Magnetosphere of Jupiter

Magnetosphere of Jupiter

Discovery[1]
Discovered by	Pioneer 10
Discovery date	December 1973
Internal field[2][3][4]
Radius of Jupiter	71,492 km
Magnetic moment	1.56 × 1020 T·m3
Equatorial field strength	428 μT (4.28 G)
Dipole tilt	~10°
Magnetic pole longitude	~159°
Rotation period	9h 55m 29.7 ± 0.1s
Solar wind parameters[5]
Speed	400 km/s
IMF strength	1 nT
Density	0.4 cm−3
Magnetospheric parameters[6][7][8]
Bow shock distance	~82 Rj
Magnetopause distance	50–100 Rj
Magnetotail length	up to 7000 Rj
Main ions	O+, S+ and H+
Plasma sources	Io, Solar wind, ionosphere
Mass loading rate	~1000 kg/s
Maximum plasma density	2000 cm−3
Maximum particle energy	up to 100 MeV
Aurora[9]
Spectrum	radio, near-IR, UV and X-ray
Total power	100 TW
Radio emission frequencies	0.01–40 MHz

The magnetosphere of Jupiter is the cavity created in the solar wind by the planet's magnetic field. Extending up to seven million kilometers in the Sun's direction and almost to the orbit of Saturn in the opposite direction, Jupiter's magnetosphere is the largest and most powerful of any planetary magnetosphere in the Solar System, and by volume the largest known continuous structure in the Solar System after the heliosphere. Wider and flatter than the Earth's magnetosphere, Jupiter's is stronger by an order of magnitude, while its magnetic moment is roughly 18,000 times larger. The existence of Jupiter's magnetic field was first inferred from observations of radio emissions at the end of the 1950s and was directly observed by the Pioneer 10 spacecraft in 1973.

Jupiter's internal magnetic field is generated by electrical currents flowing in the planet's outer core, which is composed of metallic hydrogen. Volcanic eruptions on Jupiter's moon Io eject large amounts of sulfur dioxide gas into space, forming a large torus around the planet. Jupiter's magnetic field forces the torus to rotate with the same angular velocity and direction as the planet. The torus in turn loads the magnetic field with plasma, in the process stretching it into a pancake-like structure called a magnetodisk. In effect, Jupiter's magnetosphere is shaped by Io's plasma and its own rotation, rather than by the solar wind like Earth's magnetosphere. Strong currents flowing in the magnetosphere generate permanent aurorae around the planet's poles and intense variable radio emissions, which means that Jupiter can be thought of as a very weak radio pulsar. Jupiter's aurorae have been observed in almost all parts of the electromagnetic spectrum including infrared, visible, ultraviolet and soft X-rays.

The action of the magnetosphere traps and accelerates particles, producing intense belts of radiation similar to Earth's Van Allen belts, but thousands of times stronger. The interaction of energetic particles with the surfaces of Jupiter's largest moons markedly affects their chemical and physical properties. Those same particles also affect and are affected by the motions of the particles within Jupiter's tenuous planetary ring system. Radiation belts present a significant hazard for spacecraft and potentially to human space travellers.

Structure

Jupiter's magnetosphere is a complex structure comprising a bow shock, magnetosheath, magnetopause, magnetotail, magnetodisk and other components. The magnetic field around Jupiter emanates from a number of different sources, including fluid circulation at the planet's core (the internal field), electrical currents in the plasma surrounding Jupiter and the currents flowing at the boundary of the planet's magnetosphere. The magnetosphere is embedded within the plasma of the solar wind, which carries the interplanetary magnetic field.^[10]

Internal magnetic field

The bulk of Jupiter's magnetic field, like Earth's, is generated by an internal dynamo supported by the circulation of a conducting fluid in its outer core. But whereas Earth's core is made of molten iron and nickel, Jupiter's is composed of metallic hydrogen.^[3] As with Earth's, Jupiter's magnetic field is mostly a dipole, with north and south magnetic poles at the ends of a single magnetic axis.^[2] However, on Jupiter the north pole of the dipole is located in the planet's northern hemisphere and the south pole of the dipole lies in its southern hemisphere, opposite to the Earth, whose north pole lies in the southern hemisphere and south pole lies in the northern hemisphere.^{[11][note 1]} Jupiter's field also has quadrupole, octupole and higher components, though they are less than one tenth as strong as the dipole component.^[2]

The dipole is tilted roughly 10° from Jupiter's axis of rotation; the tilt is similar to that of the Earth (11.3°).^[1][2] Its equatorial field strength is about 428 μT (4.28 G), which corresponds to a dipole magnetic moment of about 1.53 × 10²⁰ T·m³. This makes Jupiter's magnetic field 10 times stronger than Earth's, and its magnetic moment about 18,000 times larger.^{[3][note 2]} Jupiter's magnetic field rotates at the same speed as the region below its atmosphere, with a period of 9 h 55 m. No changes in its strength or structure have been observed since the first measurements were taken by the Pioneer spacecraft in the mid-1970s.^{[note 3]}

Size and shape

Jupiter's internal magnetic field prevents the solar wind, a stream of ionized particles emitted by the Sun, from interacting directly with its atmosphere, and instead diverts it away from the planet, effectively creating a cavity in the solar wind flow, called a magnetosphere, composed of a plasma different from that of the solar wind.^[6] The Jovian (i.e. pertaining to Jupiter) magnetosphere is so large that the Sun and its visible corona would fit inside it with room to spare.^[12] If one could see it from Earth, it would appear five times larger than the full moon in the sky despite being nearly 1700 times farther away.^[12]

As with Earth's magnetosphere, the boundary separating the denser and colder solar wind's plasma from the hotter and less dense one within Jupiter's magnetosphere is called the magnetopause.^[6] The distance from the magnetopause to the center of the planet is from 45 to 100 R_j (where R_j=71,492 km is the radius of Jupiter) at the subsolar point—the unfixed point on the surface at which the Sun would appear directly overhead to an observer.^[6] The position of the magnetopause depends on the pressure exerted by the solar wind, which in turn depends on solar activity.^[13] In front of the magnetopause (at a distance from 80 to 130 R_j from the planet's center) lies the bow shock, a wake-like disturbance in the solar wind caused by its collision with the magnetosphere.^[14][15] The region between the bow shock and magnetopause is called the magnetosheath.^[6]

An artist's concept of a magnetosphere, where plasmasphere (7) refers to the plasma torus and sheet

At the opposite side of the planet, the solar wind stretches Jupiter's magnetic field lines into a long, trailing magnetotail, which sometimes extends well beyond the orbit of Saturn.^[16] The structure of Jupiter's magnetotail is similar to Earth's. It consists of two lobes (blue areas in the figure), with the magnetic field in the southern lobe pointing toward Jupiter, and that in the northern lobe pointing away from it. The lobes are separated by a thin layer of plasma called the tail current sheet (orange layer in the middle).^[16] Like Earth's, the Jovian tail is a channel through which solar plasma enters the inner regions of the magnetosphere, where it is heated and forms the radiation belts at distances closer than 10 R_j from Jupiter.^[17]

