12 research outputs found

    Memory effect of Mn5_5Ge3_3 nanomagnets embedded inside a Mn-diluted Ge matrix

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    Crystalline Mn5Ge3 nanomagnets are formed inside a Mn-diluted Ge matrix using Mn ion implantation. A temperature-dependent memory effect and slow magnetic relaxation are observed below the superparamagnetic blocking temperature of Mn5Ge3. Our findings corroborate that the observed spin-glass-like features are caused by the size distribution of Mn5Ge3 nanomagnets, rather than by the inter-particle interaction through the Mn-diluted Ge matrix.Comment: 10 pages, 4 figures,. submitted to Appl. Phys. Let

    Ferromagnetic, structurally disordered ZnO implanted with Co ions

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    We present superparamagnetic clusters of structurally highly disordered Co-Zn-O created by high fluence Co ion implantation into ZnO (0001) single crystals at low temperatures. This secondary phase cannot be detected by common x-ray diffraction but is observed by high-resolution transmission electron microscopy. In contrast to many other secondary phases in a ZnO matrix it induces low-field anomalous Hall effect and thus is a candidate for magneto-electronics applications.Comment: 5 pages, 3 figure

    Unsteady Coupled Heat Transfer in the Air and Surrounding Rock Mass for Mine Excavations with Distributed Heat Sources

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    This paper presents an unsteady coupled heat transfer model in mine air and surrounding rock mass in the presence of distributed heat sources. The case of distributed heat sources is typical when analyzing the temperature distribution in mine excavations equipped with conveyor systems. For this case, the asymptotic value of the air temperature at the end of the mine excavation is determined not only by the heat exchange between the air and surrounding rock mass but also by the thermal power of distributed heat sources and the total airflow. This conclusion is confirmed by the experimental data presented in the paper for a longwall in a potash mine. We formulate the mathematical model and calculate the distribution of air parameters along the length of an excavation, considering heat release from the conveyor and surrounding rock mass. The results show that a distributed heat release is necessary for correctly calculating the air temperature in working areas. The numerical simulations allow us to recommend a redistribution of air between the haulage and conveyor roadways in the presence of distributed heat sources

    Analytical approach to estimation of water build-up effect in mine ventilation shafts

