SCIENTIFIC ABSTRACT KISELEV, A.V. - KISELEV, A.V.

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December 31, 1967
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SCIENTIFIC ABSTRACT
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The Adsorption Heat of the Vapors of Benzene and 2o-119-4-20/6o Heiane on Quartz a condensed powder there were interspaces with mostly 1600 tO 70o0 1. With'an increase of p/p from the beginning of hysteresis to saturation about 70% of the surface disappear. A further dia- gramt by way of comparisonj illuetrateB the isothermal lines of the adsorption of the same vapors on a homogeneous silica gel NZ-2. The desorption branch begins to decline steeply, near p/P R 0-7- In this domain the adsorption on quartz is not yet rendered com- plicated by any capillgry condensation in the interspace between the particles. In the initial domain of mo'nomolecular fhling-up adsorption on,quartz is greater than on silica gel Xa:-2, which is connected with,the lower skeleton density of this silica gel, Further details are given. A further diagram shows the dependence of the heat of adsorption of benzene vapors uponthe absolute value a of.the adsorption on quartz. After filling-off'of the first two layers adsorption heat exceeds condensation heat only -by 3%p and after the adsorption of 4 layers by 1%. Further re- Card 2/3 Auction of the ~4 af:6f~adsorpt ion takes,place very,slowly~'The-.,---L~ agradual deprease of adsorption he7ii observed. The authors then mention some numerical data dealing with this subject. There are 4 figures and 18 references, 13 of which are Soviet. ASSOCIATION: Moskovskiy gosudarstvennyy universitet im. M. V. Lomonosova (19oscow state university imeni N.V. Lomonosov) AUTHORS: Kiselev, A. V.,,Poshkuep D. P. SOV/20-120-4-4o/67 - TITLE: ' - The Energy- of the Coulomb Interaction Between the Hydroxyl Group of Silica Gel and the Benzene Molecule (Energiya kulonovs-- kogoi vzaimodeystviya gidroksillnoy gruppy silikagblya's mole- kuloy benzola) PERIODICAL: Doklady Akademii nauk SSSR, 1958, Vol. 12o, Nr 4, pp.- 834~ 837 (USSR) ABSTRACT: In the computations discussed in this paper the hydroxyl.group, is consideredAD be a system of two point charges the position: of which agrees approximately with the position of the oxygen atom and of the hydrogen atom. A formula is written down for the energy of the Coulomb (Kulon) interaction between the hydroxyl group and the benzene ipolecule; this energy was com- puted for various aubcases,in a vertical position of the hydroxyl group with regard,to the direction of the benzene ring.. The same energy-in-the case of a displacement of the hydroxyl, group inside the,benzene ring depends only in a low degree - on their mutual position and amounts to about 4-6 kcal/mol. This Card 1/3 interaction energy decreases considerably outside the benzene The Energy of the Coulomb Interaction Between the SOV/20-12o-4-4o/67 Hydroxyl Group of Silica Gel and the.Benzene Molecule ring. Accordihg-to the data obtained, the energy of the Coulomb interaction between the polar hydroxyl group and the non-polar benzene molecule is high and in the formation of the hydrogen binding in a given system it plays the decisive role among the other interactions. The benzene molecule adsorbed on, the surface of a completely.hydrated silica gel interacts assentiaily,with one or with only a few hydroxyl groups; besides-#* such an adsorbed benzene molecule also interacts with the other atoms of the lattice of the silica gel. Therefore the removal of the hydroxyl groups from the surface of the silica gel is bound to decrease the heat of adsorption of thebenzene molecules.on the dehydrated surface of the silica geld Besides-p the energy of,the interaction of the adsorbed benzene molecule must be increased wi-th the.volume phase. The comput ed energy of the Coulomb~inter~"ion (about 4-6 kcal/mol) agrees satis- factorily with the experimental values of the decrease of the, adsorption heat of benzene in the dehydratization of the surface of silica..gel. There are I figure and 2o references, 7 of which Card 2/3 are Soviet.. %tP, NZ -The Energy-of the Coulomb Interaction Between the SOV/2o-120-4-4o/67 .,Hydroxyl Group of Silica Gei.and,the Benzene Molecule ASSOCIATION: Moskovs,kiy gosudarstvennyy universitet im.M.V.Lomonosova (Moscow State University imeni M.V.Lomonosov) Institut fiziches- koy khimii Akad.emii nauk SSSR (Institute of Physical Ghemistry AS USSR) PRESENTED: January 18t 1958, by A.K.Frumkin, Member, Academy of Sciences, USSR SUBMITTED: January 18, 1958 radicals--Cherhical~ A, 'I Hydroxyl, -:r6actions 2. Benzenes--chemical rew--_,~~ ~i., actions 3. Benzene molecules-Adsorption 4. Silicon dioxide--Ghemi_-_ cal properties -.5. Chemical reactions-Energy Card 3/3 :~W AUTHORSt Ki .seley,'A, V., Neymark, 1. ye.p SOV/62-59-2-7/40. Poshkua, D. P., Piontkovskaya, U. A. TITLE3 Change of Porous Structure of Magnesium Hydroxide During Heat Treatment.(Izmeneniye.poristoy struktury gidrookisi magniya pri termicheskoy obrabotke) PERIODICALt Izvestiya,Akademii nauk 5SSR. Otdeleniye khimicheski.kh nauko 1959, Nr,2, pp 232-237 (USSR) ABSTRACT: In the present paper the change of the porous structure of magnesium hydroxide during heat treatment in the vacuum was investigated in a broad temperature range. It was f ound that 0 the magnesium:hydroxide pumped off at 200 repre sent s , iL broad.-porous sample (dl-450 2) with large pore volume 0-71 am 3/g). The values of the specific surfaces of the skeleton and of the adsorption layer s'are approaching, one another in the initial sample. This indicate6:that.there- in micropores are occurring to practically no extent, which, are filled up in the primary adsorption process without hysteresis. On the transition of this hydroxide into oxide Card 1/3 the specific surface is considerably increased at 350' (by Change of Porous Structure of Magnesium Hydroxide SOV/62-59-2-7/40 .During Heat Treatment about the 3-f old). Volume and size of the pores in which capillary condensation takes place remain, however, unchanged.,-,.,., The formation of the mior,o-structure,is due to water.separa- tion from the hydroxide.lamellae and to the transformation of the orystal.structure of Ug(OH )2 into Mgo structure at which 0 the molar volumes are different. At 350. the sample is of bi-dispers.e structure; it keaps the homogeneous coarsely pdrbus structure of the ir2ial substance but the walls of this structureare traversed by fine pores (cracks). A further 0 increase of the calcination temperature up to 500 causes already a certain agglomeration of the micro-structure, as the specific surface becomes smalle 9. On a further increase in temperature up to 1000 and 1400 also the large pores are oonsiderably',oontracted. In consequence of this not only the, size but also the surface of the adsorption layer s'&nd the volume of the pores de.ct:ease. In samples obtained at 1400.0 the size of the specific surface a is getting nearly as large as-the size of the adsorption layer s. This means Card 2/3 that in this.sample the fine pores disappear and the str~ucture Change of Porous Structure of Magnesium Hydroxide SOV/62-59-2-7/40 During Heat Treatment passes over again from a bi-disperse (fine and coarsely porous) into A homogeneous coarsely porous one. There are 3 figurest: I tablet and 23 references, 12 of which are Soviet. ASSOCIATIONt Instituty fizicheskoy khimii Akademiy nauk SSSR i USSR (JnStitut4ES of Physical Chemistry of the Academies of Sciences, USSR and UkrSSR) Moskovskiy gosudarstvennyy universitet im M. V.. Lomonosova (Moscow State University imeni M. V. L6monosov)- SUBMITTEDs July 1, 1957 Card 3/3 5(4) AUTHORS-,. TITLE: PERIODICAL,. ABSTRACT: Card 1/3 Kiseleyf,-A. V.p Lygin, V. 1. SOV/62-59-3-5/37 Electron-microse.opic Study of Porous Structure of Magnesium Hydroxide and, It.6,Change6 Associated With Thermal Treatment (Elektronno-mikrookopicheakoye issledovaniye poristoy'-struk- tury gidrookisi-.magniya i yeye izmeneniy pri termicheskoy obrabotke) Izvestiya Akademii nauk SSSR. Otdeleniye khimicheskikh nauk, 1959, Nr 30 n_412-416 (USS11) In the.present-paper,the mIacroporous.structure of magnesium- hydroxide samples and products of their thermal-decomposition was investigated by means of carbon copies. As investigAtiont objects-the homogeneously wide-porous magnesium-hydroxid e samples.calcined at 2000 and the magnesium-oxide.samples 'ob-. tained from,them by means of calcination at 1,000 and 1,400' were. u.sed. The~recordings of the carbon copies:and samples.. An t light.were,takenLin the electron microscope UEM- .100 a ga s .at avoliage of 60 kv. The skeleton of magnesium hydroxide has al,corpuscular structure and consists of laminar crystals.' lit es (kigs.293). Some of these crystallites have a strongly' hexagonal and some a distorted form. On the Electron-microscopic Study,of-,Porous Structure of SOV/62-59-3-5/37 Magnesium Hydroxideand lts~,.Changes.AsBociated With Thermal Treatment stereo-microphotogTaphy (Pig 6) carbon copies of samples whi.ch_ were calcined-in vacuum at 1,0000 are shown. The datalobtained by elactron-midroscopio investigation as well as the ddtermi- "nation results obtained by the adsorption method (RefJ3),are given.in the.Itable.,Itwas found that the calcinationlof the initial.sampletrin vacuum at 1,0000 is followed by a condea-: sat:Lon- of.,Ahe_ original structure .(the diameters of the pores decrease.down-to 300-350 R). The laminar form, howeveri, is. maintained.-This indicates that the changes.observed in ad~- sorption measuremen -ts (Refs 13,15) of the specific ou rface during 'calcination,in the.temperature range of 200-1,0000- Are mainly..conn.eated with the transformation of the.