The shape of Jupiter's magnetosphere described above is sustained by the neutral sheet current (also known as the magnetotail current), which flows with Jupiter's rotation through the tail plasma sheet, the tail currents, which flow against Jupiter's rotation at the outer boundary of the magnetotail, and the magnetopause currents (or Chapman-Ferraro currents), which flow against rotation along the dayside magnetopause.^[11] These currents create the magnetic field that cancels the internal field outside the magnetosphere.^[16] They also interact substantially with the solar wind.^[11]

Jupiter's magnetosphere is traditionally divided into three parts: the inner, middle and outer magnetosphere. The inner magnetosphere is located at distances closer than 10 R_j from the planet. The magnetic field within it remains approximately dipole, because contributions from the currents flowing in the magnetospheric equatorial plasma sheet are small. In the middle (between 10 and 40 R_j) and outer (further than 40 R_j) magnetospheres, the magnetic field is not a dipole, and is seriously disturbed by its interaction with the plasma sheet (see magnetodisk below).^[6]

Role of Io

Io's interaction with Jupiter's magnetosphere. The Io plasma torus is in yellow.

Although overall the shape of Jupiter's magnetosphere resembles that of the Earth's, closer to the planet its structure is very different.^[13] Jupiter's volcanically active moon Io is a strong source of plasma in its own right, and loads Jupiter's magnetosphere with as much as 1,000 kg of new material every second.^[7] Strong volcanic eruptions on Io emit huge amounts of sulfur dioxide, a major part of which is dissociated into atoms and ionized by the solar ultraviolet radiation, producing ions of sulfur and oxygen: S⁺, O⁺, S²⁺ and O²⁺.^[18] These ions escape from the satellite's atmosphere and form the Io plasma torus: a thick and relatively cool ring of plasma encircling Jupiter, located near the moon's orbit.^[7] The plasma temperature within the torus is 10–100 eV (100,000–1,000,000 K), which is much lower than that of the particles in the radiation belts—10 keV (100 million K). The plasma in the torus is forced into co-rotation with Jupiter, meaning both share the same period of rotation.^[19] The Io torus fundamentally alters the dynamics of the Jovian magnetosphere.^[20]

As a result of several processes—diffusion and interchange instability being the main escape mechanisms—the plasma slowly leaks away from Jupiter.^[19] As the plasma moves further from the planet, the radial currents flowing within it gradually increase its velocity, maintaining co-rotation.^[6] These radial currents are also the source of the magnetic field's azimuthal component, which as a result bends back against the rotation.^[21] The particle number density of the plasma decreases from around 2,000 cm⁻³ in the Io torus to about 0.2 cm⁻³ at a distance of 35 R_j.^[22] In the middle magnetosphere, at distances greater than 20 R_j from Jupiter, co-rotation gradually breaks down and the plasma begins to rotate more slowly than the planet.^[6] Eventually at the distances greater than 40 R_j (in the outer magnetosphere) this plasma escapes the magnetic field completely and leaves the magnetosphere through the magnetotail.^[23] As cold, dense plasma moves outward, it is replaced by hot, low-density plasma (temperature 20 keV (200 million K) or higher) moving from the outer magnetosphere.^[22] This plasma, adiabatically heated as it approaches Jupiter,^[24] forms the radiation belts in Jupiter's inner magnetosphere.^[7]

Magnetodisk

While Earth's magnetic field is roughly teardrop-shaped, Jupiter's is flatter, more closely resembling a disk, and "wobbles" periodically about its axis.^[25] The main reasons for this disk-like configuration are the centrifugal force from the co-rotating plasma and thermal pressure of hot plasma, both of which act to stretch Jupiter's magnetic field lines, forming a flattened pancake-like structure, known as the magnetodisk, at the distances greater than 20 R_j from the planet.^[6][26] The magnetodisk has a thin current sheet at the middle plane,^[18] approximately near the magnetic equator. The magnetic field lines point away from Jupiter above the sheet and towards Jupiter below it.^[13] The load of plasma from Io greatly expands the size of the Jovian magnetosphere, because the magnetodisk creates an additional internal pressure which balances the pressure of the solar wind.^[14] In the absence of Io the distance from the planet to the magnetopause at the subsolar point would be no more than 42 R_j, whereas it is actually 75 R_j on average.^[6]

The configuration of the magnetodisk's field is maintained by the azimuthal ring current (not an analog of Earth's ring current), which flows with rotation through the equatorial plasma sheet.^[27] The Lorentz force resulting from the interaction of this current with the planetary magnetic field creates a centripetal force, which keeps the co-rotating plasma from escaping the planet. The total ring current in the equatorial current sheet is estimated at 90–160 million amperes.^[6][21]

Dynamics

Co-rotation and radial currents

The magnetic field of Jupiter and co-rotation enforcing currents

The main driver of Jupiter's magnetosphere is the planet's rotation.^[28] In this respect Jupiter is similar to a device called a Unipolar generator. When Jupiter rotates, its ionosphere moves relatively to the dipole magnetic field of the planet. Because the dipole magnetic moment points in the direction of the rotation,^[11] the Lorentz force, which appears as a result of this motion, drives negatively charged electrons to the poles, while positively charged ions are pushed towards the equator.^[29] As a result, the poles become negatively charged and the regions closer to the equator become positively charged. Since the magnetosphere of Jupiter is filled with highly conductive plasma, the electrical circuit is closed through it.^[29] A current called the direct current^{[note 4]} flows along the magnetic field lines from the ionosphere to the equatorial plasma sheet. This current then flows radially away from the planet within the equatorial plasma sheet and finally returns to the planetary ionosphere from the outer reaches of the magnetosphere along the field lines connected to the poles. The currents that flow along the magnetic field lines are generally called field-aligned or Birkeland currents.^[21] The radial current interacts with the planetary magnetic field, and the resulting Lorentz force accelerates the magnetospheric plasma in the direction of planetary rotation. This is the main mechanism that maintains co-rotation of the plasma in Jupiter's magnetosphere.^[29]

The current flowing from the ionosphere to the plasma sheet is especially strong when the corresponding part of the plasma sheet rotates slower than the planet.^[29] As mentioned above, co-rotation breaks down in the region located between 20 and 40 R_j from Jupiter. This region corresponds to the magnetodisk, where the magnetic field is highly stretched.^[30] The strong direct current flowing into the magnetodisk originates in a very limited latitudinal range of about 16 ± 1° from the Jovian magnetic poles. These narrow circular regions correspond to Jupiter's main auroral ovals. (See below.)^[31] The return current flowing from the outer magnetosphere beyond 50 R_j enters the Jovian ionosphere near the poles, closing the electrical circuit. The total radial current in the Jovian magnetosphere is estimated at 60 million–140 million amperes.^[21][29]

The acceleration of the plasma into the co-rotation leads to the transfer of energy from the Jovian rotation to the kinetic energy of the plasma.^[6][20] In that sense, the Jovian magnetosphere is powered by the planet's rotation, whereas the Earth's magnetosphere is powered mainly by the solar wind.^[20]

