The pyrocarbon, gas phase densification of the catalytic carbon formations (CCFs), obtained on iron

Investigations on gas-phase densification of CCFs, obtained on iron, using the radially driven pyrolysis zone and, at the same time, the temperature rise in the pyrolysis zone with the speed of the 1.25 °С/h, were carried out. CCFs, bonded with pyrocarbon (CCFBPyC), not refined from iron, without de...

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Published in:Problems of Atomic Science and Technology
Date:2023
Main Authors: Fursov, S.G., Meltyukhov, M.V., Lyashenko, S.A.
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Language:English
Published: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2023
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Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/196113
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Cite this:The pyrocarbon, gas phase densification of the catalytic carbon formations (CCFs), obtained on iron / S.G. Fursov, M.V. Meltyukhov, S.A. Lyashenko // Problems of Atomic Science and Technology. — 2023. — № 2. — С. 153-156. — Бібліогр.: 7 назв. — англ.

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author Fursov, S.G.
Meltyukhov, M.V.
Lyashenko, S.A.
author_facet Fursov, S.G.
Meltyukhov, M.V.
Lyashenko, S.A.
citation_txt The pyrocarbon, gas phase densification of the catalytic carbon formations (CCFs), obtained on iron / S.G. Fursov, M.V. Meltyukhov, S.A. Lyashenko // Problems of Atomic Science and Technology. — 2023. — № 2. — С. 153-156. — Бібліогр.: 7 назв. — англ.
collection DSpace DC
container_title Problems of Atomic Science and Technology
description Investigations on gas-phase densification of CCFs, obtained on iron, using the radially driven pyrolysis zone and, at the same time, the temperature rise in the pyrolysis zone with the speed of the 1.25 °С/h, were carried out. CCFs, bonded with pyrocarbon (CCFBPyC), not refined from iron, without defects, with density and PyC content corresponding to the material: graphite bonded with pyrocarbon (GBPyC), which include 90 wt.% of PyC (GBPyC-90), were obtained. The necessity of applying the special technological methods in the process of gas-phase densification of CCFs, was confirmed. Досліджене газофазне ущільнення піровуглецем каталітичних утворень вуглецю (КУВ) на Fe за допомогою методу зони піролізу, що радіально рухається, з одночасним підвищенням температури в зоні піролізу зі швидкістю 1,25 ° С/год. Отримані бездефектні КУВ зв’язані піровуглецем (КУВЗП) з невидаленим каталізатором, зі щільністю і вмістом піровуглецю на рівні матеріалу: графіт, з’язаний піровуглецем, з його вмістом – 90 ваг.% (ГЗП-90). Підтверджена необхідність застосування спеціальних технологічних прийомів при ущільненні піровуглецем КУВ.
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fulltext ISSN 1562-6016. Problems of Atomic Science and Technology. 2023. №2(144) 153 https://doi.org/10.46813/2023-144-153 UDC 621.762 THE PYROCARBON, GAS PHASE DENSIFICATION OF THE CATALYTIC CARBON FORMATIONS (CCFs), OBTAINED ON IRON S.G. Fursov, M.V. Meltyukhov, S.A. Lyashenko National Science Center “Kharkov Institute of Physics and Technology”, Kharkiv, Ukraine E-mail: igor@kipt.kharkov.ua; tel./fax +38(057)349-10-61 Investigations on gas-phase densification of CCFs, obtained on iron, using the radially driven pyrolysis zone and, at the same time, the temperature rise in the pyrolysis zone with the speed of the 1.25 °С/h, were carried out. CCFs, bonded with pyrocarbon (CCFBPyC), not refined from iron, without defects, with density and PyC content corresponding to the material: graphite bonded with pyrocarbon (GBPyC), which include 90 wt.