-struc-m ture-within.the hydroxide lamellae. The form of the lamellaO andmide-porous skeleton formed by them does,not vary,con- siderabli.-Thus the,.electron-microseopic investigation..con- y firmd..the'conclusion drawn from the adsorption measurements (Ref 13) regerd-ing--the.formation and disappearance of the bidisperse structure in the course of thermal treatment. Quite a different character is exhibited by the.hydroxide Card 2/3 sample calcined at .1,4000 (Fig 4). The stereo-microphotograph Electron-microscopic Study.of,Porous Structure of SOV/62-59-3-5/37 Magnesium 11ydroxide and Its'Changes Associated With Thermal Treatment~ shows an extremely-porous out and the lamellae do not appear any longer. This is apparentl y a consequence of the agglomer- ation of.some lamellae taking place at this temperaturd%and of the considerable growth of crystallites within the lamellae.'. At the sam6,time.the general character of the macroporous ,structure is maintained,also at these calcination,tomperatures. This is likewise in accordance with the determination results obtained by the adsorption method. There are 7 figures, 1 table, and 16 references, 13 of vhich are Soviet.' ASSOCIATION: Moskovskiy gosudarstvennyy universitet im. M. V. LomonoGov.a oscow State University -imeni M. V. Lomonosov) (M Institut fizirhe-skoy khimii Akademii nauk SSSR (Insti tute:o.f~ Physical. Chemistry of the Academy of Sciences, USSR), SUBMITTED: July 69 1957 Card 313 AUTHORS: Avgul -Berezinf G. I., SOV/62-59-5-5/40 Kiselev, A. V.0 Lyginal I. A. I------------ TITLE: Adsorption.Heat of a N=ber,of Isoalkanes Haphthenes and of Toluene on Graphitized Carbdn Black (Teplota adsorptsii ryada izoalka- nov, naftenov i toluola. na grafitirovannoy sazhe) PERIODICAL: Izveatiya Akademii nauk SSSR. Otdeleniye khimicheskikh nank, 1959, Nr 50 pp 787 - 796 (USSR) ABSTRACT: In this Work the following hydrocarbons were investigated as to their adsorption.-heat: three isoalkanes (neohexaney isoheptane, and isooctane), two alicyclic hydrocarbonsi cyclopentane'and methyleyelopentane, and the alkylaromatic compound toluene. The hydrocarbons had-been selected in this way in order to investi- gate the effect-of the chain branchingp the ring formation of these chains, 'and the introduction of aliphatic substituents into the naphthe.ne and-benzene ring on adsorption. The hydro-~ carbons*used in -the investigations had been synthetized at the , Institut organicheskoy khimii AN SSSR (institute of Orgazz"Jlc mistry of the.AS, USSR) by Ye. A. Mikhaylova, A. F. Platef A. L& Liberman, and S. V. Zotova. The authors express their gratitade- Card 113 for their help. The constants of these substan-ces are s-ummaziz- Adsorption Heat of aNumber.of Isoalkanles, Naphthenes SOY/62-59-5-5/40 and of Toluene on Graphitized,C"bon.Blaok ed in table 1. "SferorP-6 was used as adsorbentl it was graphi- tized at 1706,.-The.differential adsorption heat.was determir.'ad at 200 in.a,cal'otim-eter with constant heat exchange; the amolvit of the adsorption was determined by means of a capillary vacaam liquid microburet.Tigures 1, 2 show the isothermal lines of. adsorption of the various substances and figures 3. 4 show the dependence OfLthe d-ifferential adsorption heat on the amount of heat adsorbed by the individual substances. The figures show that the normal adsorption heat of isoalkanes and naphthenes is lower than.that of the corresponding n-alkanes. The value of the addorption.heat of cyclopentane amounts to only half of that of.n-pentane. Cyclopentane, therefore, shows greater at- traction towards theadsorption layer, its isothermal line of.- adsorption is concave at its beginning. It can be seen from the thermodynamic evaluation of the experimental data obtained that the isothermal line of adsorption of cyolopentane cannot be re- presented by the Langmuir equation or BLT equation but by an Card 2/3 equation whichallows.for the interaction adsorbate-adsorbate Adsorption Heat of a Number-of Isoalkanest Haphthenes SOV/62-59-5-5/0 and of Toluene on Graphitized-Carbon Black ..,The 'en tropy curves (Fig 6) indicate that the state o.f (Fig 5) , - isoalkanes and naphthenes.in.the dense adsorption layer 6n,gra-,.-, phite is.much closer to the liquid state-than that.of n-alka-;.,..- nes. The methyl-group in the toluene molecule.roduees it6-mo- bility with respect to the unsubstituted benzene and-the other purely.oyclio compounds..With regard to the theoretical calou- l~ lation of adsorption heat it was assumed thats in the case of l - the ramified hydrocarbons, the adsorption heat is-an additive, function-of the number of carbon atoms in the molecule. The free adsorption energy and the surface of the adsorbent accu-1 pied by-moleculeswere determined according to the same ass Iump- tion. There are 6 figures, 3 tables, and 17 references ,12 of , which are Soviet. 'ASSOCIATION: Institut-fizicheskoy khimii Akademii naiak SSSR (Institute of Physical Chemistry of the Academy of Sciences, USSR)., SUBMITTM: July 25, 1957 Card 3/3'~ 5 '(4) AUTHORS: Kiselev A V Kovaleva, N. Ve SOV162-59-61-4M TITLE: 'The, Influence Itcercised by the Thermal Treatment of Different 1:1 Carbon Blacks V~on the -Adsorption of Vapours (VlijauVie termi-w cheskoy'obrabotki razlichnykh sazh na adsorbtsiyu-parov): PERIODICAL: Izvestiya~Akademii nauk SSSR. Otdeleniye khimicheskikh1nauk, - 195% 1qr 61 pp 989-998,(USSR) ABSTRACT: As ia well knov rn,~ an-increase in treatment temperature causes 8;1 inerqase_in this arystal,dimension up to parallel orientation,-as is the case. with the graphite lattice. Besides, there. are numerous papers which deal with.the investigation mentioned in ~the title'(4efs' 1-40). It.is only the problem of the fundamental'- . adsorption changes of different substances that has scarceli,been dealt-w'ith up.to now. As-to this.problem there are different_,,., opinions Ias to_wheth_er,the~'presence of oxygen complexes dai---,~the .~,~I surface ot.the' adsorbents, or the inhomogeneity ofthe~s aaw.-.- ,.- . I are to-be-mad6-res nEfible for the adsorption. In this _po connecti6n,i:the "Aasorption was investigated in the present work, (-roughly inhomogeneoust. asbeing.dependent on the surface quality stronglyt and weekly oxidized carbon black). Subject to Card 1/3 investigation were substances with extreme structure arA polarity The InfluenosExercioed by-theMermal Treatment of SOV/62-59-6-6/36 Oki n t~e:Adsorption.of Vapours Different' Carbon Bld :UPO such as benzene?" water, methanol. For this purpose the adsorption'. isotherms, of the above mentioned substances on carbon black. adsoibents ~ (pigs 1-6) submitted to different thermal treatment'* were dete'rmined.'It was found that with inereasing'treatment temperaturej the quantity of oxygen needed for the exchange.with ~NaOH in aqueous solution on the surface of the carbon black decre -ases, :andlsd does the.,roughneab of Us, surface.--It remains 'homogeneou's:aft6r,~~reatinent.in.hydrogen at 17000.1 The steam- adiorptio'XL,W,.gra'phite.Ltreiited- carbon blaek-which also decreases is mainly, -due t6....the elimination- of surface oxi des. With graphite -treated _'okrboir black; in a hydrogen current adsorption of water, iA-.very_,_.1.oiwi- evvri:-at-high- pressure. The adsorption of methanol vapours..aleo-d6creases by:-the.alimination :of the:surfa6e oxiaes"_'While _th&_A4br_e'ase,: im~'- the -~surface -moughnes-5 there -only a ad unimport e.' ne adsorption w V PlAy ant rol -Benze ith aphite treatment is Lmainly,reduced because of the adsorbent surface which is not:rough.enough. In general graphite treatment in hydrogen current at 17000 of different types of carbon black leads to:4Uite:similar surface qualities of the adsorbent. The Card 2/3- authors thank It. M. Dubinin for explanations he gave them. 5 (2), 5 (4) AUTHORS; Avgull N. N.1 Kiselev, A. V..9 SOT/62-59-7-7/38 Lygina-,' 1. TITLE: A Contribution :to -the, Calculation. of the Energy of the, A.daorption_'~,~ of Nonpolar.Molecules on Graphite-(K raschetu energii adsorbtaii nepolyarnykh molekul-na giafite) PERIODICAL: Izvestiya Akademii nauk SSSR. Otdeleniye khimicheskikh~naukp'. 1959,, Nr 7, pp 1196-1206 (USSR) ABSTRACT: .In this papaf:.the'details of a calculation'of the adsorption energies of simple and compound molecules carried.out,,in a previoixs, paper are rep .resIanted. The caloulatiow were carried out according:to the formulas-.from paper reference I according to -hich. the-adsorption energy is determined by the expressions, r- - 'o + B!Z: e-r j~ 'C Y: .. Ci iV 3 ij Cil 6 -10 -12 r- - C C + B't ij ii i2F- '_iJ i3Y ij 4 3. rij 3.5 the.distance of the center of the i-th adsorption Card 1A moleculefrom the center of the J-th atom.of the adsorbent# A Contribution to the Calculation of the Energy of the SOV/62-59-7-7/38 Adsorption of Nonpolar Molecules on Graphite C are constants of the dispersion reaction, BI and B" are., i1,293 the constant of the exponential fanction and the constant of.-. the repulsion preceding the powers. 9 is an exponential constant of the repulsion. The-calculation is oarried out in two Darts the geometric~~one in which the distances of the adsorbed link to all atoms j - of 'the lattice of the adsorbent, are oalualated foil. different distances of.the former from the surface. For this. calculation only the lattice constants of the adsorben.t~have to be, known.-, Pot. the, second part 'of the calculat ion: of the, forced the constants charaterizing the reactions of both substances, have to,be determined, The calculation of the sums of r' was- ij~ carried,out.Ifor n~= 6, ~0. 