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Development of the method of special ship ice observations 开发特殊船舶冰层观测方法
Pub Date : 2023-12-09 DOI: 10.30758/0555-2648-2023-69-4-394-406
T. Alekseeva, Y. I. Makarov, V. Borodkin, S. Serovetnikov, E. B. Saperstein, Yu. V. Sokolova, V. D. Kotelnikov
Since the middle of the XXth century researchers at the Arctic and Antarctic Research Institute (AARI) have been carrying out special ship ice observations in the Arctic and other freezing seas. Field data about main sea ice parameters are necessary for developing and validation of sea ice forecasts and satellite information. In keeping with technological advances and new research and practical tasks this method is ever developing. In spring 2023 sea ice observations were organized by the AARI’s reseachers onboard the nuclear icebreaker 50 let Pobedy in the south-western part of the Kara Sea. This paper presents recommendations concerning the method of special ship ice observations as developed during the expedition: dispatch to the vessel of operative and forecast hydrometeorological information from the AARI with a request for return transfer to the AARI of the processing results of the data obtained in the areas of predicted high deformation of ice cover along the route of navigation and upgrade of the ship television complex to receive information about ice layers and structure.
自二十世纪中叶以来,北极和南极研究所(AARI)的研究人员一直在北极和其他冰冻海域进行特殊的船冰观测。有关海冰主要参数的实地数据对于制定和验证海冰预报和卫星信息十分必要。随着技术的进步以及新的研究和实际任务,这种方法也在不断发展。2023 年春,美国航空航天研究所的研究人员在卡拉海西南部的 50 let Pobedy 号核动力破冰船上组织了海冰观测。本文就考察期间制定的特殊船舶冰层观测方法提出建议:向船舶发送来自美国航空航天研究所的运行和预报水文气象信息,并要求将在航行路线沿线冰盖预测高变形区域获得的数据处理结果返回美国航空航天研究所,以及升级船舶电视综合系统以接收冰层和结构信息。
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引用次数: 0
Studies of ice physical properties in Russia and USSR (late XIXth century – 1940). Ice density and porosity 俄罗斯和苏联的冰物理特性研究(十九世纪末至 1940 年)。冰的密度和孔隙度
Pub Date : 2023-12-09 DOI: 10.30758/0555-2648-2023-69-4-501-518
K. Sazonov
The paper deals with studies conducted in Russia and USSR of ice density, a most important characteristic of ice, and spans a period from the late XIXth century to 1940. It is shown that Russian scientists started their investigations of ice density only around the end of the XIX century, and those studies were often performed with specific applications in mind, e. g. works by B.P. Veinberg and his disciples in Tomsk in 1911–1914. In the USSR, there was a revival of interest in this kind of studies in the late 1920s in connection with explorations of the polar seas. Density measurements were mainly performed by hydrostatic weighing. At the request of N.N. Zubov and I.I. Mesyatsev in 1927 V.V. Shuleikin invented a simple instrument to measure ice density without weighing samples. In the early 1930s, ice porosity became an important field of research aimed at finding the causes of variance of experimental data on ice density. Ice porosity and density were studied using innovative devices developed by V.V. Shuleikin and V.I. Arnold-Alyabiev, which allowed studying ice properties in expedition conditions. The device developed by Arnold-Alyabiev found widespread use in field studies. Ice density and porosity are closely related physical quantities, therefore measuring the porosity of ice allowed researchers to estimate its density. By the end of the 1930s the ice density measurements had developed into a standard procedure of ice studies, which was due in large measure to the plans devised at the All-Union Arctic Institute headed by B.P. Veinberg to investigate ice at polar stations, which also included ice density and porosity studies.
