105 research outputs found
Increase in Intake Capacity by Dynamic Operation of Injection Wells
The method of pumping water to compensate for fluid withdrawals from an oil formation in order to maintain formation pressure has long established itself as an effective technology and is widely used at oil and gas fields. At the same time, field operator is often faced with the problem of reduction in the intake capacity of injection wells, which may be caused by various complications arising in the near-wellbore area due to a violation of water treatment technology or other factors. This problem is typical for reservoirs with low permeability values, which leads to a decrease in the performance indicators of the formation pressure maintenance system.
In order to counter contamination of the bottomhole zone of the well, as a rule, injection of specialized acid compositions for the purpose of cleaning is used. To increase the effectiveness of this procedure, the authors of the article propose to discharge the injection well at the maximum permissible speeds. This event will allow primary cleaning of the bottomhole zone of the formation from moving particles clogging the pore space, and reduce formation pressure in the vicinity of the injection well, which will subsequently improve the intake capacity of the well during treatment with acid compositions. The decrease in formation pressure in the bottomhole zone of the well also has a positive effect on the radius of acid penetration into the formation.
The proposed approach has been successfully tested on a number of injection wells at one of «Gazprom Neft» enterprises. The results of pilot operations showed an increase in the quality of cleaning the bottomhole zone of the formation and an increase in the intake capacity of injection wells with subsequent preservation of intake dynamics
Electromagnetic response of the three-layer construction on the basis of barium hexaferrite and a foam glass
This paper contains results of study of the frequency dependence of reflection coefficient of the ceramic surface coated with the construction consisting of following layers: metal, composite on the basis of ferrite with hexagonal structure, and foam glass. It is shown that foam glass layer reduces significantly the reflecting characteristics of the construction
Radiation-thermal synthesis of W-type hexaferrites
The results of investigations of the phase composition, structural parameters, static and dynamic magnetic properties of BaCo0.7Zn1.3Fe16O27 hexaferrites obtained by the method of self-propagation high-temperature synthesis in combination with mechanochemical activation and radiation-thermal post-sintering are presented. The prospects of the proposed energy-saving approach for the production of ferrite ceramics with a hexagonal structure is shown