Interchange instability and reconnection

The main problem encountered in deciphering the dynamics of the Jovian magnetosphere is the transport of heavy cold plasma from the Io torus at 6 R_j to the outer magnetosphere at distances of more than 50 R_j.^[30] The precise mechanism of this process is not known, but it is hypothesized to occur as a result of plasma diffusion due to interchange instability. The process is similar to the Rayleigh-Taylor instability in hydrodynamics.^[19] In the case of the Jovian magnetosphere, centrifugal force plays the role of gravity; the heavy liquid is the cold and dense Ionian (i.e. pertaining to Io) plasma, and the light liquid is the hot, much less dense plasma from the outer magnetosphere.^[19] The instability leads to an exchange between the outer and inner parts of the magnetosphere of flux tubes filled with plasma. The buoyant empty flux tubes move towards the planet, while pushing the heavy tubes, filled with the Ionian plasma, away from Jupiter.^[19] This interchange of flux tubes is a form of magnetospheric turbulence.^[32]

The magnetosphere of Jupiter as viewed from above the north pole^[33]

This highly hypothetical picture of the flux tube exchange was partly confirmed by the Galileo spacecraft, which detected regions of sharply reduced plasma density and increased field strength in the inner magnetosphere.^[19] These voids may correspond to the almost empty flux tubes arriving from the outer magnetosphere. In the middle magnetosphere, Galileo detected so-called injection events, which occur when hot plasma from the outer magnetosphere impacts the magnetodisk, leading to increased flux of energetic particles and a strengthened magnetic field.^[34] No mechanism is yet known to explain the transport of cold plasma outward.

When flux tubes loaded with the cold Ionian plasma reach the outer magnetosphere, they go through a reconnection process, which separates the magnetic field from the plasma.^[30] The former returns to the inner magnetosphere in the form of flux tubes filled with hot and less dense plasma, while the latter are probably ejected down the magnetotail in the form of plasmoids—large blobs of plasma. The reconnection processes may correspond to the global reconfiguration events also observed by the Galileo probe, which occurred regularly every 2–3 days.^[35] The reconfiguration events usually included rapid and chaotic variation of the magnetic field strength and direction, as well as abrupt changes in the motion of the plasma, which often stopped co-rotating and began flowing outward. They were mainly observed in the dawn sector of the night magnetosphere.^[35] The plasma flowing down the tail along the open field lines is called the planetary wind.^[18][36]

The reconnection events are analogues to the magnetic substorms in the Earth's magnetosphere.^[30] The difference seems to be their respective energy sources: terrestrial substorms involve storage of the solar wind's energy in the magnetotail followed by its release through a reconnection event in the tail's neutral current sheet. The latter also creates a plasmoid which moves down the tail.^[37] Conversely, in Jupiter's magnetosphere the rotational energy is stored in the magnetodisk and released when a plasmoid separates from it.^[35]

Influence of the solar wind

Whereas the dynamics of Jovian magnetosphere mainly depend on internal sources of energy, the solar wind probably has a role as well,^[38] particularly as a source of high-energy protons.^{[note 5][7]} The structure of the outer magnetosphere shows some features of a solar wind-driven magnetosphere, including a significant dawn–dusk asymmetry.^[21] In particular, magnetic field lines in the dusk sector are bent in the opposite direction to those in the dawn sector.^[21] In addition, the dawn magnetosphere contains open field lines connecting to the magnetotail, whereas in the dusk magnetosphere, the field lines are closed.^[16] All these observations indicate that a solar wind driven reconnection process, known on Earth as the Dungey cycle, may also be taking place in the Jovian magnetosphere.^[30][38]

The extent of the solar wind's influence on the dynamics of Jupiter's magnetosphere is currently unknown;^[39] however, it could be especially strong at times of elevated solar activity.^[40] The auroral radio,^[4] optical and X-ray emissions,^[41] as well as synchrotron emissions from the radiation belts all show correlations with solar wind pressure, indicating that the solar wind may drive plasma circulation or modulate internal processes in the magnetosphere.^[35]

Emissions

Aurorae

Image of Jupiter's northern aurorae, showing the main auroral oval, the polar emissions, and the spots generated by the interaction with Jupiter's natural satellites

Jupiter demonstrates bright, persistent aurorae around both poles. Unlike Earth's aurorae, which are transient and only occur at times of heightened solar activity, Jupiter's aurorae are permanent, though their intensity varies from day to day. They consist of three main components: the main ovals, which are bright, narrow (less than 1000 km in width) circular features located at approximately 16° from the magnetic poles;^[42] the satellites' auroral spots, which correspond to the footprints of the magnetic field lines connecting Jupiter's ionosphere with those of its largest moons, and transient polar emissions situated within the main ovals.^[42][43] Whereas the auroral emissions were detected in almost all parts of the electromagnetic spectrum from radio waves to X-rays (up to 3 keV), they are brightest in the mid-infrared (wavelength 3–4 μm and 7–14 μm) and deep ultraviolet spectral regions (wavelength 80–180 nm).^[9]

The main ovals are the dominant part of the Jovian aurorae. They have stable shapes and locations,^[43] but their intensities are strongly modulated by the solar wind pressure—the stronger solar wind, the weaker the aurorae.^[44] As mentioned above, the main ovals are maintained by the strong influx of electrons accelerated by the electric potential drops between the magnetodisk plasma and the Jovian ionosphere.^[45] These electrons carry field aligned currents, which maintain the plasma's co-rotation in the magnetodisk.^[30] The potential drops develop because the sparse plasma outside the equatorial sheet can only carry a current of a limited strength without those currents.^[31] The precipitating electrons have energy in the range 10–100 keV and penetrate deep into the atmosphere of Jupiter, where they ionize and excite molecular hydrogen causing ultraviolet emission.^[46] The total energy input into the ionosphere is 10–100 TW.^[47] In addition, the currents flowing in the ionosphere heats it by the process known as Joule heating. This heating, which produces up to 300 TW of power, is responsible for the strong infrared radiation from the Jovian aurorae and partially for the heating of the thermosphere of Jupiter.^[48]

Power emitted by Jovian aurorae in different parts of spectrum^[49]

Emission	Jupiter	Io spot
Radio (KOM, <0.3 MHz)	~1 GW	?
Radio (HOM, 0.3–3 MHz)	~10 GW	?
Radio (DAM, 3–40 MHz)	~100 GW	0.1–1 GW (Io-DAM)
IR (hydrocarbons, 7–14 μm)	~40 TW	30–100 GW
IR (H3+, 3–4 μm)	4–8 TW
Visible (0.385–1 μm)	10–100 GW	0.3 GW
UV (80–180 nm)	2–10 TW	~50 GW
X-ray (0.1–3 keV)	1–4 GW	?