本文论述了俄罗斯和苏联对冰密度(冰的最重要特征)的研究,时间跨度从十九世纪末到 1940 年。研究表明,俄罗斯科学家在十九世纪末才开始对冰密度进行研究,而且这些研究通常是以具体应用为目的,例如 B.P. Veinberg 及其弟子于 1911-1914 年在托木斯克进行的研究。在苏联,20 世纪 20 年代末,随着对极地海洋的探索,人们对这类研究的兴趣再次高涨。密度测量主要是通过静力学称重法进行的。1927 年,应 N.N. Zubov 和 I.I. Mesyatsev 的要求,V.V. Shuleikin 发明了一种无需称量样品即可测量冰密度的简单仪器。20 世纪 30 年代初,冰的孔隙度成为一个重要的研究领域,目的是找出冰密度实验数据差异的原因。冰的孔隙度和密度是利用 V.V. 舒列伊金和 V.I. 阿诺德-阿利亚比耶夫研制的创新装置进行研究的,这种装置可以在探险条件下研究冰的特性。阿诺德-阿利亚比耶夫开发的设备在实地研究中得到广泛应用。冰的密度和孔隙度是密切相关的物理量,因此,通过测量冰的孔隙度,研究人员可以估算出冰的密度。到 20 世纪 30 年代末,冰密度测量已发展成为冰研究的标准程序,这在很大程度上归功于由 B.P. Veinberg 领导的全联盟北极研究所制定的极地站冰研究计划,其中也包括冰密度和孔隙度研究。
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引用次数: 0
Characteristics of aerosol at the research base “Ice Cape Baranova” in 2018–2023 2018-2023年 "巴拉诺瓦冰角 "研究基地的气溶胶特征
Pub Date : 2023-12-09 DOI: 10.30758/0555-2648-2023-69-4-421-434
S. Sakerin, D. M. Tomsk, M. Loskutova, D. D. Rize, D. Chernov, Yu. S. Turchinovich
Atmospheric aerosol plays an important role in the processes of radiative transfers and mass exchange by different substances in the “continent–atmosphere–ocean” system. In this paper we discuss the results of a five-year measurement cycle of the atmospheric aerosol characteristics at the polar station “Ice base Cape Baranov”, located on the Bolshevik Island (the Severnaya Zemlya Archipelago). The set of the characteristics analyzed includes: the aerosol optical depth (AOD) of the atmosphere; the ground concentration of aerosol particles in the radius range of 0.15–5 microns; the content of the absorbing substance (soot) in the aerosol in the equivalent of elemental black carbon. The average values of the aerosol characteristics for the general measurement period (from April 2018 to May 2023) were: volumes of submicron and coarse aerosol particles 0.43 and 0.46 μm3/cm3, respectively; mass concentration of black carbon — 45.8 ng/m3; AOT of the atmosphere at a wavelength of 0.5 µm — 0.08; Angstrom selectivity exponent — 1.67. The average annual variation of aerosol and black carbon concentrations is characterized by a maximum in winter (January–March) and a minimum in summer (June–August). A comparison is made against the data from analogous measurements of aerosol characteristics at the polar station in Barentsburg (the Spitsbergen Archipelago) and against the data from model calculations, i. e., MERRA-2 reanalysis. A distinctive feature of the data in the Cape Baranov area is the low content of coarse aerosol — 1.7 less than in Barentsburg. There is agreement with the annual variation of black carbon concentrations at other polar stations, but the opposite nature of the seasonal variability of model (MERRA-2) concentrations: low values in winter and high values in summer. It is shown that the average spectral AODs of the atmosphere at the “Cape Baranov” are intermediate values between the data from polar stations in NyÅlesund and Barentsburg.
大气气溶胶在 "大陆-大气-海洋 "系统中不同物质的辐射传输和质量交换过程中发挥着重要作用。本文讨论了位于布尔什维克岛(塞维利亚泽姆利亚群岛)极地站 "巴拉诺夫角冰雪基地 "的大气气溶胶特征五年测量周期的结果。分析的一系列特征包括:大气气溶胶光学深度(AOD);半径范围为 0.15-5 微米的气溶胶颗粒的地面浓度;气溶胶中吸收物质(烟尘)的含量(相当于元素黑碳)。一般测量期间(2018 年 4 月至 2023 年 5 月)气溶胶特征的平均值为:亚微米和粗气溶胶颗粒体积分别为 0.43 和 0.46 μm3/cm3 ;黑碳的质量浓度 - 45.8 纳克/立方米;波长为 0.5 微米的大气 AOT - 0.08 ;安氏选择性指数 - 1.67。气溶胶和黑碳浓度的年均变化特点是冬季(1 月至 3 月)最大,夏季(6 月至 8 月)最小。与巴伦支堡极地站(斯匹次卑尔根群岛)气溶胶特征的类似测量数据和模型计算数据(即 MERRA-2 再分析)进行了比较。巴拉诺夫角地区数据的一个显著特点是粗气溶胶含量低,比巴伦支堡少 1.7。与其他极地站的黑碳浓度年变化一致,但与模型(MERRA-2)浓度的季节变化性质相反:冬季值低,夏季值高。研究表明,"巴拉诺夫角 "大气的平均光谱 AOD 值介于尼勒松和巴伦支堡极地站数据之间。
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引用次数: 0
Comparison of features of phenomena in the high latitude ionospheric F-region induced by powerful HF radio waves radiated by antennas with narrow and wide beam patterns 窄波束模式和宽波束模式天线辐射的强大高频无线电波诱发的高纬度电离层 F 区现象特征比较
Pub Date : 2023-12-09 DOI: 10.30758/0555-2648-2023-69-4-435-451
N. Blagoveshchenskaya, T. D. Borisov, A. Kalishin, I. M. Egorov, G. A. Zagorskyi, A. S. Kovalev