Electromagnetic properties of LaCa[3]Fe[5]O[12] in the microwave range
The X-ray diffraction analysis of the LaCa[3]Fe[5]O[12] ferrite (lanthanum ferrite) prepared through high-temperature synthesis via ceramic technology was performed. It was found that ferrites belong to tetragonal system. The electromagnetic response from a flat layer of the composite based on this material under electromagnetic radiation in the frequency range of 0.01-18 GHz was investigated. It is shown that the developed material effectively interacts with electromagnetic radiation. The interaction effectiveness is directly proportional to ferrite concentration. Increased concentration of ferrite leads to growth of the reflection coefficient due to high conductivity of the material and visible decrease in the transmission coefficient in the frequency range of 4-14 GHz
Carbon Supported Polyaniline as Anode Catalyst: Pathway to Platinum-Free Fuel Cells
The effectiveness of carbon supported polyaniline as anode catalyst in a fuel
cell (FC) with direct formic acid electrooxidation is experimentally
demonstrated. A prototype FC with such a platinum-free composite anode
exhibited a maximum room-temperature specific power of about 5 mW/cm2Comment: 11 pages, 3 Postscript figures, atricle tex styl
ĐĄĐžĐœŃДз, ŃŃŃŃĐșŃŃŃĐ° Đž ŃлДĐșŃŃĐŸĐŒĐ°ĐłĐœĐžŃĐœŃĐ” ŃĐČĐŸĐčŃŃĐČĐ° ĐœĐ°ĐœĐŸĐșĐŸĐŒĐżĐŸĐ·ĐžŃĐŸĐČ FeCoCu/C
FeCoCu ternary nanoparticles distributed and stabilized in the carbon matrix of FeCoCu/C metal-carbon nanocomposites have been synthesized using controlled IR pyrolysis of precursors consisting of the âpolymer / iron acetylacetate / cobalt and copper acetatesâ type system obtained by joint dissolution of components followed by solvent removal. The effect of the synthesis temperature on the structure, composition and electromagnetic properties of the nanocomposites has been studied. By XRD was shown that the formation of the FeCoCu ternary nanoparticles occurs due to the interaction of Fe3ĐĄ with the nanoparticles of the CoCu solid solution. An increase in the synthesis temperature leads to an increase in the size of the metal nanoparticles due to their agglomeration and coalescence as a result of matrix reconstruction. Furthermore, ternary alloy nanoparticles having a variable composition may form depending on the synthesis temperature and the content ratio of the metals. Raman spectroscopy has