Spots were found to correspond to three Galilean moons: Io, Europa and Ganymede.^{[note 6][50]} They develop because the co-rotation of the plasma is slowed in the vicinity of moons. The brightest spot belongs to Io, which is the main source of the plasma in the magnetosphere (see above). The Ionian auroral spot is thought to be related to Alfven currents flowing from the Jovian to Ionian ionosphere. Europa's and Ganymede's spots are much dimmer, because these moons are weak plasma sources, because of sublimation of the water ice from their surfaces.^[51]

Bright arcs and spots sporadically appear within the main ovals. These transient phenomena are thought to be related to interaction with the solar wind.^[43] The magnetic field lines in this region are believed to be open or to map onto the magnetotail.^[43] The secondary ovals observed inside the main oval may be related to the boundary between open and closed magnetic field lines or to the polar cusps.^[52] The polar auroral emissions are similar to those observed around Earth's poles: both appear when electrons are accelerated towards the planet by potential drops, during reconnection of solar magnetic field with that of the planet.^[30] The regions within both main ovals emit most of auroral X-rays. The spectrum of the auroral X-ray radiation consists of spectral lines of highly ionized oxygen and sulfur, which probably appear when energetic (hundreds of kiloelectronvolts) S and O ions precipitate into the polar atmosphere of Jupiter. The source of this precipitation remains unknown.^[41]

Jupiter as a pulsar

Jupiter is a powerful source of radio waves in the spectral region stretching from several kilohertz to tens of megahertz. Radio waves with frequencies of less than about 0.3 MHz (and thus wavelengths longer than 1 km) are called the Jovian kilometric radiation or KOM. Those with frequencies in the interval of 0.3–3 MHz (with wavelengths of 100–1000 m) are called the hectometric radiation or HOM, while emissions in the range 3–40 MHz (with wavelengths of 10–100 m) are referred to as the decametric radiation or DAM. The latter radiation was the first to be observed from the Earth, and its approximately 10 hour periodicity helped to identify it as originating from Jupiter. The strongest part of decametric emission, which is related to Io and to the Io–Jupiter current system, is called Io-DAM.^{[53][note 7]}

The spectrum of Jovian radio emissions compared with spectra of four other magnetized planets, where (N,T,S,U)KR means (Neptunian, Terrestrial, Saturnian and Uranian) kilometric radiation

The majority of these emissions are thought to be produced by a mechanism called Cyclotron Maser Instability, which develops close to the auroral regions, when electrons bounce back and forth between the poles. The electrons involved in the generation of radio waves are probably those carrying currents from the poles of the planet to the magnetodisk.^[54] The intensity of Jovian radio emissions usually varies smoothly with time; however, Jupiter periodically emits short and powerful bursts (S bursts), which can outshine all other components. The total emitted power of the DAM component is about 100 GW, while the power of all other HOM/KOM components is about 10 GW. In comparison, the total power of Earth's radio emissions is about 0.1 GW.^[53]

Jupiter's radio and particle emissions are strongly modulated by its rotation, which makes the planet somewhat similar to a pulsar.^[55] This periodical modulation is probably related to asymmetries in the Jovian magnetosphere, which are caused by the tilt of the magnetic moment with respect to the rotational axis as well as by high-latitude magnetic anomalies. The physics governing Jupiter's radio emissions is similar to that of radio pulsars. They differ only in the scale, and Jupiter can be considered a very small radio pulsar too.^[55] In addition, Jupiter's radio emissions strongly depend on solar wind pressure and, hence, on solar activity.^[53]

In addition to relatively long-wavelength radiation, Jupiter also emits synchrotron radiation (also known as the Jovian decimetric radiation or DIM radiation) with frequencies in the range of 0.1–15 GHz (wavelength from 3 m to 2 cm),^[56] which is the bremsstrahlung radiation of the relativistic electrons trapped in the inner radiation belts of the planet. The energy of the electrons that contribute to the DIM emissions is from 0.1 to 100 MeV,^[57] while the leading contribution comes from the electrons with energy in the range 1–20 MeV.^[8] This radiation is well-understood and was used since the beginning of 1960s to study the structure of the planet's magnetic field and radiation belts.^[58] The particles in the radiation belts originate in the outer magnetosphere and are adiabatically accelerated, when they are transported to the inner magnetosphere.^[24]

Jupiter's magnetosphere ejects streams of high-energy electrons and ions (energy up to tens megaelectronvolts), which travel as far as the Earth's orbit.^[59] These streams are highly collimated and vary with the rotational period of the planet like the radio emissions. In this respect as well, Jupiter shows similarity to a pulsar.^[55]

Interaction with rings and moons

See also: Rings of Jupiter, Ganymedian magnetosphere, and Space weathering

Jupiter's extensive magnetosphere envelops its ring system and the orbits of all four Galilean satellites.^[60] Orbiting near the magnetic equator, these bodies serve as sources and sinks of magnetospheric plasma, while energetic particles from the magnetosphere alter their surfaces. The particles sputter off material from the surfaces and create chemical changes via radiolysis.^[61] The plasma's co-rotation with the planet means that the plasma preferably interacts with the moons' trailing hemispheres, causing noticeable hemispheric asymmetries.^[62] In addition, the large internal magnetic fields of the moons contribute to the Jovian magnetic field.^[60]

Jupiter's variable radiation belts

Close to Jupiter, the planet's rings and small moons absorb high-energy particles (energy above 10 keV) from the radiation belts.^[63] This creates noticeable gaps in the belts' spatial distribution and affects the decimetric synchrotron radiation. In fact, the existence of Jupiter's rings was first hypothesized on the basis of data from the Pioneer 11 spacecraft, which detected a sharp drop in the number of high-energy ions close to the planet.^[63] The planetary magnetic field strongly influences the motion of sub-micrometer ring particles as well, which acquire an electrical charge under the influence of solar ultraviolet radiation. Their behavior is similar to that of co-rotating ions.^[64] The resonant interaction between the co-rotation and the orbital motion is thought to be responsible for the creation of Jupiter's innermost halo ring (located between 1.4 and 1.71 R_j), which consists of sub-micrometer particles on highly inclined and eccentric orbits.^[65] The particles originate in the main ring; however, when they drift toward Jupiter, their orbits are modified by the strong 3:2 Lorentz resonance located at 1.71 R_j, which increases their inclinations and eccentricities.^{[note 8]} Another 2:1 Lorentz resonance at 1.4 Rj defines the inner boundary of the halo ring.^[66]

All Galilean moons have thin atmospheres with surface pressures in the range 0.01–1 nbar, which in turn support substantial ionospheres with electron densities in the range of 1,000–10,000 cm⁻³.^[60] The co-rotational flow of cold magnetospheric plasma is partially diverted around them by the currents induced in their ionospheres, creating wedge-shaped structures known as Alfven wings.^[67] The interaction of the large moons with the co-rotational flow is similar to the interaction of the solar wind with the non-magnetized planets like Venus, although the co-rotational speed is usually subsonic (the speeds vary from 74 to 328 km/s), which prevents the formation of a bow shock.^[68] The pressure from the co-rotating plasma continuously strips gases from the moons' atmospheres (especially from that of Io), and some of these atoms are ionized and brought into co-rotation. This process creates gas and plasma tori in the vicinity of moons' orbits with the Ionian torus being the most prominent.^[60] In effect, the Galilean moons (mainly Io) serve as the principal plasma sources in Jupiter's inner and middle magnetosphere. Meanwhile the energetic particles are largely unaffected by the Alfven wings and have free access to the moons' surfaces (except Ganymede's).^[69]

