14 research outputs found
Influence of deformation on the structure and mechanical and corrosion properties of high-nitrogen austenitic 07Kh16AG13M3 steel
The correlation has been studied between the structure of a high-nitrogen austenitic Cr-Mn-N steel formed in the process of combined hardening treatment, including cold plastic deformation (CPD), and its mechanical and corrosion properties. The structure and properties of commercial high-nitrogen (0.8% N) 07Kh16AG13M3 steel is analyzed after rolling by CPD and aging at 500 and 800Β°C. It is shown that CPD of the steel occurs by dislocation slip and deformation twinning. Deformation twinning and also high resistance of austenite to martensitic transformations at true strains of 0.2 and 0.4 determine the high plasticity of the steel. The contribution of the structure imperfection parameters to the broadening of the austenite lines during CPD is estimated by X-ray diffraction. The main hardening factor is stated to be lattice microdistortions. Transmission electron microscopy study shows that heating of the deformed steel to 500Β°C leads to the formation of the intermediate CrN phase by a homogeneous mechanism, and the intermtallic Ο phase forms along the austenite grain boundaries in the case of heating at 800Β°C. After hardening by all investigated technological schemes, exception for aging at 800Β°C, the steel does not undergo pitting corrosion and is slightly prone to a stress corrosion cracking during static bending tests, while aging at 800Β°C causes pitting corrosion at a pitting formation potential Epf = -0.25 V. Β© 2013 Pleiades Publishing, Ltd
Local Corrosion of CR-Martensitic Steel Alloyed with Carbon and Nitrogen
The structure and mechanical properties of high-nitrogen martensitic steel 30X15AM were investigated. The tendency of steel to pitting and intergranular corrosion was studied by the method of metallographic analysis of the surface subjected to corrosion using the SIAMS 800 Photolab program in comparison with standard electrochemical methods. Both methods showed high resistance of steel to these types of local corrosion.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»ΠΈ ΡΡΡΡΠΊΡΡΡΡ ΠΈ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° Π²ΡΡΠΎΠΊΠΎΠ°Π·ΠΎΡΠΈΡΡΠΎΠΉ ΠΌΠ°ΡΡΠ΅Π½ΡΠΈΡΠ½ΠΎΠΉ ΡΡΠ°Π»ΠΈ 30Π₯15ΠΠ. Π‘ΠΊΠ»ΠΎΠ½Π½ΠΎΡΡΡ ΡΡΠ°Π»ΠΈ ΠΊ ΠΏΠΈΡΡΠΈΠ½Π³ΠΎΠ²ΠΎΠΉ ΠΈ ΠΌΠ΅ΠΆΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ½ΠΎΠΉ ΠΊΠΎΡΡΠΎΠ·ΠΈΠΈ ΠΈΠ·ΡΡΠ°Π»ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΠΌΠ΅ΡΠ°Π»Π»ΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ, ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π½ΡΡΠΎΠΉ ΠΊΠΎΡΡΠΎΠ·ΠΈΠΈ, Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΏΡΠΎΠ³ΡΠ°ΠΌΠΌΡ SIAMS 800 Photolab Π² ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΈ ΡΠΎ ΡΡΠ°Π½Π΄Π°ΡΡΠ½ΡΠΌΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΡ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ. ΠΠ±Π΅ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ Π²ΡΡΠΎΠΊΡΡ ΡΡΠΎΠΉΠΊΠΎΡΡΡ ΡΡΠ°Π»ΠΈ ΠΊ Π΄Π°Π½Π½ΡΠΌ Π²ΠΈΠ΄Π°ΠΌ Π»ΠΎΠΊΠ°Π»ΡΠ½ΠΎΠΉ ΠΊΠΎΡΡΠΎΠ·ΠΈΠΈ
Re-establishing glacier monitoring in Kyrgyzstan and Uzbekistan, Central Asia
Glacier mass loss is among the clearest indicators of atmospheric warming. The observation of these changes is one of the major objectives of the international climate monitoring strategy developed by the Global Climate Observing System (GCOS). Long-term glacier mass balance measurements are furthermore the basis for calibrating and validating models simulating future runoff of glacierised catchments. This is essential for Central Asia, which is one of the driest continental regions of the Northern Hemisphere. In the highly populated regions, water shortage due to decreased glacierisation potentially leads to pronounced political instability, drastic ecological changes and endangered food security. As a consequence of the collapse of the former Soviet Union, however, many valuable glacier monitoring sites in the Tien Shan and Pamir Mountains were abandoned. In recent years, multinational actors have re-established a set of important in situ measuring sites to continue the invaluable long-term data series. This paper introduces the applied monitoring strategy for selected glaciers in the Kyrgyz and Uzbek Tien Shan and Pamir, highlights the existing and the new measurements on these glaciers, and presents an example for how the old and new data can be combined to establish multi-decadal mass balance time series. This is crucial for understanding the impact of climate change on glaciers in this region