% of PyC (GBPyC- 90), were obtained. The necessity of applying the special technological methods in the process of gas-phase densifi- cation of CCFs, was confirmed. INTRODUCTION The surface structures of carbon – fullerenes, carbon nanotubes, nanofibers and nanomaterials (CNM), con- taining these structures, amorphous carbon or graphite, are, for a long time, the subject of scientific research due to their unique and often anomalously high physi- cochemical and electrical properties. The main methods for obtaining these structures are sublimation- desublimation of graphite and catalytic pyrolysis of hy- drocarbons. In the National Science Center “Kharkov Institute of Physics and Technology” (NSC KIPT), since 1982 and, for the present time, the numerous studies of the meth- ods for obtaining, properties and practical applications of catalytic carbon formations on transition metals Fe, Co, Ni, in methane or propane-butane media, at temper- atures of 600…1200 °C were carried out. CCFs were obtained in the form of powders and fi- bers, including, also, a rubber-like mass, with catalyst particles encapsulated in it and 30…40 wt.% of soot [1]. The remnants of the CCFs were preserved for the fur- ther work with them. CCFs had been mainly used for binding them with pyrocarbon (PyC), to produce the material: CCFs bonded with PyC – CCFBPyC. The CCFs, in this material, were the only filler of the PyC matrix. In the most of the experiments, it was not possi- ble to obtain an integral material, due to its brittle frac- ture. In 2020, a series of 5 experiments was carried out, to study the process of densification of the CCFs on Ni, with PyC. In these experiments it was found, that CCFs are a specific, anisotropic material, with a large (up to 50 wt.%) content of fine-fiber fraction, with a particle size of 0…50 µm, which inhibit the obtaining of a PyC matrix with sufficient strength. The results of the exper- iments, given in the article [2], indicate the necessity of taking into account the properties of СCFs and the tech- nological parameters of their densification with PyC, in order to create both CCFBPyC or a material modified with CCFs. The article presents the results of an experiment on the obtaining of the CCFBPyC on Fe. The experiment was carried out with taking into account the results of obtaining the CCFBPyC on Ni. EXPERIMENTAL PROCEDURE CCFs were obtained in the AGAT-3.2 unit, in a mo- dified “shaft furnace” ShP – ShP–A, with forced supply of methane into the furnace volume through the bottom and replacement of perforated thermal insulation with a solid one (Fig. 1), over 8 processes, with the following parameters: T in the furnace – 1180…1200 °С, duration – 6…24 h, methane consumption – 40…300 l/h. 1. Top graphite cover. 2. Carbon-carbon (C-C) or graphite rod. 3. C-C perforated heater (4 sections). 4, 10. Continuous thermal insulation, 3 layers of AT-3. 5. Temperature control hole. 6. Quartz capillary with a movable thermocouple. 7. Graphite washers for the distribution of plates along the height of the furnace. 8. Graphite or C-C plates with catalysts. 9. C-C heat-insulating stand. 11. Graphite stand. 12. Supply of methane to the furnace. Fig. 1. Scheme of shaft furnace ShP–А Methane supply was carried out through a GSB–400 counter, connected in series with a water bubbler, to saturate the gas in the furnace volume with water vapor. The maximum CCFs outgo, in the experiments, was ob- tained at the minimum consumption of methane, accord- ing to its actually laminar flow in the furnace volume. Subsequently, the laminar gas flow was used for obtain- ing a long CCFs [3]. In the experiments ShP–A7, ShP–A8, the largest number of CCFs, in the series, was generated. They were used in the creation of preform. 154 ISSN 1562-6016. Problems of Atomic Science and Technology. 