUTPORS; Yakovleva, A. A., Borisova, To Iot and Ves .elovski V. 1. TITLE: State of surface and mechanism of self-dissolution of germanium in hydrogen peroxide solutions PERIODICAL: Zhurnal fizicheskoy khimii, v. 36, Ino. 11, 1962, 2541-2544 TEXT: The dependence of the potential, photoeffect, and capacitance on the Y2 concentration in O.I.N NaOq was studied on n-type.and p-type L;ermanium (5 ohm-cm) (Fig. 2). Corresponding to the maximum dissolution rate at 0.5 moles/liter of H 202' maximum capacitance- alpo occuri at this -o'6nabfitration. The anodic polarization curves showed maxinium saturation current at the lowest H202 concentration. These data suEgest that the etching of ,germanium in alkaline hydrogen peroxide solutions proceeds via a stage of GeO formation, and is ttlectrochomical in nature, since H 202 is reduced on the cathode and Ge is dicsolved on the anode. With a high H 202 excess, however, GeO oxidizes to GeO,, and the dissolution process is inhibited. Card 1/2 B/076,/62/036/011/018/021 State of surface and mechanism... B10i/B180 There are 3 figures. AISSOCIMON: Pi:-.iko-khimicheskiy institu t im. L.'Ya. Karpova (Physico- oh(!mical Inatitute imeni L. Ya. Karpov) SUBUTTED: Apra 6, 1962 Pi E;. 2. Variation in potential, photoeffect, and capacitance of Ge electrode at different H 2 02 concentrations in 0.1 N NaOH; Potential of (1 n-type Go; G ' ) ty ~2 e ~5 capacitance ) P P ; ) 1 k e c otoeffect of c~s ) ?h (4 ; ) n-type Go; (5) photoeffect Of P-type Ge; absol asa: 11 0 2 2 concentration, moles/liter. --------------- J* Card 2/2 39579 S/02o/62/145/003/011/013 B101/B144 AUTHORS: Izidinov, S. 0., Borisova, T. I., and Veselovskiy, V. 1. TITLE: Characteristics of the photochemical behavior of the silicon- alkali interface PERIO=JkLi Akademiya nauk SSSR. Doklady, v. 145, no. 3, 1962, 5ga-6ol TEXT: ExDosure of the Si - KOH int erface to light showed paeeivation of the Si electrode and activation of the passive electrode. 'Passivation occurred only with anodic currents i