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    ΠΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ исслСдования обусловлСна Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒΡŽ сниТСния Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ Π½Π°Π³Ρ€ΡƒΠ·ΠΊΠΈ Π½Π° Π³Π»Π°Π²Π½Ρ‹Π΅ вСнтиляторныС установки, связанной с Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΠ΅ΠΌ ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ тяги ΠΏΡ€ΠΈ ΠΊΠ°ΠΏΠ΅ΠΆΠ΅ Π² вСнтиляционных стволах ΡˆΠ°Ρ…Ρ‚ ΠΈ Ρ€ΡƒΠ΄Π½ΠΈΠΊΠΎΠ². НаиболСС остро ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌΠ° Π½ΠΎΡ€ΠΌΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ Ρ€Π°Π±ΠΎΡ‚Ρ‹ вСнтилятора Π²ΠΎΠ·Π½ΠΈΠΊΠ°Π΅Ρ‚ Π² случаС Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΠ³ΠΎ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π° Π΅Π³ΠΎ Π² Ρ€Π΅ΠΆΠΈΠΌ нСустойчивой Ρ€Π°Π±ΠΎΡ‚Ρ‹, Ρ‡Ρ‚ΠΎ сопряТСно с Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒΡŽ Π½Π΅ Ρ‚ΠΎΠ»ΡŒΠΊΠΎ энСргосбСрСТСния, Π½ΠΎ ΠΈ прСдотвращСния Π΅Π³ΠΎ Π°Π²Π°Ρ€ΠΈΠΉΠ½ΠΎΠ³ΠΎ останова. ЦСль: выяснСниС ΠΏΡ€ΠΈΡ‡ΠΈΠ½ ΠΈ ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌΠ° возникновСния эффСкта «водяной ΠΏΡ€ΠΎΠ±ΠΊΠΈΒ» Π² вСнтиляционных стволах с ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ΠΈΠ΅ΠΌ качСствСнных ΠΈ количСствСнных ΠΎΡ†Π΅Π½ΠΎΠΊ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρ‹ ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ тяги Π² зависимости ΠΎΡ‚ скорости двиТСния Π²ΠΎΠ·Π΄ΡƒΡ…Π°, Π³Π»ΡƒΠ±ΠΈΠ½Ρ‹ ΠΈ интСнсивности источника выдСлСния Π²Π»Π°Π³ΠΈ. ΠžΠ±ΡŠΠ΅ΠΊΡ‚Ρ‹: вСнтиляционныС стволы ΡˆΠ°Ρ…Ρ‚. ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹: аналитичСскоС ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ процСссов кондСнсации Π²Π»Π°Π³ΠΈ ΠΈ двиТСния капСль Π² восходящСм Π²ΠΎΠ·Π΄ΡƒΡˆΠ½ΠΎΠΌ ΠΏΠΎΡ‚ΠΎΠΊΠ΅; ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΉ Π°Π½Π°Π»ΠΈΠ· ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΈ ΠΌΠΎΠ΄Π΅Π»ΡŒΠ½Ρ‹Ρ… Π΄Π°Π½Π½Ρ‹Ρ…. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. ΠŸΡ€ΠΎΠ²Π΅Π΄Ρ‘Π½ Π°Π½Π°Π»ΠΈΠ· ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… Π΄Π°Π½Π½Ρ‹Ρ… ΠΏΠΎ ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΡŽ ΠΈ двиТСнию капСльной Π²Π»Π°Π³ΠΈ Π² вСнтиляционных стволах Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… Ρ€ΡƒΠ΄Π½ΠΈΠΊΠΎΠ². ΠžΡ‚ΠΌΠ΅Ρ‡Π΅Π½ΠΎ, Ρ‡Ρ‚ΠΎ эффСкт водяной ΠΏΡ€ΠΎΠ±ΠΊΠΈ Π½Π°Π±Π»ΡŽΠ΄Π°Π΅Ρ‚ΡΡ Π² ΠΎΠ³Ρ€Π°Π½ΠΈΡ‡Π΅Π½Π½ΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ скоростСй двиТСния Π²ΠΎΠ·Π΄ΡƒΡ…Π° ΠΎΡ‚ 7 Π΄ΠΎ 12 ΠΌ/с, Π½ΠΎ Π² Π½Π΅ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… случаях эффСкт отсутствуСт, Π΄Π°ΠΆΠ΅ нСсмотря Π½Π° Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ густого Ρ‚ΡƒΠΌΠ°Π½Π° ΠΈ обильной кондСнсации