10 and 12 for the diff,erent-distances.,,, of the adsorbed link from.the basia of the adsorbent equal,td*, 2t 2-5, 3t:30.5 a (a is, -the distance of the nearest atom),Jn table I the results of the calculation of the sums rr-n are-combined. The distances of the remaining gr'tILphite ij Card 2/4 volume were determined from the int -egrals (3)! (4)o (9 Tab e 1 2) A Contribution to the Calculation of the Energy of the SOV/62-59-7-7/38. Adsorption of Nonpolair Molecules -on Graphite ri n The sums rij. .+ are represented in tables 4 and 5 and the: -rij/0026 graphio-repres6ntation in figure 2. The value e for 9 in table-6.wasequated to 0.28 according to reference 6., For the sums ~of,--tables+ 4, 5 a simplified formwith the constants: pzx an4-q *-the values,6f which are given intable 7, is: introduced+,. and the functions (1) and (2) are represented in the variable z r f -qn) (6), (7) + Next, the calculation of the ij .7Pnz n reaction conBtant:c is carried out. The values+for, 1213 different adsorptives-are given in table 7 with the constants OLand-W (pblarizabilit ' magnetic susceptibility) being V, necesoary-for the calculation of Cil,2-3. ~' and V were then Card 3/4 deItermined by the aid of computed constants. The results for A Contribution to the Calculation of the Energy of the SOV/62-59-7-7/38 Adsorption of Nonpolar Molecules on~Graphitel are giv ,en2in tables 10 and,11. The calculation of the.attraction- and,reptilsion.constants'was carried out from the balance enexg., ,of the adsorption of compound molecules on the basis of an aa.ditive scheme. There are.6 figures, 11 tables, and 8 references, 2 of which are Soviet. ASSOCIATION: Institut fizicheskoy khimii Akademii nauk SSSR (Institute of Physical Chemistry-of the.Academy of Sciences,.UMR) Kh3*.micheskiy:fakulltet Moskovskogo gosudarstvennogo universiteta: im. 11. V. Lomonosava (Chemical Department of the Moscow State University im'eni M. V. Lomonosov) SUBMITTED: November 16, 1957 Card 4/4 5(4)- SOV/T6-33-2-2.3/45 AUTHORS: lsiril.-.Yan, A. A.,_Xizelov, A. V, Prolov, B. A. TITLE: The Heat of Adsorption of Normal Alkanes on Silica Gels (Teplota adsorbtsii nor-nallnykh alkanov na silikagele) PERIODICAL: Zhurnal fizicheskoy khimii, 1959, Vol 33, Nr 2, vp 3,89 -.394 (USSR) ABSTRACT: In continuation of the work of previous papers (Ilafs,10,111 16 - 19) the heat of adsorption (m) of n-pentan,e.(I) and. n-octane (Moon coarsely porous silica gels was measured. An adsorption calorimetric apparatus was used which is a, simplified variant (Ref.20) constrlicted in COODeration -dith G. G. Muttik and which rill be described separately. As in .the other papers (Refs 10,11,13,16) a homogeneously porous dh- ca gel KSK-2.with a specific surface of 320 m2/g end a pore diameter of a bout 100 R was used. A comParison of the ob- tained,.absolute adsorption iqotherms (Fig 1) for (1) and. (IT) with those for n-hexane --id n-heptane on. the same silica. gel (Ref 10) chors*that the (AH) from pentan Ie to octane increaces and it is not' possible -,,o apply the BET equation. Card 1/ 2 Since the constant of the induction inter-action with the The Heat of Adsorption of Normal Alkanes on Silica Gels SOV/76-33-2-23/45 electrostatic field is proportional to the polarizability of the n-alkanes the general adsorption energy on,'Uhe silica gel also increases linearly with the number of carbon atoms in the molecule. The linear Ainctions Q0 of n ( n. number a of carbon ata~16)(Fig 3) and the standard differential (AH) of the n-alkates were dc-ived for adsorption on silica Lis, carbon black (Refs-4,5), M90 (Ref 7), and water (Hof 271. The values for any particular n-alkane can be calculated from the follo'i.iing equatio-no- Adsorption on carbon black 0-7+1.9 n kcal/mol (n= number of carbons) nl /~Joj MgO 4 1.5 nket kcal/rol to silica , e 1KSKI-9 QO= '.0+4.3 n Heats of condensation L 0. r. k ca!/mol Adsorption.on viat er Q 1 .7+0.7 "kcal/mol. There are 3~fid-ures, 1 table, and 27 references, 24 of which are Soviet. ASSOCIATION: Mozqkovskiy gosudarstvenryy universitet im. M. V. Lomonosova (Mobcor, State University imeni 11. V. Lomonos3v) SUBMITTED: July 17, 1957 Card.2/2., 5 ( 4) AUTHORS: Belyakova,' L.D.9 Kiselev, A. V. 507/76-33-7-;-14/40 TITLE: Adsorption and Chemisorption of Methanol by Silica Gels With Different Degrees of Surface Hydratioa PERIODICAL: Zhurnal fizicheskoy khimii, 1959, Vol 33,,Nr 79 PP 1534 1543 (USSR) ABSTRACT- It was already found in previous papers (Refs 4) that the adsorption.(A) of methanol (1) by silica,gel W) depends larEely on-the degree of,surface hydration, and that chemi- zorption takes place. In the present paper, the authors in- vestigated a variation in the adsorption and ehemisorption properties of coarse-pored silica gels (UK-.2) (with respect = to (I)).which was due to great changes in the a 00,11- (' 0 OR 0H oentration. of OR on the silioa-gel surface" in the case of small structuralchanges of the pores. Experiments were made in a vacuum apparatus,-(Fig 1) consisting of three separate mea-. suring arrangements. The samples were annealed at various tem- peratures (200 -~10200). The specific surface a of the sample was determined from the (A) of nitrogen, and on the basis of Card 1/3 these'daia and the.content of structure water the aul%ors Adsorption and Chemisorption of Methanol by Silica SOY/76-33-7-14/40 Gels With Different.Degrees of Surface Hydration 0 calculated the values of aOH (Fig 2). Within the range 200 800 aOH falls pract.ioIally ina linear manner. Heating up to 9500 reduces s and v (total volume of the pores) only 'by 20~, while the size of the pores (dF--1-00 1) does not vary. Heating up to, 0 1020.C,.howeverg decreases s and vB by about 75%, and d drops to 55 - 70 1. A comparison (Table 1) of the quantity of irre- versibly che'misorbed W.'a with a indicates that, con- OCH on 3 trary to the-rapid physical adsorption, cc increases with GCH 3 decreasing a The primary,(A) of (I) from KSK-2 (at 200') ''OH proceeds much taster than on KSK-2 (at 6150') or Y-SK-2 (at1020 Kinetic curves.indioate that the chemisorption of W on the hydrated surface.of (II) differs greatly from that on dehy- drated surfaces. Experiments on thermal decomposition of the Card 2/3 surface compound of (I) with (II) showed (Table 2) that only Aasbrption and Chemisorption of Methanol by Silica S07/76-33-7-14/40 "els 17i,'.,h Different Degrees of Surface Hydration, 7~ of the irreversibly adsorbed substance are removed by heat- ing to 2000 approximately. Methoxylation of the (ii)-surfaae reduces the (A)-of:(I)-vaporsy i.e. the reaction of.(I)*'4'L,,h.' +he OR-groups of the (11)-surface is greater than the one with the PCH~ groups. The chemisorption of (1) on (II) increase a with decreasing concentration of the OH.-groups on the (11)-sur- face. This is due to the surface me-LIhoxylation. In this process, a reaction takes place between the OH-gro-ap of silicio acid, and the bond SJ_ - 0 - S1 decomposes to form Si-OH and Si-OCH 3 groups. The adsorption of (1), water, and benzene decreases_ partioularly strongly (4 times approximately) within the range aoff = 7 - 4 Pmol~~M in conclusions the authors thank V. Bronshvagerl.and G. G. Muttik for.their assistance.-There are 8 figures, 2 tables, and 27 references, 24 of which are Soviet.. ASSOCIATION: Moskovskiy gosudarstvennyy universitet im. M. V. Lomonosova (Moscow State University imeni 14. V. Lomonosov) SUBMITTED: December 30, 1957 Card 3/3 5W. AUTHORSt Gryazevp No No BOV/76-33-7-1.0/40 LEM T IT Adsorption Isothermal Lines From Three-companent, Z PERIODICAM hurnal fizicheskoy kUmii, IT.5-9, Vol 33, Nr 79 PP '581-1593 (USSR) ABSTRACT.- The development of adsorption chromatography of wmiti-componsm-t mixtuixres requires -investigation of the adsorption equ!_l11.j_.T4, ,.imp if-se. of the adsorption isothermal lines (AI) of the oompcnents of such mixtures'. The (AI) of the fDllcyring liquil tba-qel-orompsD- neat solutions were investigated in this oaae: ceuans W + acetia a3id. II) + lauria a cid 'III), (I) + (11) .+ pqlmjti-~; aoid (IV) and M.+ (II) + c,4-methyl naphthalene (V). The authors chose these mixtures.,because (I) and (IV) Eelve the puipose of.modeling the adsorptive xegeter aUon of n1ingral Oils; on the other handi (iI) is soluble in (I) to a certain extsnl~q while (III) and (IV) are perfectly soluble in (I) p and 'be--J%Use the influence exercised by a variation of - tGhe solu1bility of the three-oomponent solutions,.upon their adsorption can be investigated. One of i~e most*a^-tive sedimentation rocks with a Card -1.13 _Mv nmwnw, Adsorption Isothermal Lines From Three.-component SOV/76-33-7-20/40. high silica content, called "opok" (Kr 120 from the area ronna the village of.Kamennyy Yar, Etalingrad oblast') and an, industrial XSK-4 silica gel were used as adsorbents. Thb~ characteristic values of the mixture componefits applied are giver. Adsorption experiments vorere made by a method devilsed by the Laboratoriya adsorbtsii Moskovskago universiteta(Laboratory for Adsorption of Moscow University)(Ref 15). An ITR-2-intexr- ferometer an& an IRP-22 Tefractometer were used for analyzing the binary systems. The method of analysis of the three-cLmpo- nent'solutions and the evaluation of the results obteLned a-re described. Three -dime nsional diagrams illustrate the.resultant (AI). The authors found that additions of the third component,to the binary mixture decrease tile adsorption of the components and change the course of the (AI). A change in the solubility of the components from limited into unlimited solubility effects S variation of the S-sha with a ped Isothermal lines into nes Card 2/3 Adsoz,ptlix-r, Isatherma'L Lines rrom Three-oomponent SOV/?