Personal growth      04.11.2021

The passage of starlight through the solar corona. Mystery of the solar corona. This is a star with a middle age

Under the influence of gravity, S., like any star, tends to shrink. This compression is counteracted by the pressure drop resulting from the high temperature and density of the internal. layers C. In the center of C. temperature T ≈ 1.6. 10 7 K, density ≈ 160 gcm -3 . Such a high temperature in the central regions of S. can be maintained for a long time only by the synthesis of helium from hydrogen. These reactions and yavl. main source of energy C.

At temperatures ~10 4 K (chromosphere) and ~10 6 (corona), as well as in the transition layer with intermediate temperatures, ions of various elements appear. The emission lines corresponding to these ions are quite numerous in the short-wavelength region of the spectrum (λ< 1800 . Спектр в этой области состоит из отдельных эмиссионных линий, самые яркие из к-рых - линия водорода L a (1216 ) и линия нейтрального (584 ) и ионизованного (304 ) гелия. Излучение в этих линиях выходит из области эмиссии практически не поглощаясь. Излучение в радио- и рентг. областях сильно зависит от степени солнечной активности, увеличиваясь или уменьшаясь в несколько раз в течение 11-летнего и заметно возрастая при вспышках на Солнце.

Phys. characteristics of different layers are shown in fig. 5 (the lower chromosphere with a thickness of ≈ 1500 km, where the gas is more homogeneous, is conventionally distinguished). The heating of the upper atmosphere of S. - the chromosphere and the corona - may be due to mechanical. the energy carried by the waves arising in the upper part of the convective zone, as well as the dissipation (absorption) of electrical energy. currents generated by the magnet. fields moving along with convective currents.

The existence of a surface convective zone in the north is responsible for a number of other phenomena. Cells of the uppermost tier of the convective zone are observed on the surface of S. in the form of granules (see). Deeper large-scale motions in the second tier of the zone appear as supergranulation cells and a chromospheric network. There are reasons to believe that convection in an even deeper layer is observed in the form of giant structures - cells with larger dimensions than supergranulation.

Large local magnets. fields in the zone ± 30 o from the equator lead to the development of the so-called. active regions with spots included in them. The number of active regions, their position on the disk, and the polarities of sunspots in groups change with a period of ≈ 11.2 years. During the period of an unusually high maximum in 1957-58. activity affected almost the entire solar disk. In addition to strong local fields, there is a weaker large-scale magnetic field in the north. field. This field changes sign with a period of approx. 22 years and near the poles vanishes at maximum solar activity.

With a large flash, enormous energy is released, ~10 31 -10 32 erg (power ~10 29 erg/s). It is drawn from the energy of the magnet. hotspot fields. According to ideas, to-rye have been successfully developing since the 1960s. in the USSR, the interaction of magnetic fluxes gives rise to current sheets. Development in the current sheet can lead to acceleration of particles, and there are trigger (starting) mechanisms that lead to the sudden development of the process.


Rice. 13. Types of impact of a solar flare on the Earth (according to D. X. Menzel).

X-ray radiation and solar cosmic rays coming from the flare (Fig. 13) cause additional ionization of the earth's ionosphere, which affects the propagation conditions of radio waves. The flow of particles ejected during the flare reaches the Earth's orbit in about a day and causes a magnetic storm and auroras on Earth (see , ).

In addition to corpuscular flows generated by flares, there is continuous corpuscular radiation C. It is associated with the outflow of rarefied plasma from the external. areas of the solar corona into interplanetary space - the solar wind. Losses of matter due to the solar wind are small, ≈ 3 . 10 -14 per year, but it represents the main. component of the interplanetary medium.

The solar wind carries a large-scale magnetic field into interplanetary space. field C. The rotation of C. twists the lines of the interplanetary magnetic field. field (IMF) into the Archimedean spiral, which is clearly observed in the plane of the ecliptic. Since the main a feature of a large-scale magnet. fields of S. yavl. two circumpolar regions of opposite polarity and fields adjacent to them, with calm S. the northern hemisphere of interplanetary space is filled with a field of one sign, the southern - of another (Fig. 14). Near the maximum activity, due to a change in the sign of the large-scale solar field, this regular magnetic field is reversed. fields of interplanetary space. Magn. the flows of both hemispheres are separated by a current sheet. With the rotation of S. the Earth is several. days, now above, now below the curved "corrugated" surface of the current sheet, i.e., it enters the IMF, directed now towards the north, now away from it. This phenomenon is called interplanetary magnetic field.

