Pub Date : 2025-01-16DOI: 10.1134/S0040601524700630
L. B. Direktor, V. A. Sinelshchikov
A mathematical model of a high-temperature cylindrical reactor for heterogeneous pyrolysis of methane during its filtration through a moving layer formed by granules of carbonized wood is presented. The carbon matrix was modeled by spheres of the same diameter with a simple cubic packing. The carbon matrix was heated through the reactor wall. Preheated methane was fed into the lower part of the reactor. The process of pyrocarbon formation as a result of heterogeneous pyrolysis of methane was described by one gross reaction taking into account hydrogen inhibition and changes in the reaction surface. It was assumed that the rate of pyrocarbon deposition is directly proportional to the partial pressure of methane. The system of two-dimensional, nonstationary differential equations describing the operation of the reactor in a cyclic mode with periodic unloading of a portion of carbon–carbon composite and synchronous loading of carbonized wood granules was solved numerically using the DIFSUB algorithm. The reactor radius and operating parameters (specific mass flow rate of methane, carbon composite unloading frequency) were varied in calculations. Based on the obtained results, the dependences of the quality of the carbon–carbon composite (average density and maximum density spread), the composition of the hydrogen-containing gas mixture at the reactor outlet, the degree of methane conversion, the reactor productivity for carbon composite and hydrogen on the operating parameters, and the reactor radius were analyzed. Data are provided on energy consumption for heating methane and carbonized granules loaded into the reactor as well as for compensation of the endothermic effect accompanying methane pyrolysis.
{"title":"Numerical Model of a Heterogeneous Pyrolysis Reactor of Methane","authors":"L. B. Direktor, V. A. Sinelshchikov","doi":"10.1134/S0040601524700630","DOIUrl":"10.1134/S0040601524700630","url":null,"abstract":"<p>A mathematical model of a high-temperature cylindrical reactor for heterogeneous pyrolysis of methane during its filtration through a moving layer formed by granules of carbonized wood is presented. The carbon matrix was modeled by spheres of the same diameter with a simple cubic packing. The carbon matrix was heated through the reactor wall. Preheated methane was fed into the lower part of the reactor. The process of pyrocarbon formation as a result of heterogeneous pyrolysis of methane was described by one gross reaction taking into account hydrogen inhibition and changes in the reaction surface. It was assumed that the rate of pyrocarbon deposition is directly proportional to the partial pressure of methane. The system of two-dimensional, nonstationary differential equations describing the operation of the reactor in a cyclic mode with periodic unloading of a portion of carbon–carbon composite and synchronous loading of carbonized wood granules was solved numerically using the DIFSUB algorithm. The reactor radius and operating parameters (specific mass flow rate of methane, carbon composite unloading frequency) were varied in calculations. Based on the obtained results, the dependences of the quality of the carbon–carbon composite (average density and maximum density spread), the composition of the hydrogen-containing gas mixture at the reactor outlet, the degree of methane conversion, the reactor productivity for carbon composite and hydrogen on the operating parameters, and the reactor radius were analyzed. Data are provided on energy consumption for heating methane and carbonized granules loaded into the reactor as well as for compensation of the endothermic effect accompanying methane pyrolysis.</p>","PeriodicalId":799,"journal":{"name":"Thermal Engineering","volume":"71 12","pages":"1067 - 1075"},"PeriodicalIF":0.9,"publicationDate":"2025-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142994537","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-01-16DOI: 10.1134/S0040601524700605
V. V. Klimenko, A. V. Klimenko, A. G. Tereshin, O. B. Mikushina
The prospects for achieving carbon neutrality in economically developed countries that are members of the Organization for Economic Cooperation and Development (OECD) and other countries are examined. An analysis of the energy and land use structure in these countries was carried out. Scenario assessments of the dynamics of changes in carbon indicators of the study economies have been developed, and a comparison has been made with forecasts from leading global energy agencies. It has been shown that, at the current rate of decarbonization and development of the carbon capture and storage (CCS) industry, it is impossible for countries in both groups to fulfill their commitments to achieve climate neutrality in 2050–2070; this goal cannot be achieved before the end of this century. The central challenge in achieving climate neutrality is the rapid and large-scale implementation of CCS technologies in all their possible manifestations. Using a set of global climate system models, calculations of the global average temperature (GAT) were performed for the proposed scenarios, and their results were compared with other works. Despite the fact that climate change occupies almost a leading place on the global agenda, the actual results of efforts in this area are far from those declared, and it is now impossible to cap warming to within 1.5°C. The key task is to minimize the time the global climate system remains in the dangerous extreme zone (above 1.5°C), which will require the emergence of a global economy with negative greenhouse gas (GHG) emissions.