Π²Π»Π°Π³ΠΈ Π½Π° повСрхности ΠΊΡ€Π΅ΠΏΠΈ ΠΈ Π°Ρ€ΠΌΠΈΡ€ΠΎΠ²ΠΊΠΈ ствола. РассмотрСны Ρ‚Ρ€ΠΈ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½Ρ‹Ρ… сцСнария возникновСния эффСкта: Π½Π°ΠΊΠΎΠΏΠ»Π΅Π½ΠΈΠ΅ большого количСства Π·Π°Π²ΠΈΡΠ°ΡŽΡ‰ΠΈΡ… Π² Π²ΠΎΠ·Π΄ΡƒΡ…Π΅ капСль ΠΎΠΏΡ€Π΅Π΄Π΅Π»Ρ‘Π½Π½ΠΎΠ³ΠΎ Ρ€Π°Π·ΠΌΠ΅Ρ€Π°; ΠΏΠ°Π΄Π΅Π½ΠΈΠ΅ капСль ΠΊΡ€ΡƒΠΏΠ½Ρ‹Ρ… Ρ€Π°Π·ΠΌΠ΅Ρ€ΠΎΠ² ΠΏΠΎ всСй Π³Π»ΡƒΠ±ΠΈΠ½Π΅ ствола с источником выдСлСния Π²Π»Π°Π³ΠΈ Π² Π΅Π³ΠΎ Π²Π΅Ρ€Ρ…Π½Π΅ΠΉ части ΠΈ Ρ€Π°Π·Π½ΠΎΠ½Π°ΠΏΡ€Π°Π²Π»Π΅Π½Π½ΠΎΠ΅ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠ΅ капСль Π² зависимости ΠΎΡ‚ ΠΈΡ… Ρ€Π°Π·ΠΌΠ΅Ρ€Π° с источником влаговыдСлСния, располоТСнным Π½Π° ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ»ΡŒΠ½ΠΎΠΉ Π³Π»ΡƒΠ±ΠΈΠ½Π΅. УстановлСно, Ρ‡Ρ‚ΠΎ ΠΏΠ΅Ρ€Π²Ρ‹Π΅ Π΄Π²Π΅ ΠΌΠΎΠ΄Π΅Π»ΠΈ Π½Π΅ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ ΠΏΠΎΠ»ΡƒΡ‡ΠΈΡ‚ΡŒ ΠΊΠΎΠ»ΠΈΡ‡Π΅ΡΡ‚Π²Π΅Π½Π½ΡƒΡŽ ΠΎΡ†Π΅Π½ΠΊΡƒ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρ‹ эффСкта Π²Π²ΠΈΠ΄Ρƒ нСопрСдСлённости Ρ„Ρ€Π°ΠΊΡ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ состава капСль, критичСский Ρ€Π°Π·ΠΌΠ΅Ρ€ зависания ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… ΡƒΠ²Π΅Π»ΠΈΡ‡ΠΈΠ²Π°Π΅Ρ‚ ΠΎΠ±Ρ€Π°Ρ‚Π½ΡƒΡŽ тягу Π΄ΠΎ бСсконСчности. Π­Ρ‚ΠΎΡ‚ нСдостаток устранён Π² Ρ‚Ρ€Π΅Ρ‚ΡŒΠ΅ΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ Π²Π²Π΅Π΄Π΅Π½ΠΈΠ΅ΠΌ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΈ распрСдСлСния капСль ΠΏΠΎ Ρ€Π°Π·ΠΌΠ΅Ρ€Π°ΠΌ, Ρ‡Ρ‚ΠΎ Π΄Π°Π»ΠΎ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ ΠΏΠΎΠ»ΡƒΡ‡ΠΈΡ‚ΡŒ количСствСнныС Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. Π”ΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ Π²Ρ‹Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π²Π»Π°Π³ΠΈ ΠΈΠ· Π²ΠΎΠ·Π΄ΡƒΡ…Π° Π½Π΅ ΠΌΠΎΠΆΠ΅Ρ‚ ΡΠ²Π»ΡΡ‚ΡŒΡΡ ΠΏΡ€ΠΈΡ‡ΠΈΠ½ΠΎΠΉ возникновСния эффСкта «водяной ΠΏΡ€ΠΎΠ±ΠΊΠΈΒ», Π° ΠΏΡ€ΠΈΡ‡ΠΈΠ½ΠΎΠΉ ΡΠ²Π»ΡΡŽΡ‚ΡΡ Π²ΠΎΠ΄ΠΎΠΏΡ€ΠΈΡ‚ΠΎΠΊΠΈ Π² ствол с ΠΈΠ½Ρ‚Π΅Π½ΡΠΈΠ²Π½ΠΎΡΡ‚ΡŒΡŽ, Π½Π° порядок ΠΏΡ€Π΅Π²Ρ‹ΡˆΠ°ΡŽΡ‰Π΅ΠΉ ΠΊΠΎΠ½Π΄Π΅Π½ΡΠ°Ρ†ΠΈΡŽ. По Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌ числСнного модСлирования ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ максимальная обратная тяга Π²ΠΎΠ·Π½ΠΈΠΊΠ°Π΅Ρ‚ ΠΏΡ€ΠΈ ΠΏΡ€ΠΎΠ½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΠΈ Π² ствол повСрхностных Π³Ρ€ΡƒΠ½Ρ‚ΠΎΠ²Ρ‹Ρ… Π²ΠΎΠ΄.The relevance of the study is caused by the need to reduce the additional aerodynamic load on the main fans associated with the occurrence of pressure drop caused by water build-up effect in mine ventilation shafts. This negative effect can lead to significant increase in the air resistance of the mine and to subsequent unstable operation mode of main fan. Avoiding this effect is important not only for energy save mine ventilation, but