Plasma tori created by Io and Europa

The icy Galilean moons, Europa, Ganymede and Callisto, all generate induced magnetic moments in response to changes in Jupiter's magnetic field. These varying magnetic moments create dipole magnetic fields around them, which act to compensate for changes in the ambient field.^[60] The induction is thought to take place in subsurface layers of salty water, which are likely to exist in all of Jupiter's large icy moons. These underground oceans can potentially harbor life, and evidence for their presence was one of the most important discoveries made in the 1990s by spacecraft.^[70]

The interaction of the Jovian magnetosphere with Ganymede, which has an intrinsic magnetic moment, differs from its interaction with the non-magnetized moons.^[70] Ganymede's internal magnetic field carves a cavity inside Jupiter's magnetosphere with a diameter of approximately two Ganymede diameters, creating a mini-magnetosphere within Jupiter's magnetosphere. Ganymede's magnetic field diverts the co-rotating plasma flow around its magnetosphere. It also protects the moon's equatorial regions, where the field lines are closed, from energetic particles. The latter can still freely strike Ganymede's poles, where the field lines are open.^[71] Some of the energetic particles are trapped near the equator of Ganymede, creating mini-radiation belts.^[72] Energetic electrons entering its thin atmosphere are responsible for the observed Ganymedian polar aurorae.^[71]

Charged particles have a considerable influence on the surface properties of Galilean moons. Plasma originating from Io carries sulfur and sodium ions farther from the planet,^[73] where they are implanted preferentially on the trailing hemispheres of Europa and Ganymede.^[74] On Callisto however, for unknown reasons, sulfur is concentrated on the leading hemisphere.^[75] Plasma may also be responsible for darkening the moons' trailing hemispheres (again, except Callisto's).^[62] Energetic electrons and ions, with the flux of the latter being more isotropic, bombard surface ice, sputtering atoms and molecules off and causing radiolysis of water and other chemical compounds. The energetic particles break water into oxygen and hydrogen, maintaining the thin oxygen atmospheres of the icy moons (since the hydrogen escapes more rapidly). The compounds produced radiolytically on the surfaces of Galilean moons also include ozone and hydrogen peroxide.^[76] If organics or carbonates are present, carbon dioxide, methanol and carbonic acid can be produced as well. In the presence of sulfur, likely products include sulfur dioxide, hydrogen disulfide and sulfuric acid.^[76] Oxidants produced by radiolysis, like oxygen and ozone, may be trapped inside the ice and carried downward to the oceans over geologic time intervals, thus serving as a possible energy source for life.^[73]

Discovery

The path of the Ulysses spacecraft through the magnetosphere of Jupiter in 1992

It has been suggested that the radio emissions from Jupiter's magnetosphere may have been first heard by Nikola Tesla in 1899, when he claimed to have possibly received radio signals from Martians. As early radio receivers were very broadband (as waveband filters were not common until the 1920s), it would have been possible for the Jovian shortwave emissions to have been received by Tesla. Tesla confusing the emissions as coming from Mars may have been due to Mars and Jupiter being located close to each other in the sky at the time.^[77] The first evidence for the existence of Jupiter's magnetic field came in 1955, with the discovery of the decametric radio emission or DAM.^[78] As the DAM's spectrum extended up to 40 MHz, astronomers concluded that Jupiter must possess a magnetic field with a strength of about 1 milliteslas (10 gauss).^[56]

In 1959, observations in the microwave part of the electromagnetic (EM) spectrum (0.1–10 GHz) led to the discovery of the Jovian decimetric radiation (DIM) and the realization that it was synchrotron radiation emitted by relativistic electrons trapped in the planet's radiation belts.^[79] These synchrotron emissions were used to estimate the number and energy of the electrons around Jupiter and led to improved estimates of the magnetic moment and its tilt.^[7]

By 1973 the magnetic moment was known within a factor of two, whereas the tilt was correctly estimated at about 10°.^[12] The modulation of Jupiter's DAM by Io (the so called Io-DAM) was discovered in 1964, and allowed Jupiter's rotation period to be precisely determined.^[4] The definitive discovery of the Jovian magnetic field occurred in December 1973, when the Pioneer 10 spacecraft flew near the planet.^{[1][note 9]}

Exploration after 1970

As of 2009 a total of eight spacecraft have flown around Jupiter and all have contributed to the present knowledge of the Jovian magnetosphere. The first space probe to reach Jupiter was Pioneer 10 in December 1973, which passed within 2.9 R_j^[12] from the center of the planet.^[1] Its twin Pioneer 11 visited Jupiter a year later, traveling along a highly inclined trajectory and approaching the planet as close as 1.6 R_j.^[12]

Pioneer provided the best coverage available of the inner magnetic field.^[6] The level of radiation at Jupiter was ten times more powerful than Pioneer's designers had predicted, leading to fears that the probe would not survive; however, with a few minor glitches, it managed to pass through the radiation belts, saved in large part by the fact that Jupiter's magnetosphere had "wobbled" slightly upward at that point, moving away from the spacecraft. However, Pioneer 11 did lose most images of Io, as the radiation had caused its imaging photo polarimeter to receive a number of spurious commands. The subsequent and far more technologically advanced Voyager spacecraft had to be redesigned to cope with the massive radiation levels.^[25]

Voyagers 1 and 2 arrived to Jupiter in 1979–1980 and traveled almost in its equatorial plane. Voyager 1, which passed within 5 R_j from the planet's center,^[12] was first to encounter the Io plasma torus.^[6] Voyager 2 passed within 10 R_j^[12] and discovered the current sheet in the equatorial plane. The next probe to approach Jupiter was Ulysses in 1992, which investigated the planet's polar magnetosphere.^[6]

The Galileo spacecraft, which orbited Jupiter from 1995 to 2003, provided a comprehensive coverage of Jupiter's magnetic field near the equatorial plane at distances up to 100 R_j. The regions studied included the magnetotail and the dawn and dusk sectors of the magnetosphere.^[6] While Galileo successfully survived in the harsh radiation environment of Jupiter, it still experienced a few technical problems. In particular, the spacecraft's gyroscopes often exhibited increased errors. Several times electrical arcs occurred between rotating and non-rotating parts of the spacecraft, causing it to enter safe mode, which led to total loss of the data from the 16th, 18th and 33rd orbits. The radiation also caused phase shifts in Galileo's ultra-stable quartz oscillator.^[80]

When the Cassini spacecraft flew by Jupiter in 2000, it conducted coordinated measurements with Galileo.^[6] The last spacecraft to visit Jupiter was New Horizons in 2007, which carried out a unique investigation of the Jovian magnetotail, traveling as far as 2500 R_j along its length.^[33] The coverage of Jupiter's magnetosphere remains much poorer than for Earth's magnetic field. Future missions (Juno, for instance) are important to further understand the Jovian magnetosphere's dynamics.^[6]

In 2003, NASA conducted a conceptual study called "Human Outer Planets Exploration" (HOPE) regarding the future human exploration of the outer solar system. The possibility was mooted of building a surface base on Callisto, because of the low radiation levels at the moon's distance from Jupiter and its geological stability. Callisto is the only one of Jupiter's Galilean satellites for which human exploration is feasible. The levels of ionizing radiation on Io, Europa and Ganymede are inimical to human life, and adequate protective measures have yet to be devised.^[81]

Notes

1. ^ The north and south poles of the Earth's dipole should not be confused with Earth's North magnetic pole and South magnetic pole, which lie in the northern and southern hemispheres, respectively.
2. ^ The magnetic moment is proportional to the product of the equatorial field strength and cube of Jupiter's radius, which is 11 times larger than that of the Earth.
3. ^ For instance, the azimuthal orientation of the dipole changed by less than 0.01°.^[2]
4. ^ The direct current in the Jovian magnetosphere is not to be confused with the direct current used in electrical circuits. The latter is the opposite of the alternating current.
5. ^ The Jovian ionosphere is another significant source of protons.^[7]
6. ^ Callisto may have a spot as well; however, it would be unobservable because it would coincide with the main auroral oval.^[50]
7. ^ The non-Io-DAM is much weaker than the Io-DAM, and is the high-frequency tail of the HOM emissions.^[53]
8. ^ A Lorentz resonance is one that exists between a particle's orbital speed and the rotation period of a planet's magnetosphere. If the ratio of their angular frequencies is m:n (a rational number) then scientists call it an m:n Lorentz resonance. So, in the case of a 3:2 resonance, a particle at a distance of about 1.71 R_j from Jupiter makes three revolutions around the planet, while the planet's magnetic field makes two revolutions.^[66]
9. ^ Pioneer 10 carried a helium vector magnetometer, which measured the magnetic field of Jupiter directly. The spacecraft also made observations of plasma and energetic particles.^[1]

References

1. ^ ^{a b c d e} Smith, 1974
2. ^ ^{a b c d e} Khurana, 2004, pp. 3–5
3. ^ ^{a b c} Russel, 1993, p. 694
4. ^ ^{a b c} Zarka, 2005, pp. 375–377
5. ^ Blanc, 2005, p. 238 (Table III)
6. ^ ^{a b c d e f g h i j k l m n o p q r} Khurana, 2004, pp. 1–3
7. ^ ^{a b c d e f g} Khurana, 2004, pp. 5–7
8. ^ ^{a b} Bolton, 2002
9. ^ ^{a b} Bhardwaj, 2000, p. 342
10. ^ Khurana, 2004, pp. 12–13
11. ^ ^{a b c d} Kivelson, 2005, pp. 303–313
12. ^ ^{a b c d e f g} Russel, 1993, pp. 715–717
13. ^ ^{a b c} Russell, 2001, pp. 1015–1016
14. ^ ^{a b} Krupp, 2004, pp. 15–16
15. ^ Russel, 1993, pp. 725–727
16. ^ ^{a b c d} Khurana, 2004, pp. 17–18
17. ^ Khurana, 2004, pp. 6–7
18. ^ ^{a b c} Krupp, 2004, pp. 3–4
19. ^ ^{a b c d e f} Krupp, 2004, pp. 4–7
20. ^ ^{a b c} Krupp, 2004, pp. 1–3
21. ^ ^{a b c d e f} Khurana, 2004, pp. 13–16
22. ^ ^{a b} Khurana, 2004, pp. 10–12
23. ^ Russell, 2001, pp. 1024–1025
24. ^ ^{a b} Khurana, 2004, pp. 20–21
25. ^ ^{a b} Wolverton, 2004, pp. 100–157
26. ^ Russell, 2001, pp. 1021–1024
27. ^ Kivelson, 2005, pp. 315–316
28. ^ Blanc, 2005, pp. 250–253
29. ^ ^{a b c d e} Cowley, 2001, pp. 1069–76
30. ^ ^{a b c d e f g} Blanc, 2005, pp. 254–261
31. ^ ^{a b} Cowley, 2001, pp. 1083–87
32. ^ Russell, 2008
33. ^ ^{a b} Krupp, 2007, p. 216
34. ^ Krupp, 2004, pp. 7–9
35. ^ ^{a b c d} Krupp, 2004, pp. 11–14
36. ^ Khurana, 2004, pp. 18–19
37. ^ Russell, 2001, p. 1011
38. ^ ^{a b} Nichols, 2006, pp. 393–394
39. ^ Krupp, 2004, pp. 18–19
40. ^ Nichols, 2006, pp. 404–405
41. ^ ^{a b} Elsner, 2005, pp. 419–420
42. ^ ^{a b} Palier, 2001, pp. 1171–73
43. ^ ^{a b c d} Bhardwaj, 2000, pp. 311–316
44. ^ Cowley, 2003, pp. 49–53
45. ^ Bhardwaj, 2000, pp. 316–319
46. ^ Bhardwaj, 2000, pp. 306–311
47. ^ Bhardwaj, 2000, p. 296
48. ^ Miller, 2005, pp. 335–339
49. ^ Bhardwaj, 2000, Tables 2 and 5
50. ^ ^{a b} Clarke, 2002
51. ^ Blanc, 2005, pp. 277–283
52. ^ Palier, 2001, pp. 1170–71
53. ^ ^{a b c d} Zarka, 1998, pp. 20,160–168
54. ^ Zarka, 1998, pp. 20, 173–181
55. ^ ^{a b c} Hill, 1995
56. ^ ^{a b} Zarka, 2005, pp. 371–375
57. ^ Santos-Costa, 2001
58. ^ Zarka, 2005, pp. 384–385
59. ^ Krupp, 2004, pp. 17–18
60. ^ ^{a b c d e} Kivelson, 2004, pp. 2–4
61. ^ Johnson, 2004, pp. 1–2
62. ^ ^{a b} Johnson, 2004, pp. 3–5
63. ^ ^{a b} Burns, 2004, pp. 1–2
64. ^ Burns, 2004, pp. 12–14
65. ^ Burns, 2004, pp. 10–11
66. ^ ^{a b} Burns, 2004, pp. 17–19
67. ^ Kivelson, 2004, pp. 8–10
68. ^ Kivelson, 2004, pp. 1–2
69. ^ Cooper, 2001, pp. 137,139
70. ^ ^{a b} Kivelson, 2004, pp. 10–11
71. ^ ^{a b} Kivelson, 2004, pp. 16–18
72. ^ Williams, 1998, p. 1
73. ^ ^{a b} Cooper, 2001, pp. 154–156
74. ^ Johnson, 2004, pp. 15–19
75. ^ Hibbitts, 2000, p. 1
76. ^ ^{a b} Johnson, 2004, pp. 8–13
77. ^ Corum, Kenneth L.; James F. Corum (1996) (PDF). Nikola Tesla and the electrical signals of planetary origin. p. 14. OCLC 68193760. http://www.teslasociety.com/mars.pdf. 
78. ^ Burke, 1955
79. ^ Drake, 1959
80. ^ Fieseler, 2002
81. ^ Troutman, 2003