{"title":"Zero Carbon World: Is It Possible to Achieve Global Climate Neutrality?","authors":"V. V. Klimenko, A. V. Klimenko, A. G. Tereshin, O. B. Mikushina","doi":"10.1134/S0040601524700605","DOIUrl":"10.1134/S0040601524700605","url":null,"abstract":"<p>The prospects for achieving carbon neutrality in economically developed countries that are members of the Organization for Economic Cooperation and Development (OECD) and other countries are examined. An analysis of the energy and land use structure in these countries was carried out. Scenario assessments of the dynamics of changes in carbon indicators of the study economies have been developed, and a comparison has been made with forecasts from leading global energy agencies. It has been shown that, at the current rate of decarbonization and development of the carbon capture and storage (CCS) industry, it is impossible for countries in both groups to fulfill their commitments to achieve climate neutrality in 2050–2070; this goal cannot be achieved before the end of this century. The central challenge in achieving climate neutrality is the rapid and large-scale implementation of CCS technologies in all their possible manifestations. Using a set of global climate system models, calculations of the global average temperature (GAT) were performed for the proposed scenarios, and their results were compared with other works. Despite the fact that climate change occupies almost a leading place on the global agenda, the actual results of efforts in this area are far from those declared, and it is now impossible to cap warming to within 1.5°C. The key task is to minimize the time the global climate system remains in the dangerous extreme zone (above 1.5°C), which will require the emergence of a global economy with negative greenhouse gas (GHG) emissions.</p>","PeriodicalId":799,"journal":{"name":"Thermal Engineering","volume":"71 12","pages":"1025 - 1037"},"PeriodicalIF":0.9,"publicationDate":"2025-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142994674","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-01-16DOI: 10.1134/S0040601524700563
O. O. Milman, G. G. Yankov, A. V. Kondratiev, A. V. Ptakhin, V. S. Krylov, V. B. Perov, A. A. Zhinov, A. Yu. Kartuesova
Heat exchange during condensation of freons has been studied quite well; however, various flow regimes of the steam-condensate mixture may arise during condensation inside heat-exchange pipes. There is a large amount of experimental data on the condensation of freons inside pipes with different internal diameters. However, the results obtained by different authors are contradictory, and experimental dependencies can give a high error in the event of a discrepancy between the calculated and actual flow regimes of the steam-condensate mixture. Due to the difficulty of identifying these modes for each such case, reliable recommendations for the calculation and design of heat exchangers must be based on experimental data. In order to obtain such materials, an experimental stand was developed and manufactured, allowing the study of condensation processes of various working fluids in a horizontal cooled tube. The working section of the stand was a copper pipe with an external diameter of 32 mm and a wall thickness of 2 mm, built into an external steel pipe with a diameter of 45 × 3 mm with an annular gap of 3.5 mm. Five chromel-copel thermocouples were installed in the gap to measure the water temperature; they were led to the measuring instruments through the wall of the outer pipe. Thermocouples were also installed in the copper pipe wall. The stand’s thermocouples were precalibrated, and the freon and cooling water consumption was determined by the differences on the flow diaphragms with an error not exceeding 1.5%. The temperatures of cooling water and condensing freon R142b along the length of the heat-exchange pipe were obtained for some flow regimes with different parameters of the working fluid at the pipe inlet. A sharp decrease in the local heat-transfer coefficient along the length of the heat-exchange pipe during complete condensation is shown and is especially significant at its inlet section. The obtained data will be used in the design of heat exchangers with condensation of R142b freon in horizontal pipes.
