New data on the character of 137Cs lateral and vertical migration in soil-litter-moss cover within undisturbed elementary landscape geochemical systems on the test site in the Chernobyl abandoned zone, Russia

Author(s):  
Denis Dolgushin ◽  
Elena Korobova

<p>A study of <sup>137</sup>Cs distribution in two new landscape cross-sections characterizing the ELGS system (top-slope-closing depression) in the “Vyshkov-2” test site located in the Chernobyl abandoned zone, the Bryansk region, Russia, has been performed in 2020. The test site (70×100 m) is located on the Iput’ river terrace in a pine forest characterized by undisturbed soil-plant cover. The soil cover is presented by sod-podzolic sandy illuvial-ferruginous soils. The initial level of <sup>137</sup>Cs contamination of the area varied from 1480 kBq/m<sup>2</sup> to 1850 kBq/m<sup>2</sup>. Cs-137 activity was measured in the soil, moss and litter cover along two parallel (the distance was 5 m) cross-sections with 1 m step. Moisture content was also determined in the studied objects to roughly assess the influence of water regime on radiocaesium migration. Surface <sup>137</sup>Cs activity was measured in field conditions by adapted gamma-spectrometer Violinist-III. Cs-137 content in the soil and plant samples was determined in laboratory conditions by Canberra gamma-spectrometer with HPGe detector.</p><p>Analysis of the obtained data showed that a major part of <sup>137</sup>Cs is now fixed in the soil layer 2-10 cm deep while the highest specific activity of radiocaesium is found at a depth of 2-8 cm that can be explained mainly by the burial of the initially contaminated layer under the annual leaf fall.</p><p>Along the first cross-section we observed positive correlation between <sup>137</sup>Cs surface activity and the content radiocaesium in the top soil layer 0-2 cm (r<sub>0.05</sub>=0.643, n=15). Cs-137 activity in the moss samples correlated with the radionuclide activity in soil samples 4-6 cm deep (r<sub>0.05</sub>=0.627; n=15). In the moss samples the highest correlation was observed between the green and rhizoid moss parts (r<sub>0.01</sub>=0.704, n=60). Correlation between radiocaesium activity of the green part of mosses and the underlain litter samples was lower, but also significant (r<sub>0.01</sub>=0.612, n=60). Values of <sup>137</sup>Cs activity in the rhizoid part of moss and in litter were also positively linked, but to a lower degree (r<sub>0.01</sub>=0.402, n=60).</p><p>Along the second cross-section correlation between <sup>137</sup>Cs surface activity and the content radiocaesium in the top soil layer 0-2 cm equaled to r<sub>0.05</sub>=0.507 (n=7). Radiocaesium content in moss samples (green, rhizoid parts) and litter was higher correlated with <sup>137</sup>Cs content in soil layer 2-4 cm (r<sub>0.05</sub>=0.640; 0.410; 0.460, n=7). Similar to the first cross-section the highest correlation was observed between the green and rhizoid parts of moss (r<sub>0.01</sub>=0.780, n=39). Relation between <sup>137</sup>Cs activity in green part of moss and litter samples appeared smaller than along the first cross-section but still significant (r<sub>0.01</sub>=0.419, n=39) while that between the rhizoid part of moss and litter was higher (r<sub>0.01</sub>=0.509, n=39).</p><p>Performed study showed that<strong> </strong>in the studied objects <sup>137</sup>Cs secondary migration has a specifically stable character which may be related to spatial peculiarities of radionuclide migration in soil-plant cover controlled by water regime in the ELGS system. In our opinion this may form a characteristic cyclic variation of <sup>137</sup>Cs activity observed along cross-sections of ELGS.</p><p> </p><p>The reported study was funded by RFBR according to the research project № 19-05-00816.</p>

2020 ◽  
Author(s):  
Denis Dolgushin ◽  
Elena Korobova ◽  
Vladimir Baranchukov ◽  
Nikolay Dogadkin