shown that the crystallinity of the carbon matrix of the nanocomposites increases with the synthesis temperature. The frequency responses of the relative permittivity and permeability of the nanocomposites have been studied at 3â13 GHz. It has been shown that a change in the content ratio of the metals noticeably increases both the dielectric and the magnetic losses. The former loss is caused by the formation of a complex nanostructure of the nanocomposite carbon matrix while the latter one originates from an increase in the size of the nanoparticles and a shift of the natural ferromagnetic resonance frequency to the low-frequency region. The reflection loss has been calculated using a standard method from the experimental data on the frequency responses of the relative permittivity and permeability. It has been shown that the frequency range and the absorption of electromagnetic waves (from â20 to â52 dB) can be controlled by varying the content ratio of the metals in the precursor. The nanocomposites obtained as a result of the experiment deliver better results in comparison with FeCo/C nanocomposites synthesized under similar conditions.ĐĄĐžĐœŃДзОŃĐŸĐČĐ°ĐœŃ ŃŃĐŸĐčĐœŃĐ” ĐœĐ°ĐœĐŸŃĐ°ŃŃĐžŃŃ FeCoCu, ŃĐ°ŃĐżŃĐ”ĐŽĐ”Đ»Đ”ĐœĐœŃĐ” Đž ŃŃабОлОзОŃĐŸĐČĐ°ĐœĐœŃĐ” ĐČ ŃглДŃĐŸĐŽĐœĐŸĐč ĐŒĐ°ŃŃĐžŃĐ” ĐŒĐ”ŃĐ°Đ»Đ»ĐŸŃглДŃĐŸĐŽĐœŃŃ
ĐœĐ°ĐœĐŸĐșĐŸĐŒĐżĐŸĐ·ĐžŃĐŸĐČ FeCoCu/C. ĐĄĐžĐœŃДз ĐœĐ°ĐœĐŸĐșĐŸĐŒĐżĐŸĐ·ĐžŃĐŸĐČ ĐŸŃŃŃĐ”ŃŃĐČĐ»Đ”Đœ ĐŒĐ”ŃĐŸĐŽĐŸĐŒ ĐșĐŸĐœŃŃĐŸĐ»ĐžŃŃĐ”ĐŒĐŸĐłĐŸ ĐĐ-пОŃĐŸĐ»ĐžĐ·Đ° ĐżŃĐ”ĐșŃŃŃĐŸŃĐŸĐČ ŃОпа Â«ĐżĐŸĐ»ĐžĐŒĐ”Ń â Đ°ŃĐ”ŃОлаŃĐ”ŃĐŸĐœĐ°Ń Đ¶Đ”Đ»Đ”Đ·Đ° â Đ°ŃĐ”ŃĐ°ŃŃ ĐșĐŸĐ±Đ°Đ»ŃŃĐ° Đž ĐŒĐ”ĐŽĐžÂ», ĐżĐŸĐ»ŃŃĐ”ĐœĐœŃŃ
ŃĐŸĐČĐŒĐ”ŃŃĐœŃĐŒ ŃĐ°ŃŃĐČĐŸŃĐ”ĐœĐžĐ”ĐŒ ĐșĐŸĐŒĐżĐŸĐœĐ”ĐœŃĐŸĐČ Ń ĐżĐŸŃлДЎŃŃŃĐžĐŒ ŃĐŽĐ°Đ»Đ”ĐœĐžĐ”ĐŒ ŃĐ°ŃŃĐČĐŸŃĐžŃДлŃ. ĐŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐŸ ĐČлОŃĐœĐžĐ” ŃĐ”ĐŒĐżĐ”ŃĐ°ŃŃŃŃ ŃĐžĐœŃДза ĐœĐ° ŃŃŃŃĐșŃŃŃŃ, ŃĐŸŃŃĐ°ĐČ Đž ŃлДĐșŃŃĐŸĐŒĐ°ĐłĐœĐžŃĐœŃĐ” ŃĐČĐŸĐčŃŃĐČĐ° ĐœĐ°ĐœĐŸĐșĐŸĐŒĐżĐŸĐ·ĐžŃĐŸĐČ. ĐĐ”ŃĐŸĐŽĐŸĐŒ ŃĐ”ĐœŃĐłĐ”ĐœĐŸŃĐ»ŃĐŸŃĐ”ŃŃĐ”ĐœŃĐœĐŸĐłĐŸ Đ°ĐœĐ°Đ»ĐžĐ·Đ° ĐżĐŸĐșĐ°Đ·Đ°ĐœĐŸ, ŃŃĐŸ ĐŸĐ±ŃĐ°Đ·ĐŸĐČĐ°ĐœĐžĐ” ŃŃĐŸĐčĐœŃŃ
ĐœĐ°ĐœĐŸŃĐ°ŃŃĐžŃ FeCoCu ĐżŃĐŸĐžŃŃ
ĐŸĐŽĐžŃ Đ·Đ° ŃŃĐ”Ń ĐČĐ·Đ°ĐžĐŒĐŸĐŽĐ”ĐčŃŃĐČĐžŃ Fe3ĐĄ Ń ĐœĐ°ĐœĐŸŃĐ°ŃŃĐžŃĐ°ĐŒĐž ŃĐČĐ”ŃĐŽĐŸĐłĐŸ ŃĐ°ŃŃĐČĐŸŃĐ° CoCu. ĐĄ ĐżĐŸĐČŃŃĐ”ĐœĐžĐ”ĐŒ ŃĐ”ĐŒĐżĐ”ŃĐ°ŃŃŃŃ ŃĐžĐœŃДза ŃĐČДлОŃĐžĐČĐ°Đ”ŃŃŃ ŃĐ°Đ·ĐŒĐ”Ń ĐœĐ°ĐœĐŸŃĐ°ŃŃĐžŃ ĐŒĐ”ŃĐ°Đ»Đ»ĐŸĐČ, ŃŃĐŸ ĐŸĐ±ŃŃĐ»ĐŸĐČĐ»Đ”ĐœĐŸ ĐżŃĐŸŃĐ”ŃŃĐ°ĐŒĐž ĐžŃ