{"title":"Heat Exchange Inside a Horizontal Pipe at the Initial Section with Complete Condensation of R142b Freon Vapor","authors":"O. O. Milman, G. G. Yankov, A. V. Kondratiev, A. V. Ptakhin, V. S. Krylov, V. B. Perov, A. A. Zhinov, A. Yu. Kartuesova","doi":"10.1134/S0040601524700563","DOIUrl":"10.1134/S0040601524700563","url":null,"abstract":"<p>Heat exchange during condensation of freons has been studied quite well; however, various flow regimes of the steam-condensate mixture may arise during condensation inside heat-exchange pipes. There is a large amount of experimental data on the condensation of freons inside pipes with different internal diameters. However, the results obtained by different authors are contradictory, and experimental dependencies can give a high error in the event of a discrepancy between the calculated and actual flow regimes of the steam-condensate mixture. Due to the difficulty of identifying these modes for each such case, reliable recommendations for the calculation and design of heat exchangers must be based on experimental data. In order to obtain such materials, an experimental stand was developed and manufactured, allowing the study of condensation processes of various working fluids in a horizontal cooled tube. The working section of the stand was a copper pipe with an external diameter of 32 mm and a wall thickness of 2 mm, built into an external steel pipe with a diameter of 45 × 3 mm with an annular gap of 3.5 mm. Five chromel-copel thermocouples were installed in the gap to measure the water temperature; they were led to the measuring instruments through the wall of the outer pipe. Thermocouples were also installed in the copper pipe wall. The stand’s thermocouples were precalibrated, and the freon and cooling water consumption was determined by the differences on the flow diaphragms with an error not exceeding 1.5%. The temperatures of cooling water and condensing freon R142b along the length of the heat-exchange pipe were obtained for some flow regimes with different parameters of the working fluid at the pipe inlet. A sharp decrease in the local heat-transfer coefficient along the length of the heat-exchange pipe during complete condensation is shown and is especially significant at its inlet section. The obtained data will be used in the design of heat exchangers with condensation of R142b freon in horizontal pipes.</p>","PeriodicalId":799,"journal":{"name":"Thermal Engineering","volume":"71 12","pages":"1061 - 1066"},"PeriodicalIF":0.9,"publicationDate":"2025-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142994594","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-01-16DOI: 10.1134/S0040601524700599
R. V. Akulich, N. V. Arzhinovskaya
Currently, power facilities that operate turbine lubrication and control systems using fire-resistant oil only use fire-resistant fluids from foreign manufacturers (Reolube-OMTI, Reolube 46RS, and Fyrquel-L). The impossibility of domestic production of fire-resistant oil is connected with the loss of a special industrial raw material base in Russia in the 1990s. Restoring the entire technological cycle is not a matter for the immediate future. To maintain the operational readiness of oils used in process equipment, extend their service life, and reduce the volume of replacement, it is necessary to organize a high-quality cleaning process. For this purpose, the All-Russia Thermal Engineering Research Institute developed technology for the comprehensive cleaning of fire-resistant liquids and created equipment for its implementation at energy facilities. The results are presented of the analysis of complex cleaning and restoration of oils with their draining from the oil system and “on the go.” The quality indicators of the oils in both variants have been significantly improved—the acid number, deaeration and demulsification time, moisture content, and corrosive aggressiveness of the oil have been reduced, the industrial purity class has been lowered, etc.—and values for individual indicators have been achieved that meet the requirements for fresh oils. It has been shown that it is advisable to carry out complex oil cleaning “on the go,” which helps to clean the oil system from accumulated deposits due to the simultaneously occurring process of sludge dissolution and also allows to significantly reduce the rate of degradation of the restored oil under operating conditions.
{"title":"Implementation Results for the Technology of Comprehensive Purification of Fire-Resistant Oils","authors":"R. V. Akulich, N. V. Arzhinovskaya","doi":"10.1134/S0040601524700599","DOIUrl":"10.1134/S0040601524700599","url":null,"abstract":"<p>Currently, power facilities that operate turbine lubrication and control systems using fire-resistant oil only use fire-resistant fluids from foreign manufacturers (Reolube-OMTI, Reolube 46RS, and Fyrquel-L). The impossibility of domestic production of fire-resistant oil is connected with the loss of a special industrial raw material base in Russia in the 1990s. Restoring the entire technological cycle is not a matter for the immediate future. To maintain the operational readiness of oils used in process equipment, extend their service life, and reduce the volume of replacement, it is necessary to organize a high-quality cleaning process. For this purpose, the All-Russia Thermal Engineering Research Institute developed technology for the comprehensive cleaning of fire-resistant liquids and created equipment for its implementation at energy facilities. The results are presented of the analysis of complex cleaning and restoration of oils with their draining from the oil system and “on the go.” The quality indicators of the oils in both variants have been significantly improved—the acid number, deaeration and demulsification time, moisture content, and corrosive aggressiveness of the oil have been reduced, the industrial purity class has been lowered, etc.—and values for individual indicators have been achieved that meet the requirements for fresh oils. It has been shown that it is advisable to carry out complex oil cleaning “on the go,” which helps to clean the oil system from accumulated deposits due to the simultaneously occurring process of sludge dissolution and also allows to significantly reduce the rate of degradation of the restored oil under operating conditions.</p>","PeriodicalId":799,"journal":{"name":"Thermal Engineering","volume":"71 12","pages":"1094 - 1100"},"PeriodicalIF":0.9,"publicationDate":"2025-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142994536","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-01-16DOI: 10.1134/S0040601524700587