Physical experiments in natural free plasma (ionosphere) using controlled injection of powerful HF radio waves (HF pump waves) into the high latitude upper (F-region) ionosphere allow the investigation of various nonlinear phenomena. HF pump waves with ordinary (O-mode) polarization are commonly used for the modification of the upper ionosphere (F-region). This is due to the fact that extraordinary (X-mode) polarized HF pump waves are reflected from altitudes significantly below the reflection altitude of the O-polarized HF pump wave and the altitude of electrostatic plasma waves. Because of that they are not able to generate such waves or, as a consequence, cause artificial plasma turbulence and accompanying phenomena. However, the results of experiments carried out by AARI researchers at the EISCAT/Heating facility (Tromsø, Norway) have clearly demonstrated for the first time that X-polarized HF pump waves are able to produce artificial ionosphere disturbances which may be much stronger compared with O-mode disturbances. This opens up new possibilities for the investigation of nonlinear phenomena and ionospheric disturbances in the upper ionosphere, leading to the development of technologies allowing one to observe the processes in the Arctic zone ionosphere. In contrast to the traditional investigations of artificial ionospheric disturbances induced by O-mode HF pump waves, X-mode disturbances in the upper ionosphere are poorly investigated, the mechanisms of their generation are not understood. Therefore, such investigations require serious experimental and theoretical development. We present investigation results of the influence of the HF Phased Array beam width at the EISCAT/Heating facility (Tromsø, Norway) on the features of artificial disturbances in the high latitude upper (F-region) ionosphere induced by powerful HF radio waves. The paper analyzes the features, behavior, and spatial structure of electron density and temperature (Ne and Te), Langmuir and ion-acoustic plasma waves, artificial field-aligned irregularities (AFAIs), and narrowband (±1кHz relative to heating frequency) stimulated electromagnetic emission (NSEE) induced by X-mode HF pumping by phased Arrays with a narrow beam width of 5–6° (A1) and a wide beam width of 10–12° (at — 3 dB level) (A3). It is shown that the spatial size in the north-south direction of the Neducts and HF-enhanced plasma and ion lines (HFPL and HFIL) depends on the width of the HF Heating facility antenna beam. It corresponds to the angle width of 7° for the A3 antenna and 4° for A1, which is approximately two times less than the width of th pattern of A3 and A1. The relationship between the Ne duct transverse size and the size of the region occupied by the X-mode artificial irregularities is found. It has been established that the intensities of all the discrete components in the NSEE spectra are 10–20 dB higher when a powerful X-wave is emitted to the antenna A1, providing ERP = 820 MW, compared
在天然自由等离子体(电离层)中进行物理实验,利用向高纬度上电离层(F 区)有控制地注入强大的高频无线电波(高频泵波),可以研究各种非线性现象。通常使用普通(O 模)极化的高频泵波来改变上电离层(F 区)。这是由于非凡(X 模)极化高频泵浦波的反射高度大大低于 O 极化高频泵浦波的反射高度和静电等离子体波的高度。因此,它们无法产生这种波,也就无法引起人造等离子体湍流和伴随现象。然而,AARI 研究人员在 EISCAT/加热设施(挪威特罗姆瑟)进行的实验结果首次清楚地表明,X 极化高频泵波能够产生人工电离层扰动,这种扰动可能比 O 模式扰动强得多。这为研究电离层上部的非线性现象和电离层扰动提供了新的可能性,有助于开发能够观测北极区电离层过程的技术。与对 O 模式高频泵波引起的人工电离层扰动的传统研究不同,对上电离层 X 模式扰动的研究很少,对其产生机制也不了解。因此,这类研究需要认真的实验和理论发展。我们介绍了 EISCAT/加热设施(挪威特罗姆瑟)的高频相控阵波束宽度对强力高频无线电波诱发的高纬度上层(F 区)电离层人工扰动特征的影响的研究结果。论文分析了电子密度和温度(Ne 和 Te)、朗缪尔和离子声等离子体波、人工场对齐不规则现象(AFAIs)以及窄带(相对于加热频率为 ±1кHz)刺激电磁辐射(NSEE)的特征、行为和空间结构,这些特征、行为和空间结构是由相控阵(X-mode HF pumping by phased Arrays with a narrow beam width of 5-6° (A1) and a wide beam width of 10-12° (at - 3 dB level) (A3))诱发的。结果表明,在南北方向上,Neducts 和高频增强等离子体和离子线(HFPL 和 HFIL)的空间大小取决于高频加热设施天线波束的宽度。A3 天线的角宽为 7°,A1 天线的角宽为 4°,大约是 A3 和 A1 图案宽度的两倍。发现了 Ne 管道横向尺寸与 X 模式人工不规则所占区域大小之间的关系。已经确定,与向天线 A3 辐射(ERP = 230 MW)相比,向天线 A1 辐射(ERP = 820 MW)时,NSEE 频谱中所有离散成分的强度要高 10-20 dB。比较了天线 A1 和 A3 的辐射模式宽度对 O 模式和 X 模式高频抽运期间干扰特性的影响。结果表明,在 O 模式加热过程中,频率低于 F2 层临界频率的 Ne 管道和窄带受激电磁发射在天线 A1 和 A3 发射泵波时根本不会受到激励。然而,在 O 模式加热期间,电子温度、AFAI 强度和 AFAI 所占区域大小的扰动要大于 X 模式加热期间。
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引用次数: 0
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Arctic and Antarctic Research
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