Đ°ĐłĐ»ĐŸĐŒĐ”ŃĐ°ŃОО Đž ĐșĐŸĐ°Đ»Đ”ŃŃĐ”ĐœŃОО ĐżŃĐž пДŃĐ”ŃŃŃĐŸĐčĐșĐ” ĐŒĐ°ŃŃĐžŃŃ. йаĐșжД ĐČ Đ·Đ°ĐČĐžŃĐžĐŒĐŸŃŃĐž ĐŸŃ ŃĐ”ĐŒĐżĐ”ŃĐ°ŃŃŃŃ ŃĐžĐœŃДза Đž ŃĐŸĐŸŃĐœĐŸŃĐ”ĐœĐžŃ ĐŒĐ”ŃĐ°Đ»Đ»ĐŸĐČ ĐŒĐŸĐłŃŃ ĐŸĐ±ŃĐ°Đ·ĐŸĐČŃĐČĐ°ŃŃŃŃ ĐœĐ°ĐœĐŸŃĐ°ŃŃĐžŃŃ ŃŃĐŸĐčĐœĐŸĐłĐŸ ŃплаĐČĐ° Ń ŃазлОŃĐœŃĐŒ ŃĐŸŃŃĐ°ĐČĐŸĐŒ. ĐĐ”ŃĐŸĐŽĐŸĐŒ ŃĐ°ĐŒĐ°ĐœĐŸĐČŃĐșĐŸĐč ŃпДĐșŃŃĐŸŃĐșĐŸĐżĐžĐž ĐżĐŸĐșĐ°Đ·Đ°ĐœĐŸ, ŃŃĐŸ Ń ĐżĐŸĐČŃŃĐ”ĐœĐžĐ”ĐŒ ŃĐ”ĐŒĐżĐ”ŃĐ°ŃŃŃŃ ŃĐžĐœŃДза ŃŃĐ”ĐżĐ”ĐœŃ ĐșŃĐžŃŃаллОŃĐœĐŸŃŃĐž ŃглДŃĐŸĐŽĐœĐŸĐč ĐŒĐ°ŃŃĐžŃŃ ĐœĐ°ĐœĐŸĐșĐŸĐŒĐżĐŸĐ·ĐžŃĐŸĐČ ĐČĐŸĐ·ŃĐ°ŃŃĐ°Đ”Ń. ĐŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœŃ ŃĐ°ŃŃĐŸŃĐœŃĐ” Đ·Đ°ĐČĐžŃĐžĐŒĐŸŃŃĐž ĐŸŃĐœĐŸŃĐžŃДлŃĐœĐŸĐč ĐșĐŸĐŒĐżĐ»Đ”ĐșŃĐœĐŸĐč ĐŽĐžŃлДĐșŃŃĐžŃĐ”ŃĐșĐŸĐč Đž ĐŒĐ°ĐłĐœĐžŃĐœĐŸĐč ĐżŃĐŸĐœĐžŃĐ°Đ”ĐŒĐŸŃŃĐž ĐœĐ°ĐœĐŸĐșĐŸĐŒĐżĐŸĐ·ĐžŃĐŸĐČ ĐČ ĐŽĐžĐ°ĐżĐ°Đ·ĐŸĐœĐ” 3â13 ĐĐŃ. ĐĐŸĐșĐ°Đ·Đ°ĐœĐŸ, ŃŃĐŸ ĐžĐ·ĐŒĐ”ĐœĐ”ĐœĐžĐ” ŃĐŸĐŸŃĐœĐŸŃĐ”ĐœĐžŃ ĐŒĐ”ŃĐ°Đ»Đ»ĐŸĐČ ĐżŃĐžĐČĐŸĐŽĐžŃ Đș Đ·ĐœĐ°ŃĐžŃДлŃĐœĐŸĐŒŃ ŃĐČДлОŃĐ”ĐœĐžŃ ĐșĐ°Đș ĐŽĐžŃлДĐșŃŃĐžŃĐ”ŃĐșĐžŃ
, ŃĐ°Đș Đž ĐŒĐ°ĐłĐœĐžŃĐœŃŃ
ĐżĐŸŃĐ”ŃŃ. ĐĐ”ŃĐČŃĐ” ŃĐČŃĐ·Đ°ĐœŃ Ń ŃĐŸŃĐŒĐžŃĐŸĐČĐ°ĐœĐžĐ”ĐŒ ŃĐ»ĐŸĐ¶ĐœĐŸĐč ĐœĐ°ĐœĐŸŃŃŃŃĐșŃŃŃŃ ŃглДŃĐŸĐŽĐœĐŸĐč ĐŒĐ°ŃŃĐžŃŃ ĐœĐ°ĐœĐŸĐșĐŸĐŒĐżĐŸĐ·ĐžŃĐ°, Đ° ĐČŃĐŸŃŃĐ” ĐŸĐ±ŃŃĐ»ĐŸĐČĐ»Đ”ĐœŃ ŃĐČДлОŃĐ”ĐœĐžĐ”ĐŒ ŃĐ°Đ·ĐŒĐ”ŃĐ° ĐœĐ°ĐœĐŸŃĐ°ŃŃĐžŃ Đž ŃĐŽĐČĐžĐłĐŸĐŒ ŃĐ°ŃŃĐŸŃŃ Đ”ŃŃĐ”ŃŃĐČĐ”ĐœĐœĐŸĐłĐŸ ŃĐ”ŃŃĐŸĐŒĐ°ĐłĐœĐžŃĐœĐŸĐłĐŸ ŃĐ”Đ·ĐŸĐœĐ°ĐœŃĐ° ĐČ ĐœĐžĐ·ĐșĐŸŃĐ°ŃŃĐŸŃĐœŃŃ ĐŸĐ±Đ»Đ°ŃŃŃ. Đ Đ°ŃŃĐ”ŃŃ ĐżĐŸŃĐ”ŃŃ ĐœĐ° ĐŸŃŃĐ°Đ¶Đ”ĐœĐžĐ” ĐżŃĐŸĐČĐ”ĐŽĐ”ĐœŃ ĐżĐŸ ŃŃĐ°ĐœĐŽĐ°ŃŃĐœĐŸĐč ĐŒĐ”ŃĐŸĐŽĐžĐșĐ” ĐœĐ° ĐŸŃĐœĐŸĐČĐ” ŃĐșŃпДŃĐžĐŒĐ”ĐœŃĐ°Đ»ŃĐœŃŃ
ĐŽĐ°ĐœĐœŃŃ
ŃĐ°ŃŃĐŸŃĐœŃŃ
Đ·Đ°ĐČĐžŃĐžĐŒĐŸŃŃĐ”Đč ĐșĐŸĐŒĐżĐ»Đ”ĐșŃĐœĐŸĐč ĐŒĐ°ĐłĐœĐžŃĐœĐŸĐč Đž ĐŽĐžŃлДĐșŃŃĐžŃĐ”ŃĐșĐŸĐč ĐżŃĐŸĐœĐžŃĐ°Đ”ĐŒĐŸŃŃĐž. ĐĐŸĐșĐ°Đ·Đ°ĐœĐŸ, ŃŃĐŸ ŃДгŃлОŃĐŸĐČĐ°ĐœĐžĐ” ŃĐ°ŃŃĐŸŃĐœĐŸĐłĐŸ ĐŽĐžĐ°ĐżĐ°Đ·ĐŸĐœĐ° Đž Đ·ĐœĐ°ŃĐ”ĐœĐžŃ ĐżĐŸĐłĐ»ĐŸŃĐ”ĐœĐžŃ ŃлДĐșŃŃĐŸĐŒĐ°ĐłĐœĐžŃĐœŃŃ
ĐČĐŸĐ»Đœ (ĐŸŃ â20 ĐŽĐŸ â52 ĐŽĐ) ĐŒĐŸĐ¶Đ”Ń ĐŸŃŃŃĐ”ŃŃĐČĐ»ŃŃŃŃŃ ĐżŃŃĐ”ĐŒ ĐžĐ·ĐŒĐ”ĐœĐ”ĐœĐžŃ ŃĐŸĐŸŃĐœĐŸŃĐ”ĐœĐžŃ ĐŒĐ”ŃĐ°Đ»Đ»ĐŸĐČ ĐČ ĐżŃĐ”ĐșŃŃŃĐŸŃĐ”. ĐĐŸĐ»ŃŃĐ”ĐœĐœŃĐ” ĐœĐ°ĐœĐŸĐșĐŸĐŒĐżĐŸĐ·ĐžŃŃ ĐŸĐ±Đ”ŃпДŃĐžĐČĐ°ŃŃ Đ±ĐŸĐ»Đ”Đ” ĐČŃŃĐŸĐșОД ŃДзŃĐ»ŃŃĐ°ŃŃ ĐżĐŸ ŃŃĐ°ĐČĐœĐ”ĐœĐžŃ Ń ĐœĐ°ĐœĐŸĐșĐŸĐŒĐżĐŸĐ·ĐžŃĐ°ĐŒĐž FeCo/C, ĐżĐŸĐ»ŃŃĐ”ĐœĐœŃĐŒĐž ĐżŃĐž Đ°ĐœĐ°Đ»ĐŸĐłĐžŃĐœŃŃ
ŃŃĐ»ĐŸĐČĐžŃŃ
Shattered pellet injection experiments at JET in support of the ITER disruption mitigation system design
A series of experiments have been executed at JET to assess the efficacy of the newly installed shattered pellet injection (SPI) system in mitigating the effects of disruptions. Issues, important for the ITER disruption mitigation system, such as thermal load mitigation, avoidance of runaway electron (RE) formation, radiation asymmetries during thermal quench mitigation, electromagnetic load control and RE energy dissipation have been addressed over a large parameter range. The efficiency of the mitigation has been examined for the various SPI injection strategies. The paper summarises the results from these JET SPI experiments and discusses their implications for the ITER disruption mitigation scheme