Cited sources

• Bhardwaj, A.; Gladstone, G.R. (2000). "Auroral emissions of the giant planets" (pdf). Reviews of Geophysics 38 (3): 295–353. Bibcode 2000RvGeo..38..295B. doi:10.1029/1998RG000046. http://www.bu.edu/csp/uv/cp-aeronomy/Bhardwaj_Gladstone_RG_2000.pdf. 
• Blanc, M.; Kallenbach, R.; Erkaev, N.V. (2005). "Solar System magnetospheres". Space Science Reviews 116 (1-2): 227–298. Bibcode 2005SSRv..116..227B. doi:10.1007/s11214-005-1958-y. 
• Bolton, S.J.; Janssen, M. et al. (2002). "Ultra-relativistic electrons in Jupiter's radiation belts". Nature 415 (6875): 987–991. doi:10.1038/415987a. PMID 11875557. http://www.nature.com/nature/journal/v415/n6875/full/415987a.html. 
• Burke, B.F.; Franklin, K.L. (1955). "Observations of a variable radio source associated with the planet Jupiter". Journal of Geophysical Research 60 (2): 213–217. Bibcode 1955JGR....60..213B. doi:10.1029/JZ060i002p00213. 
• Burns, J.A.; Simonelli, D.P. et al. (2004). "Jupiter's ring-moon system". In Bagenal, F. et al. (pdf). Jupiter: The Planet, Satellites and Magnetosphere. Cambridge University Press. ISBN 0521818087. http://www.astro.umd.edu/~hamilton/research/preprints/BurSimSho03.pdf. 
• Clarke, J.T.; Ajello, J. et al. (2002). "Ultraviolet emissions from the magnetic footprints of Io, Ganymede and Europa on Jupiter" (pdf). Nature 415 (6875): 997–1000. doi:10.1038/415997a. PMID 11875560. http://www2.iap.fr/users/lotfi/jupiter.pdf. 
• Cooper, J.F.; Johnson, R.E. et al. (2001). "Energetic ion and electron irradiation of the icy Galilean satellites" (pdf). Icarus 139 (1): 133–159. Bibcode 2001Icar..149..133C. doi:10.1006/icar.2000.6498. http://icymoons.com/europaclass/Cooper_gllsat_irrad.pdf. 
• Cowley, S.W.H.; Bunce, E.J. (2001). "Origin of the main auroral oval in Jupiter's coupled magnetosphere–ionosphere system". Planetary and Space Science 49 (10-11): 1067–66. Bibcode 2001P&SS...49.1067C. doi:10.1016/S0032-0633(00)00167-7. 
• Cowley, S.W.H.; Bunce, E.J. (2003). "Modulation of Jovian middle magnetosphere currents and auroral precipitation by solar wind-induced compressions and expansions of the magnetosphere: initial response and steady state". Planetary and Space Science 51 (1): 31–56. Bibcode 2003P&SS...51...31C. doi:10.1016/S0032-0633(02)00130-7. 
• Drake, F.D.; Hvatum, S. (1959). "Non-thermal microwave radiation from Jupiter". Astronomical Journal 64: 329. Bibcode 1959AJ.....64S.329D. doi:10.1086/108047. 
• Elsner, R.F.; Ramsey, B.D. et al. (2005). "X-ray probes of magnetospheric interactions with Jupiter's auroral zones, the Galilean satellites, and the Io plasma torus" (pdf). Icarus 178 (2): 417–428. Bibcode 2005Icar..178..417E. doi:10.1016/j.icarus.2005.06.006. http://wwwastro.msfc.nasa.gov/research/papers/icarus.pdf. 
• Fieseler, P.D.; Ardalan, S.M. et al. (2002). "The radiation effects on Galileo spacecraft systems at Jupiter" (pdf). Nuclear Science 49 (6): 2739–58. Bibcode 1959AJ.....64S.329D. doi:10.1086/108047. http://trs-new.jpl.nasa.gov/dspace/bitstream/2014/11661/1/02-0220.pdf. 
• Hill, T.W.; Dessler, A.J. (1995). "Space physics and astronomy converge in exploration of Jupiter's Magnetosphere". Earth in Space 8: 6. Archived from the original on 1997-05-01. http://web.archive.org/web/19970501040601/http://www.agu.org/sci_soc/hill.html. 
• Hibbitts, C.A.; McCord, T.B.; Hansen, T.B. (2000). "Distribution of CO₂ and SO₂ on the surface of Callisto". Journal of Geophysical Research 105 (E9): 22,541–557. Bibcode 2000JGR...10522541H. doi:10.1029/1999JE001101. 
• Johnson, R.E.; Carlson, R.V. et al. (2004). "Radiation Effects on the Surfaces of the Galilean Satellites". In Bagenal, F. et al. (PDF). Jupiter: The Planet, Satellites and Magnetosphere. Cambridge University Press. ISBN 0521818087. http://people.virginia.edu/~rej/papers04/chap20.pdf. 
• Khurana, K.K.; Kivelson, M.G. et al. (2004). "The configuration of Jupiter's magnetosphere". In Bagenal, F.; Dowling, T.E.; McKinnon, W.B. (PDF). Jupiter: The Planet, Satellites and Magnetosphere. Cambridge University Press. ISBN 0521818087. http://www.igpp.ucla.edu/people/mkivelson/Publications/279-Ch24.pdf. 
• Kivelson, M.G. (2005). "The current systems of the Jovian magnetosphere and ionosphere and predictions for Saturn" (pdf). Space Science Reviews (Springer) 116 (1-2): 299–318. Bibcode 2005SSRv..116..299K. doi:10.1007/s11214-005-1959-x. http://www.igpp.ucla.edu/people/mkivelson/Publications/285-SSR11629905.pdf. 
• Kivelson, M.G.; Bagenal, F. et al. (2004). "Magnetospheric interactions with satellites". In Bagenal, F.; Dowling, T.E.; McKinnon, W.B. (PDF). Jupiter: The Planet, Satellites and Magnetosphere. Cambridge University Press. ISBN 0521818087. http://www.igpp.ucla.edu/people/mkivelson/Publications/277-Ch21.pdf. 
• Krupp, N.; Vasyliunas, V.M. et al. (2004). "Dynamics of the Jovian Magnetosphere". In Bagenal, F. et al. (PDF). Jupiter: The Planet, Satellites and Magnetosphere. Cambridge University Press. ISBN 0521818087. http://www.igpp.ucla.edu/people/mkivelson/Publications/280-Ch25.pdf. 
• Krupp, N. (2007). "New surprises in the largest magnetosphere of Our Solar System". Science 318 (5848): 216–217. Bibcode 2007Sci...318..216K. doi:10.1126/science.1150448. PMID 17932281. 
• Miller, S.; Aylword, A. and Milliword, G. (2005). "Giant planet ionospheres and thermospheres: the importance of ion-neutral coupling". Space Science Reviews 116 (1-2): 319–343. Bibcode 2005SSRv..116..319M. doi:10.1007/s11214-005-1960-4. 
• Nichols, J.D.; Cowley, S.W.H. and McComas, D.J. (2006). "Magnetopause reconnection rate estimates for Jupiter's magnetosphere based on interplanetary measurements at ~5 AU". Annales Geophysicae 24 (1): 393–406. Bibcode 2006AnGeo..24..393N. doi:10.5194/angeo-24-393-2006. http://www.ann-geophys.net/24/393/2006/angeo-24-393-2006.html. 
• Palier, L. (2001). "More about the structure of the high latitude Jovian aurorae". Planetary and Space Science 49 (10-11): 1159–73. Bibcode 2001P&SS...49.1159P. doi:10.1016/S0032-0633(01)00023-X. 
• Russell, C.T. (1993). "Planetary Magnetospheres" (pdf). Reports on Progress in Physiscs 56 (6): 687–732. Bibcode 1993RPPh...56..687R. doi:10.1088/0034-4885/56/6/001. http://www.iop.org/EJ/article/0034-4885/56/6/001/rp930601.pdf. 
• Russell, C.T. (2001). "The dynamics of planetary magnetospheres". Planetary and Space Science 49 (10-11): 1005–1030. Bibcode 2001P&SS...49.1005R. doi:10.1016/S0032-0633(01)00017-4. 
• Russell, C.T.; Khurana, K.K.; Arridge, C.S.; Dougherty, M.K. (2008). "The magnetospheres of Jupiter and Saturn and their lessons for the Earth" (pdf). Advances in Space Research 41 (8): 1310–18. Bibcode 2008AdSpR..41.1310R. doi:10.1016/j.asr.2007.07.037. http://www-ssc.igpp.ucla.edu/personnel/russell/papers/magnetospheres_jupiter_saturn.pdf. 
• Santos-Costa, D.; Bourdarie, S.A. (2001). "Modeling the inner Jovian electron radiation belt including non-equatorial particles". Planetary and Space Science 49 (3-4): 303–312. Bibcode 2001P&SS...49..303S. doi:10.1016/S0032-0633(00)00151-3. 
• Smith, E.J.; Davis, L. Jr. et al. (1974). "The Planetary Magnetic Field and Magnetosphere of Jupiter: Pioneer 10". Journal of Geophysical Research 79 (25): 3501–13. Bibcode 1974JGR....79.3501S. doi:10.1029/JA079i025p03501. 
• Troutman, P.A.; Bethke, K. et al. (28 January 2003). "Revolutionary concepts for Human Outer Planet Exploration (HOPE)". American Institute of Physics Conference Proceedings 654: 821–828. doi:10.1063/1.1541373. 
• Williams, D.J.; Mauk, B.; McEntire, R.W. (1998). "Properties of Ganymede's magnetosphere as revealed by energetic particle observations". Journal of Geophysical Research 103 (A8): 17,523–534. Bibcode 1998JGR...10317523W. doi:10.1029/98JA01370. 
• Wolverton, M. (2004). The Depths of Space. Joseph Henry Press. ISBN 978-0-309-09050-6. 
• Zarka, P.; Kurth, W.S. (1998). "Auroral radio emissions at the outer planets: Observations and theory". Journal of Geophysical Research 103 (E9): 20,159–194. Bibcode 1998JGR...10320159Z. doi:10.1029/98JE01323. 
• Zarka, P.; Kurth, W.S. (2005). "Radio wave emissions from the outer planets before Cassini". Space Science Reviews 116 (1-2): 371–397. Bibcode 2005SSRv..116..371Z. doi:10.1007/s11214-005-1962-2. 