-5-33-7-90 C 0 -XIS maximum. The component that Is better adsorbed from the ~-inaxy Mixture is also 'batter adsorbed from the thrse-aampoapntl, Lafxture The absolute (AI) of the oomronents of the systems ur-der iisoussion are similar for eat7h of the 41-wc employed adso.rbents. There are 13 figwes and 18 refe:renies, 15 Of wh', oh are Soviq~,. ASSOCIATIONi Moskovskiy gosudarstvan;*7 mdvazei'et in. V. (M-3soow St ty imen:L Y. V. I-:m-1Cn-zSCv) ate Universi SUBMITTED-. jawlanr 9,1958: Oazd 5(4) SOY/2o-124-3- Korolev,.A. Ya.,Shch bakova,K.D. AUTHORS: elev A alevat N. V. ' :V. M _L_ vr -*X T TLE U t e e, odi , icati n of I : s Surface of Adsor ben b and It's- Influence on Adsorption Properties (Khimicheskoye modifitsirovaniy-e'poverkhnosti adsorbentov-i yego vliyaniye na adsorbtsionnyye evoystva) PERIODICAL: Doklady Akademii-nauk SSSR9 19599 Vol 124, Nr 3, pp 617-620 (USSR) ABSTRACT: The present'-report deals with the chemical modification and variation of,-the adsorption properties of silica and graphite bodies. Hig4ly dispersive silica aerosil and gas-black are used for this:purpoee..This modifj4cat~on was carried out for the purpose'of rendering silica hydrophobic and of making soot hydrophific.'The firIat-part of this paper deals with the. modifioation' ~.of silice.4 Sil Pa with a hydrated outface ad- , sorbs poldr.substances well.-By a reaction with silicon'-organio compounds-At,ispoesible.to modify the nature of.their our-, fact essentially in the direction of -attaining a,stable.hydro- phobic statep.which is of practical interest for the applica- t1on of silica as filling media for polymeric materials and- as a thickening medium for lubricants. The modification con-, sisted of a reaction-of silica hydroxyl with trime-thyl chloro-'.,.. Card 1/4 silane according-to the scheme - Ml~ ~gg SOV/2,D-124-3-35/67. The Chemical Modification of the Surface of Adsorbents and ',n8: Influence on Adsorption Properties 0 CH 0 CH3 -0-Si-OH+Cl-Si-CH -0-Si-O-Si-CH +HCl 3 3 0 CH 0 CH 2/g Aerosil with a surfaoe-of about 1F m was treated for eight days at a temperature of 20 with saturated trimethyl chlorosilane'vapor.or,with its solution in benzine. The greatest difference in the isothermal lines of adsorption is observed in,steam. The adsorption of steam on a modified sample is several dozens of times lower than in the case of a normal.s.ample. The.isothermal line of the.adsorptio,n of steam on-a modified sample is reversible, and it Iis not modified even after several months of contact with waterv whichis indicative of the strength of the surface compound formed. The second part of this paper deals Card 2/4 with the formation of carbon black. The adsorption proper- SOV/20-124-3-35/67 The Chemical Nodification of the Surface of Adsorbents and !t-4 Influence on Adsorption Properties ties of soot with respect to many adsorbed substances, especial- ly with respect to polar ones, depend on the quantity of oxygen they contain. The authors modified gas black.for the purp8se of further graphitization. By annealing at more *than 1500 the acid surface compounds are destroyed, the.growth of graphite cryst.allites.is promoted (chemical and crystallo- chemical modification) and the adsorption of the vapors of watert methanol, ammoniag methylamine, sulfur dioxide and other polar substances is considerably reduced. Thermal treatment, especially.at temperatures of more than 25000, makes the soot-surface more homogeneous and prevents the adsorption of non-polar substances. Such a treatment of soot also increases-its hydrophobic properties. An increase of the affinity of soot to,polar substances. especially water, is of practical interest,for polygraphical pigments and also for other polygraphically important cases. Also the nature of the surface and the colloid-chemical properties of soot Card 3/4 are considerably modified by the oxide-treatment. The modi- SOV/2o-124-3 35/67 The Chemical Modification of the Surface of Adeorbents and Their Influence:---- on Adsorption Properties fication of,soot also modifies the adsorption of steam con- siderably. The variations of the corresponding isothermal lines-are diicussed. The double hysteresis found,,on this occasion is-typioal of the superposition of two phenomena, viz ohemosorption and capillary condensation. The thermal. treatment of soot and its oxidation in the liquid--phase is able to modify soot to such an extent that the adsorption of steams on it is modified by dozens and hundreds of times of its amount. There are 2 figures and 25 references, 12 Pf which are.Soviet. PRESENTM: September 6, '1958, by M. M. Dubining Academician SUBMITTED: September 5, 1958 Card 4/4 lax g.k E a .1 p a-3 *A 4A :jj:~j u;; c I - I o a ".4m, laviv s -1 =~.V! Bit 'r Lo"o Amik o lip: o 10; a a ------------- ~7777777-17,~~ PEASE I BOOK XVLCXTATION SOV/4"l Nelftwsavskaye soveshchanlya PC khtmil nertil Moscow, 1956. Sboralk trudov Methvuzovskogo boveshchanlya po khimii neftl tion of Transactions of the Inter-UnIveralty Con- ic=": on Petroleum Chemistry) (Moscow] Izd-vo Moak. univ., 2960. 313 V. Xrrata allp Inserted. 1,600 4oqI4s printed. Organizing Conmaittee of the Conferences Chairmant B. A. Kazanskiy, Academician; Vice-Chairmant S. 1. Khromov# Docentj 0. X. Panahenkov, Professorl A. Y. Plate, Pro- Teseer; Secretaryt Ye. S. Baaankova, Scientific Worker. Zdltoria2 Board: Romp. Ed.s A. P. Plate; 1. V, Goatun- key-, 1. N. Tits-Skvortgo% L. A. grivanakeya. PURPOSE. Thin collection or articles Is Intended for the tqachUg staff at' unlvaraLtles and schools of higher ad- ucation training specialists for the petroleum and patrol- *ues-refining Industries. Card 1~T tCn:NAGZj__7be collection includes articles dealing with the M present state Of the patrol*= Industrys the scientific research problems In petroleum chemlstr7~ the chomistr7 Of o , the composition or petrels= and petroleum r ts!T* scientific principles of refining petroleum I,r= into motor fuels and lubricantes and the maroifacture of eyoth*tjo products from hydrocarbon Sues and petroleum- one article discusses the effect of chemical composition and additives an fuel combustion In jet engines. The 03- terlAa max presented at the Inter-University Conference .00 Petroleum Chendstr7o bold at the Moscow State UnLyartl- -2B, 1956. No periwoct- ty la"I X. Ir. 14monasov November 26 alitlas are mentioned. Reforenoes.accoupwr most of the TANA OF CONTINTS I None given ~ The authors and the titles of articles are as followst ' Kazanskly, Academician lotroducticn by B. A. C.-d. 2/7 Collection of Transactions (Cont.) SOV/4941 _nselev,_A,_V.,, Laboratoriya adsorbtaii Moskovskogo gosudarstvennogo, universiteta (Adsorption Laboratory of the Moscow State University) and Laboratoriya sorbtsionnykh protsessov Instituta fizicheskoy khimii AN SSSR (Labora- tory oi Sorption Processes, Institute of,Physical Chemi- stry, AS USSR). Hydrocarbon Adsorption Energy Paushkin, Ya. M., R. V. Sychev, T. P. Vishnyakova, and A. K. Zhomov, Moscow Petroleum Institute imeni I. M. Gubkin. Effect of Chemical Composition and Additives on Fuel Combustion in Jet Engines 293 AVAILABLE: Library of Congress (TP690.AlM445 1956) JA/iorc/ec lip 4-20-bl 5.1190 77935 sov/65-6o-3-8/19 AUTHORS-. K*3elev A V Nikitin, Yu. S. TITLE: The Effect of:,Production Conditions of Alumina-Silica Gels on.Structure.of Their Pores PERIODICAL: Xhimiya i tekhnologiya topliv,i masel, 1960, Nr -3, Pp. 35 -42 (USSR) ABSTRACT: The structure of pores.-of alumina-silica gels was studied ;in relation to thp amount of Al 0 in catalysts prepared 2 3 .The results of experiments are by the alumina,method. ., shown.in Tablel., Four additional samples,of alumina- silica gels.were prepared from solutions of lower con- centration containing two-fold lesser amount of-dry substance. -The.results of analysis of their pores are .shown in Table-2. There are 4 figures; 2 tables, and'15 references; 10 Soviet; 5 U.S. The 5 U.S. references are: Plank, C _' ',J. 'Drake, L.. C., J. Coll. Sci., 2, 399 ' (1947); Plank -C. J., J. Coll. Sci., 2, 413 (1947); Card l/V Ashley, K. D.J Imes, W. B., Ind. Eng. Chem., 44.,2 68700 _67 V'2 Do 00 AUTHORS and-Poshkus, D.P. Kiselevi. 4. TITLEi *The.- Heat;.-.and Entropy .ofi.Adsorption of..Benzene and-N- he 'jVapors_-_o_n_M-g esium'Hydroxide xane n PERIODICAL: Kolloidnyj~-zhurnal-, 1960, Vol XXII, Nr 1, pp 25-30 '(USSR) .ABSTRACT.- The _authoj~s -report -on a-study intended., -to determine tlie', , heat:'. and- entropy...--o-f-nbLdsorption~of benzene and n"hexane . Vapoj7s on magneslum-Eydroxide,with weakly d~ h44i-ated - ' ' , -surf ace. As ~adb6j~bbd authors selected a (6H) , the 2 SpScimen moderately--freed of'water at a temperature of * - s de- The differential heat.of--adsorbtion Q wa 20 U. a termined.from the-isotherms 'of adsorption on the given specimen. The.isotherms were getermined at the tem- peratures T and, T (10 and 30 C) according to the 2 formula . .Card 1/4 68700, S/069/60/022/0,1/005/025 D034/DO03 The'Heat.and Entropy of Adsorption of Benzene-and N-haxan Vapors.on. Magnesium.Hydroxide be determined __frox.';isotherms~ as-presented in a pre-- vious publication of,the authors fRef. 22) The investigation,has"shown that the standard heat of -3 specimen adsorption of benzene vapors on the'Mg(HO) .2 is greater than. the: standard heat of adsorption of PI n~hexane vapors (gbaph.l). A comparison of the stan-~ dard heats of,adsorptlon on various adsorbentB (table., and graph I4):makes evident that the heat of adsorption of benzenevapors,on polar,adsorbents is greater or close to the heat.of adsorption of hexane, whereas ,on a non-polar adsorbent the heat of adsorption of benzene is considerably below the,-heat of adsorption of n-hexane. The-increase in the ratio of the heats of adsorption of benzene and n-hexane vapors on polar ad- sorbents as compared to.this ratio on a non-polar Card 3/4 68700 S/069/60/022/01/005/025 D034/D003 The Heat and Entropy of Adsorption of Benzene and N-hexane Vapors on MagneBiUM Hydroxide adsorbent-(graphitized carbon black) is explained as dtie mainly to the stronger electrostatic interaction of benzene moleculesq as compared to the interaction,. with the-electric field at the polar ad- of hexane, , sorbent surface. There are 4,graphs, 1 table and 13 references, 11 of which are Soviet, 1 English and 1 German. ASSOCIATION: Moskovskiy universi-tet im. M.V. Lomonosova, Khimi- cheskiy fakullt6t,:Laboratoriya adsorbtsii - In- stitut fizichesko :khimii AN SSSR, Laboratoriya. Y. sorbt si onnykJ3L: -PrOtSeS Soy (Mogg- Universit im. M.Y. Lomonosoy '-Chemical Department, Laboratory of Adsorption - Institute of Physical Chemistry AS USSRI Laboratory of Sorptive Processes) SUBMITTED. September 3V 1958 ~Card 4/4 8/069160/022/03/10/019 B004/BOO7 AUTHORS: Kiselevo A.