S. V. Kiseleva, N. I. Chernova, M. S. Vlaskin, A. V. Grigorenko, E. A. Chunzhuk, S. Ya. Malaniy, E. A. Bakumenko, T. V. Rositskaya
Reducing greenhouse gas emissions remains a topical issue in fundamental and applied scientific research, including in terms of analyzing developed and applied CO2 capture technologies. The main focus is on methods of carbon dioxide burial in stable geological formations, absorption, filtration, etc. The absorption of carbon dioxide during photosynthesis is usually associated with terrestrial biota, although aquatic organisms have a higher productivity of photosynthesis. The use of microalgae as photosynthetic agents is determined mainly by their value for obtaining high-quality food and feed additives, pharmaceutical products, and biofuels, but it is important to consider their effectiveness in the associated absorption of CO2. When producing products with a long carbon sequestration period, this method can be included in the list of effective carbon capture technologies. To estimate the specific energy costs for CO2 absorption, proven cultivation methods were considered: open-plane cultivators (microalgae Arthrospira platensis, growth rate from 20 to 40 g/m2 per day on dry matter) and cylindrical closed photobioreactors (microalgae Chlorella vulgaris, growth rate 0.7 g/dm3 per day in dry matter). Based on experimental results of microalgae cultivation under conditions of elevated CO2 concentrations, it is shown that specific energy consumption is in the range from 27 to 768 GJ/t when cultivating A. platensis microalgae and from 59 to 373 GJ/t in microalgae cultivation of C. vulgaris. The greatest energy costs are required for heating and lighting microalgae plantations as well as for separating biomass from the culture liquid for microalgae with small cell sizes. Specific energy consumption can be reduced by maximizing the use of natural light and waste heat from industrial facilities and optimizing biomass collection systems.
{"title":"Carbon Dioxide Absorption by Microalgae: Analysis of Technologies and Energy Costs","authors":"S. V. Kiseleva, N. I. Chernova, M. S. Vlaskin, A. V. Grigorenko, E. A. Chunzhuk, S. Ya. Malaniy, E. A. Bakumenko, T. V. Rositskaya","doi":"10.1134/S0040601524700587","DOIUrl":"10.1134/S0040601524700587","url":null,"abstract":"<p>Reducing greenhouse gas emissions remains a topical issue in fundamental and applied scientific research, including in terms of analyzing developed and applied CO<sub>2</sub> capture technologies. The main focus is on methods of carbon dioxide burial in stable geological formations, absorption, filtration, etc. The absorption of carbon dioxide during photosynthesis is usually associated with terrestrial biota, although aquatic organisms have a higher productivity of photosynthesis. The use of microalgae as photosynthetic agents is determined mainly by their value for obtaining high-quality food and feed additives, pharmaceutical products, and biofuels, but it is important to consider their effectiveness in the associated absorption of CO<sub>2</sub>. When producing products with a long carbon sequestration period, this method can be included in the list of effective carbon capture technologies. To estimate the specific energy costs for CO<sub>2</sub> absorption, proven cultivation methods were considered: open-plane cultivators (microalgae <i>Arthrospira platensis,</i> growth rate from 20 to 40 g/m<sup>2</sup> per day on dry matter) and cylindrical closed photobioreactors (microalgae <i>Chlorella vulgaris</i>, growth rate 0.7 g/dm<sup>3</sup> per day in dry matter). Based on experimental results of microalgae cultivation under conditions of elevated CO<sub>2</sub> concentrations, it is shown that specific energy consumption is in the range from 27 to 768 GJ/t when cultivating <i>A. platensis</i> microalgae and from 59 to 373 GJ/t in microalgae cultivation of <i>C. vulgaris</i>. The greatest energy costs are required for heating and lighting microalgae plantations as well as for separating biomass from the culture liquid for microalgae with small cell sizes. Specific energy consumption can be reduced by maximizing the use of natural light and waste heat from industrial facilities and optimizing biomass collection systems.</p>","PeriodicalId":799,"journal":{"name":"Thermal Engineering","volume":"71 12","pages":"1038 - 1048"},"PeriodicalIF":0.9,"publicationDate":"2025-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142994554","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-01-16DOI: 10.1134/S0040601524700575
D. A. Ognerubov, Ya. I. Listratov
The effect of dimensionless operating parameters (Reynolds (Re) and Prandtl (Pr) numbers) on the dimensionless heat-transfer coefficient (Nusselt (Nu) number) is examined in a liquid metal flow in a round tube. The Nu number dependences at Pr ( ll ) 1 (liquid metals) are often presented as Nu = f (Pe), where Pe = Re Pr is the Peclet number. The simplified dependence for Nu relies very much on the fact that determination of the dependence Nu = f (Re, Pr) from the experiments with liquid metal coolants is a challenging matter since such experiments involve great difficulties. Moreover, the measurement error in in such experiments is 10–20% or higher, which is comparable with the deviation of the Nusselt number under the effect of the Prandtl number. In addition, when making experiments under earthly environment conditions, the effect of natural convection on the experimental results cannot be eliminated. In this work, to study the dependence of the Nusselt number on the Prandtl number, a series of calculations of a liquid metal flow in a round tube at a constant Peclet number was performed using the direct numerical simulation (DNS) technique. The predictions demonstrate an increase in the Nusselt number by approximately 10% as the Prandtl number drops from Pr = 0.025 (mercury) to Pr = 0.005 (liquid sodium) at Pe = 125. The influence of the Pr number on the Nu number decreases (in percentage terms) as the Pe number increases.
