93 research outputs found

    A Model for the Sources of the Slow Solar Wind

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    Models for the origin of the slow solar wind must account for two seemingly contradictory observations: The slow wind has the composition of the closed field corona, implying that it originates from the continuous opening and closing of flux at the boundary between open and closed field. On the other hand, the slow wind also has large angular width, up to ~ 60{\circ}, suggesting that its source extends far from the open-closed boundary. We propose a model that can explain both observations. The key idea is that the source of the slow wind at the Sun is a network of narrow (possibly singular) open-field corridors that map to a web of separatrices and quasi-separatrix layers in the heliosphere. We compute analytically the topology of an open-field corridor and show that it produces a quasi-separatrix layer in the heliosphere that extends to angles far from the heliospheric current sheet. We then use an MHD code and MDI/SOHO observations of the photospheric magnetic field to calculate numerically, with high spatial resolution, the quasi-steady solar wind and magnetic field for a time period preceding the August 1, 2008 total solar eclipse. Our numerical results imply that, at least for this time period, a web of separatrices (which we term an S-web) forms with sufficient density and extent in the heliosphere to account for the observed properties of the slow wind. We discuss the implications of our S-web model for the structure and dynamics of the corona and heliosphere, and propose further tests of the model

    Molecular and phenotypic characterisation of NS maize inbred lines.