-Vag Pogoeyang T. A. TITLE: The. Theory of.,the Corpusoular Structure of Xerogele. 1. The Preparation of Silica Gels From Large Globules. With Varying Number .of Contacts and.-Their Investigation by the Adsorption Kethod PERIODICAL: KolloidVy shurnal, 1960, Vol. 22v No. 3, PP. 314 322 .TEXT: The theory of the~cdrpuscular structure of xerogels was developed by A. V. Kiselev in Refe.'165- Accordftqfty, the skeleton of xerogels con- gists of primary partiolesp which are-spherical in the case of silica gelso The authors iLim at producing brines with particles of such a size that their shape may,be determined by means of an electron microseopeg and that their behavior in-the,process brine - hydrogel, - x9rogel, may. be followed. The present paper desoribee the produ9tion of such brines and gels and the investigation of their adsorption7lpropertioa. The brines were prepared by exchanging the sodium ion for the hydrogen ions .in solutions of sodium silicate by means of the KI-1 (KU-1) oation ex- Card 1/ 4 -3 The Theory of the Corpus6ular Struoture.of S/069J60/022/03/10/019 Xerogels. 1. The Preparation of.,Silioa Gels B0041BOO7 Prom Large.Globules With Varying Nuaber of Contacts and Their Investigation by the Adsorption Method changer. kdescription in given of the formation of germs'in the silioic aoid, solution stabilized,~y alkali_-by means of heatingg the addition of fresh silioio aoid.. and the formation of hydrogel by a mmll addition of HC1. The xerogels were obtained'by drying at 110-1200C. Fig. 1 shows the methanol adoorption.on,eight xerogel samples which had been produce& at various pffe The flWaleft, speoifio surface was found in the case of xerogel obtainedat-pHo,10-7-90 that for the further experiments only brines with PS~10-7 were used* For the purpose of avoiding a structural change, the water was sublimated from the hydrogels in a vacuum accord- ing to N. M. Kamakin (RI ef 12). Theng,the hydrogko were dried at 110-120000' The adsorption isothermal-lines for methanol- and benzene vapors were determined by means of an apparatus with a quartz spring scale (Fig. 2). The d Ni f this.apparatus had been begun byq :e3d . 0 (TSP-4) hermo- L. ff. Soboleva (decea Lr It--was located in a Mr-A stat developed by G. G. Nuttik in the authors' labor-aVory. Fig, 3 shown the benzene-adsorption isothermal lines for four silioak%drogels at 200C~ 15000, and for the xetogels produced therefrom at 150 Go The Card 2/4 3 The Theo of the Corpusoular:Structure of 8/06~/60/022/03/10/09 Urogels. 1. The Prepirationof Silica Gels 3004/BO07 Prom Large Globules With-Varying Number of Contacts and Their Investigation by-the Adsorption Method specific ..surface* was determined by B, G., Aristov by means of nitrogen .adsorption at low'temperatureso-A table contains these values as well as the pore diameters and the number of contacts whiohy on the average, was 2-5. Fig, 4 shows thatithe specific sufface had not been changed by dry- ing. Duxing transition from,hydrogel to xerogel merely a contraction of, the pores occurs (Pig--5).- The iample6~obtained were homogeneounly,coarse- Pored with &'particle diameter of about 300 1. The benzene-adsorption. isothermal lines of silica gels are compared in Fig. 6 with those of quartz and further4ith the data for KCK-2 (KSK-2) silica gel obtained in the laboratory of the authors by Yu. A. Elltekov and D. P. Poshkus. Results of measurement show good ag.reement. Only at-the stage of poly- molecular adsorption,and capillary condensation does the influence exerted by the paokings of different densities become notioalabla. Thera are 6 figures, I tablev and 23 references: 18 Soviet and 5 English- Card LYGIM, V.I.; NOTALWA, LT.; UTSW21, K.L; KISIM. A.T. Adsorption properties and infrared spectra of oxidized carbon blacks. 11oll.shur. 2,2:-, no.3'..334-339 W-40 '60~ (KIRA 13:7) I.. Institut nsichesimy khWi AN WM Kookm (Carbon bl"k-Spectra) (AAsorption) S/069/60/022/006/002/008 BO13/BO66 AUTHORS: Kiselev, A. V.i Korolev, A. Ya.p Petrova, R. S., and Shcherbakrva-,K. D. TITLE: Effect of the Degree of Chemical Modification of the Silica, Surface.With Tetramethyl Chloro Silane on the AdBorption:of Nitrogen- and Krypton Vapors PERIODICAL: Kolloidnyy zhurnal, 1960, Vol. 22, No- 6, pp. 671-679 TEXT;. The authors of the present paper studied the effect of the silica surface modification on-the adsorption of nitrogen- and krypton vapors. They achieved a considerable-reduction of the interaction energy adsorbate - adsorbent by substituting trimethyl silyl groups for the hydrogen of the hydroxyl groups on the silicon dioxide surface. The adsorption of nitrogen-, and krypton vapors was studied on five Aerosil samples. Aerosil is a non-porous, highly disperse silica which was treated with trimethyl chloro Bilane vapor of solution in benztne. -To obtain samples modified as completel as possible, kerosil is hydrated for 19.5 L9C and 169 atm with water, and then treated hours.in the autoclave at 350 Card 1/4 Effect of the Degree.of Chemical Modification S/069/60/022/006/002/008 of the Silica Surface With Tetramethyl Chloro B013/BO66 Silane on the Adsorption of Nitrogen-,and Krypton Vapors with ClSi(CH 3)3 This led to an up to.90% occupation of the Aerosil surface with Si(CH ) groups. The adsorption isotherms of nitrogen and 3 3 krypton vapors were plotted attemperatures of liquid nitrogen. The adsorption of. the two substances was found to be reduced by modifying the silica surface with trimethyl silyl groups. The krypton adsorption considerably decreases at a.high.degree of modification. Also the shape of the adsorption isotherms varies i.e., they are less bent.-The isotherms for the above vapors are plotted in coordinates of the BET equation. It may be seen from it that owing to thereduction of the absolute adsorption quantity the BET equation is.less satisfied, because with the less intense interaction of adsorbate - adsorbentj the interaction of adso-ebate - adsorbate must not be neglected any longer. The specific surface for non-modified silica samples may be determined by the BET method, e.g. on the basis of the nitrogen vapor adsorption. For modified samples, however, the values obtained by the BET method are too low. It was found that the adsorption of nitrogen- and krypton vapors depends on the degree Card 2/4C ---------- Effect of ...the Degree of-Che.mical,Modification S/069 60/022/006/002/008 of the:Silic!~,Surface With Tdtramethyl Chloro, B01 3YB066 'Ni Silaneon thi Adsorption of .,trogen-mand Krypton Vapors -that the BET methoft is not plicable of modification to-such an extent ap for determining the'specific surface of considerably modified sam'les. p The adsorption-isotherms obtained for the.nitrogen and krypton Vapors Tlere compared with the isotherms previously obtained (Refs. 6,7,10) for vapors of n-hexane, benzene,.methanol,.and water (Fig. 3). Modification was shown~ to effect a considerable reduction of adsorption in all adsorbents. I F.: 9. 4! illustrates the approximat e.'o ours e -of. the adsorption decrease at p/p -. O.I.-aith iner.easihg occupation 9 of the surface by Si(CH groups. 1. s 3 3 V. P. Dreving is thanked for, developing a volumetric apparatus, and' V B. G. Aristov for plottingthe adsorption isot.herms of nitrogen. There.are, 4 figures, 3 tables, and 35 references:.22 Soviet, 5 Britisho 4 US,.