Meteorite magnetization and paleointensity

The five chemical classes of chondrite, i.e. E-, H-, L-, LL- and C-chondrite, and three major classes of achondrite, i.e. diogenite, eucrite plus howardite, and ureilite, are magnetically identified to respective separated domains on an I_s (α)/I_s versus I_s diagram, where I_s and I_s (α) denote respectively the saturation magnetization and the saturation magnetization of α-phase alone. Three major groups of iron meteorite, i.e. hexahedrite plus Ni-poor ataxite, octahedrite and Ni-rich ataxite, are magnetically identified to respective domains on an I_s (α)/I_s versus

→ α diagram, where

→ α denotes

→ α transition temperature of kamacite phase in the cooling process. The magnetic classification schemes well represent the chemical characteristics of each meteorite class. The paleointensity (F_p) of meteorites determined to date can be summarized as F_p=0.01 ～ 0.1 Oe for eucrites and ureilites, F_p^? 1 Oe for C-chondrites, and F_p^? 10 Oe for E-chondrites.     

SMM observation of a cosmic gamma-ray burst from 20 keV to 100 MeV

The Solar Maximum Mission γ-ray spectrometer (GRS) has detected an intense γ-ray burst that occurred on 1984 August 5. The burst originated from a source in the constellation Hydra and lasted about 45 s. Its integral fluence

20 keV was 3 × 10⁻³ erg cm⁻². Spectral evolution similar to other bursts detected by SMM was observed. The overall shape of the spectrum from 20 keV to 100 MeV, on timescales as short as 2 s, is relatively constant. This shape can be fitted by the sum of an exponential-type function and a power law. The spectral shape of this event may be characteristic of many γ-ray bursts. There is no evidence for narrow or broadened emission lines.     

Conjecture on superrotation in planetary atmospheres: A diffusion model with mixing length theory

Superrotation on Venus is discussed in the context of comparative planetary atmospheres. In our planetary system, the rigid shell component (global average) of superrotation is ubiquitous (Jupiter, Saturn, Earth, Venus, Mars, Titan). The largest equatorial values of the component are between 25 and 150 m/sec. We present a simplified, heuristic analysis, utilizing mixing length theory to describe the small scale non-linear advections of energy and angular momentum, thereby providing a closure of the dynamic system. This leads to the conjecture that the zonal velocity may be crudely estimated by

, approximating the observed planetary trends; with c the speed of sound, the parameter a being 1 or 2 for geostrophic or cyclostrophic conditions respectively, P_α an effective Prandtl number which becomes less than one when radiative cooling is important, S_o the average stability, Γ the adiabatic lapse rate and γ the ratio of specific heats.     

Movement of a material point in the gravity field of a homogeneous ring

A ring-like mass exerts a well computable gravitational attraction on a material point located along a straight line, being perpendicular to the plane of the ring in its centre. In the state of weightlessness, an oscillatory movement will develop owing to this effect. The period, T, of oscillation depends on the gravity constant, on the density and dimensions of the ring, as well as on the amplitude of the oscillation. Its exact computation can be based on the determination of the gravity potential function of the ring. The oscillation has the following form:

$\text{T=}\text{1}\text{√f√}\textcolor{red}{}\text{.I(r,R,z)}$

where f is the gravitational constant.

is the density of the ring, r and R are the radii of the ring, z is the distance of the turning point of the oscillation from the centre of the ring, while I/r,R,z/ is an improper integral which can be computed with any desired accuracy owing to the favourable function-theoretical character of the potential. We computed the oscillation period for various possible values of the parameters and obtained time data of an order of magnitude which falls into a well observable interval.The outlined conceptual experiment for the improved determination of the gravitational constant may present, of course, many technical difficulties and error sources /e.g. the path of the oscillating point is quite unstable owing to the extremely small acting forces, electric charges and also radiation pressure might be present, the gravity field would show a gradient on the spot of the experiment, etc./. Nevertheless, it seems to be worthwhile to consider carrying out such an experiment, using the possibilities offered by modern techniques in observing distances and time. For the path distortions caused by errors, we give a few estimates, but in case of realization of the experiment, a more detailed error analysis must be made.     

The role of weightlessness in the genetic damage from preflight gamma-irradiation of organisms in experiments aboard the Salyut 6 orbital station

The effect of weightlessness on chromosomal aberration frequency in preflight irradiated $\text{Crepis capillaris}$ seeds, on the viability, fertility and mutation frequency in $\text{Arabidopsis thaliana}$, and on the frequency of nondisjunction and loss of X chromosomes in preflight irradiated $\text{Drosophila melanogaster}$ gametes was studied aboard the Salyut 6 orbital station. The following effects were observed: a flight-time dependent amplification of the effects of preflight

-irradiation in $\text{A}$. $\text{thaliana}$ with respect to all the parameters studied; unequal effects in seeds and seedlings of $\text{Crepis capillaris}$; and a significant increase in the frequency of nondisjunction and loss of chromosomes during meiosis in $\text{Drosophila}$ females. These observations are discussed in terms of the data of ground-based model experiments and flight experiments with a different time of exposure of objects to weightlessness. An attempt is made to elucidate the role of weightlessness in the modification of ionizing radiation effects.     

V.L.A. observations of flare build-up in coronal loops

Very Large Array (V.L.A.) measurements at 20 cm wavelength map emission from coronal loops with second-of-arc angular resolution at time intervals as short as 3.3 seconds. The total intensity of the 20 cm emission describes the evolution and structure of the hot plasma that is detected by satellite X-ray observations of coronal loops. The circular polarization of the 20 cm emission describes the evolution, strength and structure of the coronal magnetic field. Preburst heating and magnetic changes that precede burst emission on time scales of between 1 and 30 minutes are discussed. Simultaneous 20 cm and soft X-ray observations indicate an electron temperature $\text{T}{}_{\mathrm{e}}\textcolor{red}{}\text{2.5 × 10}{}^7\text{K}$ and electron density $\text{N}{}_{\mathrm{e}}\textcolor{red}{}\text{10}{}^{10}\text{cm}{}^{\mathrm{?3}}$ during preburst heating in a coronal loop that was also associated with twisting of the entire loop in space. We also discuss the successive triggering of bursts from adjacent coronal loops; highly polarized emission from the legs of loops with large intensity changes over a 32 MHz change in observing frequency; and apparent motions of hot plasma within coronal loops at velocities V > 2,000 kilometerspersecond.