Influence of deformation on the structure and mechanical and corrosion properties of high-nitrogen austenitic 07Kh16AG13M3 steel
Snow-cover reconstruction methodology for mountainous regions based on historic in situ observations and recent remote sensing data
Spatially distributed snow-cover extent can be derived from remote sensing
data with good accuracy. However, such data are available for recent decades
only, after satellite missions with proper snow detection capabilities were
launched. Yet, longer time series of snow-cover area are usually
required, e.g., for hydrological model calibration or water availability
assessment in the past. We present a methodology to reconstruct historical
snow coverage using recently available remote sensing data and long-term
point observations of snow depth from existing meteorological stations. The
methodology is mainly based on correlations between station records and
spatial snow-cover patterns. Additionally, topography and temporal
persistence of snow patterns are taken into account. The methodology was
applied to the Zerafshan River basin in Central Asia β a very data-sparse
region. Reconstructed snow cover was cross validated against independent
remote sensing data and shows an accuracy of about 85%. The methodology
can be used in mountainous regions to overcome the data gap for earlier
decades when the availability of remote sensing snow-cover data was strongly
limited
Structure and mechanical and corrosion properties of new high-nitrogen Cr-Mn steels containing molybdenum
The structure, mechanical properties, and pitting corrosion of nickel-free high-nitrogen (0.8% N) austenitic 06Kh18AG19M2 and 07Kh16AG13M3 steels have been studied in various structural states obtained after hot deformation, quenching, and tempering at 300 and 500Β°C. Both steels are shown to be resistant to the Ξ³ β Ξ± and Ξ³ β e{open} martensite transformations irrespective of the decomposition of a Ξ³ solid solution (06Kh18AG19M2 steel). Austenite of the steel with 19 wt% Mn shows lower resistance to recrystallization, which provides its higher plasticity (Ξ΄ 5) and fracture toughness at a lower strength as compared to the steel with 13 wt% Mn. Electrochemical studies of the steels tempered at 300 and 500Β°C show that they are in a stable passive state during tests in a 3.5% NaCl solution and have high pitting resistance up to a potential E pf = 1.3-1.4 V, which is higher than that in 12Kh18N10T steel. In the quenched state, the passive state is instable but pitting formation potentials E pf retain their values. In all steels under study, pitting is shown to form predominantly along the grain boundaries of nonrecrystallized austenite. The lowest pitting resistance is demonstrated by the structure with a double grain boundary network that results from incomplete recrystallization at 1100Β°C and from the existence of initial and recrystallized austenite in the 07Kh16AG13M3 steel. To obtain a set of high mechanical and corrosion properties under given rolling conditions (1200-1150Β°C), annealing of the steels at temperatures no less than 1150Β°C (for 1 h) with water quenching and tempering at 500Β°C for 2 h are recommended. Β© 2012 Pleiades Publishing, Ltd
Mechanical and magnetic properties of high-nitrogen austenitic steel (HNS) 06H18AG19M2
Submitted by investigating the mechanical properties of focused bend testing of High-nitrogen austenitic steel (HNS) 06H18AG19M2 in air and 3.5% NaCl aqueous solution after hardening from 1150 Β°C, subsequent aging at 500 and 800 Β°C and equal channel angular pressing (ECAP) with different degrees of deformation. Also the studies of magnetic properties were conducted after different structural states of steel. It is shown that the steel is paramagnetic regardless of the mode of its processing, the exception is a state after quenching from 1200 Β° C, when detected significant spontaneous magnetization of steel in an external magnetic field.ΠΡΠΏΠΎΠ»Π½Π΅Π½Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ²ΠΎΠΉΡΡΠ² ΠΏΡΡΠ΅ΠΌ ΠΈΡΠΏΡΡΠ°Π½ΠΈΠΉ Π½Π° ΡΠΎΡΡΠ΅Π΄ΠΎΡΠΎΡΠ΅Π½Π½ΡΠΉ ΠΈΠ·Π³ΠΈΠ± Π²ΡΡΠΎΠΊΠΎΠ°Π·ΠΎΡΠΈΡΡΠΎΠΉ Π°ΡΡΡΠ΅Π½ΠΈΡΠ½ΠΎΠΉ ΡΡΠ°Π»ΠΈ (ΠΠΠ‘) 06Π₯18ΠΠ19Π2 Π½Π° Π²ΠΎΠ·Π΄ΡΡ
Π΅ ΠΈ Π² 3,5%-Π½ΠΎΠΌ Π²ΠΎΠ΄Π½ΠΎΠΌ ΡΠ°ΡΡΠ²ΠΎΡΠ΅ NaCl ΠΏΠΎΡΠ»Π΅ Π·Π°ΠΊΠ°Π»ΠΊΠΈ ΠΎΡ 1150 Β°Π‘, ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅Π³ΠΎ ΡΡΠ°ΡΠ΅Π½ΠΈΡ ΠΏΡΠΈ 500 ΠΈ 800 Β°Π‘, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠ°Π²Π½ΠΎΠΊΠ°Π½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ³Π»ΠΎΠ²ΠΎΠ³ΠΎ ΠΏΡΠ΅ΡΡΠΎΠ²Π°Π½ΠΈΡ (Π ΠΠ£Π) Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌΠΈ ΡΡΠ΅ΠΏΠ΅Π½ΡΠΌΠΈ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ. Π’Π°ΠΊΠΆΠ΅ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Ρ ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΡΠ°Π»ΠΈ Π² ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΡΡΡΠΊΡΡΡΠ½ΡΡ