Near the activity maximum, the particle fluxes accelerated during flares have the most effective effect on the Earth's atmosphere and magnetosphere. At the activity decline phase, by the end of the 11-year activity cycle, with a decrease in the number of flares and the development of an interplanetary current sheet, the stationary streams of the enhanced solar wind become more significant. Rotating together with S., they cause geomagnets repeating every 27 days. indignation. This recurrent (repetitive) activity is especially high for even-numbered cycle ends when the magnetic direction is the fields of the solar "dipole" are antiparallel to the earth's.

Lit.:
Martynov D. Ya., Course of General Astrophysics, 3rd ed., M., 1978;
Menzel D. G., Our Sun, trans. from English, M., 1963; Solar and solar-terrestrial physics. Illustrated dictionary of terms, trans. from English, M., 1980;
Shklovsky I. S., Physics of the solar corona, 2nd ed., M., 1962;
Severny A. B., Magnetic fields of the Sun and stars, "UFN", 1966, v. 88, c. 1, p. 3-50; - Solar corona - granulation


We got acquainted with the rotation of the Sun and with the solar-terrestrial mutual-centric motion.
Now let's turn our eyes to the moon!

How does the Moon rotate, how does it move around the planet Earth and in the system of mutual-centrism the Sun - Earth?
Since school course In astronomy, we know that the Moon revolves around the Earth in the same direction as the Earth around its axis. The time of a complete revolution (period of rotation) of the Moon around the Earth relative to the stars is called sidereal or starry month (lat. sidus - star). He makes up 27,32 days.
synodic month, or lunation (Greek synodos - connection) is the period of time between two successive identical phases of the moon or the period of time between successive new moons - averages 29.53 days (709 hours). The synodic month is longer than the sidereal month. The reason for this is the rotation of the Earth (together with the Moon) around the Sun. In 27.32 days, the Moon makes a complete revolution around the Earth, which during this time passes an arc of approximately 27 ° in orbit. More than two days are needed for the Moon to again take the appropriate place relative to the Sun and the Earth, i.e. so that this phase (new moon) comes again.
lunar path (trajectory of the Moon on the celestial sphere), like the solar ecliptic, passes through 12 zodiac constellations. The reason for this is the actual rotation of the Moon around the Earth in a plane that almost coincides with the plane of the orbit of our planet. The angle between the planes of the ecliptic and the monthly lunar path is only 5°9".
The moon rotates on its axis , but it always faces the Earth with the same side, that is, the Moon revolves around the Earth and rotates around own axis synchronized.

How to practically confirm the official statements?

To this end, let us turn to such a phenomenon as an eclipse of the Sun, in which it is the Moon that plays a key role.
Solar eclipse - an astronomical phenomenon, which consists in the fact that the Moon closes (eclipses) the Sun in whole or in part from an observer on Earth. A solar eclipse is possible only on a new moon, when the side of the moon facing the Earth is not illuminated, and the moon itself is not visible. Eclipses are possible only if the new moon occurs near one of the two lunar nodes (points of intersection of the apparent orbits of the Moon and the Sun), no more than about 12 degrees from one of them.
The moon's shadow on the earth's surface does not exceed 270 km in diameter, so a solar eclipse is observed only in a narrow band along the path of the shadow. Since the Moon revolves in an elliptical orbit, the distance between the Earth and the Moon at the time of an eclipse can be different, respectively, the diameter of the moon's shadow spot on the Earth's surface can vary widely from maximum to zero (when the top of the cone of the moon's shadow does not reach the Earth's surface). If the observer is in the shadow band, he sees a total solar eclipse, in which the Moon completely hides the Sun, the sky darkens, and planets and bright stars can appear on it. Around the solar disk hidden by the Moon, one can observe solar corona , which is not visible under the normal bright light of the Sun. Because the temperature of the corona is much higher than that of the photosphere, it has a faint bluish color that is unexpected to first-timers and is very different from the expected color of the Sun. When the eclipse is observed by a stationary ground observer, the total phase lasts no more than a few minutes. The minimum speed of the moon's shadow on the earth's surface is just over 1 km/s. During the full solar eclipse astronauts in orbit can observe the moving shadow of the moon on the surface of the earth.

Let's look at the video, how Wikipedia presents the passage of the Moon through the disk of the sun at a great distance from the Earth.

https://upload.wikimedia.org/wikipedia/commons/transcoded/2/29/Moon_transit_of_sun_large.ogv/Moon_transit_of_sun_large.ogv.480p.vp9.webm
Video 1.

