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Lecture 10
Lecture 10

... Weak hydrogen lines, strong lines of ionized calcium ...
7. Energy Harvesting From Solar Wind and Galactic Cosmic Rays
7. Energy Harvesting From Solar Wind and Galactic Cosmic Rays

... Solar wind is a stream of charged particles that originates in the upper atmosphere of the sun. It comprises of mostly electrons and protons along with a few heavier ions, and blows continuously from the surface of the Sun [1]. The solar wind may be considered as an extension of the outer atmosphere ...
3.MSJ0290.Solar_.2017.v1
3.MSJ0290.Solar_.2017.v1

... atoms are arranged together in a tightly bound structure. By squeezing small quantities of other elements into this structure, two different types of silicon are created: n-type, which has spare electrons, and p-type, which is missing electrons, leaving ‘holes’ in their place. When these two materia ...
Why the Model of a Hydrogen
Why the Model of a Hydrogen

... silicon (Si), magnesium (Mg), sulfur (S) and calcium (Ca). He concluded that “... in the evolution of elements much more material has gone into the even-numbered elements than into those which are odd...” (p. 869). However, in the 1920s, Payne2 and Russell3 showed that the solar atmosphere is mostly ...
- Lorentz Center
- Lorentz Center

... suggested that the the physical source of the solar and stellar dyanamo is turbulent convection, and not the shear induced by rotation (Parker 1955) ...
106_1.pdf
106_1.pdf

... particle event to solar X-ray events and set limits on the propagation length of the ions along the magnetic field lines. ...
The impact of black holes on the Universe
The impact of black holes on the Universe

... – Plasma can flow along but not across field lines. – A section of a line with less plasma is less weighed down, so B-pressure causes it to arch up, speeding flow of plasma from this section (Parker instability) – Soon there are loops of field connecting foot points in the disc that are in relative ...
The Interior of the Sun
The Interior of the Sun

... found at the bottom of the Convection Zone disappear from the top of the Interface Layer to its bottom where the Radiation Zone begins which is calmer. Consequently, the speed of gas within this layer changes abruptly and there is even a difference between how fast this fluid motion changes when you ...
Three-scale structure of diffusion region of magnetic reconnection in
Three-scale structure of diffusion region of magnetic reconnection in

... events with plasma containing hot and cold ion components of comparable densities [Andre and Cully, 2012]. It was suggested that such ion distribution alters properties of the magnetic reconnection regions at the magnetopause [Toledo‐Redondo et. al., 2016]. Motivated by these recent findings, we per ...
The sun is a star. It is a huge, spinning, glowing sphere of hot gas
The sun is a star. It is a huge, spinning, glowing sphere of hot gas

... The average sunspot is about the size of the entire planet Earth! However, sunspots come in a variety of sizes ranging from hundreds to tens of thousands of miles across (many times larger that Earth). Scientists measure the total size (area) of all of the sunspots seen on the sun every day to get a ...
The Ionosphere - Stanford Solar Center
The Ionosphere - Stanford Solar Center

... The other main source of variability in the ionosphere comes from charged particles responding to the neutral atmosphere in the thermosphere. The ionosphere responds to the thermospheric winds; they can push the ionosphere along the inclined magnetic field lines to a different altitude. The ionosphe ...
Magnetic Confinement of the Plasma Fusion by Tokamak Machine
Magnetic Confinement of the Plasma Fusion by Tokamak Machine

... The figure 1 presents the efficient sections of different reactions of the fusion mentioned above [3] according to the energy of deuterium. Among these the D-T reaction (Fig. 2) appears the most attractive since it necessitate a least energy between the reagents. The mass of the helium core is lower ...
Astronomy 112: Physics of Stars Problem set 2: Due April 29 1. Time
Astronomy 112: Physics of Stars Problem set 2: Due April 29 1. Time

... 8. Polytropes: Helium burning: We shall see later that after they finish central and shell hydrogen burning, many stars, including the sun, go on to ignite helium burning in their centers at a temperature ∼ 1.5×108 K. (aside: This temperature does not vary very much due to the extreme temperature se ...
Note - Overflow Education
Note - Overflow Education

... At a solar maximum there is usually over 100 sunspots appearing simultaneously on the surface of the Sun, while at solar minimum there may be none at all; ...
Oxygen Isotopes Anomalies in the Solar System and the G0
Oxygen Isotopes Anomalies in the Solar System and the G0

... produced in stellar nucleosynthesis by He burning provided to ISM by supernovae rare isotopes 17O and 18O produced in CNO cycles novae and supernovae  Expected that ISM would have regions that are inhomogeneous  Is an observed galactic gradient (Wilson and Rood 1992)  Solar values 16O/18O  500 ...
The Stellar Dynamo - Academic Program Pages
The Stellar Dynamo - Academic Program Pages

... others, began telescopic studies of sunspots. These records, as the German astronomer Samuel Heinrich Schwabe announced in 1843, displayed a prominent periodicity of roughly 10 years in the number of observed sunspot groups. By the 20th century George Ellery Hale of the Mount Wilson Observatory in C ...
The Stellar Dynamo - Department of Atmospheric Sciences
The Stellar Dynamo - Department of Atmospheric Sciences