-.and 3 German. ASSOCIATION: Moskovskiy universitet im.' M. V. Lomonosova Khimicheskiy. fakulltet,,Labo-ratoriya adsorbtsii (Moscow University imeni I V. Lo onoso Chemical Division, Adsorption Labor ry) d. m v ato 3/0 S/07~J60/034/012/001/027 B02o/Bo67 kUTHORS: Poshkus, D. P. and Kiselev, L. V. TITLE: Energy of Dispersion Interaction of Benzene and n-Hexane With the Surface of Magnesium Hydroxide PERIODICAL: Zhurnal fixiohookoy khimiip 1*' Vol- 34, No. 12, 2640-2645 TEXT: In a preceding paper (Ref. 1)p the authors assumed that the change in the ratio between the adsorption heats of benzene and n-hexa 'ne vapors on polar adsorbents is mainly due to the stronger electrostatic inter- action of the benzene molecules as compared with the n-hexane molecules. Thus, an electric field is generated above,the surface of the polar . adsorbents, mainly above the lattioeLof Mg(OH) 2. Therefore, the author a studied the energy of interaction forces between benzene and n-hexane molecules and the Kg(OH)2 surface, Ug(OH)2 has a multi-layer,rhombohedral ionic crystal lattice of the type CeI 20 Each lattice layer consists of an Card 113 Energy of Dispersion Interaction of Benzene and S/07 60/034/012/001/027 n-Hexa'ne With the Surface of Magnesium Hydroxide B020YB067 Ug ion plane which lies between two hydroxyl ion planes which, in turn,. consist.of oxygen and hydrogen ion planes. The potential of iD diapeirsion-interaction of the member i of the chain of hydrocarbon .Molecules (CH CH and CH with the centers of force j of the 3' 2 arom vg(60 lattice (H, 0, a*nd Mg) was calculated for three layers above the 2 basal~plane of Mg(OH)21 i.e., A) above the hydroxyl ion of the first. (external) plane (layer k), 2) above the center of the hydroxyl-ion triangle of the first plane, below.which lies the magnesium ion of the second plane (layer B),, or 3)~the hydroxyl ion of the third plane (layer C). When expanding the dispersion potential in a series, only the first two terms are considered which repres'ent the potential of dipole - dipole and the dipole - quadrupole interactions. The others influence the entire poteatial only slightly. The constants of dispersion interaction were calculat~id. The sums of the exponential functions r-n , where n 6 and 8,1and J H, 0, or Mg 2+ . were calculated by assuming that a 3.11 A, c - 4.73 A, u = 0.22, and that the distance Card 2/3 Energy of Dispersion Interaction of Benzene and 5/076 60~034/012/001/027 n-Hexane With the Sur'faoe of.gagnesium Hydroxide B020YB06 betweenthe hydrogen and oxygen atom centers in the hydroxyl ion in 1 0-97 1- Summation was-performed up to r 10 A. Henoe, the great OH ij indrease in th' *.tio between-th adsorption heats of benzene and Mg7or e n-hexane,on compared to those of the vapors of these H)2 as- compounds on graphiie is not causedlay the dispersion interaction of benzene and n-herahe molsoules with the basal plane of Mg(OH)'2 . Thire are 3 figures, 5 tables, and 15 references% 6 Soviet, 2 US, 3 British, and 4 German. ASSOCIATION: Moskovskiy goeudarstvennyy universitet im. M. V. Lomonosova (Moscow State University imeni M.,V. Lomonosov). Akademiya nauk 'SSSR, Institut fizioheekoy khimii (Academy of Sciences USSR, Institute of Physical Chemistry) SUBMITTED: October 25t 1958 Card 3/3 R Ml- t 14511 AMEN' T-111 0 5/076j6O/O34/012/0012/027 B020/Bo67 AUTHORS: Poshkusp D. and Kiselev, 1. V. TITLE: Electrostatic Field Above the Basal Plane of Magnesium Hydroxide and Its Interaction With Benzene and a-Rexane .Molecules PERIODICAL: Zhurnal fizichoskoy khimiij 1960, Vol. 34, No* 12, pp. 2646-2653 TEXT: In continuation of:the,calculation of the energies of.dispersion interaotion~ of benzene: -and n-hox ano Moleoules with the Mg(OH)2 basalt planeywhich was desoribed in the preceding paper (Ref. 1) the authors studied the onergy.of electrostatic interaction of benzene and n-hexane molecules with the electric field above the Mg(OH)2 basal plane They. determined the voltag-e,component of the electric field F zover the Mg(OH)2 basal planeas depending on 1) the dipole moment of the OH ions# 2) the degree of homeopolarity of the bond between magnesium ions and Card 1/4 Electrostatic Field Above the-Basal Plane S/076/60/034/012/002/027 of Magnesium Hydroxide and Its Interaction With B020067 Benzene and a'-Hexane M61ecules OH ions, 3) the distance.z between two layers above this plane, i.e.,, a) over the OH ion and b).over the center of the triangle formed.by the OH ions. The voltage of_the electric field over the basal plane of P ions. (above the, infinite_'~ hexagonal lattice of the8e ions) Was Calcu- lated by summingthe-individual charges in the plane of such a lattice to a certain height.The'values-o.f F,,,/(E/a') above the infinite two- dimensional hexagonal lattice ofAbe point oharges are given in Table 1. Fig. 1 shows the diagram F_ /(F,/a ) as a function of z/a. The values F V, 26 were determined from Fig. 1. Tables 2 and 3 give the calculated results for the voltage of-the electric field above the two-dimensional, hexagonal lattice of the dipoles p of the hydroxyl ions perpendicular to the lattice plane, F - Fig. 2 shows the voltage.of the electric field F over the ZP Z basal plane~of Mg(OH)2 with z - 2.6 A. as a function of the dipole moment p of the hydroxyl 'groups with two extreme states of the Mg(OH), lattice. In Fig. 3 F. over the basal plane of the Mg(OH)2 lattice is graphically Card 2/4 Electrostatic Field Above.thi Basal Plane 8/076/60/034/012/002/027 of Magnesium Hydroxide and Its.Interaotion With B02O/BO67 Benzene and n-Hexane Molecules represented as a function,of.Ithe, degree of-bomeopolarity of the bonds between Mg ions and, OH-ions*- As an example,Table 4 shows the contributions of the negative charges and.the dipoles of the first and second OH-ion- planes and the positive charges of the Mg-ion surfaces of the first basal layer of Ug(OH) 2 to FZ above this layer,with z - 3.0 A and p - 2-4 D if a pure ionic bond exists between Xg- and OH ions. The voltage of the electric field above the basal plane depends only little on the homeo- polarity of the ionic bonds Mg - OR whereas it.strongly depends on the dipole moment of the OR ionsy above all *on the dipole moment of the OR ions on the surface. With increasing dipole moment the.field voltage for both layers changes almostlinearly. The voltage of the field above the OR ions has the opposite sign and its absolute value is approximately twice that of those above the-center of the triangle formed by the OR ions. With increasing distance the electric field is gradually weakened. The induction interaction of,benzene and n-hexane molecules with the basal plane of magnesium hydroxide oannot be caused by-strong changes in the ratio, of the absorption heats of benzene/n-heiane compared to that Card 3/4 Electrostatic Field Above.the Basal Plane S/076/60/034/012/002/027 of Magnesium Hydroxide and Its Interaction With B02O/BO67 Benzene and n-Hexane Molecules with graphite. These changes-are due to the strong electrostatic inter- action of the constant multipoles.of the benzene molecules with-the electric field.above the ]Kg(OH) basal plane. There are 4 figures, 4 1 2 tables,,and 10 references:, 7 Soviet, 2 British, and 1 Japanese. ASSOCIATIOV: Institut:fisicheakoy khimii.Akademii nauk SSSR (institute of Physical Chemistry of the Academy of Sciences USSR). Hoskovskiy.gosudarstvennyy universitet im. M.V. Lomonosova (Moscow State.University imeni M. V. Lomonosov) SUBMITTED: October 259 1958 Card 4/4, S/076j6O/O34/012/020/027 B020/B067 AUTHORs:. Isiriky&np le: is andjKiselsvj A. V, TITLE: Adsorption Heats of Hydrocarbons on Magnesium Oxide PE RIO DICAL: Zhurnal- fisichao'koy-khimii, 196o, Vol- 34, No. 12, pp. 2817-2824 0 the complete values of the adsorption heate''of TEXT.' In this pap r n'heiane and benzene,on magnesium oxide are given, which in an earlier Paper (Ref.*2)-had been-used for a comparison with the theoretically. calculated'values, The measurement results of the isothermal lines ana.ths, differential, heats of adsorption of the vapors on benzene, n-hexaneq and fi-octanb on MgO are evaluated. The calorimetric determination of the heats. bf adsorption was.made in an.apparatus described in Refs. 13 and 14, The results are shown in Figs. 1-3. The adsorption of n-hexane and benzene vapors was studied until the formation of approximately two adsorption layers, whereas theadeorption.of n-octane vapors was studied almost until saturation. This allowed the determination of the maximum desorption ,temperature near the saturation and the calculation of the distribution of Card 1/) Adsorption Heats of Hydrccarbons on. S10761601034101210201027 Magnesium Oxide 3020/B067 the pore volumee,from the desorption branch of the isotherm. When determining theabsoluts val,us,~.of adsorption per,aurfaoe unit, the specific surface s must be known whicht.in,turn, is determined from the surface 00 that is-occupied by-the molecule adsorbed in the monomolecular layer. By using the equationsof La Ingmuir, BET or other varieties the, isothermail lines.'of adsorption.. can -be evaluated to determine the capacity of the monolay r a orlthe energetic characteristics of the system 9 m investigated. The values thus obtained are, however, often contradictory. The constants of the-equations-BET and of HU"ttig for the isothermal lines of adsorption of the benzenap-n-hexane, and n-octane vapors on MgO are listed in Table 1. Table-2 gives-the values Wo for hydrocarbons, which were calculated by various methods. Fig- 4 shows the heats of adsorption of the benzene, n-hexane and n-octane vaporson MgO as depending on the surface filling. Fig. 5-show,a the,differential entropies of adsorption for the systems investigated.(standard state - normal liquid), and Fig. 6 gives a comparison of the isothermal lines of the dependence of the adsorption heats and the adsorption on the relative vapor pressure of oc-,, tane on coarse-pored MgO..There are 6 figures, 2 tables, and 27 references: 20 Soviet, 3-US, 3 British,.and 3 German. Card 24 Z_ J Y-j lit? IJ 3; LP lid j 0 1 M I 0- 9~r ~ 11 1 n .. 