New H-mode regimes with small ELMs and high thermal confinement in the Joint European Torus
New H-mode regimes with high confinement, low core impurity accumulation, and small edge-localized mode perturbations have been obtained in magnetically confined plasmas at the Joint European Torus tokamak. Such regimes are achieved by means of optimized particle fueling conditions at high input power, current, and magnetic field, which lead to a self-organized state with a strong increase in rotation and ion temperature and a decrease in the edge density. An interplay between core and edge plasma regions leads to reduced turbulence levels and outward impurity convection. These results pave the way to an attractive alternative to the standard plasmas considered for fusion energy generation in a tokamak with a metallic wall environment such as the ones expected in ITER.& nbsp;Published under an exclusive license by AIP Publishing
Overview of JET results for optimising ITER operation
The JET 2019â2020 scientific and technological programme exploited the results of years of concerted scientific and engineering work, including the ITER-like wall (ILW: Be wall and W divertor) installed in 2010, improved diagnostic capabilities now fully available, a major neutral beam injection upgrade providing record power in 2019â2020, and tested the technical and procedural preparation for safe operation with tritium. Research along three complementary axes yielded a wealth of new results. Firstly, the JET plasma programme delivered scenarios suitable for high fusion power and alpha particle (α) physics in the coming DâT campaign (DTE2), with record sustained neutron rates, as well as plasmas for clarifying the impact of isotope mass on plasma core, edge and plasma-wall interactions, and for ITER pre-fusion power operation. The efficacy of the newly installed shattered pellet injector for mitigating disruption forces and runaway electrons was demonstrated. Secondly, research on the consequences of long-term exposure to JET-ILW plasma was completed, with emphasis on wall damage and fuel retention, and with analyses of wall materials and dust particles that will help validate assumptions and codes for design and operation of ITER and DEMO. Thirdly, the nuclear technology programme aiming to deliver maximum technological return from operations in D, T and DâT benefited from the highest DâD neutron yield in years, securing results for validating radiation transport and activation codes, and nuclear data for ITER
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