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    ΠšΡƒΠΊΡƒΡ€ΡƒΠ· јС Π±ΠΈΡ™Π½Π° врста која испољава Π²Π΅Π»ΠΈΠΊΡƒ фСнотипску ΠΈ Π³Π΅Π½Π΅Ρ‚ΠΈΡ‡ΠΊΡƒ Π²Π°Ρ€ΠΈΡ˜Π°Π±ΠΈΠ»Π½ΠΎΡΡ‚. Π£ ΠΎΠ²ΠΎΠΌ Ρ€Π°Π΄Ρƒ ΠΈΠ·Π²Ρ€ΡˆΠ΅Π½Π° јС фСнотипска ΠΈ ΠΌΠΎΠ»Π΅ΠΊΡƒΠ»Π°Ρ€Π½Π° ΠΊΠ°Ρ€Π°ΠΊΡ‚Π΅Ρ€ΠΈΠ·Π°Ρ†ΠΈΡ˜Π° Π΄ΠΈΠ²Π΅Ρ€Π³Π΅Π½Ρ‚Π½ΠΈΡ… ΠΈΠ½Π±Ρ€Π΅Π΄ линија ΠΊΡƒΠΊΡƒΡ€ΡƒΠ·Π° којС сС користС Ρƒ ΠΎΠΏΠ»Π΅ΠΌΠ΅ΡšΠΈΠ²Π°Ρ‡ΠΊΠΈΠΌ ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΈΠΌΠ° ΠΈ којС ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²Ρ™Π°Ρ˜Ρƒ ΠΌΠΎΠ³ΡƒΡ›ΠΈ ΠΈΠ·Π²ΠΎΡ€ Π°Π»Π΅Π»Π° са ΠΏΠΎΠ·ΠΈΡ‚ΠΈΠ²Π½ΠΈΠΌ ΡƒΡ‚ΠΈΡ†Π°Ρ˜Π΅ΠΌ Π½Π° агромонски Π²Π°ΠΆΠ½Π΅ особинС. Π’Π°ΠΊΠΎΡ’Π΅, ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ„ΠΈΠΊΠΎΠ²Π°Π½ΠΈ су Π°Π»Π΅Π»ΠΈ карактСристични Π·Π° ΠΎΠ΄Ρ€Π΅Ρ’Π΅Π½Π΅ Ρ…Π΅Ρ‚Π΅Ρ€ΠΎΡ‚ΠΈΡ‡Π½Π΅ Π³Ρ€ΡƒΠΏΠ΅ ΠΈ ΡƒΡ‚Π²Ρ€Ρ’Π΅Π½Π΅ су ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΡ˜Π°Π»Π½ΠΎ Π·Π½Π°Ρ‡Π°Ρ˜Π½Π΅ Π²Π΅Π·Π΅ ΠΈΠ·ΠΌΠ΅Ρ’Ρƒ ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π° ΠΈ агрономски Π²Π°ΠΆΠ½ΠΈΡ… ΡΠ²ΠΎΡ˜ΡΡ‚Π°Π²Π° ΠΏΡ€ΠΈΠΌΠ΅Π½ΠΎΠΌ Π°ΡΠΎΡ†ΠΈΡ˜Π°Ρ‚ΠΈΠ²Π½Π΅ Π°Π½Π°Π»ΠΈΠ·Π΅, са Ρ†ΠΈΡ™Π΅ΠΌ Π΄Π°Ρ™Π΅ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅ Ρƒ ΠΌΠ°Ρ€ΠΊΠ΅Ρ€ Π°ΡΠΈΡΡ‚ΠΈΡ€Π°Π½ΠΎΡ˜ ΡΠ΅Π»Π΅ΠΊΡ†ΠΈΡ˜ΠΈ. Анализирани ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΡ˜Π°Π» ΡΠ°ΡΡ‚ΠΎΡ˜Π°ΠΎ сС ΠΎΠ΄ 96 ΠΈΠ½Π±Ρ€Π΅Π΄ линија ΠΈΠ· Ρ‡Π΅Ρ‚ΠΈΡ€ΠΈ Ρ…Π΅Ρ‚Π΅Ρ€ΠΎΡ‚ΠΈΡ‡Π½Π΅ Π³Ρ€ΡƒΠΏΠ΅. ВридСсСт ΡˆΠ΅ΡΡ‚ микросатСлитских ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π° ΠΊΠΎΡ€ΠΈΡˆΡ›Π΅Π½ΠΎ јС Π·Π° ΠΈΠ·Ρ€Π°Ρ‡ΡƒΠ½Π°Π²Π°ΡšΠ΅ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Π°Ρ€Π° Π΄ΠΈΠ²Π΅Ρ€Π·ΠΈΡ‚Π΅Ρ‚Π° гСнских локуса. ΠŸΡ€ΠΈΠΌΠ΅ΡšΠ΅Π½Π΅ су Ρ‚Ρ€ΠΈ кластСр Π°Π½Π°Π»ΠΈΠ·Π΅ Π½Π° ΠΏΠΎΠ΄Π°Ρ†ΠΈΠΌΠ° добијСним ΠΌΠΎΠ»Π΅ΠΊΡƒΠ»Π°Ρ€Π½ΠΎΠΌ Π°Π½Π°Π»ΠΈΠ·ΠΎΠΌ. ΠŸΠΎΡ™ΡΠΊΠΈ ΠΎΠ³Π»Π΅Π΄ΠΈ су постављСни Ρƒ Ρ‚ΠΎΠΊΡƒ Π΄Π²Π΅ Π³ΠΎΠ΄ΠΈΠ½Π΅, ΠΏΠΎ ΠΏΠΎΡ‚ΠΏΡƒΠ½ΠΎ ΡΠ»ΡƒΡ‡Π°Ρ˜Π½ΠΎΠΌ Π±Π»ΠΎΠΊ систСму са Ρ‚Ρ€ΠΈ ΠΏΠΎΠ½Π°Π²Ρ™Π°ΡšΠ°. ДСскриптивна