Step by step it looks like this:


Fig 1. The passage of the Moon through the disk of the sun at a great distance from the Earth 25.02.2007 .
The moon passes across the solar disk in the videofrom left to right. It must have been satellite imagery.

How does the Moon's shadow travel across the Earth during an eclipse?

Consider the recent real total solar eclipse!
Total solar eclipse August 21, 2017.
Total solar eclipse on August 21st 2017 is the 22nd eclipse one hundred and forty-fifth Saros.
The region of its best visibility falls in the middle and subtropical latitudes of the northern hemisphere.

Video 2. Animation SZ 21.08.2017
This animation shows that The moon's shadow shifts across the western hemisphere of the Earth, North America from left to right or from west to east.

The eclipse reaches its maximum at the point with coordinates 37°N, 87.7°W, lasts a maximum of 2 minutes 40 seconds, and the width of the moon's shadow on the earth's surface is 115 kilometers. At the moment and at the point of greatest eclipse, the direction to the sun (azimuth) is 198°, and the height of the sun above the horizon is 64°.
dynamic world time at the time of greatest eclipse: 18:26:40, dynamic time correction: 70 seconds.
The axis of the shadow passes between the center of the earth and north pole, the minimum distance from the center of the Earth to the axis of the cone of the lunar shadow is 2785 kilometers. Thus, the Gamma of the eclipse is 0.4367, and the maximum phase reaches 1.0306.

total solar eclipse - a solar eclipse in which the cone of the moon's shadow crosses the earth's surface (the moon is close enough to the earth to completely block the sun). The average length of the moon's shadow is 373320 km, and the distance from the Earth to the Moon on August 21, 2017 is 362,235 km. At the same time, the apparent diameter of the Moon is 1.0306 times greater than the apparent diameter of the solar disk. During a total eclipse, the solar corona, stars and planets that are close to the Sun are visible.


Figure 2. The passage of the moon's shadow across the western hemisphere of the Earth.

Look at the NW in the original, through the eyes of US observers.

https://youtu.be/lzJD7eT2pUE
Video 3.


Fig 3. Phases of the solar eclipse.
(above), gradually covers the Sun, forming its left crescent. Closes completely, then opens the right crescent of the Sun.
We see a picture opposite to that shown in Video and Fig. 1.

2017 total solar eclipse from Idaho Falls, state Idaho, August 21, 2017.

Video 4. NW in Idaho.






Rice. 4,5,6. NW in Idaho.
An interesting breakthrough of the sun's rays after a total eclipse?

Total Solar Eclipse 2017 from Beatrice, Nebraska, August 21, 2017
https://youtu.be/gE3rmKISGu4
Video 5. NW in Nebraska.
Also in these videos, the Moon passes through the Sun from the top right, goes down to the left, revealing the Sun.

Now let's see how telescopes mounted on artificial satellites earth.
Solar eclipse 2017 as seen by Hinode JAXA on August 21, 2017.

Video 6.
The solar observation satellite Hinode captured the partial solar eclipse on August 21, 2017. The images were taken with the X-Ray Telescope (XRT) aboard the Hinode during its flight over Pacific Ocean(off the west coast of the United States). at an altitude of 680 km.

From satellite too The moon "runs over" the sun from the right, only below.

Now consider the movement of the moon's shadow on the globe.

2017 total solar eclipse as observed by DSCOVR EPIC (4K)

Video 7.

NASA's Polychromatic Earth Imaging Camera (EPIC) aboard the NOAA Deep Space Observatory (DSCOVR) captured the total solar eclipse on August 21, 2017 from space.
We see the movement of a shadow on the surface of the western hemisphere. It moves from west to east, ahead of its own rotation of the globe in the same direction!
Still, the picture is not perceived by a living planet; as if the "simulator" reproduces some programmed fragment of the movement. Clouds rotate synchronously with the Earth. Several questions arise: Why do clouds stay the same as the earth rotates? How fast and why does the moon's shadow move in this direction? How long did it take for this shadow to cross America?

Let's look at a nice animation of this solar eclipse.

Video 8. Total solar eclipse 2017.






