Solar wind

Other related phenomena include the aurora (northern and southern lights), comet tails that always point away from the Sun, and geomagnetic storms that can change the direction of magnetic field lines.

[6] In 1910, British astrophysicist Arthur Eddington essentially suggested the existence of the solar wind, without naming it, in a footnote to an article on Comet Morehouse.

[7] Eddington's proposition was never fully embraced, even though he had also made a similar suggestion at a Royal Institution address the previous year, in which he had postulated that the ejected material consisted of electrons, whereas in his study of Comet Morehouse he had supposed them to be ions.

In the mid-1950s, British mathematician Sydney Chapman calculated the properties of a gas at such a temperature and determined that the corona being such a superb conductor of heat, it must extend way out into space, beyond the orbit of Earth.

As solar gravity weakens with increasing distance from the Sun, the outer coronal atmosphere is able to escape supersonically into interstellar space.

[15] There was strong opposition to Parker's hypothesis on the solar wind; the paper he submitted to The Astrophysical Journal in 1958[15] was rejected by two reviewers, before being accepted by the editor Subrahmanyan Chandrasekhar.

[16][17] In January 1959, the Soviet spacecraft Luna 1 first directly observed the solar wind and measured its strength,[18][19][20] using hemispherical ion traps.

This allowed energetic electrons from the Sun to flow to Earth in narrow beams known as "strahl", which caused a highly unusual "polar rain" event, in which a visible aurora appeared over the North Pole.

[26] The STEREO mission was launched in 2006 to study coronal mass ejections and the solar corona, using stereoscopy from two widely separated imaging systems.

At the same temperature, electrons, due to their much smaller mass, reach escape velocity and build up an electric field that further accelerates ions away from the Sun.

In near-Earth space, the slow solar wind is observed to have a velocity of 300–500 km/s, a temperature of ~100 kilokelvin and a composition that is a close match to the corona.

By contrast, the fast solar wind has a typical velocity of 750 km/s, a temperature of 800 kilokelvin[citation needed] and it nearly matches the composition of the Sun's photosphere.

[clarification needed] The exact coronal structures involved in slow solar wind formation and the method by which the material is released is still under debate.

[49] Both the fast and slow solar wind can be interrupted by large, fast-moving bursts of plasma called coronal mass ejections, or CMEs.

[51] Sheath and ejecta have very different impact on the Earth's magnetosphere and on various space weather phenomena, such as the behavior of Van Allen radiation belts.

[57] The solar wind contributes to fluctuations in celestial radio waves observed on the Earth, through an effect called interplanetary scintillation.

[58] Where the solar wind intersects with a planet that has a well-developed magnetic field (such as Earth, Jupiter or Saturn), the particles are deflected by the Lorentz force.

Fluctuations in its speed, density, direction, and entrained magnetic field strongly affect Earth's local space environment.

For example, the levels of ionizing radiation and radio interference can vary by factors of hundreds to thousands; and the shape and location of the magnetopause and bow shock wave upstream of it can change by several Earth radii, exposing geosynchronous satellites to the direct solar wind.

From the European Space Agency's Cluster mission, a new study has taken place that proposes that it is easier for the solar wind to infiltrate the magnetosphere than previously believed.

This latest discovery occurred through the distinctive arrangement of the four identical Cluster spacecraft, which fly in a controlled configuration through near-Earth space.

As they sweep from the magnetosphere into interplanetary space and back again, the fleet provides exceptional three-dimensional insights on the phenomena that connect the sun to Earth.

The research characterised variances in formation of the interplanetary magnetic field (IMF) largely influenced by Kelvin–Helmholtz instability (which occur at the interface of two fluids) as a result of differences in thickness and numerous other characteristics of the boundary layer.

This study suggests that Kelvin–Helmholtz waves can be a somewhat common, and possibly constant, instrument for the entrance of solar wind into terrestrial magnetospheres under various IMF orientations.

A smaller number of particles from the solar wind manage to travel, as though on an electromagnetic energy transmission line, to the Earth's upper atmosphere and ionosphere in the auroral zones.

Although Mars is larger than Mercury and four times farther from the Sun, it is thought that the solar wind has stripped away up to a third of its original atmosphere, leaving a layer 1/100 as dense as the Earth's.

[63] Mercury, the nearest planet to the Sun, bears the full brunt of the solar wind, and since its atmosphere is vestigial and transient, its surface is bathed in radiation.

The distance to the heliopause is not precisely known and probably depends on the current velocity of the solar wind and the local density of the interstellar medium, but it is far outside Pluto's orbit.

Scientists hope to gain perspective on the heliopause from data acquired through the Interstellar Boundary Explorer (IBEX) mission, launched in October 2008.

The heliopause is noted as one of the ways of defining the extent of the Solar System, along with the Kuiper Belt and the radius at which the Sun's gravitational influence is matched by other stars.

An illustration of the structure of the Sun
Ulysses 's observations of solar wind speed as a function of helio latitude during solar minimum. Slow wind (≈ 400 km/s ) is confined to the equatorial regions, while fast wind (≈ 750 km/s ) is seen over the poles. [ 1 ] Red/blue colors show outward/inward polarities of the heliospheric magnetic field .
Laboratory simulation of the magnetosphere's influence on the solar wind; these aurora-like Birkeland currents were created in a terrella , a magnetised anode globe in an evacuated chamber.
Plot showing a dramatic decrease in the rate of solar wind particle detection by Voyager 1
This is thought to show the solar wind from the star L.L. Orionis generating a bow shock (the bright arc).
CME erupts from Earth's Sun
Parker Solar Probe observed switchbacks — traveling disturbances in the solar wind that caused the magnetic field to bend back on itself.
The heliospheric current sheet results from the influence of the Sun's rotating magnetic field on the plasma in the solar wind.
Schematic of Earth's magnetosphere . The solar wind flows from left to right.
Noon meridian section of magnetosphere
Apollo's SWC experiment
Apollo's Solar Wind Composition Experiment on the Lunar surface
NASA animation of the Parker Solar Probe passing through the Sun's corona. Inside the corona's boundary, its Alfvén surface, plasma waves travel back and forth to the Sun's surface.
An infographic featuring the outer regions of the heliosphere based on results from the Voyager spacecraft