1 1 K:j I . FOR 0 co t~ to all a i -]Ills 4 92 Z 4:5 tP a kip k S/069/61/023/001/005/009 1424/B904 AUTHORS3 Isirikyin, A, As and Kiselev TITLEs Effect of *ompression of carbon black on the isothermal line and heat of adsorption of n-hexane PERIODICALs Kolloidnyy Z~~nalp v. 23, no- 1, '19619 67-75 TEXTs The aim of the, present paper is an explanation of the nature of inhomogeneities arising in,carbon black compressiong as well as of their effeot upon the isothermal:line and heat of adsorption of vaporcus,hydro- carbons. OePOH -6 (eforon-6) canal lampblack annealed in a hel Iium atmosphere at 280001 as uned in the work under Refs 17P was used. as an ad- sorbento This sample was/oompressed in a mechanical press at pressures of up to 4 and up to 10 t =2. The-'resulting isothermal lines of adsorp- tion are illustrated'in Figs. I and 2. Table i shows the speoifio sur-. faces as determined from'the isothermal line of n-hexane adsorption by the BET methodl the specific surface determined.by the authors agrees well with published values. The limiting volume V of sorption (bulk volume of the pores) decreases rapidly already at a relatively soft compression Card 1/W 27 S/069/61/,023/001/005/009. Effect of compression BI 24/B,204: (4 V02), whereas it varies only slightly with further compress ion up to 2 10 t/om . The coordination number n displays the, same character (Table i), The absolute isotherm al lines of adsorption and the curves of adsorption heat obtained for the'range 0t monomoleoular filling and transition to pol7molecular filling are shown in Fig. 2 (below) and Fig, 3. Table 2 presents.the standard-diffe,rential-thermodynamia characteristics of n- hexane adsorption correspond .ing to a 50% filling of the monolayer 0-0*5 upon aferon-6 carbonIlaok (annealed at 170000 in a hydrogen stream) and upon the carbon black samples of the authors* At 1700OCt channel was graphitized only to a slight extent since the adsorption energy of n- hexane during a heating of the carbon black to 28000C rose by 0.25 kcavmole, whereas the adsorption entropy in the same case deoreased by 0-68 units of entropy. For comparibonp .. Figa 3 shows also the curve of the differential adsorption' heat of n-hexane.on P-33 (R-33) carbon black heated to.only 10000C. The arrows indicate the direction of the curve of differential adsorption heat upon non-porous carbon black with a homogeneous surface in the case of oompressiono Fig- 4 shows the heat difference in capillary condensation of n-hexane"upon compressed and uncOMpreBsed carbon black Card 2/M s/o,69/61/023/00 2/002/008 B101/B208 AUTHORS: Kiselev, A. V. and Khrapova$ Ye. V. TITLE: Approximate expression for the wave-like isotherms of nitroyn adsorption on graphitized carbon black,-considering adsorbate- adsorbate interaction in the.first-and second layers PERTODICAL:~ Kolloidnyy zhurnal, v..23, no. 2, 1961, 163-169 TEXT: It was shown in previous papers (Ref. 1: Kolloidn. zh.,129:572, 19571 Ref. 2: ibid.p LO, 444, 1958) that the adsorption isotherm of vapors, particularly of nitrogen, begins with a concave section owing to adsorbate- adsorbate interaction. For the first section of the prevalent occupation of the monolayert the following equation is written; 9) (1 j while the~approximate equation h G/K11(l - 9)(1 + K ) . h Q(1 - h) 2/K GO - h)] (2) holds for the transi- 1 [1 - G(I - h)] [1 + K n 1 tion to the adsorption of the second ljLyer. h denotes the relative pressure, 9 the total degree of surface occupation, K' the equilibrium constant for th b t t t t t th l e-adsorbah e adsor a interac for ibrium constan e he equi ion, and Kn Card 1 S/d6g/61/023/002/002/008 Approximate expression B101/B208 adsorbate-adsorbate interaction. The authors studied the adsorption of nitrogen vapor in a wide range of Q,and tried to obtain a better approxima- tion-of equation (2) to the wave-like course of the adsorption isotherm. Adsorption of N2 was performed at.-1950C on Soviet T-1 (T-1) carbon black (annealed at 30000CI specific-surface s -:28.1 M2/g), afid T-2 (T-2) (32000C, 8 M 6.9 m2/g) by means of anapparatus.,*.Ltah has already been despribed by the authors (Ref 15:- Izv-- AN SSSIR, Otd. khim. n., 1956P 390). Fig. 1 gives the results and compares them with those obtained by 8- Ross, W. Winkler (Ref. 3, see below), and S. Ross, W. W.'Pultz (Ref. 4, see below). The waves of the isotherm of successive occupation of the black surface first with the monomolecular nitrogen layer and then with the following layers are given by G" am )/%, where. am - 10.2 5 pmole/m2'is the occupation of the monomolecular layer; (a - a 2)/a. witha 2 - 18.0 Pmole/m 2 is the occupation of the second layer. These parts of the isotherm are expressed by Eq.(2) if for each part another value of the constants is taken. This is shown in Fig. 4. The constants thus calculated are presented in Table 2. Fig- 5 shows that agreement was brought about between calculation and experimental data by substituting the various values for the constants of Card 2/43 .. - - %2jr~ ~ .- -~, - . ~-- - , ..- ; ~ -. . I I - ~, , _-,y ~ -, , - - -~- - -,,~ ~IWMINI 28280 S/069/61/023/005/005/006 B120101 AUTHORS: Kiselev, A. V., Kovaleva, N. V., Korolev, A. Ya. TITLE: Adsorptive.properties of oxidized carbon blacks~ 1. Oxidation of channel black in an aqueous medium PERIODICAL: Kolloidnyy zhurnal, v. 23, no. 5. 1961, 582 591 TEXT: In this'paper, the adsorptive power of channel gas carbon black samples from Ukhta with a specific surface of about 150 m2/g and an oxygen content" of 4-06 which had been oxidized in aqueous solution without heating with sodium hypochlorite, hydrogen peroxide, and a mixture of HNO3 and H2S0 47 was investigated. The chemiso.rbed-oxygen a,ontent, hydrophilic properties, and wettability of the carbon black are increased by polar organic liquids. The carbon black.forms highly disperse colloidal hydrosols without addition of organic wetting agents. After drying and removing substances adsorbed on carbon black by exhaustionat 150 C. the C and H conterts w3re determined by a microanalytical technique, and the total oxygen content was established Card 1/6 V( 2M0 5/069/61/023 005/005/006 Adsorptive'properties ofo.. B124/B101 from the difference. The presence of active oxygen was detected by adsorption of NaOH from the aqueous solution and by determining the content of hydroxyl or phenol groups according to Grignard. The volatile substances content was,,determined by heating the carbon black to 8200C. The nitrogen content in the carbon black samples treated with the MTO - H so mixture was determined by the Kjeldahl technique, 3 2 4 and was found to be 0.27i~, The specific surface was calculated from the adsorption isotherms of nitrogen vapor at the boiling point of niti7o-en according to BET. Data on-the specific surface and the chemical composition of carbon blacks oxidized by various techniques are given in a table, The oxidation of the carbon black surface leads to a reduced adsorption of n-hexane vapor. This is due to the fact . that the oxidized surface is covered with oxygen-containing groups.so tightly that there is no.more room available for the large n-hexane. molecules. The increase in the adsorptive power for benzene vapor with the oxidation degree of.the carbon black surface is due to the fact that the interaction of thet-bonds in the benzene molecules with the OH groups on the surface of oxidized carbon black samples is intensified. The difference between oxidized and non-oxidized carbon black surfaces Card 2/6 28280 B/069/61/023/005/005/008 Adsorptive properties of... B124/B101 becomes still more pronounced when methanol and water vapors (Fig. 2) are adsorbed. Methanol is probably chemically sorbed, too. The carbon black surface modified by graphitization or oxidation which becomes either strongly hydrophobe or strongly hydrophilic, can change the adsorption of water vapor by one or two orders of magnitude. Methanol vapor is most strongly adsorbed on surfaces oxidized.with an HNO -H SO mixture, 3 2 4 although these samples contain less oxygen than samples oxidized ith NaOC1; the same holds for.the,adsorption of water vapor. The.adsKption of all vapors investigated generally increases with the degree of oxidation. The authors thank,G.- M. Lyulina, N. N*Avgull, A. P. Arkhipova, L. I. Doroshinaq and M. G. KuZ1mina for assistance. There are 5 figures, 1 table, and 20 references,: 13 Soviet and 7 non-Soviet. The two most recent. referencesto English-language'publication8 read.as follows: M. L. Stude- baker, E. Hoffman# A. C,..Wolfe, L. G. Nabors, Industr. and Engng. Chem. 48, 162, 1956; J. V.. Hallum:,,H~ V.,Drushell, J. Phys. Chem. 61, 110, 1958- ASSOCIATION: Institut fizichesko khimii AN SSSR, Gruppa khimii poverknosti Moskva ~Institute of Physical Chemistry AS USSR, Card 3/6 Group of Surface.Chemistry, Moscow) B/076j6l/O35/002/601/015 Energy of~.'anteracti6n. adsiorbate B124/B202 the centers.~of b car on.atoms he'external.basal plane; iij is the dista.nceo'f the center i ~:fro M_: the center J_of the graphite lattice, C e aozistants:.~of -the eleotroahemical attraction of type- C 11 29. and C are, th dipole d ip2e, d ipol e* PoI6 d'. quadrupole quadrupole,!and quadru an is,the 'constant~of -repulsion." _Cj- Iwas - calculated from the X irkwood.Mliller e equation by means .of - the".polarizabilit ,y and the magnetic suse ptibility of :the centers :~i and-.,J, C2 and C3 we' Iculated in the same w re ca ay,,q *as 11Y obtained from the.correeponding lattice~oonstants Q anMj, and, I ina 9 -equi ibr*ium o n 0,; BI was obtained from the 1 o dition (Z ~z - (2j, Z-Z The potential of,the.interiietion.'-adoorbate adsorbate for no~~polar, e e 0 molecul.es- fij' was det rmin d fr in the :e4uation C it Y, r,,4 + bij r7,n) 'PY _2 2'- wheie.ji is thej~otential of,the..-interaotion between two isolated~,-centeri on was and rii,the*distance of hes6 centers The oonstaht of iepulsi e 'd teimined from the- e4uilibrium,condition at values of rii which T ard 2 C A 02/661/015, tn~ S/076J61/035/6 ii sotbate. Energy of-_':interac on.ad B124/B202. correspond o-a'.. egr our ac 0 t d eC of, 1 at:0 5, the ritpuleibn'- -Ij -of .~~eziergy.in:jj~ may-- e-.neg ea. ed.. -._-_Tab16 -1 shows a comparison -the. a oul6ted Value a and the~meae'ur ats of aas rpVion edA iffeien tial he 0 0 '6bt'i ed*'-',When,st dsorotion of~` i!L, 5 emeht;'as ud ing -the * AL at. 9.0 GooUagre v a n , q y 4,' complem'nonpolar mo n,'t I _11 e es o" he.;bas ,p ane o :-gr o tion 1 oul al* I f aphite the' idd rV a of' their energy was.