{"title":"An Investigation into the Effect of Prandtl Number on Heat Transfer in a Liquid Metal Flow in a Round Tube at a Constant Peclet Number","authors":"D. A. Ognerubov, Ya. I. Listratov","doi":"10.1134/S0040601524700575","DOIUrl":"10.1134/S0040601524700575","url":null,"abstract":"<p>The effect of dimensionless operating parameters (Reynolds (Re) and Prandtl (Pr) numbers) on the dimensionless heat-transfer coefficient (Nusselt (Nu) number) is examined in a liquid metal flow in a round tube. The Nu number dependences at Pr <span>( ll )</span> 1 (liquid metals) are often presented as Nu = <i>f</i> (Pe), where Pe = Re Pr is the Peclet number. The simplified dependence for Nu relies very much on the fact that determination of the dependence Nu = <i>f</i> (Re, Pr) from the experiments with liquid metal coolants is a challenging matter since such experiments involve great difficulties. Moreover, the measurement error in in such experiments is 10–20% or higher, which is comparable with the deviation of the Nusselt number under the effect of the Prandtl number. In addition, when making experiments under earthly environment conditions, the effect of natural convection on the experimental results cannot be eliminated. In this work, to study the dependence of the Nusselt number on the Prandtl number, a series of calculations of a liquid metal flow in a round tube at a constant Peclet number was performed using the direct numerical simulation (DNS) technique. The predictions demonstrate an increase in the Nusselt number by approximately 10% as the Prandtl number drops from Pr = 0.025 (mercury) to Pr = 0.005 (liquid sodium) at Pe = 125. The influence of the Pr number on the Nu number decreases (in percentage terms) as the Pe number increases.</p>","PeriodicalId":799,"journal":{"name":"Thermal Engineering","volume":"71 12","pages":"1076 - 1082"},"PeriodicalIF":0.9,"publicationDate":"2025-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142994597","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-01-16DOI: 10.1134/S0040601524700551
S. V. Tsaun, A. A. Butov, I. A. Klimonov, E. V. Moiseenko, N. A. Mosunova, V. F. Strizhov, E. V. Usov, V. I. Chukhno
For substantiating liquid metal cooled reactor plants, the EUCLID/V2 integrated code is being developed, and its verification and validation are carried out for certifying it at the Scientific and Technical Center for Nuclear and Radiation Safety (NTC NRB). One of the integrated code’s main parts is the severe accident block, which includes the SAFR module for calculating the destruction of fuel pins, fuel assemblies (FAs) and the entire core, as well as the HEFEST-FR module for calculating the melt retention and cooling down in the sodium-cooled reactor core catcher. The HEFEST-FR module implements the possibility to perform 2D simulation of the structural elements and fuel melt behavior in liquid metal cooled reactors. In accordance with the NTC NRB requirements, for the HEFEST-FR module to be used as part of the EUCLID/V2 code for analyzing the safety of fast reactors, it must be validated with the use of available experimental data; the validation shall be accompanied with an uncertainty and sensitivity analysis and assessment of the calculation result error. The article presents the results obtained from verification of the EUCLID/V2 integrated code HEFEST-FR module through solving the analytical problem of settling a stationary temperature of a homogeneous bounded cylinder uniformly heated from below with boundary conditions of the third kind and through solving the Stefan single-phase problem, as well as the results of validating the HEFEST-FR module based on the SCARABEE BF1 experiment. It is shown that the average absolute value by which the numerical calculation deviates from the analytical solution of the problem of settling a stationary temperature of a homogeneous bounded cylinder uniformly heated from below with boundary conditions of the third kind makes approximately 1.1 K. The maximum relative deviation of the results of calculations carried out using the computer program from the results of analytical solution of the Stefan problem (determination of the melt front) makes 0.46%. An assessment of the errors of modeling using the melt retention module as part of the EUCLID/V2 code (HEFEST-FR) based on the BF1 test of the SCARABEE experiment has shown that the temperature calculation error lies in the interval [‒82.3; 182.5] K, and the error of calculating the radial heat flux lies in the interval [‒55.2; 31.2] kW/m2.