статистика, Π°Π½Π°Π»ΠΈΠ·Π° Π²Π°Ρ€ΠΈΡ˜Π°Π½ΡΠ΅, Π»ΠΈΠ½Π΅Π°Ρ€Π½Π΅ ΠΊΠΎΡ€Π΅Π»Π°Ρ†ΠΈΡ˜Π΅ ΠΈ Π°Π½Π°Π»ΠΈΠ·Π° Π³Π»Π°Π²Π½ΠΈΡ… ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ΠΈ ΠΈΠ·Ρ€Π°Ρ‡ΡƒΠ½Π°Ρ‚Π΅ су Π·Π° 13 особина. Π’Π΅Π·Π΅ ΠΈΠ·ΠΌΠ΅Ρ’Ρƒ ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π° ΠΈ особина ΡƒΡ‚Π²Ρ€Ρ’Π΅Π½Π΅ су ΠΏΡ€ΠΈΠΌΠ΅Π½ΠΎΠΌ ΠΎΠΏΡˆΡ‚Π΅Π³ ΠΈ ΠΌΠ΅ΡˆΠΎΠ²ΠΈΡ‚ΠΎΠ³ Π»ΠΈΠ½Π΅Π°Ρ€Π½ΠΎΠ³ ΠΌΠΎΠ΄Π΅Π»Π°. ΠŸΡ€ΠΎΡΠ΅Ρ‡Π°Π½ Π±Ρ€ΠΎΡ˜ Π°Π»Π΅Π»Π° износио јС 8,3, просСчна полиморфност ΠΏΠΎΡ˜Π΅Π΄ΠΈΠ½Π°Ρ‡Π½ΠΈΡ… локуса износила јС 0,64, Π° ΠΏΡ€ΠΎΡ†Π΅Π½Π°Ρ‚ Ρ€Π΅Ρ‚ΠΊΠΈΡ… Π°Π»Π΅Π»Π° 8,5% ΠΏΠΎ локусу. Π£ΠΎΡ‡Π΅Π½ јС Π²Π΅Ρ›ΠΈ Π³Π΅Π½Π΅Ρ‚ΠΈΡ‡ΠΊΠΈ Π΄ΠΈΠ²Π΅Ρ€Π·ΠΈΡ‚Π΅Ρ‚ ΠΊΠΎΠ΄ BSSS Π½Π΅Π³ΠΎ ΠΊΠΎΠ΄ Lancaster линија. Π’ΠΈΡˆΠ΅ ΠΎΠ΄ Ρ‚Ρ€Π΅Ρ›ΠΈΠ½Π΅ Π°Π»Π΅Π»Π° Π±ΠΈΠ»ΠΎ јС карактСристично Π·Π° само Ρ˜Π΅Π΄Π½Ρƒ Π³Ρ€ΡƒΠΏΡƒ. Π Π΅Π·ΡƒΠ»Ρ‚Π°Ρ‚ΠΈ кластСр Π°Π½Π°Π»ΠΈΠ·Π° су Ρƒ вСликој ΠΌΠ΅Ρ€ΠΈ Π±ΠΈΠ»ΠΈ Ρƒ ΠΌΠ΅Ρ’ΡƒΡΠΎΠ±Π½ΠΎΡ˜ сагласности. Анализа Π²Π°Ρ€ΠΈΡ˜Π°Π½ΡΠ΅ ΡƒΠΊΠ°Π·Π°Π»Π° јС Π½Π° ΠΏΠΎΡΡ‚ΠΎΡ˜Π°ΡšΠ΅ статистички Π·Π½Π°Ρ‡Π°Ρ˜Π½ΠΈΡ… Ρ€Π°Π·Π»ΠΈΠΊΠ° особина ΠΌΠ΅Ρ’Ρƒ ΠΈΠ½Π±Ρ€Π΅Π΄ линијама, Π³ΠΎΠ΄ΠΈΠ½Π°ΠΌΠ° ΠΈ Π»ΠΎΠΊΠ°Π»ΠΈΡ‚Π΅Ρ‚ΠΈΠΌΠ°. Π Π΅Π·ΡƒΠ»Ρ‚Π°Ρ‚ΠΈ кластСр Π°Π½Π°Π»ΠΈΠ·Π΅ фСнотипских ΠΏΠΎΠ΄Π°Ρ‚Π°ΠΊΠ° Π±ΠΈΠ»ΠΈ су Ρƒ мањој ΠΌΠ΅Ρ€ΠΈ сагласни са ΠΏΠ΅Π΄ΠΈΠ³Ρ€Π΅ΠΈΠΌΠ° линија, Π½Π΅Π³ΠΎ Ρ€Π΅Π·ΡƒΠ»Π°Ρ‚ΠΈ Π°Π½Π°Π»ΠΈΠ·Π΅ ΠΌΠΎΠ»Π΅ΠΊΡƒΠ»Π°Ρ€Π½ΠΈΡ… ΠΏΠΎΠ΄Π°Ρ‚Π°ΠΊΠ°. Анализа Π³Π»Π°Π²Π½ΠΈΡ… ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ΠΈ издвојила јС линијС ΠΏΡ€Π΅ΠΌΠ° Ρ…Π΅Ρ‚Π΅Ρ€ΠΎΡ‚ΠΈΡ‡Π½ΠΈΠΌ Π³Ρ€ΡƒΠΏΠ°ΠΌΠ° ΠΈ истакла ΡšΠΈΡ…ΠΎΠ²Π΅ ΠΎΠΏΡˆΡ‚Π΅ карактСристикС. Π’Π΅Π»ΠΈΠΊΠΈ Π±Ρ€ΠΎΡ˜ ΡƒΡ‚Π²Ρ€Ρ’Π΅Π½ΠΈΡ… Π°Π»Π΅Π»Π° ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π° са стабилним ΠΏΠΎΠ·ΠΈΡ‚ΠΈΠ²Π½ΠΈΠΌ Π΅Ρ„Π΅ΠΊΡ‚ΠΈΠΌΠ° Π½Π° принос ΡƒΠΊΠ°Π·ΡƒΡ˜Π΅ Π½Π° ΠΌΠΎΠ³ΡƒΡ›ΠΈ Π·Π½Π°Ρ‡Π°Ρ˜ ΠΎΠ²ΠΈΡ… ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π° Ρƒ ΠΎΠΏΠ»Π΅ΠΌΠ΅ΡšΠΈΠ²Π°ΡšΡƒ ΠΊΡƒΠΊΡƒΡ€ΡƒΠ·Π°.Maize has great phenotypic and genotypic variability. In this study a diverse set of maize