2023. №2(144) OBTAINING OF THE CCFs Commercial iron sulphate: FeSO4×7H2O was used as a catalyst and a source of sulfur for the following rea- sons: – when obtaining CCFs on carbonyl iron, at T = 1100…1200 °C and introducing into the volume of the ShP furnace and into the pyrolysis chamber the sul- fur evaporation, the CCFs had the form of a fine-fibered brush. According to [4], it is known that the presence of sulfur in the reaction volume leads to the formation of precisely fibrous CCFs and not their continuous mass; – during the annealing of ferrous sulfate in the ShP furnace, iron and sulfur are formed in the environments of methane, hydrogen, carbon, namely; – according to [5], ferrous sulfate immerses the last water molecule at Т = 400 °С and at Т = 600…725 °С it decomposes into hematite Fe2О3, sulfur dioxide SO2 and oxygen O2: 2FeSO4 = Fe2О3+2SO2+1/2 O2; – hematite, in hydrogen, carbon monoxide, in the presence of carbon and T > 1000 °C is reduced to iron; – during the reduction of sulfur dioxide in methane and oxygen environments, at Т = 1200…1300 °С, sulfur is released [6]: SO2+CH4+O2 = CO2+2H2O+1/2S2; – at T > 730 °C, sulfur can be formed by the inter- ?ction of sulfur dioxide with carbon: 2C+SO2 = 2CO+1/2 S2; 2CO+SO2 = 2CO2+1/2 S2. On supported Ni catalysts, at T = 900 °C, CO can be formed by the reaction: CH4+H2O = CO+2H2. According to this equation, the gas, in the experiments, was bubbling through the water. It is well known that CCFs, obtained on iron, are segregated from its Fe3C carbide. At 1153 °С, the first liquid phase is formed in the Fe–C system from the Fe–Fe3C eutectic. The dissolution of carbon and the creation of carbide in liquid iron (compared to solid) is greatly facilitated and contributes to the growth of CCFs. At a temperature of “light red heat” iron com- bines with sulfur, forming iron sulfide FeS and at T = 998 °C a second liquid phase is created from the Fe–FeS eutectic. For the sustainable production of ССFs, it is critically important that sulfur or its dioxide be retained in the reaction volume, until FeS is formed. Therefore, the temperature rise in the ShP–A furnace was carried out as quickly as possible – in 1.5…2 h. Since the chemical analysis of sediments in the trays of the ShP–A furnace was not carried out, the statement about the participation of FeS in the creation of ССFs is only an assumption. The forced supply of methane to the ShP–A furnace was used to remove excess hydrogen, which is created during the pyrolysis of methane and leaches sulfur from the reaction space of the furnace in the form of hydro- gen sulfide. CFe in СCFs was calculated from its ash content, based on the content of Fe in Fe2O3 = 70 wt.%. The ash content was determined after the oxidation of СCFs in the air, at T = 900 °C, for 56 h. A homogeneous mass of СCFs, for a perform, was obtained by rubbing the combined СCFs from the ShP– A7–ShP–A8 experiments through a sieve with a mesh size of 1 mm. PREFORM MANUFACTURING When planning the experiment, we took into account the features of the pyrolytic densification of CCFs on Ni, described in the article [2], namely (Fig. 2): 1,7. Stands, EG-0 2. Cover, GBPyC 3. Shell - URAL-T-22 4. CCFs, Ø 70.5 mm 5. Bottom, GBPyC 6. Shell retainer 8. Thermal insulation of stands, AT - 3 9. Mo heater 10. Damper, Ø7.5mm x Ø6mm, paper on PVA 11. Buffer, URAL-T-22 Fig. 2. Scheme of the experiment 1) the preform shell – 3 was made of a single layer of carbon fabric URAL-T-22, impregnated with 50 % aqueous PVA solution, to prevent surface cracking of CCFBPyC under the action of significantly different co- efficients of linear thermal expansion (CLTE) of CCFBPyC and the shell, made of asbestos fabric. In Fig. 3, the cracking of the turned workpiece of the CCFBPyC on Ni is shown. (CNi = 2,47 wt.