also for preventing emergency stop of the main fan. Purpose: finding out the causes and mechanism of the water build-up effect with obtaining qualitative and quantitative estimates of the pressure drop value depending on the air velocity, shaft depth and intensity of the groundwater inflows. Objects: ventilation shafts. Methods: analytical modeling of moisture condensation and droplet movement in an ascending air flow in ventilation shaft; comparative analysis of experimental and model data. Results. The authors have analyzed the experimental data on formation and movement of droplet moisture in the ventilation shafts of various mines. It is noted that the water build-up effect is observed in the range of air velocities from 7 to 12 m/s, but in some cases the effect is absent even despite the presence of thick fog and abundant condensation of moisture on the surface of the shaft lining and other equipment. Three possible scenarios of the effect are considered: accumulation of a large number of drops of a certain size hanging in the air; drops of large size fall along the entire depth of the shaft with a source of moisture release in its upper part and multidirectional movement of drops depending on their size with a source of moisture release located at arbitrary depth. It is established that the first two models do not allow us to obtain a quantitative estimate of the water build-up effect value due to the uncertainty of the fractional composition of drops, the critical size of which increases the pressure drop to infinity. This drawback was eliminated in the third model by introducing the droplet size distribution function, which made it possible to obtain quantitative results. It is proved that the release of moisture from the air cannot be the cause of the water build-up effect, and the cause is the ground water flows into the shaft with intensity of an order of magnitude higher than moisture condensation. Based on the results of numerical modeling, it is shown that the maximum pressure drop occurs when surface groundwater enters the shaft

    Methods for microclimate normalization in deep long blind drifts

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    ΠΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ исслСдования обусловлСна Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒΡŽ Ρ€ΡƒΠ΄Π½ΠΈΠΊΠΎΠ² Ρ€Π΅ΡˆΠ°Ρ‚ΡŒ Π½ΠΎΠ²Ρ‹Π΅ ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌΡ‹ Π½ΠΎΡ€ΠΌΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΌΠΈΠΊΡ€ΠΎΠΊΠ»ΠΈΠΌΠ°Ρ‚Π°, Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡŽΡ‰ΠΈΠ΅ ΠΏΡ€ΠΈ ΠΏΡ€ΠΎΡ…ΠΎΠ΄ΠΊΠ΅ всС Π±ΠΎΠ»Π΅Π΅ Π³Π»ΡƒΠ±ΠΎΠΊΠΈΡ… ΠΈ Π½Π°Π³Ρ€Π΅Ρ‚Ρ‹Ρ… ΠΏΠΎΡ€ΠΎΠ΄Π½Ρ‹Ρ… массивов протяТСнными