inbred lines used in breeding programmes as a potential source of alleles with positive effects on important agronomic traits, was characterised at phenotypic and molecular level. Furthermore, alleles specific to heterotic groups were identified and potentially significant associations between markers and important agronomic traits which could be employed in marker assisted selection were determined. Ninety eight inbred lines from four heterotic groups were analysed. Thirty six microsatellite markers were used to obtain parameters for genetic diversity and three claster analyses were employed based on molecular data. The field trials were set in randomised block design with three replications during two years to acquire phenotypic data. Descriptive statistics, analysis of variance, linear correlations and principal component analysis were performed for 13 traits. The associations between markers and traits were identified by the application of general and mixed linear model. The average number of alleles was 8,3, the average value of polymorphism information content was 0,64, whereas the percentage of rare alleles was 8,5%. Greater genetic diversity of BSSS inbred lines compared to the lines from Lancaster group were observed. More than one third of alleles were specific to only one of these two groups. The results of cluster analyses were to a large extent in agreement with each other. Analysis of variance indicated statistically significant differences in traits among inbred lines, years and locations. Cluster analysis based on phenotypic data was in less consistent with pedigrees of the inbred lines than the cluster analysis based on molecular data. Principal component analysis grouped inbreds into heterotic groups and indicated their general characteristics. A large number of identified marker alleles with stable positive effects on grain yield suggested the potential importance of these markers in maiz