ΡΠΎΡΡΠΎΡΠ½ΠΈΡΡ
. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΡΠ°Π»Ρ ΠΎΡΡΠ°Π΅ΡΡΡ ΠΏΠ°ΡΠ°ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠΉ Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΠΎ ΠΎΡ ΡΠ΅ΠΆΠΈΠΌΠ° ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ, ΠΈΡΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅ ΡΠΎΡΡΠ°Π²Π»ΡΠ΅Ρ ΡΠΎΡΡΠΎΡΠ½ΠΈΠ΅ ΠΏΠΎΡΠ»Π΅ Π·Π°ΠΊΠ°Π»ΠΊΠΈ ΠΎΡ 1200 Β°Π‘, ΠΊΠΎΠ³Π΄Π° ΠΎΠ±Π½Π°ΡΡΠΆΠΈΠ²Π°Π΅ΡΡΡ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½Π°Ρ ΡΠΏΠΎΠ½ΡΠ°Π½Π½Π°Ρ Π½Π°ΠΌΠ°Π³Π½ΠΈΡΠ΅Π½Π½ΠΎΡΡΡ ΡΡΠ°Π»ΠΈ Π²ΠΎ Π²Π½Π΅ΡΠ½Π΅ΠΌ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠΌ ΠΏΠΎΠ»Π΅
Comparison of Adsorption Coefficients of Argon, Krypton, and Xenon on Various Activated Charcoal Grades in Static Conditions
Coefficients of adsorption (Henryβs constants)
of noble
gases (argon, krypton, xenon) on activated charcoal grades AG-3, VSK-5,
SKT-3, NWC 12x40 in the temperature range of 15 Β°C to 80 Β°C
were determined. Temperature dependence parameters of Henryβs
constants were determined with a calculation of isosteric adsorption
heat values. The experimental data were used to calculate stationary
operating conditions of a radiochromatographic column in NPPβs
noble gas delay system. Out of all the studied charcoals, the results
show that coconut charcoals VSK-5 and NWC 12x40 have the highest decontamination
factor to airflow purification from radioactive noble gases. They
far outweigh sulfurβpotassium activated peat charcoal SKT-3
used presently at most Russian nuclear power plants. Activated charcoal
AG-3 does not ensure the decontamination level required. The results
also show that the overall decontamination factor depends heavily
on temperature. Precooling gas flow at the adsorberβs input
can considerably increase air decontamination factor from radioactive
noble gases
Calculation of the Henry’s Constant and the Thickness of the Equilibrium Adsorption Layer of Radon in the Layer-by-Layer Measurement of the Sorbent Activity
The radioactive gas radon is ubiquitous in the environment and is a major contributor to the human inhalation dose. It is the second leading cause of lung cancer after smoking. Radon concentrations are particularly high in the air of radon-hazardous facilities—uranium mines and radioactive waste repositories containing radium. To reduce the dose load on the staff, air in these premises should be continuously or periodically purified of radon. Carbon adsorbers can be successfully used for this purpose. The design of sorption systems requires information on both equilibrium and kinetic parameters of radon dynamic adsorption. The traditional way of obtaining such characteristics of the sorbent is to analyze the breakthrough curves. The present paper proposes a simple alternative method for determining parameters of dynamic radon adsorption (Henry’s constant and equilibrium adsorption layer thickness) from the results of a layer-by-layer gamma-spectrometric measurement of the sorbent. The analytical equation for smooth distribution of radon activity in the sorbent layer is obtained based on equilibrium adsorption layer theory for elute chromatography (pulsed injection of radon into the column). Using the dynamic adsorption of 222Rn on AG-3 activated carbon as an example, both equilibrium (Henry’s constant) and kinetic (thickness of the equilibrium adsorption layer) parameters of the adsorption dynamics were calculated. It was shown that the exposure duration of the column bed in the air flow and superficial gas velocity do not affect the result of the Henry’s constant calculation. The dependence of the equilibrium adsorption layer thickness on the superficial gas velocity over a wide range of values (5–220 cm/min) is described by the van Deemter equation. It was shown that the optimum air flow velocity, which corresponds to the maximum effectiveness of the bed, is 15–30 cm/min. This corresponds to the minimum of the equilibrium adsorption layer thickness (about 0.6 cm). The developed mathematical model makes it easy to define both equilibrium and kinetic parameters of dynamic adsorption of radon based on discrete distribution of its activity over the sections of the adsorption column. These parameters can then be used to calculate and design gas delay systems. It can be useful for studying the sorption capacity of various materials relative to radon