Rice. 7,8,9. The movement of the lunar shadow across the globe during the SZ on 08/21/2017

ecliptic line - the plane of motion, clearly seen in the eclipse of the Moon and the Sun. We are taught that the eclipse occurs only along the described line.
We are also well aware that the line of the ecliptic does not rise above the Tropic of Cancer (23.5° above the celestial equator) nor does it fall below the Tropic of Capricorn (-23.5° below the celestial equator).
The sun is at its zenith (a point in the celestial sphere located above the observer's head) only in the region of the globe lying between the tropics of Cancer and Capricorn. The tropics are imaginary parallel circles on the surface of the globe, 23 degrees and 27 minutes north and south of the equator. To the north of the equator is the Northern Tropic (aka the Tropic of Cancer), to the south - the Southern Tropic (the Tropic of Capricorn). In the tropics, once a year (June 22 at the Tropic of Cancer and December 22 at the Tropic of Capricorn), the center of the Sun at noon passes through the zenith. Between the tropics lies a region in which the sun is at its zenith twice a year at every point. North of the Tropic of Cancer and south of the Tropic of Capricorn, the Sun never rises to its zenith.

As projected onto the globe, the ecliptic runs between 23.5° north latitude and south latitude, between the Tropics of Cancer and Capricorn.


Rice. 10. Earth, the equator and the tropics of Cancer, Capricorn are indicated.

The question arises: Why do eclipses occur above the Tropic of Cancer and below the Tropic of Capricorn if the Sun's ecliptic is not projected onto these regions?

We look carefully at Fig 6,7,8- animation of the NW, for the shift of the point - the center of the total eclipse of the Sun in North America. This point runs from left to right, from west to east, from the 50th to the 30th parallel north. So the projection of a total eclipse is shadow point movement(the total phase of the eclipse) passes above the Tropic of Cancer, above 23.5 ° north latitude.
Consequently, the assertion that eclipses occur only along the line of the solar ecliptic is refuted!

According to the credits on the animation:
To the state Oregon in the northwest the shadow of the total eclipse was entering 10.15.50 am , 44°53"N, 125°88"W. (Fig. 7)
out of state South Carolina(Charleston) in the southeast the shadow came into 02.48.50 pm (14.48.50) , 32°49"N, 79°03"W. (Fig. 9)
Between these points of order 4000 km. the shadow-point passed in 4 hours 33 minutes ( 16380 sec). So the shadow passed at a speed 0.244 km/s.
According to the data obtained, the complete SZ occurred on a trajectory line much higher than the ecliptic, at a latitude of 32° - 44 ° and above the Tropic of Cancer (23.5°). And we do not take the movement of the penumbra, but only the movement of the point of total eclipse, when the Moon completely covers the Sun. What does it mean? Sun and Moon in this moment are not in the region of the ecliptic if projected onto the 44th degree north latitude on Earth? And the declination of the Sun in the sky at this moment is +12° (see below) above the celestial equator and does not go beyond the boundaries of the tropic. And astronomers know that the declination is fully consistent with the earth's latitude. Are they lying? So, the celestial equator does not coincide with the earth? Why is this happening?

Let's compare with the data of the Astrocalculator.


Screenshot 1. 08/21/2017 observation point 37°N, 87.7°W

The angle between the planes of the ecliptic and the moon's monthly path is small, maximum 5°9".
The ecliptic is indicated by one white line, and the trajectory of the Moon's motion is multiple.
We see that the eclipse occurs at the ascending node of the moon.






Screen 2,3,4. Phases of a solar eclipse. The Moon "runs over" the Sun from the west (right).

The astrocalculator reproduces the sky through the eyes of an observer who is facing south. East on the left, west on the right. We see that the moon is moving to the right (west), “runs into” the sun, we see its left sickle. After the total eclipse we see the right solar crescent. Everything is exactly as in Rice. 3. The Moon and the Sun for the observer move from left to right, from east to west - sunrise, sunset (visibility due to earth's rotation).

On the frames (screenshots) of the calculator, it is noticeable that the Sun and the Moon are on 10 hour meridian(right ascension) in the zodiac constellation Leo, almost next to the star Regulus.


Screenshot 5. SZ occurs in constellation Leo, next to the star Regul.
Sun Declination +11°52".

The earth rotates counterclockwise (from West to East) at a speed 0.465 km/s
The moon revolves around the earth counterclockwise(from West to East)at orbital speed 1,023 km/sec ( divide the orbit length 2x3.14xR (R=384000 km) by a rotation period of 27.32 days).
In Wiki we read: Minimum moon shadow speed on the earth's surface is slightly more 1 km/s. It turns out that the speed of the Moon in orbit is equal to the speed of the moon's shadow on the Earth. More and more linear speed of rotation of the earth around its axis.
Is it so? Above, we have already calculated the speed of the moon's shadow - 0.244 km/s. Speed ​​calculated from the official eclipse animation.
Let's continue the research.