{"title":"Verification and Validation of the EUCLID/V2 Integrated Code’s HEFEST-FR Module","authors":"S. V. Tsaun, A. A. Butov, I. A. Klimonov, E. V. Moiseenko, N. A. Mosunova, V. F. Strizhov, E. V. Usov, V. I. Chukhno","doi":"10.1134/S0040601524700551","DOIUrl":"10.1134/S0040601524700551","url":null,"abstract":"<p>For substantiating liquid metal cooled reactor plants, the EUCLID/V2 integrated code is being developed, and its verification and validation are carried out for certifying it at the Scientific and Technical Center for Nuclear and Radiation Safety (NTC NRB). One of the integrated code’s main parts is the severe accident block, which includes the SAFR module for calculating the destruction of fuel pins, fuel assemblies (FAs) and the entire core, as well as the HEFEST-FR module for calculating the melt retention and cooling down in the sodium-cooled reactor core catcher. The HEFEST-FR module implements the possibility to perform 2D simulation of the structural elements and fuel melt behavior in liquid metal cooled reactors. In accordance with the NTC NRB requirements, for the HEFEST-FR module to be used as part of the EUCLID/V2 code for analyzing the safety of fast reactors, it must be validated with the use of available experimental data; the validation shall be accompanied with an uncertainty and sensitivity analysis and assessment of the calculation result error. The article presents the results obtained from verification of the EUCLID/V2 integrated code HEFEST-FR module through solving the analytical problem of settling a stationary temperature of a homogeneous bounded cylinder uniformly heated from below with boundary conditions of the third kind and through solving the Stefan single-phase problem, as well as the results of validating the HEFEST-FR module based on the SCARABEE BF1 experiment. It is shown that the average absolute value by which the numerical calculation deviates from the analytical solution of the problem of settling a stationary temperature of a homogeneous bounded cylinder uniformly heated from below with boundary conditions of the third kind makes approximately 1.1 K. The maximum relative deviation of the results of calculations carried out using the computer program from the results of analytical solution of the Stefan problem (determination of the melt front) makes 0.46%. An assessment of the errors of modeling using the melt retention module as part of the EUCLID/V2 code (HEFEST-FR) based on the BF1 test of the SCARABEE experiment has shown that the temperature calculation error lies in the interval [‒82.3; 182.5] K, and the error of calculating the radial heat flux lies in the interval [‒55.2; 31.2] kW/m<sup>2</sup>.</p>","PeriodicalId":799,"journal":{"name":"Thermal Engineering","volume":"71 12","pages":"1083 - 1093"},"PeriodicalIF":0.9,"publicationDate":"2025-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142994598","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-01-16DOI: 10.1134/S0040601524700617
B. A. Shifrin, O. O. Mil’man, A. S. Goldin, V. B. Perov
Various design versions of the rotor of hydro-steam turbines (HSTs) and their application fields are reviewed. It is shown that the design with nozzles arranged over the periphery has certain shortcomings resulting in a decreased energy efficiency, including a thermodynamically unjustified increase of pressure at the nozzle inlet, which results in excessively high velocities in the nozzle “throat,” a short period of time for which the evaporating medium resides in the nozzle divergent part, and poor aerodynamic characteristics of the peripheral area, which cause increased friction losses during the impeller rotation in a two-phase medium. A hydro-steam turbine impeller design with helical nozzle-channels is proposed. Such design has features that create prerequisites for increasing the turbine efficiency, including a longer time for which the medium resides in the nozzle, a possibility to obtain aerodynamically smooth lateral and peripheral surfaces of the impeller, and better conditions for moisture separation from the medium surrounding the rotating impeller. The conditions under which superheated water enters the impeller are considered, and statements on shaping the impeller profile part are formulated. A procedure for determining the nozzle-channel divergent part’s camber line shape is proposed proceeding from the minimal force interaction between the liquid phase fragments and channel walls. An algorithm for determining the areas of the channel divergent part’s cross sections when the velocity increase and pressure decrease patterns become monotonic in nature as the flow moves from the inlet to the outlet is developed. A solid-state 3D model of the HST four-nozzle impeller obtained in designing the turbine is presented.