<p>Cs-137 distribution was studied in the regular grid and in landscape cross-sections characterizing the ELGS system (top-slope-closing depression) in the “Vyshkov-2” test site located in the Chernobyl abandoned zone, the Bryansk region, Russia. The test site (70×100 m) located on the Iput’ river terrace in a pine forest formed on sod-podzolic soils is characterized by a pronounced elevation gradient (ca 4.5 m). In 1986 the level of <sup>137</sup>Cs contamination of the area varied from 1480 kBq/m<sup>2</sup> to 1850 kBq/m<sup>2</sup>. The distribution of <sup>137</sup>Cs was studied in the topsoil, soil, moss and litter cover in a grid manner with a step of 10 m and along cross-sections with 1 m step. To assess the influence of water regime on radiocaesium migration moisture content was also determined in the studied objects. The data showed that the major part of <sup>137</sup>Cs is now fixed in the soil layer 2-10 cm thick while the highest activity of radiocaesium is found at a depth of 2-8 cm that can be explained mainly by the burial of the initially contaminated layer under the annual leaf fall. In the ELGS system the content of <sup>137</sup>Cs in the top soil layer (0-2 cm) determined in laboratory conditions by Canberra gamma-spectrometer with HPGe detector correlated with the surface Cs-137 activity measured by field gamma-spectrometer Violinist III (r=0.643, n=15). Cs-137 activity in the green part of moss samples correlated with the radionuclide activity in soil layer samples 4-6 cm deep (r=0.627, n=15). In the moss samples the highest correlation was observed between the green and rhizoid moss parts (r<sub>0.01</sub>=0.718, n=60, along cross-sections), (r<sub>0.05</sub>=0.858, n=20, in regular grid). Correlation between radiocesium activity of the green part of mosses and the underlain litter samples was lower, but also significant (r<sub>0.01</sub>=0.617, n=60, along cross-sections), (r<sub>0.05</sub>=0.481, n=20, in regular grid). Cs-137 activity in the rhizoid part of moss and in litter were also positively linked, but to a lower degree (r<sub>0.01</sub>=0.402, n=60). Studies performed in 2015-2019 confirmed our earlier finding that radiocaesium had not moved in unidirectional manner down the slope to the closing depression, but formed a more complex polycentric structure in ELGS.</p><p>The study was financially supported by the Russian Foundation for Basic Research (grant # 19-05-00816).</p>


2020 ◽  
pp. 49-58 ◽  
Author(s):  
Changbin He ◽  
Yong You ◽  
Decheng Wang ◽  
Hongjian Wu ◽  
Bingnan Ye

Unclear soil layer coupling failure characteristics on natural grassland impeded the design and optimization of appropriate tillage tools. The coupling failure characteristics including surface disturbance and profile, disturbed cross-section area, soil over-turning rate, and coupling forces between the soil layer of natural grassland and selected passive subsoiler-type openers were investigated in this paper. Three single-shoot openers (i.e. CO, AO and WAO) and a test unit were designed, and furrow opening experiments under different working depths were conducted. Results showed that, along the passages, U-shaped disturbed cross-sections were usually created with soil-root clods overturned along the furrows. The roots were usually broken in a pulling or dragging way underground. Both disturbed cross-section area and draft force values increased with the working depth increasing linearly (R2≥0.93), contrary to the tendency of the specific draft force with the depth. Winged opener (i.e. WAO) had larger draft forces and disturbed soil layer cross-section areas than no-winged openers (i.e. AO and CO). The soil layer failure processes of the natural grassland were affected by its composite soil layer structure and the geometry parameters of the openers. The results provide original references for designing novel furrow openers applicable to improve degraded natural grassland.