-determined 9~,the:sum 6f th#~adsorption energies individual. links A by taking:ao'count- *a f, 1he'differen' distances zi*~f the -(z different links ~i from'the plane rj z6) for the most favorabl6 surface rie-- F , ': 0 ntIat ion~.~of -the.m .a ecule at*. n-al kanes with n,carb s on at!6ms ih Ahe molecul'' e 4 ~n. (D. 24Dc + (4-72) 4D,~H,~- 2 (McIll -tq olds from'whioh,:the' lat +.1.88n(kcal/mol6). SI re ion In 0 .85 - -alk,t obtain ed for-n-alkanes and.: '2 + 1.88n(kcal/m~.le "for a4mono,dl A a-mofioolefines..,Table 2 compares:the calculated 'values of vita. the., - 0. -a or 9 5 me sure v a d :alues f 0. jor some isoalkanes,~oyolaijes, pd: (f j aromatic-hydrocirbons. -The. -authoi. also deals with the adsorption.of polar~,.`T4i Card*3/A j~ U ~A 81016161103510021061'10151 Energy- f interaotion.adsorbate . B124/D202 f 0 ae:, . molec les' n ne.*-.of hite'.' Table 3 shows a comparison.of u .0 tfie.:basal'pla' grap calculated f or 0 1. - v~-O and Q`:_ 1 with the a:dsorption heats. 'the values. eleotrokinetia- attraction aud the enO Yffien calculating --..(Io the rgy 9f. , I . electrostatic inductive attractiofi"_ .2 6 Acopunt.',': Table 4,shows a comparison of:the r were taken into , , i j- ii ,.' doo hea a rp~tion: to. of water alcohols ammonia, adsorptimenergy:ana, the . and methylamine. In this:oase both'the electrokinetio and the' electro- f static (inductive): interaction of.-:*,,the molecules with the carbon atoFs 0 -,~' the graphite lattice- and the Alfferent, degree ~ of their mutual '4asoctation " i i~'i ~~ at the expense of-the hydrogen bond vere.taken into account. in connection,il- 6r with'the adsorption of nonpolar molecules. on ion crystals the~auth red the calculated values of-potential adsorption energy~;--~ with compa: Uoii. e isoster (Table measured in the calorimeter,and calculated from th .- The aut~or.then discusses the-adsorption of n-hexane and of benzene.on magneuium hydroxide and-th~.adsorption of.silicio acid and silicon dioxid the'' 69 'of the Table 6 ds the hift ti f e c ill e. 4 .oso a -s s on r oompar quen y a hydroxyl groups. on. -the surface with the-differences o:e adsorpt! on*he t 9 ' Card 4 S107616110351,002109-11015 - rg. -on-- a sorbi e... B124/B202:' d Y: ~of interaoti -and':* 6ider* of the quantities. -A~ 'and e e!i -A hor,also s 8 ativ -agr _eemen f! d di' cusses'ads di e O,rPt ~on'on' -chemic 11y* . 4 rft 6- theoretica .mo a u es. In u 0 calculation,,of ith ::coAstant:th6' e eq ilibrium' Autho j~ :the interaoti r.-first'determines the Potential curves of -bent, and, -adsorbate - ads rbat 0 e. on ad -f - sorbate._~-. ad 0~~ ollowing.ho 6 lculA ed on'funofions of the system TI the -the diitributi n ddsorbe -by e methods. -s n- th 'of tat-i adsorbate stioal mechanics by using certairit d Ynam cal:models:.-in he :adsor~ti6n compi ex- POIYani and D. PoAkus ar mentioned. '.-,The -pr ese a resented at the Gordoz~ Conference e n paper wa p on ce'Chemistry, _Meridan :(Ne .shire, Surfa are 18-figures USA), July 4, 1-966. ."There, r-ef e~ e' 6 tables' and r nces: 47 Soviet-bloolAnd 310 .77 non-Soviet- 10c; E. L em. 64:. 961- 1960.:-' b -Pace' A. J. Phys. Ch R. ~,S 'ASSOCIATION: Akad miya nauk SSSRI~ Izi'titut fizicheakoy khimi' .(Ac~Ademy of. e Sciences USSR$- Institute of Physical ChemiE Itry):; Moiiovskiy. gosudarstvennyy universitet im. m. V. Lomonosov Xhimicheskiy fak-ul:1 te t '(Moscow State Universit imerti M. Lomonosov--Divisi ofi~of_~Chemistr y Card 5/9 MELEV, A.V. Gordon conference on interfacial chemistry in the U.oSoA* held on Tuly 164, 1960. Zhu. fiz. khim, 35 no,2:1+76-477 F 16le- (mm 16:7) (Swface ahemistry-"Congresses) B/076/61/035/008/016/016 B110/B301 AUTHORSt Vasillyeva, V. A. V., Nikitin, Yu. S., Petrova, R. S., and Shcherbakovap K. D. TITLE t Graphitized carbon black as adsorbent in gas chromatography PERIODICALs Zhurnal fizicheskoy khimii, v. 35, no, 8 19619 1889 1891 TEXTt In the work under consideration, the authors made use of geometrically and ohemically,modified silica gel as the carrier of another. solid body. Thermal types of carbon black annealed at r4 30000C are' high- disperse bodies with a very homogeneous surface. Their.absolute adsorp- tion values are much greater than those of other adsorbents. Tablets are difficult to produce without binding agents. Therefore, the carbon black, is introduced into the large pores of the solid carrier. Thus, a powdery adsorbent,with homogeneous surface may be introduced into the column. The carrier should be a large-porous body with thermally and chemically stable and very poorly adsorbing surface. In the present case, the authors used large-porous silica gel with a very small surface covered by chemically grafted trimethyl silyl-groups. A 2-hr hydrothermal treatment in the Card 116 S/076/61/035/000/016/016 Graphitized carbon black..,. B110/B.101 autbalave,at 35000 reduced the silica gel-surface to 15 m'/g; the enlargement of skeleton globules and pores was established by electron microscopy. Purther grafts of trimethyl silyl groups an the silica gel sitiftoe according to I. V. Borisenko led to a sharp decrease of adsorption. AM% blown out and sieved graphitized thermal carbon black T-1 (T-1) .000000) was then introduced into the porea. The silica gel was thereupon introduced into the column ohromatographp where it was heated for 2 hr in the nitrogen flow at 15000. Graph a) in the figure shows chromatograms of vapor, mixtures of benzen4p, acetone, and-.n-hexane on geometrically modified silica gel with hydr6,ts&-, surface; d) shows chromatograms of these three individual vapors on sifica, gel modified with trimethyl silyl groups; and 6) chromatograms of the mixture on silica gel modified with carbon black at different temperatures. The succession of peaks was, however, the inverse compared with silica gel with hydrated surface. The acetone peak ha.d a pronounced tail due to reaction between carbonyl groups and accessible hydroxyl groups of the 1ilica, gel crarrier. The form of benzene- ,and n-hexane peaks corresponds to the form'of'ourves illustrating the I adsorption heats as functions of the form.of'idsorption isotherms. The peaks become narrower at.higher temperatures. According to theory, the Gard 2A S/O 61/035/008/016/016 Graphitized carbon black... B110Y3101 ratio between band width and-retardation time is conserved. A study of chromatograms of individual benzene.and hexane vapors at five temperatures allowed estimating their adsorption heats on carbon black from the dependence of logarithm of relardation time versus inverse temperature; results were consistent with calorimetric data. The combination described is.well suited for gas chromatography as well as for a rapid physico- chemical analysis of the utilized powders.alike. Silica gels_modified in this way can also serve as carriers bf,steady liquid phases. There are 1_figure and 6 referencess 3 Soviet-bloc and 3 non-Soviet-bloc. The two references to English-language publications read as follows: Ref. 31 J. Bohemen, Stanley H-. Langer, R. H., Perett, J. H. Purnell, J. Chem. Boo., 24441 196o. Ref- 51 F.- T. Eggertsen, H. S. Knight, S. Groennings, Analyto Chem. , L8-, 3.03, 1.956. ASSOCIATIONt Laboratoriya--.adeorptsii i gazovoy khromatografii khimicheskogo fakulfteta Moskovskogo gosudarstvennogo universiteta im. M. V. Lomonosova (Laboratory for Adsorption and Gas Chromatographi.of...,t4p-C,hemistry Division of Moscow State University imeni M. T'.*,Lomonosov) Card 3/6 8/020/61/136/002/025/034 B004/BO56 AUTHORSt Babkint I.Yu. Kiselev A V and Korolev, A.Ya. TITLEt Adsorption Heats-and:-Entropies of Hexane and Benzene Vapors-on an'-Aerosilalith a Surface Modified by Trimetb u ylsilyl Gro p9 PERIODICALs Doklady Akademii naukSSSR, 1961, Vol-136, No.20 PP*373 376~ TEXT: The authors studied-the adsorption of hydrocarbon vapors on the.sur- face of.aerosils, which had been treated with trimethylahlorosilane. A theoretical calculation of the adsorption energy of n-hexane and benzene molecules (Ref, 3) resulted, with increasing'modification of the silicon dioxide, in a drop of the.adsoption energy below the value of condensation heat. It was assumed that in the case of sufficiently modified aerosil, the adsorption heat of these hyArocarbona.must become negative. It.was the.pur- pose of the present work'to check this assumption. In order to give the aerosil surface greater homogeneity and reactivity with respect to tri- mathylohlorosilane', a hydrothermal treatment in an autoolave was carried' Card 1A Adsprption Heats,andzEntropies of Hexane and S/020/61/136/002/025/034 Benzene Vapors on .an Aerosils With a Sur- B004/Bo56 face Modified by Trimethylsilyl Groups out..at 120 265 C for 8 19. 5 -hours. Specimens of aerosils were obtained, whose surface was ocoupied'by Si (OR ) groups degree of occupation: 0, 60, 85 90, or 100%. For these spMmens' Fig. I shows the calorimetric differential adsorption.heat., qs~_ (kcal/mo-le)asa function of adsorption ,*_Molelm2), and,Pig. 2~ahows the isothermal lines fore/, as a- function of the relative vapor pressure 13/p The dropping of q a below the conden- sation heat L was observed,..and for~the completely 000%) modified ape- cimen, the true adsorption.heat was found to bet q a - L - -0-5 with n- .hexane; Q - L 1.0 w.ith,benzene., .s. Accordingly,.adsorption decreases considerably with ~ constantly rising modification (Fig. 2). In the oase-of large p/p , the surface is occupied 8 with hydrocarbon molecules- to such a small content that capillary conden- sation may ocour in between-The adsorption heats measured thus include the heat of capillary condensation, and the true adsorption heats must be still lower. From the adsorption isothermal lines and the adsorption heats, the differential adsorption entropies for n-hexane and benzene Card 2/w.