Rice. 5. Solar eclipse.

Let's look closely at this general educational picture of the origin of a solar eclipse.

The direction of the Earth's movement is counterclockwise, from west to east red arrow.
If the moon were static, then the shadow of the moon would shift to opposite side, to the west, black shooters.
However, the Moon is moving in the direction of the Earth's rotation ( along the red arrow), its orbital speed is more than twice the speed of its rotation. That is why the movement of the moon's shadow on the earth's surface from west to east is observed. But with what speed should the shadow move away from the observer on the ground to the left, i.e. towards the east (observer facing south) - the question is open? … open for discussion!

So, let's sum up some results in our study of the motion of the Moon.

The Moon is moving to the left of the stationary stellar sphere (for an observer from the earth facing south), from west to east, in the direction of the rotation of the Earth itself, but faster, at a rate of one revolution in 27.3 days, 13.2 ° per day, or 1,023 km/s D lights up the Sun and "runs" on it from the right during a solar eclipse. This happens because the Sun moves along the signs of the zodiac also to the east, making a full circle in 365.24 days, slower than 1 ° per day.

The shadow of the Moon moves to the left, overtakes the rotation of the Earth, passes along the earth's surface from west to east.

For the observer from the Earth (in the northern hemisphere), the picture of the eclipse itself, the displacement of the luminaries of the Sun and the Moon will occur to the right, to the west, i.e. from sunrise to sunset. This movement is connected with the rotation of the Earth around its axis from west to east.

Some questions raised in the topic remain open, I will be glad to hear answers and justifications.

I myself will try in the next part to clarify these issues, based on the actual rotation of the moon.
To be continued…

Earthly life owes its origin to the heavenly body. It warms and illuminates everything on the surface of our planet. No wonder the worship of the Sun and its representation as a great heavenly god was reflected in the cults of the primitive peoples who inhabited the Earth.

Centuries, millennia have passed, but its importance in human life has only increased. We are all children of the Sun.

What is the Sun?

star from the galaxy Milky Way, his geometric shape, representing a huge, hot, gaseous ball, constantly radiating energy flows. The only source of light and heat in our star-planetary system. Now the Sun is in the age of a yellow dwarf, according to the generally accepted classification of the types of stars in the universe.


Characteristics of the Sun

The sun has the following properties:

  • Age -4.57 billion years;
  • Distance to Earth: 149,600,000 km
  • Mass: 332,982 Earth masses (1.9891 10³⁰ kg);
  • The average density is 1.41 g / cm³ (it increases 100 times from the periphery to the center);
  • The orbital speed of the Sun is 217 km/s;
  • Rotation speed: 1.997 km/s
  • Radius: 695-696 thousand km;
  • Temperature: from 5,778 K on the surface to 15,700,000 K in the core;
  • Corona temperature: ~1,500,000 K;
  • The sun is stable in its brightness, it is in the 15% of the most bright stars our Galaxy. It emits less ultraviolet rays, but has a greater mass compared to similar stars.

What is the sun made of?

In my own way chemical composition our star is no different from other stars and contains: 74.5% hydrogen (by mass), 24.6% helium, less than 1% other substances (nitrogen, oxygen, carbon, nickel, iron, silicon, chromium, magnesium and others). Inside the nucleus, there are continuous nuclear reactions that turn hydrogen into helium. The absolute majority of the mass solar system- 99.87% belongs to the Sun.

Already this Saturday, August 11, 2018, a new mission to study the Sun - the Parker Solar Probe (or the Parker solar probe) will go into space. In a few years, the device will come closer to the Sun than any man-made object has yet managed to do. Editorial N+1 With the help of Sergei Bogachev, chief researcher at the Laboratory of X-ray Solar Astronomy at the Lebedev Physical Institute, she decided to find out why scientists send the device to such a hot place and what results are expected from it.

When we look at the night sky, we see a huge number of stars - the most numerous category of objects in the universe that can be observed from Earth. It is these huge shining gas balls that are produced in their thermonuclear "furnaces" by many chemical elements heavier than hydrogen and helium, without which our planet, and all life on it, and ourselves would not exist.

The stars are at great distances from the Earth - the distance to the nearest of them, Proxima Centauri, is estimated at several light years. But there is one star whose light takes only eight minutes to reach us - this is our Sun, and observing it helps us learn more about other stars in the Universe.