{"title":"Design Calculation and Shaping of the Hydro-Steam Turbine Flow Path with Helical Nozzles","authors":"B. A. Shifrin, O. O. Mil’man, A. S. Goldin, V. B. Perov","doi":"10.1134/S0040601524700617","DOIUrl":"10.1134/S0040601524700617","url":null,"abstract":"<p>Various design versions of the rotor of hydro-steam turbines (HSTs) and their application fields are reviewed. It is shown that the design with nozzles arranged over the periphery has certain shortcomings resulting in a decreased energy efficiency, including a thermodynamically unjustified increase of pressure at the nozzle inlet, which results in excessively high velocities in the nozzle “throat,” a short period of time for which the evaporating medium resides in the nozzle divergent part, and poor aerodynamic characteristics of the peripheral area, which cause increased friction losses during the impeller rotation in a two-phase medium. A hydro-steam turbine impeller design with helical nozzle-channels is proposed. Such design has features that create prerequisites for increasing the turbine efficiency, including a longer time for which the medium resides in the nozzle, a possibility to obtain aerodynamically smooth lateral and peripheral surfaces of the impeller, and better conditions for moisture separation from the medium surrounding the rotating impeller. The conditions under which superheated water enters the impeller are considered, and statements on shaping the impeller profile part are formulated. A procedure for determining the nozzle-channel divergent part’s camber line shape is proposed proceeding from the minimal force interaction between the liquid phase fragments and channel walls. An algorithm for determining the areas of the channel divergent part’s cross sections when the velocity increase and pressure decrease patterns become monotonic in nature as the flow moves from the inlet to the outlet is developed. A solid-state 3D model of the HST four-nozzle impeller obtained in designing the turbine is presented.</p>","PeriodicalId":799,"journal":{"name":"Thermal Engineering","volume":"71 12","pages":"1049 - 1060"},"PeriodicalIF":0.9,"publicationDate":"2025-01-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142994555","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-11-22DOI: 10.1134/S0040601524700496
D. S. Sinitsyn, D. A. Nazarov, N. A. Mosunova, A. A. Sorokin
A description is given of the model of formation of iodine oxide nanoparticles in the volume of the containment of a nuclear reactor during radiation-chemical reactions and clustering with subsequent formation of nanoparticles. The results of test calculations are presented. Nanoparticles of radioactive iodine oxides pose a potential hazard as a source of long-term radiation exposure to NPP personnel. They also penetrate outside the power plant through the air-ventilation system even if the enclosure remains sealed. In addition, calculations have shown that the formation of radioactive iodine oxide nanoparticles is closely related to the formation of volatile iodine compounds in the gas phase. Moreover, the intensity of formation of the latter depends significantly on air humidity. The main feature of the proposed model is the consideration of the kinetics of phenomena for processes in both the gas and aerosol phases when exposed to ionizing radiation on oxygen and water vapor in the air. The main result of the calculations is confirmation of the fundamental possibility of the formation of aerosol nanoparticles consisting of iodine oxides in a humid atmosphere even with a relatively low dose rate of radiation energy absorbed by the air. At the same time, radiolysis of water vapor has a weak effect on the size and concentration of iodine oxide nanoparticles. However, taking into account the chemical interaction of radiolysis products, in particular hydrogen radicals, induced by water vapor radiolysis, significantly affects the formation of volatile iodine compounds with hydrogen: HI and HOI. The obtained results, despite their preliminary nature, are important since they indicate the inevitability of the formation of suspended nanoparticles of iodine oxides and hydrogen iodide in the atmosphere of the reactor premises in the event of emergency situations with the release of radionuclides beyond the first circuit of the reactor. Therefore, this mechanism must be taken into account when developing models of the formation and behavior of fission product aerosols at NPPs.