Further reading

• Carr, Thomas D.; Gulkis, Samuel (1969). "The magnetosphere of Jupiter". Annual Review of Astronomy and Astrophysics 7 (1): 577–618. Bibcode 1969ARA&A...7..577C. doi:10.1146/annurev.aa.07.090169.003045. 
• Edwards, T.M.; Bunce, E.J.; Cowley, S.W.H. (2001). "A note on the vector potential of Connerney et al.'s model of the equatorial current sheet in Jupiter's magnetosphere". Planetary and Space Science 49 (10-11): 1115–23. Bibcode 2001P&SS...49.1115E. doi:10.1016/S0032-0633(00)00164-1. 
• Gladstone, G.R.; Waite, J.H.; Grodent, D. (2002). "A pulsating auroral X-ray hot spot on Jupiter". Nature 415 (6875): 1000–03. doi:10.1038/4151000a. PMID 11875561. http://www.nature.com/nature/journal/v415/n6875/full/4151000a.html. 
• Kivelson, Margaret G.; Khurana, Krishan K. and Walker, Raymond J. (2002). "Sheared magnetic field structure in Jupiter's dusk magnetosphere: Implications for return currents" (pdf). Journal of Geophysical Research 107 (A7): 1116. Bibcode 2002JGRA..107.1116K. doi:10.1029/2001JA000251. http://www.igpp.ucla.edu/people/mkivelson/Publications/262-2001JA000251.pdf. 
• Kivelson, M.G. (2005). "Transport and acceleration of plasma in the magnetospheres of Earth and Jupiter and expectations for Saturn" (pdf). Advances in Space Research 36 (11): 2077–89. Bibcode 2005AdSpR..36.2077K. doi:10.1016/j.asr.2005.05.104. http://www.igpp.ucla.edu/people/mkivelson/Publications/287-ASR362077.pdf. 
• Kivelson, Margaret G.; Southwood, David J. (2003). "First evidence of IMF control of Jovian magnetospheric boundary locations: Cassini and Galileo magnetic field measurements compared" (pdf). Planetary and Space Science 51 (A7): 891–98. Bibcode 2003P&SS...51..891K. doi:10.1016/S0032-0633(03)00075-8. http://www.igpp.ucla.edu/people/mkivelson/Publications/270-PSS51891.pdf. 
• McComas, D.J.; Allegrini, F.; Bagenal, F. et al. (2007). "Diverse Plasma Populations and Structures in Jupiter's Magnetotail". Science 318 (5848): 217–20. Bibcode 2007Sci...318..217M. doi:10.1126/science.1147393. PMID 17932282. 
• Maclennan, G.G.; Maclennan, L.J.; Lagg, Andreas (2001). "Hot plasma heavy ion abundance in the inner Jovian magnetosphere (<10 Rj)". Planetary and Space Science 49 (3-4): 275–82. Bibcode 2001P&SS...49..275M. doi:10.1016/S0032-0633(00)00148-3. 
• Russell, C.T.; Yu, Z.J.; Kivelson, M.G. (2001). "The rotation period of Jupiter" (pdf). Geophysics Research Letters 28 (10): 1911–12. Bibcode 2001GeoRL..28.1911R. doi:10.1029/2001GL012917. http://www.igpp.ucla.edu/people/mkivelson/Publications/245-2001GL012917.pdf. 
• Zarka, Philippe; Queinnec, Julien; Crary, Frank J. (2001). "Low-frequency limit of Jovian radio emissions and implications on source locations and Io plasma wake". Planetary and Space Science 49 (10-11): 1137–49. Bibcode 2001P&SS...49.1137Z. doi:10.1016/S0032-0633(01)00021-6. 

External links