The sun is much closer to us than it seems at first glance. In a certain sense, the Earth is inside the Sun - it is constantly washed by the flow of the solar wind coming from the corona - the outer part of the star's atmosphere. It is the streams of particles and radiation from the Sun that control the "space weather" near the planets. The emergence of auroras and disturbances in the magnetospheres of the planets depends on these streams, while solar flares and coronal mass ejections disable satellites, affect the evolution of life forms on Earth, and determine the radiation load on manned space missions. Moreover, similar processes occur not only in the solar system, but also in other planetary systems. Therefore, understanding the processes in the solar corona and the inner heliosphere allows us to better navigate the behavior of the plasma "ocean" surrounding the Earth.

Structure of the Sun

Wikimedia Commons

“Due to the remoteness of the Sun, we receive almost all information about it through the radiation it generates. Even some simple parameters, such as temperature, which can be measured with an ordinary thermometer on Earth, are determined for the Sun and stars in a much more complicated way - by their radiation spectrum. This also applies to more complex characteristics, such as the magnetic field. The magnetic field is able to influence the radiation spectrum, splitting the lines in it - this is the so-called Zeeman effect. And it is precisely due to the fact that the field changes the radiation spectrum of the star that we are able to register it. If such an influence did not exist in nature, then we would not know anything about the magnetic field of stars, since there is no way to directly fly up to a star, ”says Sergey Bogachev.

“But this method also has limitations - take at least the fact that the absence of radiation deprives us of information. If we talk about the Sun, then the solar wind does not emit light, so there is no way to remotely determine its temperature, density and other properties. Does not emit light or magnetic field. Yes, in the lower layers of the solar atmosphere magnetic tubes are filled with luminous plasma and this makes it possible to measure the magnetic field near the surface of the Sun. However, already at a distance of one solar radius from its surface, such measurements are impossible. And there are many such examples. How to be in such a situation? The answer is very simple: you need to launch probes that can fly directly to the Sun, plunge into its atmosphere and into the solar wind, and take measurements directly on the spot. Such projects are widespread, although less known than those of space telescopes, which make remote observations and provide much more spectacular data (such as photographs) than probes that produce boring streams of numbers and graphs. But if we talk about science, then, of course, few remote observations can be compared in strength and persuasiveness with the study of an object that is located nearby, ”continues Bogachev.

Mysteries of the Sun

Observations of the Sun have been made since Ancient Greece and in Ancient Egypt, and over the past 70 years, more than a dozen space satellites, interplanetary stations and telescopes, ranging from Sputnik-2 to space observatories operating today, such as SDO, SOHO or STEREO, have closely monitored (and are monitoring) the behavior of the closest to us the stars and its surroundings. Nevertheless, astronomers still have many questions related to the structure of the Sun and its dynamics.

For example, for more than 30 years, scientists have been facing the problem of solar neutrinos, which consists in the lack of registered electron neutrinos produced in the core of the Sun as a result of nuclear reactions, compared with their theoretically predicted number. Another mystery is related to the anomalous heating of the corona. This outermost layer of the star's atmosphere has a temperature of more than a million degrees Kelvin, while the visible surface of the Sun (the photosphere), above which the chromosphere and corona are located, is heated to only six thousand degrees Kelvin. This seems strange, because logically, the outer layers of the star should be colder. Direct heat transfer between the photosphere and the corona is not enough to provide these temperatures, which means that other coronal heating mechanisms are at work here.


The corona of the Sun during the total solar eclipse in August 2017.

NASA's Goddard Space Flight Center/Gopalswamy

There are two main theories to explain this anomaly. According to the first one, magnetoacoustic waves and Alfven waves are responsible for heat transfer from the convective zone and photosphere of the Sun to the chromosphere and corona, which, being scattered in the corona, increase the plasma temperature. However, this version has a number of disadvantages, for example, magnetoacoustic waves cannot ensure the transfer of a sufficiently large amount of energy to the corona due to scattering and reflection back to the photosphere, and Alfvén waves convert their energy into thermal plasma energy relatively slowly. In addition, for a long time there was simply no direct evidence of wave propagation through the solar corona - it was not until 1997 that the SOHO space observatory first recorded magnetoacoustic solar waves at a frequency of one millihertz, which provide only ten percent of the energy needed to heat the corona to the observed temperatures.


The second theory relates the anomalous heating of the corona to constantly occurring microflares arising from the continuous reconnection of magnetic lines in local regions of the magnetic field in the photosphere. This idea was proposed in the 1980s by the American astronomer Eugene Parker, whose name is the probe and who also predicted the presence of the solar wind, a stream of high-energy charged particles continuously emitted by the Sun. However, the theory of microoutbursts has not yet been confirmed either. It is possible that both mechanisms work on the Sun, but this needs to be proven, and for this it is necessary to fly up to the Sun at a fairly close distance.

