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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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impact velocities A factor in crater formation<br />

that determines crater size <strong>and</strong> is controlled<br />

by the thickness of the atmosphere around the<br />

planet (assuming cosmic velocities are constant<br />

throughout the solar system for the same sized<br />

objects). Thus, the moon has a higher impact<br />

velocity than Mars. For example, a typical<br />

asteroid may hit Mars at 10 km/sec <strong>and</strong> the<br />

moon at 14 km/sec, causing the crater formed<br />

on Mars to be smaller by 0.66. By recognizing<br />

that smaller craters are produced on Mars, sizefrequency<br />

curves developed there can be displaced<br />

to make them directly comparable with<br />

those on the moon, etc. This is also applicable<br />

to the other solar system planets.<br />

impermeable Does not allow penetration by<br />

a fluid.<br />

impulsive flare Solar flares with short duration<br />

electromagnetic radiation occurring low in<br />

the corona in compact volumina. In contrast<br />

to gradual flares, impulsive flares are not accompanied<br />

by coronal mass ejections. In more<br />

detail, the properties of an impulsive flare are:<br />

(a) the soft X-ray emission lasts less than one<br />

hour, (b) the decay constant of the soft X-ray<br />

emission is less than 10 minutes, (c) the duration<br />

of the hard X-ray emission is less than<br />

10 minutes, (d) the duration of the microwave<br />

emission is less than 5 minutes, (e) impulsive<br />

flares are always accompanied by metric type<br />

III bursts, about 75% of them are also accompanied<br />

by metric type II bursts, but metric type IV<br />

emission is observed only rarely, (f) the height in<br />

the corona is less than 10 4 km, (g) the flare occupies<br />

a volume between 10 26 cm 3 <strong>and</strong> 10 27 cm 3 ,<br />

(h) the energy density is high, (i) the size in Hα<br />

is small, <strong>and</strong> (j) impulsive flares are rarely accompanied<br />

by coronal mass ejections. If coronal<br />

mass ejections are observed in impulsive<br />

flares, they tend to be small <strong>and</strong> slow with speeds<br />

well below the combined solar wind <strong>and</strong> Alfven<br />

speed which is required to drive a shock.<br />

If an impulsive flare gives rise to a particle<br />

event in interplanetary space, this event has<br />

properties different from the ones of particle<br />

events caused by gradual flares. These properties<br />

include: (a) the event is electron-rich <strong>and</strong> the<br />

H/He ratio is about 10, (b) the 3 He/ 4 He ratio is of<br />

the order of 1, which is enhanced by a factor of<br />

© 2001 by CRC Press LLC<br />

impulsive flare<br />

2000 compared to abundances in the corona <strong>and</strong><br />

in the solar wind, (c) the Fe/O ratio is about 1.2,<br />

an enhancement by a factor of 8 compared to the<br />

corona or the solar wind, (d) the charge states of<br />

iron are about 20, indicative for the acceleration<br />

out of a very hot environment with temperatures<br />

of about 10 million K, (e) the particles event lasts<br />

(at the orbit of Earth) for some hours up to about<br />

1 day, (f) particles can be observed only in a relatively<br />

narrow cone of ±30 ◦ around the source<br />

region, <strong>and</strong> (g) there is no interplanetary shock<br />

accompanying the event. Event rates are up to<br />

about 1000 per year during solar maximum.<br />

In impulsive flares, particles are accelerated<br />

in a hot but confined volume low in the corona.<br />

The enrichment in 3 He <strong>and</strong> in heavier elements<br />

such as Fe can be explained by the process of selective<br />

heating: Particles are accelerated inside a<br />

close loop, giving rise to electromagnetic emission<br />

(the flare). The loop is very stable, preventing<br />

particles from escaping into interplanetary<br />

space. As the particles bounce back <strong>and</strong> forth<br />

in the closed loop, they excite electromagnetic<br />

waves which can propagate into all directions,<br />

in particular also perpendicular to the magnetic<br />

field lines. When these waves interact with the<br />

ambient plasma, they can accelerate particles.<br />

If these “secondary” particles are accelerated on<br />

open field lines, they can escape into interplanetary<br />

space. Because the acceleration requires<br />

particles <strong>and</strong> waves to be in resonance, different<br />

particles are accelerated by different types<br />

of waves. If a particle species is common in the<br />

corona, such as H <strong>and</strong> 4 He, the corresponding<br />

waves are absorbed more or less immediately;<br />

thus, these particles are predominately accelerated<br />

inside the closed loop <strong>and</strong> therefore do not<br />

escape into interplanetary space. Other waves,<br />

however, can travel larger distances before being<br />

absorbed by the minor constituents <strong>and</strong> therefore<br />

are more likely to accelerate these species<br />

on open field lines. Since the escaping particle<br />

component is selectively enriched in these<br />

minor species, the acceleration process is called<br />

selective heating.<br />

impulsive flare Flares displaying impulsive<br />

spikes or bursts in their hard X-ray time profiles.<br />

These flares are generally confined in long<br />

(10 4 km) sheared loops <strong>and</strong> are considered as<br />

non-thermal X-ray sources.<br />

239

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