... others, began telescopic studies of sunspots. These records, as the German astronomer Samuel Heinrich Schwabe announced in 1843, displayed a prominent periodicity of roughly 10 years in the number of observed sunspot groups. By the 20th century George Ellery Hale of the Mount Wilson Observatory in C ...
2003 Venkatakrishnan and Ravindra Relation between CME speed
2003 Venkatakrishnan and Ravindra Relation between CME speed

... projected speed of halo CME. The following physical conclusions can be drawn from the study. Although emerging flux in the core of an AR may be responsible for the occurrence of a CME [Nitta and Hudson, 2001], the maximum kinetic energy released in the CME seems to be well related to the total magne ...
A Solar Polar Imager Concept - The National Academies of
A Solar Polar Imager Concept - The National Academies of

... proposed SPI orbit allows the study of the evolution of the solar wind from its source to the spacecraft nearly free of the effects of stream-stream interactions. This, along with improved magnetic field extrapolations using the multi-viewpoint synoptic magnetograms, provides an unprecedented opport ...
Estimating the total radiative power output from the hot outer layers
Estimating the total radiative power output from the hot outer layers

... the abundances. Throughout, we used the coronal abundances as given by Meyer (1985), i.e. C, N, O & Ne di er by factors of 2 to 3 from the solar photospheric abundances. The coronal abundances given by Feldman et al. (1992) are di erent from those given here and are closer to the photospheric abunda ...
Twisting and Writhing with George Ellery Hale
Twisting and Writhing with George Ellery Hale

... •Alexei Pevtsov, Ph.D. (Solar and Planetary Physics), Institute of SolarTerrestrial Physics, Irkutsk, 1992 •Tetsuya Magara, Ph.D. (Solar Physics), University of Kyoto, Japan 1998 •Robert Leamon, Ph.D. (Physics), University of Delaware, Newark, 1999 •Stephane Regnier, Ph.D. (Physics), Inst. d'Astroph ...
Final Exam, Dec. 19, 2015 - Physics@Brock
Final Exam, Dec. 19, 2015 - Physics@Brock

... 37. Stars U and W have the same luminosity and star U is ten times more distant than star W. The brightness of U is that of W. (a) 1/10 (b) 1/100 (c) 100 times (d) 10 times 38. Stars S and U are equally bright and the luminosity of S is four times larger than the that of U. luminosity of U. Then the ...
Sunspots - Academic Program Pages at Evergreen
Sunspots - Academic Program Pages at Evergreen

... • Sunspots are dark regions on the solar surface. – They appear dark because they are generally between 1,500 and 2,000 K cooler than their surroundings.1 » It is generally accepted that sunspots manifest as a result of interactions between the Sun’s magnetic field and convection currents. Caprino B ...
talk-tutorial - Helioseismic and Magnetic Imager
talk-tutorial - Helioseismic and Magnetic Imager

... Asymmetric spot motions (leading vs following) can be explained by the asymmetric shapes of Ω-loops. The asymmetric shapes result from the Coriolis force. The morphological asymmetry (the leading side being more compact than following side) of active regions may be explained by a field strength asym ...
Conservation Laws in Ideal MHD - Harvard
Conservation Laws in Ideal MHD - Harvard

... In ideal MHD, the magnetic field and plasma are frozen-in to each other ...
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Corona



A corona (Latin, 'crown') is an aura of plasma that surrounds the sun and other celestial bodies. The Sun's corona extends millions of kilometres into space and is most easily seen during a total solar eclipse, but it is also observable with a coronagraph. The word ""corona"" is a Latin word meaning ""crown"", from the Ancient Greek κορώνη (korōnē, “garland, wreath”).The high temperature of the Sun's corona gives it unusual spectral features, which led some in the 19th century to suggest that it contained a previously unknown element, ""coronium"". Instead, these spectral features have since been explained by highly ionized iron (Fe-XIV). Bengt Edlén, following the work of Grotrian (1939), first identified the coronal lines in 1940 (observed since 1869) as transitions from low-lying metastable levels of the ground configuration of highly ionised metals (the green Fe-XIV line at 5303 Å, but also the red line Fe-X at 6374 Å). These high stages of ionisation indicate a plasma temperature in excess of 1,000,000 kelvin, much hotter than the surface of the sun.Light from the corona comes from three primary sources, which are called by different names although all of them share the same volume of space. The K-corona (K for kontinuierlich, ""continuous"" in German) is created by sunlight scattering off free electrons; Doppler broadening of the reflected photospheric absorption lines completely obscures them, giving the spectral appearance of a continuum with no absorption lines. The F-corona (F for Fraunhofer) is created by sunlight bouncing off dust particles, and is observable because its light contains the Fraunhofer absorption lines that are seen in raw sunlight; the F-corona extends to very high elongation angles from the Sun, where it is called the zodiacal light. The E-corona (E for emission) is due to spectral emission lines produced by ions that are present in the coronal plasma; it may be observed in broad or forbidden or hot spectral emission lines and is the main source of information about the corona's composition.
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