Another secret of the Sun is connected with the corona - the mechanism of the formation of the solar wind that fills the entire solar system. It is on him that such phenomena depend. space weather like northern lights or magnetic storms. Astronomers are interested in the mechanisms of origin and acceleration of the slow solar wind, born in the corona, as well as the role of magnetic fields in these processes. Here too, there are several theories with both evidence and flaws, and it is expected that the Parker probe will help to dot the i's.

“In general, at present, there are sufficiently developed models of the solar wind that predict how its characteristics should change as it moves away from the Sun. The accuracy of these models is quite high at distances of the order of the Earth's orbit, but it is not clear how accurately they describe the solar wind at close distances from the Sun. Perhaps Parker can help with that. Still pretty interest Ask- acceleration of particles on the Sun. After flares, streams of a large number of accelerated electrons and protons come to the Earth. It is not completely clear, however, whether their acceleration occurs directly on the Sun, and then they simply move towards the Earth by inertia, or whether these particles are additionally (and maybe completely) accelerated on their way to the Earth by interplanetary magnetic field. Perhaps, when data collected by a probe near the Sun arrives on Earth, this issue can also be dealt with. There are several other similar problems that can be solved in the same way - by comparing similar measurements near the Sun and at the level of the Earth's orbit. In general, the mission is aimed at solving such issues. We can only hope that the device will be successful,” says Sergey Bogachev.

Straight into hell

The Parker probe will be launched on August 11, 2018 from the launch complex SLC-37 at Cape Canaveral Air Force Base, it will be launched into space by a heavy launch vehicle Delta IV Heavy - this is the most powerful rocket in operation, it can launch into low orbit almost 29 tons of cargo. In terms of carrying capacity, it is surpassed only by, but this carrier is still in the testing stage. To get to the center of the solar system, it is necessary to extinguish the very high speed that the Earth (and all objects on it) has relative to the Sun - about 30 kilometers per second. In addition to a powerful rocket, this will require a series of gravitational maneuvers near Venus.

According to the plan, the process of approaching the Sun will last seven years - with each new orbit (there are 24 in total), the device will come closer to the star. The first perihelion will be passed on November 1, at a distance of 35 solar radii (about 24 million kilometers) from the star. Then, after a series of seven gravitational maneuvers near Venus, the device will approach the Sun to a distance of about 9-10 solar radii (about six million kilometers) - this will happen in mid-December 2024. That's seven times closer than the perihelion of Mercury's orbit, no man-made yet. spacecraft did not get so close to the Sun (the current record belongs to the Helios-B apparatus, which approached the star at 43.5 million kilometers).


Scheme of the flight to the Sun and the main working orbits of the probe.


The main stages of work on each of the orbits.

The choice of such a position for observations is not accidental. According to the calculations of scientists, at a distance of ten radii from the Sun is the Alfven point - the region where the solar wind accelerates so much that it leaves the Sun, and the waves propagating in the plasma no longer affect it. If the probe can be near the Alfven point, then we can assume that it entered the solar atmosphere and touched the Sun.


Probe "Parker" in the assembled state, during installation on the third stage of the launch vehicle.

"The task of the probe is to measure the main characteristics of the solar wind and the solar atmosphere along its trajectory. The scientific instruments on board are not unique, they do not have record characteristics (except for the ability to withstand solar radiation fluxes at the perihelion of the orbit). The Parker Solar Probe is a spacecraft with conventional instruments but in a unique orbit Most (perhaps even all scientific instruments) are planned to be kept off at all parts of the orbit except perihelion, where the spacecraft is closest to the Sun. scientific program additionally emphasizes that the main task of the mission is to study the solar wind and solar atmosphere. When the device moves away from perihelion, the data from the same instruments will turn into ordinary ones, and in order to save the resource of scientific instruments, they will simply be switched to the background until the next approach. In this sense, the ability to reach a given trajectory and the ability to live on it for a given time are the factors on which the success of the mission will primarily depend,” says Sergey Bogachev.


The device of the heat shield "Parker".

Greg Stanley/Johns Hopkins University


View of the heat shield at the stage of installation on the probe.

NASA/Johns Hopkins APL/Ed Whitman


Probe "Parker" with installed heat shield.