Author(s):  
А.Ю. Полякова

В статье рассматриваются физические и воднофизические показатели почв Дворцового парка. Исследованы семь участков парка, из которых четыре являются островами. Показано влияние насыпных и намывных почв на исследуемые воднофизические свойства. Определена плотность почвенных горизонтов, их влажность. Для интерпретации воднофизических показателей был произведен расчет средневзвешенной влажности. Для сравнения участков по степени увлажнения были посчитаны запасы воды в верхнем слое почвы толщиной 30 и 50 см. Определена вероятность затопления корнеобитаемых горизонтов почвы. Рассматривается связь показателей (плотность, уровень грунтовых вод) с вмешательством человека в парковую среду. Предлагается улучшение водного режима почв методом подсыпки плодородного грунта на острова и в пониженные участки парка, планирование реставрации с элементами реконструкции. The article deals with the physical and waterphysical indicators of the soils of the Palace Park. Seven sites of the park, four of which are islands, were explored. The influence of bulk and alluvial soils on the studied waterphysical properties is shown. The density and the humidity of soil horizons has been determined. To interpret the waterphysical parameters, the weighted average humidity was calculated. For the comparing of the plots according to the degree of moisture the water reserves in the top soil layer with a thickness of 30 cm and 50 cm were calculated. The probability of flooding of rootoccupied soil horizons was determined. The relationship of indicators (density, groundwater level) with human intervention in the park environment is considered. It is proposed to improve the water regime of the soil by adding fertile soil to the islands and to lower areas of the park, also the planning of the restoration with elements of reconstruction is offered.


2009 ◽  
Vol 33 (6) ◽  
pp. 1603-1611 ◽  
Author(s):  
Mário Lopes da Silva Júnior ◽  
Thierry Desjardins ◽  
Max Sarrazin ◽  
Vânia Silva de Melo ◽  
Paulo Fernando da Silva Martins ◽  
...  

Soil plays an important role in the C cycle, and substitution of tropical forest by cultivated land affects C dynamic and stock. This study was developed in an area of expansion of human settlement in the Eastern Amazon, in Itupiranga, State of Pará, to evaluate the effects of native forest conversion to Brachiaria brizantha pasture on C contents of a dystrophic Oxisol. Soil samples were collected in areas of native forest (NF), of 8 to 10 year old secondary forest (SF), 1 to 2 year old SF (P1-2), 5 to 7 year old SF (P5-7), and of 10 to 12 year old SF (P10-12), and from under pastures, in the layers 0-2, 2-5 and 5-10 cm, to evaluate C levels and stocks and carry out separation of OM based on particle size. After deforestation, soil density increased to a depth of 5 cm, with greater increase in older pastures. Variation in C levels was greatest in the top soil layer; C contents increased with increasing pasture age. In the layers 2-5 and 5-10 cm, C content proved to be stable for the types of plant cover evaluated. Highest C concentrations were found in the silt fraction; however, C contents were highest in the clay fraction, independent of the plant cover. An increase in C associated with the sand fraction in the form of little decomposed organic residues was observed in pastures, confirming greater sensitivity of this fraction to change in soil use.


Author(s):  
J. P. Colson ◽  
D. H. Reneker

Polyoxymethylene (POM) crystals grow inside trioxane crystals which have been irradiated and heated to a temperature slightly below their melting point. Figure 1 shows a low magnification electron micrograph of a group of such POM crystals. Detailed examination at higher magnification showed that three distinct types of POM crystals grew in a typical sample. The three types of POM crystals were distinguished by the direction that the polymer chain axis in each crystal made with respect to the threefold axis of the trioxane crystal. These polyoxymethylene crystals were described previously.At low magnifications the three types of polymer crystals appeared as slender rods. One type had a hexagonal cross section and the other two types had rectangular cross sections, that is, they were ribbonlike.


Author(s):  
R.D. Leapman ◽  
P. Rez ◽  
D.F. Mayers

Microanalysis by EELS has been developing rapidly and though the general form of the spectrum is now understood there is a need to put the technique on a more quantitative basis (1,2). Certain aspects important for microanalysis include: (i) accurate determination of the partial cross sections, σx(α,ΔE) for core excitation when scattering lies inside collection angle a and energy range ΔE above the edge, (ii) behavior of the background intensity due to excitation of less strongly bound electrons, necessary for extrapolation beneath the signal of interest, (iii) departures from the simple hydrogenic K-edge seen in L and M losses, effecting σx and complicating microanalysis. Such problems might be approached empirically but here we describe how computation can elucidate the spectrum shape.The inelastic cross section differential with respect to energy transfer E and momentum transfer q for electrons of energy E0 and velocity v can be written as