%, Т = 900 °С, the rate of movement of the pyrolysis zone is υPZ = 0,5 mm/h, asbestos sheath); 2) to equalize the vertical temperature gradient, stands – 1, 7 had a diameter of 50 mm, cover – 2 and bottom – 5 were made of GBPyC – to reduce the differ- ence in CLTE between them and CCFBPyC. The density of the CCFs, shaked in the preform, de- termined during the preparation to the experiment, was 0.155 g/cm 3 . At such a density, the backfilling of CCFs, obviously, has a large electrical resistance and heating of CCFs by direct current passing through them, as in esperiments with CCFs on Ni, is impossible. Therefore, the Mo preform heater – 9, Ø 6 mm was used in the ex- periment, in order to avoid the rupture of the CCFBPyC by the heater (during the perform cooling), with the damping layer of paper, applied to it, on PVA glue, Ø 7.5 mm – 10 (Fig. 4 shows the rupture of the CCFBPyC on Ni, with a Mo heater, without a damper on it (CNi = 0,67 wt.%, T = 900 °С, υPZ = 0,25 mm/h, shell made of carbon fabric URAL-T-22)). When obtaining the CCBPyC on Ni, without cracks, the CCFs, during the formation of the perform, were separated from the bottom 5 and cover 2 with the help of dampers 11, made of EG-0 graphite powder. ISSN 1562-6016. Problems of Atomic Science and Technology. 2023. №2(144) 155 Fig. 3. Superficial cracking of CCFBPyC on Ni with ground off asbestos sheath Fig. 4. Rupture of CCFBPyC on Ni with Mo heater, without a demper. The shell is made of carbon fabric URAL-T22 Table 1 CCFs and CCFBPyC parameters CCFs parameters CCFBPyC parameters diameter, mm mass, g ρFREE, g/cm 3 ρSHAKE, g/сm 3 CFe, wt.% tOXID, h ρPYCN, g/сm 3 ρHYDROST, g/сm 3 ρPYCN, g/сm 3 P, % δ PyC, µm α PyC, wt.% 70.5х7.5 109 0.099 0.155 3.21 56 1.55–1.58 1.8 1.88 4.04–4.11 5–30 91.4 Table 2 Temperature gradients in the experiment Pyrolysis zone, m 5 10 15 20 25 28 Radius from the center, mm 13 18 23 28 33 36 Т, °С 1204 1176 1150 1097 1042 1004 ΔТ, °С/mm – 5.6 5.2 10.6 11.0 12.7 This made it possible to avoid cracking of CCFBPyC under the influence of significantly different CLTR of CCFBPyC and graphite. At the shaking densi- ty of dampers made of EG-0 – 0.8 g/cm 3 and CCFs – 0.6 g/cm 3 , there was no mixing between EG-0 and CCFs. Taking into account the significant difference in the shaking densities of CCFs on Fe – 0.155 g/cm 3 (Ta- ble 1) and EG –0 – 0.6 g/cm 3 and the existence of a risk of their mixing, during the manufacturing of the pre- form, the dampers 11 (with the size of one layer – Ø 70 x Ø 8 mm) were made of carbon fabric URAL-T- 22, pre-impregnated with a 2 % aqueous solution of PVA and dried in a drying cabinet. Impregnation with a PVA solution greatly simplifies the work with the fluffing fabric and does not affect on its properties, when binding PyC. Before the experiment, the density of the shaked CCFs, was preliminarily determined. For this purpose, the bottom 5 was fixed in the shell 3 and, in the contain- er formed in this way, the density of: free backfill of the CCFs in the container and after vibro-compaction, with an external load of 1200 g, were determined. At the lower end of the Mo heater, a lower buffer 11 was formed (from fabric URAL-T-22, with the dimentions: Ø 70 x Ø 6 x30 mm) and the heater, with a buffer, was installed in the bottom 5 and a technological stand, Ø 70 mm. In the center of the height of the container was placed a paper cup for the quartz cover of the ther- mocouple, with the dimentions: Ø 10 x Ø 8 x42 mm. The cup was fixed on the side surface with tape and pressed to the heater. 