NASA/Johns Hopkins APL/Ed Whitman

To survive near the star, the probe is equipped with a heat shield that acts as an "umbrella" under which all scientific instruments will hide. The front of the shield will withstand temperatures in excess of 1,400 degrees Celsius, while the back of the shield, where the scientific instruments are located, must not exceed thirty degrees Celsius. Such a temperature difference is provided by the special design of this "solar umbrella". With a total thickness of just 11.5 centimeters, it consists of two panels made of carbon-graphite composite, between which there is a layer of carbon foam. The front of the shield has a protective coating and a white ceramic layer that increases its reflective properties.


In addition to the shield, the cooling system is designed to solve the problem of overheating, using 3.7 liters of pressurized deionized water as a coolant. The electrical wiring of the apparatus is made using high-temperature materials such as sapphire tubes and niobium, and during approaches to the Sun, the solar panels will be removed under the heat shield. In addition to strong heating, mission engineers will have to take into account strong light pressure from the Sun, which will interfere with the correct orientation of the probe. To facilitate this work, solar sensors are installed on the probe in different places, helping to control the protection of scientific equipment from the influence of the Sun.

Tools

Almost all scientific instruments of the probe are "sharpened" for the study of electromagnetic fields and the properties of the solar plasma surrounding it. The only exception is the optical telescope WISPR (Wide-field Imager for Solar PRobe), whose task will be to obtain images of the solar corona and solar wind, the inner heliosphere, shock waves and any other structures observed by the device.

The corona makes up the outer atmosphere of the Sun, passing in its outermost parts into the interplanetary medium. Outwardly, it looks like a silver and pearl radiance around the Sun. There are many details in it - rays, feathers, fans, arches, etc. During the years of maximum sunspots, the corona surrounds the entire Sun in a rather symmetrical manner and has a generally "disheveled" appearance (Fig. 27). During sunspot minimum years, it is compressed at the poles and extended along the equator (Fig. 28). Thus, to a certain extent, the corona is a product of solar activity.

The solar corona where it touches the chromosphere is incomparably brighter than, say, at a distance of 10-12 from the solar edge, and further on its brightness continues to decrease with height, but very slowly, so that it can be traced in good photographs up to distances from the edge Suns reaching several solar radii.

(click to view scan)

The limit here puts the brightness of the sky background, reaching high level even during very long eclipses. Photos taken during eclipses from high mountains and high-altitude aircraft, show the extension of the corona to a dozen or more degrees from the Sun, where the corona imperceptibly merges with the phenomenon of zodiacal light (see Chapter IX, § 39). The integral brightness of the corona is only one millionth of the brightness of the Sun (from to). Even its brightest parts were previously inaccessible to observations outside of eclipses.

Rice. 29. Fine structure of the inner crown. The photograph was taken outside the eclipse with a Lyot coronagraph in the light of the green coronal line

In spectral terms, the solar corona contains three components: L, K and F, L is an emission component consisting of two to three dozen bright lines extending to a height of about 9. These lines are visible against the background of the K-component - a continuous spectrum. At a height of about 3 from the edge of the Sun, a small amount of the F component, i.e., the Fraunhofer spectrum, qualitatively no different from the spectrum of the solar photosphere, begins to be mixed into the K spectrum. The F-spectrum is very clearly visible already at height 10, where the L-spectrum ends, and this height is considered the boundary of the inner corona (Fig. 29). Above lies the outer corona, whose spectrum at a height of 20 and more consists mainly of the F component. The integrated brightness of the F component is about the brightness of the Sun.

The light from the inner corona is markedly polarized. After a height of 10 above the edge, the polarization, reaching a value of about 45%, rapidly decreases.

We can assume that the K-component is polarized, while the F-component is not. The polarization is such that electric vector polarized component of light is perpendicular to the radius vector (in the picture plane) emanating from the center of the Sun.

The duration of observations of the solar corona during an eclipse along the entire band of the total phase is usually 2-3 hours. During this time, only the most insignificant movements are detected in the corona. But if the corona is systematically observed outside of eclipses on a Lyo coronograph, it is not difficult to notice changes in the corona from one day to the next. The repetition of the shape of the isophotes of the L-corona in the light of one or another line, as well as a steadily repeating increase in its radiation after about two weeks (the isophotes that were on one edge are transferred to the other edge of the Sun) and after four weeks (the isophotes are repeated on this edge) made it possible establish with full confidence the fact of the rotation of the corona and find the period of its rotation - it coincided with the period of rotation of the Sun, derived from sunspots and torches. Coronal formations, spots and plumes are inextricably linked.