Author(s):  
Xudong Weng ◽  
Peter Rez

In electron energy loss spectroscopy, quantitative chemical microanalysis is performed by comparison of the intensity under a specific inner shell edge with the corresponding partial cross section. There are two commonly used models for calculations of atomic partial cross sections, the hydrogenic model and the Hartree-Slater model. Partial cross sections could also be measured from standards of known compositions. These partial cross sections are complicated by variations in the edge shapes, such as the near edge structure (ELNES) and extended fine structures (ELEXFS). The role of these solid state effects in the partial cross sections, and the transferability of the partial cross sections from material to material, has yet to be fully explored. In this work, we consider the oxygen K edge in several oxides as oxygen is present in many materials. Since the energy window of interest is in the range of 20-100 eV, we limit ourselves to the near edge structures.


Author(s):  
P.A. Crozier

Absolute inelastic scattering cross sections or mean free paths are often used in EELS analysis for determining elemental concentrations and specimen thickness. In most instances, theoretical values must be used because there have been few attempts to determine experimental scattering cross sections from solids under the conditions of interest to electron microscopist. In addition to providing data for spectral quantitation, absolute cross section measurements yields useful information on many of the approximations which are frequently involved in EELS analysis procedures. In this paper, experimental cross sections are presented for some inner-shell edges of Al, Cu, Ag and Au.Uniform thin films of the previously mentioned materials were prepared by vacuum evaporation onto microscope cover slips. The cover slips were weighed before and after evaporation to determine the mass thickness of the films. The estimated error in this method of determining mass thickness was ±7 x 107g/cm2. The films were floated off in water and mounted on Cu grids.


Author(s):  
Stanley J. Klepeis ◽  
J.P. Benedict ◽  
R.M Anderson

The ability to prepare a cross-section of a specific semiconductor structure for both SEM and TEM analysis is vital in characterizing the smaller, more complex devices that are now being designed and manufactured. In the past, a unique sample was prepared for either SEM or TEM analysis of a structure. In choosing to do SEM, valuable and unique information was lost to TEM analysis. An alternative, the SEM examination of thinned TEM samples, was frequently made difficult by topographical artifacts introduced by mechanical polishing and lengthy ion-milling. Thus, the need to produce a TEM sample from a unique,cross-sectioned SEM sample has produced this sample preparation technique.The technique is divided into an SEM and a TEM sample preparation phase. The first four steps in the SEM phase: bulk reduction, cleaning, gluing and trimming produces a reinforced sample with the area of interest in the center of the sample. This sample is then mounted on a special SEM stud. The stud is inserted into an L-shaped holder and this holder is attached to the Klepeis polisher (see figs. 1 and 2). An SEM cross-section of the sample is then prepared by mechanically polishing the sample to the area of interest using the Klepeis polisher. The polished cross-section is cleaned and the SEM stud with the attached sample, is removed from the L-shaped holder. The stud is then inserted into the ion-miller and the sample is briefly milled (less than 2 minutes) on the polished side. The sample on the stud may then be carbon coated and placed in the SEM for analysis.


The work of multilayer glass structures for central and eccentric compression and bending are considered. The substantiation of the chosen research topic is made. The description and features of laminated glass for the structures investigated, their characteristics are presented. The analysis of the results obtained when testing for compression, compression with bending, simple bending of models of columns, beams, samples of laminated glass was made. Overview of the types and nature of destruction of the models are presented, diagrams of material operation are constructed, average values of the resistance of the cross-sections of samples are obtained, the table of destructive loads is generated. The need for development of a set of rules and guidelines for the design of glass structures, including laminated glass, for bearing elements, as well as standards for testing, rules for assessing the strength, stiffness, crack resistance and methods for determining the strength of control samples is emphasized. It is established that the strength properties of glass depend on the type of applied load and vary widely, and significantly lower than the corresponding normative values of the strength of heat-strengthened glass. The effect of the connecting polymeric material and manufacturing technology of laminated glass on the strength of the structure is also shown. The experimental values of the elastic modulus are different in different directions of the cross section and in the direction perpendicular to the glass layers are two times less than along the glass layers.


Sign in / Sign up

Export Citation Format

Share Document