109 g of CCFs were freely poured into the container and the density of their free filling was calculated. Then, the CCFs were vibro-compacted (on a technological stand) on the ‘IV-107’ vibrostand, with an external load of 1200 g applied and their density was also calculated (see Table 1). Upper buffer 11, with the dimentions: Ø 70 x Ø 8 x 38 mm, cover 2 and stand 1 were installed on top of the CCFs. The technological stand was replaced by stand 7 and the preform was placed in the AGAT-1.6 pyrolysis chamber, No. 1, for densification with PyC. The densification process in methane, with an over- pressure of 300 mm w st., was carried out according to the regime: temperature rise to 900 °C in 2 h, exposure to 900 °C for 6 h, temperature rise from 900 to 1010 °C at a rate 1.25 °C/h, with simultaneous movement of the pyrolysis zone at a speed of υPZ = 0.33 mm/h. After that there was the exposure at 1010 °C for 6 h. During the exposure, the temperature gradient was measured (Table 2). Cooling from 1010 °C to 400 °C was controlled, with an average speed of 120 °C/h. RESULTS OF THE EXPERIMENT After densification, the workpiece was turned on a 1K62 lathe to Ø 68.5 mm, the buffers (turned into car- bon–carbon composite material – CCCM) were cut off, and the Mo heater was removed. 2 pancakes, with a thickness of 5 mm, were cut from the lower end for the research. On the lower pancake, which bordered with the CCFs (Fig. 5), the cracks, opposite to the Mo heater, were found. After cutting another 20 mm from the lower end, the cracks disappeared, indicating that the CCFs, at the junction with the lower buffer, were in contact with the Mo heater. The surface cracks, that were on the Ni CCFBPyC, with an asbestos shell (see Fig. 3), were not detected. The hydrostatic (ρHYDROST), pycnometric (ρPYCN) densities and open (P) porosity were determined for the workpiece by the hydrostatic method after 4 hours boil- ing in distilled water. Content of PyC, α, was calculated by the formula: α = (ρHYDROST – ρSHAKE)/ρHYDROST×100%. The CCFs pycnometric density (ρPYCN), measured in kerosene and iron content CFe are given in the Table 1. CCFBPyC polishes were made on a grinding ma- chine and analyzed on MMP-4 microscope. A monolith- ic, almost without pores structure, with individual pores in size of 100 µm х 200 μm and metal inclusions with diameters: 100 µm, 140 µm, 240 µm, 500 μm were found on them. 156 ISSN 1562-6016. Problems of Atomic Science and Technology. 2023. №2(144) Thickness of PyC layer was 5…30 μm. There were no damage detected in the workpiece, after PyC densifi- cation and lathe turning. The appearance of the turned workpiece of the CCFBPyC is derived in Fig. 6. Fig. 6. External view of the CCFBPyC on Fe CONCLUSIONS In the conducted experiment an almost damageless workpiece of CCFBPyC, with iron present in him, low open porosity, high density and PyC content equal 91 wt.%, was obtained, in a one cycle. The PyC content in the workpiece is the same as in the CCCM, known as “GBPyC–90”, which is based on the EG-0 powder and is obtained in algorithm: PyC densification of EG-0, turning the workpiece to powder and minimun once more PyC dencification of the CCCM, up to the density of 1.8 g/cm 3 [7]. The presence of slight cracks near Mo heater, at the junction of the CCFBPyC and the lower damper, can be explained by the penetration of the CCFs to the heater through the cracks between its paper winding and the lower carbon tissue damper or when vibro-compaction, or when temperature lifting, during the preform heating for densification with PyC. In order to avoid the scatter- ing of the CCFs, it is necessary to “pull” the fabric of the separating layer between the CCF and the bottom of the perform, onto a paper damper. Application of technological techniques for receiv- ing CCFs on Ni, without defects, namely: – manufaturing of preform shell of carbon tissue; – separation of CCFs and graphite details with the damper layers; – usage of heating stands on the billets; – controlled cooling of the CCFBPyC, with a speed not higher, than 200 °C/h – allowed to obtain the same CCFBPyC on iron. The application of the dampher layer, formed with paper on the PVA glue, on the Mo heater, had allowed to avoid cracks in the material, which could be formed as a result of a significant difference between Mo and CCFBPyC CLTRs. Usage in the densification mode of the CCFs with PyC, the temperature rise, simultaneous with the movement of the pyrolysis zone, is advisable, due to the high density of the obtained CCFBPyC. The assumption on the possible participation of iron sulfide in the formation of CCFs, may be checked after a chemical analysis of the ingredients in the plates of the SP–A furnace. REFERENCES 1. V.