Ρ‚ΡƒΠΏΠΈΠΊΠΎΠ²Ρ‹ΠΌΠΈ Π²Ρ‹Ρ€Π°Π±ΠΎΡ‚ΠΊΠ°ΠΌΠΈ. ЦСль: ΠΎΠΏΡ€Π΅Π΄Π΅Π»ΠΈΡ‚ΡŒ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… способов Π½ΠΎΡ€ΠΌΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΌΠΈΠΊΡ€ΠΎΠΊΠ»ΠΈΠΌΠ°Ρ‚Π° Π² Π·Π°Π±ΠΎΠ΅ Ρ€Π°Π·Π²Π΅Π΄ΠΎΡ‡Π½ΠΎΠΉ Π²Ρ‹Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ-2 ПАО Β«Π“ΠœΠš "ΠΠΎΡ€ΠΈΠ»ΡŒΡΠΊΠΈΠΉ никСль"Β». ΠžΠ±ΡŠΠ΅ΠΊΡ‚Ρ‹: гСологоразвСдочная Π²Ρ‹Ρ€Π°Π±ΠΎΡ‚ΠΊΠ°-2 ПАО Β«Π“ΠœΠš "ΠΠΎΡ€ΠΈΠ»ΡŒΡΠΊΠΈΠΉ никСль"Β». ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹: числСнноС ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ тСпломассопСрСноса Π² атмосфСрС Π³ΠΎΡ€Π½ΠΎΠΉ Π²Ρ‹Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ, ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² модСлирования. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. РассмотрСны способы Π½ΠΎΡ€ΠΌΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΌΠΈΠΊΡ€ΠΎΠΊΠ»ΠΈΠΌΠ°Ρ‚Π° Π² Π³Π»ΡƒΠ±ΠΎΠΊΠΈΡ… протяТСнных Ρ‚ΡƒΠΏΠΈΠΊΠΎΠ²Ρ‹Ρ… Π²Ρ‹Ρ€Π°Π±ΠΎΡ‚ΠΊΠ°Ρ…, ΠΈΡ… особСнности, прСимущСства ΠΈ нСдостатки. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Π° матСматичСская модСль тСпломассопСрСноса Π² атмосфСрС Π³ΠΎΡ€Π½ΠΎΠΉ Π²Ρ‹Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ с вСнтиляционным Ρ‚Ρ€ΡƒΠ±ΠΎΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΎΠΌ, ΡƒΡ‡ΠΈΡ‚Ρ‹Π²Π°ΡŽΡ‰Π°Ρ ΠΊΠΎΠ½Π²Π΅ΠΊΡ‚ΠΈΠ²Π½Ρ‹ΠΉ ΠΈ лучистый Ρ‚Π΅ΠΏΠ»ΠΎΠΎΠ±ΠΌΠ΅Π½. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ расчСта Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… способов сниТСния Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ Π²ΠΎΠ·Π΄ΡƒΡ…Π°, ΠΏΠΎΠ΄Π°Π²Π°Π΅ΠΌΠΎΠ³ΠΎ Π² Π·Π°Π±ΠΎΠΉ Π³Π΅ΠΎΠ»ΠΎΠ³ΠΎΡ€Π°Π·Π²Π΅Π΄ΠΎΡ‡Π½ΠΎΠΉ Π²Ρ‹Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ, строящСйся Π½Π° ΠΌΠ΅Π΄Π½ΠΎ-Π½ΠΈΠΊΠ΅Π»Π΅Π²ΠΎΠΌ Ρ€ΡƒΠ΄Π½ΠΈΠΊΠ΅ ΠΊΠΎΠΌΠΏΠ°Π½ΠΈΠΈ ПАО Β«Π“ΠœΠš "ΠΠΎΡ€ΠΈΠ»ΡŒΡΠΊΠΈΠΉ никСль"Β». ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΉ Π°Π½Π°Π»ΠΈΠ· Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… горнотСхничСских ΠΈ тСплотСхничСских мСроприятий ΠΏΠΎ сниТСнию Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ Π²ΠΎΠ·Π΄ΡƒΡ…Π° Π² Π·Π°Π±ΠΎΠ΅ Π²Ρ‹Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ Π΄ΠΎ Π·Π½Π°Ρ‡Π΅Π½ΠΈΠΉ, допустимых согласно ΠŸΡ€Π°Π²ΠΈΠ»Π°ΠΌ бСзопасности. ВыявлСно, Ρ‡Ρ‚ΠΎ ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠ΅ объСма ΠΏΠΎΠ΄Π°Ρ‡ΠΈ Π²ΠΎΠ·Π΄ΡƒΡ…Π° Π½Π΅ позволяСт Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΡΠ½ΠΈΠ·ΠΈΡ‚ΡŒ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρƒ Π² Π·Π°Π±ΠΎΠ΅. ΠŸΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Ρ‚Π΅ΠΏΠ»ΠΎΠΈΠ·ΠΎΠ»ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ вСнтиляционного Ρ‚Ρ€ΡƒΠ±ΠΎΠΏΡ€ΠΎΠ²ΠΎΠ΄Π° сущСствСнно сниТаСт Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρƒ ΠΏΠΎΠ΄Π°Π²Π°Π΅ΠΌΠΎΠ³ΠΎ Π² Π·Π°Π±ΠΎΠΉ Π²ΠΎΠ·Π΄ΡƒΡ…Π°, Π½ΠΎ Π΅Ρ‘ Π·Π½Π°Ρ‡Π΅Π½ΠΈΠ΅ ΠΏΠΎ-ΠΏΡ€Π΅ΠΆΠ½Π΅ΠΌΡƒ остаСтся Π²Ρ‹ΡˆΠ΅ допустимых Π·Π½Π°Ρ‡Π΅Π½ΠΈΠΉ. Показано, Ρ‡Ρ‚ΠΎ использованиС ΠΊΠ°ΠΌΠ΅Ρ€Ρ‹ ΠΎΡ€ΠΎΡˆΠ΅Π½ΠΈΡ позволяСт ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΡ‚ΡŒ Π΄ΠΎΠΏΡƒΡΡ‚ΠΈΠΌΡƒΡŽ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρƒ Π²ΠΎΠ·Π΄ΡƒΡ…Π° Π² Π·ΠΈΠΌΠ½ΠΈΠΉ ΠΏΠ΅Ρ€ΠΈΠΎΠ΄, Π½ΠΎ Π½Π΅ позволяСт ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΡ‚ΡŒ Π΅Ρ‘ Π² Π»Π΅Ρ‚Π½ΠΈΠΉ ΠΏΠ΅Ρ€ΠΈΠΎΠ΄. НаиболСС ΡƒΠ½ΠΈΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½Ρ‹ΠΌ, эффСктивным, Π½ΠΎ дорогостоящим способом сниТСния Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ Π²ΠΎΠ·Π΄ΡƒΡ…Π° являСтся ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΏΠΎΠ΄Π·Π΅ΠΌΠ½Ρ‹Ρ… систСм кондиционирования Π²ΠΎΠ·Π΄ΡƒΡ…Π° Π½Π° Π±Π°Π·Π΅ парокомпрСссионных машин.The relevance of the research is provided by the complexity of microclimate normalization in long blind drifts which are driven deeply through geothermally heated rocks. The aim of the research is the evaluation of usability of different ways for microclimate normalization in the working section of the exploration drift-2 in the mine of PJSC Β«MMC "Norilsk Nickel"Β». Objects: the exploration mine exploration drift-2 of PJSC Β«MMC "Norilsk Nickel"Β». Methods: the numerical simulation of heat and mass transfer in the atmosphere of the long exploration drift, the comparative analysis of simulation results. Results. The paper reviews ways, comparing their features, advantages, and disadvantages, for microclimate normalization in deep blind drifts. The presented mathematical model describes the heat and mass transfer in the working section of the blind drift with ventilation through the air duct. The model considers convective and radiant heat transfers. The results of the numerical simulation are given for different air-cooling methods which are applicable in the case of the deep copper-nickel mine of PJSC Β«MMC "Norilsk Nickel"Β». Drawing on this, different mining and thermal engineering operations for normalization of air temperatures in the working section regarding safety requirements are compared. It is defined that increasing the intake air flowrate could not decrease the air temperature near the face. The use of thermally insulated duct significantly decreases the air temperature in the working section but does not reduce it to the permitted value. It is shown, that the air irrigation could normalize temperatures in winter and not during the summer months. Underground air conditioning is the most universal and effective way for this purpose but highly expensive
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