    Genetic Variability in Different Lucerne (\u3cem\u3eMedicago Sativa\u3c/em\u3e) Genotypes

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    One of the basic goals of modern lucerne breeding programmes is creation of new cultivars with a great potential for high quality and stable yields of both forage and hay (Riday & Brummer, 2002). Such cultivars meet increased needs of animal husbandry and must contribute to diverse farming systems (Luki , 2000). Our trial was aimed at determining genetic variability of yield components in 7 lucerne genotypes, as well as at evaluation of their breeding potential as gene donors to new lucerne cultivar

    Evidence for topological nonequilibrium in magnetic configurations

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    We use direct numerical simulations to study the evolution, or relaxation, of magnetic configurations to an equilibrium state. We use the full single-fluid equations of motion for a magnetized, non-resistive, but viscous fluid; and a Lagrangian approach is used to obtain exact solutions for the magnetic field. As a result, the topology of the magnetic field remains unchanged, which makes it possible to study the case of topological nonequilibrium. We find two cases for which such nonequilibrium appears, indicating that these configurations may develop singular current sheets.Comment: 10 pages, 5 figure

    Nonlinear force-free magnetic field extrapolations: comparison of the Grad-Rubin and Wheatland-Sturrock-Roumeliotis algorithm

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    We compare the performance of two alternative algorithms which aim to construct a force-free magnetic field given suitable boundary conditions. For this comparison, we have implemented both algorithms on the same finite element grid which uses Whitney forms to describe the fields within the grid cells. The additional use of conjugate gradient and multigrid iterations result in quite effective codes. The Grad-Rubin and Wheatland-Sturrock-Roumeliotis algorithms both perform well for the reconstruction of a known analytic force-free field. For more arbitrary boundary conditions the Wheatland-Sturrock-Roumeliotis approach has some difficulties because it requires overdetermined boundary information which may include inconsistencies. The Grad-Rubin code on the other hand loses convergence for strong current densities. For the example we have investigated, however, the maximum possible current density seems to be not far from the limit beyond which a force free field cannot exist anymore for a given normal magnetic field intensity on the boundary.Comment: 21 pages, 13 figure

    3D Coronal Density Reconstruction and Retrieving the Magnetic Field Structure during Solar Minimum

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    Measurement of the coronal magnetic field is a crucial ingredient in understanding the nature of solar coronal phenomena at all scales. We employed STEREO/COR1 data obtained during a deep minimum of solar activity in February 2008 (Carrington rotation CR 2066) to retrieve and analyze the three-dimensional (3D) coronal electron density in the range of heights from 1.5 to 4 Rsun using a tomography method. With this, we qualitatively deduced structures of the coronal magnetic field. The 3D electron density analysis is complemented by the 3D STEREO/EUVI emissivity in the 195 A band obtained by tomography for the same CR. A global 3D MHD model of the solar corona was used to relate the reconstructed 3D density and emissivity to open/closed magnetic field structures. We show that the density maximum locations can serve as an indicator of current sheet position, while the locations of the density gradient maximum can be a reliable indicator of coronal hole boundaries. We find that the magnetic field configuration during CR 2066 has a tendency to become radially open at heliocentric distances greater than 2.5 Rsun. We also find that the potential field model with a fixed source surface (PFSS) is inconsistent with the boundaries between the regions with open and closed magnetic field structures. This indicates that the assumption of the potential nature of the coronal global magnetic field is not satisfied even during the deep solar minimum. Results of our 3D density reconstruction will help to constrain solar coronal field models and test the accuracy of the magnetic field approximations for coronal modeling.Comment: Published in "Solar Physics

    Structure and Dynamics of the Sun's Open Magnetic Field

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    The solar magnetic field is the primary agent that drives solar activity and couples the Sun to the Heliosphere. Although the details of this coupling depend on the quantitative properties of the field, many important aspects of the corona - solar wind connection can be understood by considering only the general topological properties of those regions on the Sun where the field extends from the photosphere out to interplanetary space, the so-called open field regions that are usually observed as coronal holes. From the simple assumptions that underlie the standard quasi-steady corona-wind theoretical models, and that are likely to hold for the Sun, as well, we derive two conjectures on the possible structure and dynamics of coronal holes: (1) Coronal holes are unique in that every unipolar region on the photosphere can contain at most one coronal hole. (2) Coronal holes of nested polarity regions must themselves be nested. Magnetic reconnection plays the central role in enforcing these constraints on the field topology. From these conjectures we derive additional properties for the topology of open field regions, and propose several observational predictions for both the slowly varying and transient corona/solar wind.Comment: 26 pages, 6 figure

    Slip-Squashing Factors as a Measure of Three-Dimensional Magnetic Reconnection

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    A general method for describing magnetic reconnection in arbitrary three-dimensional magnetic configurations is proposed. The method is based on the field-line mapping technique previously used only for the analysis of magnetic structure at a given time. This technique is extended here so as to analyze the evolution of magnetic structure. Such a generalization is made with the help of new dimensionless quantities called "slip-squashing factors". Their large values define the surfaces that border the reconnected or to-be-reconnected magnetic flux tubes for a given period of time during the magnetic evolution. The proposed method is universal, since it assumes only that the time sequence of evolving magnetic field and the tangential boundary flows are known. The application of the method is illustrated for simple examples, one of which was considered previously by Hesse and coworkers in the framework of the general magnetic reconnection theory. The examples help us to compare these two approaches; they reveal also that, just as for magnetic null points, hyperbolic and cusp minimum points of a magnetic field may serve as favorable sites for magnetic reconnection. The new method admits a straightforward numerical implementation and provides a powerful tool for the diagnostics of magnetic reconnection in numerical models of solar-flare-like phenomena in space and laboratory plasmas.Comment: 39 pages, 9 figures, corrected typos, to appear in ApJ, March 200
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