А. Gurin, S.V. Gabelkov, N.S. Poltavtsev, I.V. Gurin, S.G. Phursov. Crystal structure of py- rographite and catalytically deposited carbon // Prob- lems of Atomic Science and Technology. Series “Physics of Radiation Effect and Radiation Materials Science” (89). 2006, N 4, p. 195-199. 2. S.G. Fursov, V.V. Guida, S.A. Lyashenko, M.V. Meltyukhov, O.S. Aulova. The investigations of a peculiarities of pyrocarbon gas phase densification of powders of the catalytic carbon formations (CCFs), ob- tained on nickel // Problems of Atomic Science and Technology. Series “Physics of Radiation Effect and Radiation Materials Science” (132). 2021, N 2, p. 100-108. 3. I.V. Gurin, B.P. Vvedenskyy, V.A. Gurin, A.N. Bukolov, S.G. Fursov. Obtaining of long length carbon catalytic formations and investigation of their biocompatibility // Biotekhnolohiia. 2011, v. 4, N 2, p. 54-60 (in Russian). 4. А.I. Kharlamov, N.V. Kyrylova. New model of carbon nanostructures forming // Coll. of works of the 8th International. conferences “Hydrogen material sci- ence and chemistry of carbon nanomaterials”, Septem- ber 14–20, 2003, Sudak, Crimea, с. 438-439. 5. Studies in the field of sulfuric acid production // Proceedings of the NIUIF, Pubp. 225, M., 1975, p. 150. 6. V.S. Arutyunov et al. Technology of hydrocar- bon gas processing: Textbook for universities. M.: “Yurat”, 2020. 7. V.N. Voyevodin, Yu.A. Gribanov, V.A. Gurin, I.V. Gurin, V.V. Guyda. Carbon-graphite materials in nuclear power (review) // Problems of Atomic Science and Technology. Series “Physics of Radiation Effect and Radiation Materials Science” (96). 2015, N 2, p. 52-64. Article received 17.03.2023 УЩІЛЬНЕННЯ ПІРОВУГЛЕЦЕМ КАТАЛІТИЧНИХ УТВОРЕНЬ ВУГЛЕЦЮ (КУВ) НА ЗАЛІЗІ С.Г. Фурсов, М.В. Мельтюхов, С.А. Ляшенко Досліджене газофазне ущільнення піровуглецем каталітичних утворень вуглецю (КУВ) на Fe за допомо- гою методу зони піролізу, що радіально рухається, з одночасним підвищенням температури в зоні піролізу зі швидкістю 1,25 °С/год. Отримані бездефектні КУВ зв'язані піровуглецем (КУВЗП) з невидаленим каталіза- тором, зі щільністю і вмістом піровуглецю на рівні матеріалу: графіт, зв'язаний піровуглецем, з його вмістом – 90 ваг.% (ГЗП-90). Підтверджена необхідність застосування спеціальних технологічних прийомів при ущільненні піровуглецем КУВ. Fig. 5. External view of the CCFBPyC sections and the pancake on the border of the CCFBPyC and lower buffer https://vant.kipt.kharkov.ua/CONTENTS/CONTENTS_2005_5.html https://vant.kipt.kharkov.ua/CONTENTS/CONTENTS_2005_5.html https://vant.kipt.kharkov.ua/CONTENTS/CONTENTS_2005_5.html https://vant.kipt.kharkov.ua/CONTENTS/CONTENTS_2005_5.html https://vant.kipt.kharkov.ua/CONTENTS/CONTENTS_2005_5.html https://vant.kipt.kharkov.ua/CONTENTS/CONTENTS_2005_5.html
id nasplib_isofts_kiev_ua-123456789-196113
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
issn 1562-6016
language English
last_indexed 2025-12-07T13:26:29Z
publishDate 2023
publisher Національний науковий центр «Харківський фізико-технічний інститут» НАН України
record_format dspace
spelling Fursov, S.G.
Meltyukhov, M.V.
Lyashenko, S.A.
2023-12-10T12:59:30Z
2023-12-10T12:59:30Z
2023
The pyrocarbon, gas phase densification of the catalytic carbon formations (CCFs), obtained on iron / S.G. Fursov, M.V. Meltyukhov, S.A. Lyashenko // Problems of Atomic Science and Technology. — 2023. — № 2. — С. 153-156. — Бібліогр.: 7 назв. — англ.