{"title":"Model for the Formation of Iodine Oxide Nanoparticles within the Reactor Containment","authors":"D. S. Sinitsyn, D. A. Nazarov, N. A. Mosunova, A. A. Sorokin","doi":"10.1134/S0040601524700496","DOIUrl":"10.1134/S0040601524700496","url":null,"abstract":"<p>A description is given of the model of formation of iodine oxide nanoparticles in the volume of the containment of a nuclear reactor during radiation-chemical reactions and clustering with subsequent formation of nanoparticles. The results of test calculations are presented. Nanoparticles of radioactive iodine oxides pose a potential hazard as a source of long-term radiation exposure to NPP personnel. They also penetrate outside the power plant through the air-ventilation system even if the enclosure remains sealed. In addition, calculations have shown that the formation of radioactive iodine oxide nanoparticles is closely related to the formation of volatile iodine compounds in the gas phase. Moreover, the intensity of formation of the latter depends significantly on air humidity. The main feature of the proposed model is the consideration of the kinetics of phenomena for processes in both the gas and aerosol phases when exposed to ionizing radiation on oxygen and water vapor in the air. The main result of the calculations is confirmation of the fundamental possibility of the formation of aerosol nanoparticles consisting of iodine oxides in a humid atmosphere even with a relatively low dose rate of radiation energy absorbed by the air. At the same time, radiolysis of water vapor has a weak effect on the size and concentration of iodine oxide nanoparticles. However, taking into account the chemical interaction of radiolysis products, in particular hydrogen radicals, induced by water vapor radiolysis, significantly affects the formation of volatile iodine compounds with hydrogen: HI and HOI. The obtained results, despite their preliminary nature, are important since they indicate the inevitability of the formation of suspended nanoparticles of iodine oxides and hydrogen iodide in the atmosphere of the reactor premises in the event of emergency situations with the release of radionuclides beyond the first circuit of the reactor. Therefore, this mechanism must be taken into account when developing models of the formation and behavior of fission product aerosols at NPPs.</p>","PeriodicalId":799,"journal":{"name":"Thermal Engineering","volume":"71 11","pages":"941 - 949"},"PeriodicalIF":0.9,"publicationDate":"2024-11-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142679736","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-11-22DOI: 10.1134/S0040601524700502
G. V. Tomarov, V. N. Lovchev, A. F. Gromov, A. A. Shipkov
Operation of nuclear power plant units is accompanied by the development of various metal degradation mechanisms (MDM) under the influence of the working environment. Prevention of damage and elimination of sudden destruction of equipment and pipelines (E&P) at operating nuclear power plants depends on the timely identification of those elements and units in which the preconditions for the manifestation and intensification of metal degradation mechanisms are created. In this case, the search for the causes of damage to pipeline lines and equipment parts should be based on the determination of the dominant MDM. The effectiveness of the technical measures being developed to restore and prevent similar damage in the future depends on the correct solution to these problems. Despite significant experience and accumulated statistical data on damage to the metal of the working contours of nuclear power plant units, the establishment of identification features and the detection of dominant MDM in the operating conditions of turbine installations of nuclear power plant units remain highly relevant. This is confirmed by the existing differences in approaches to the classification of MDM and the lack of a clear methodology for their identification when detecting defects and analyzing cases of damage to pipeline elements and equipment. Due to the complexity of the physical and chemical processes and patterns of MDM, their deep and fairly large-scale study is required; therefore, as a rule, the study of a specific MDM is carried out by separate specialized scientific organizations and institutes. This circumstance makes it difficult to form a unified approach to their systematization and classification in order to obtain a complete picture of the dominant mechanisms of damage to E&P turbine installations of nuclear power plant units. At the same time, the achievements of recent years in this area make it possible to formulate more advanced criteria and recommendations for classification and identification of MDM, which are advisable to use in practice, including in the development of industry guidance documentation on this topic.
{"title":"Mechanisms of Metal Degradation in Equipment and Pipelines of Turbo Plants of Nuclear Power Plant Units: Classification and Identification","authors":"G. V. Tomarov, V. N. Lovchev, A. F. Gromov, A. A. Shipkov","doi":"10.1134/S0040601524700502","DOIUrl":"10.1134/S0040601524700502","url":null,"abstract":"<p>Operation of nuclear power plant units is accompanied by the development of various metal degradation mechanisms (MDM) under the influence of the working environment. Prevention of damage and elimination of sudden destruction of equipment and pipelines (E&P) at operating nuclear power plants depends on the timely identification of those elements and units in which the preconditions for the manifestation and intensification of metal degradation mechanisms are created. In this case, the search for the causes of damage to pipeline lines and equipment parts should be based on the determination of the dominant MDM. The effectiveness of the technical measures being developed to restore and prevent similar damage in the future depends on the correct solution to these problems. Despite significant experience and accumulated statistical data on damage to the metal of the working contours of nuclear power plant units, the establishment of identification features and the detection of dominant MDM in the operating conditions of turbine installations of nuclear power plant units remain highly relevant. This is confirmed by the existing differences in approaches to the classification of MDM and the lack of a clear methodology for their identification when detecting defects and analyzing cases of damage to pipeline elements and equipment. Due to the complexity of the physical and chemical processes and patterns of MDM, their deep and fairly large-scale study is required; therefore, as a rule, the study of a specific MDM is carried out by separate specialized scientific organizations and institutes. This circumstance makes it difficult to form a unified approach to their systematization and classification in order to obtain a complete picture of the dominant mechanisms of damage to E&P turbine installations of nuclear power plant units. At the same time, the achievements of recent years in this area make it possible to formulate more advanced criteria and recommendations for classification and identification of MDM, which are advisable to use in practice, including in the development of industry guidance documentation on this topic.</p>","PeriodicalId":799,"journal":{"name":"Thermal Engineering","volume":"71 11","pages":"991 - 1005"},"PeriodicalIF":0.9,"publicationDate":"2024-11-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142679570","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}