1562-6016
DOI: https://doi.org/10.46813/2023-144-153
https://nasplib.isofts.kiev.ua/handle/123456789/196113
621.762
Investigations on gas-phase densification of CCFs, obtained on iron, using the radially driven pyrolysis zone and, at the same time, the temperature rise in the pyrolysis zone with the speed of the 1.25 °С/h, were carried out. CCFs, bonded with pyrocarbon (CCFBPyC), not refined from iron, without defects, with density and PyC content corresponding to the material: graphite bonded with pyrocarbon (GBPyC), which include 90 wt.% of PyC (GBPyC-90), were obtained. The necessity of applying the special technological methods in the process of gas-phase densification of CCFs, was confirmed.
Досліджене газофазне ущільнення піровуглецем каталітичних утворень вуглецю (КУВ) на Fe за допомогою методу зони піролізу, що радіально рухається, з одночасним підвищенням температури в зоні піролізу зі швидкістю 1,25 ° С/год. Отримані бездефектні КУВ зв’язані піровуглецем (КУВЗП) з невидаленим каталізатором, зі щільністю і вмістом піровуглецю на рівні матеріалу: графіт, з’язаний піровуглецем, з його вмістом – 90 ваг.% (ГЗП-90). Підтверджена необхідність застосування спеціальних технологічних прийомів при ущільненні піровуглецем КУВ.
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Національний науковий центр «Харківський фізико-технічний інститут» НАН України
Problems of Atomic Science and Technology
Irradiation installations, diagnostic and research methods
The pyrocarbon, gas phase densification of the catalytic carbon formations (CCFs), obtained on iron
Ущільнення піровуглецем каталітичних утворень вуглецю (КУВ) на залізі
Article
published earlier
spellingShingle The pyrocarbon, gas phase densification of the catalytic carbon formations (CCFs), obtained on iron
Fursov, S.G.
Meltyukhov, M.V.
Lyashenko, S.A.
Irradiation installations, diagnostic and research methods
title The pyrocarbon, gas phase densification of the catalytic carbon formations (CCFs), obtained on iron
title_alt Ущільнення піровуглецем каталітичних утворень вуглецю (КУВ) на залізі
title_full The pyrocarbon, gas phase densification of the catalytic carbon formations (CCFs), obtained on iron
title_fullStr The pyrocarbon, gas phase densification of the catalytic carbon formations (CCFs), obtained on iron
title_full_unstemmed The pyrocarbon, gas phase densification of the catalytic carbon formations (CCFs), obtained on iron
title_short The pyrocarbon, gas phase densification of the catalytic carbon formations (CCFs), obtained on iron
title_sort pyrocarbon, gas phase densification of the catalytic carbon formations (ccfs), obtained on iron
topic Irradiation installations, diagnostic and research methods
topic_facet Irradiation installations, diagnostic and research methods
url https://nasplib.isofts.kiev.ua/handle/123456789/196113
work_keys_str_mv AT fursovsg thepyrocarbongasphasedensificationofthecatalyticcarbonformationsccfsobtainedoniron
AT meltyukhovmv thepyrocarbongasphasedensificationofthecatalyticcarbonformationsccfsobtainedoniron
AT lyashenkosa thepyrocarbongasphasedensificationofthecatalyticcarbonformationsccfsobtainedoniron
AT fursovsg uŝílʹnennâpírovuglecemkatalítičnihutvorenʹvuglecûkuvnazalízí
AT meltyukhovmv uŝílʹnennâpírovuglecemkatalítičnihutvorenʹvuglecûkuvnazalízí
AT lyashenkosa uŝílʹnennâpírovuglecemkatalítičnihutvorenʹvuglecûkuvnazalízí
AT fursovsg pyrocarbongasphasedensificationofthecatalyticcarbonformationsccfsobtainedoniron
AT meltyukhovmv pyrocarbongasphasedensificationofthecatalyticcarbonformationsccfsobtainedoniron
AT lyashenkosa pyrocarbongasphasedensificationofthecatalyticcarbonformationsccfsobtainedoniron