1,724 research outputs found
Cliff collapse on Comet 67P/Churyumov-Gerasimenko -- I. Aswan
The Aswan cliff on Comet 67P/Churyumov-Gerasimenko collapsed on 2015 July 10.
Thereby, relatively pristine comet material from a depth of ~12 m was exposed
at the surface. Observations of the collapse site by the microwave instrument
Rosetta/MIRO have been retrieved from 8 months prior to collapse, as well as
from 5, 7, and 11 months post-collapse. The MIRO data are analysed with
thermophysical and radiative transfer models. The pre-collapse observations are
consistent with a 30 MKS thermal inertia dust mantle with a thickness of at
least 3 cm. The post-collapse data are consistent with: 1) a dust/water-ice
mass ratio of 0.90.5 and a molar abundance of ~30 per cent
relative to water; 2) formation of a dust mantle after ~7 months, having a
thickness of a few millimetres or a fraction thereof; 3) a ice
sublimation front at 0.4 cm that withdrew to 2.0 cm and later to 206 cm;
4) a thermal inertia ranging 10-45 MKS; 5) a gas diffusivity that decreased
from to ; 6) presence
of a solid-state greenhouse effect parts of the time. The data and the analysis
provide a first empirical glimpse of how ice-rich cometary material ages and
evolves when exposed to solar heating.Comment: 22 pages, 24 figures. This is a pre-copyedited, author-produced PDF
of an article accepted for publication in MNRAS following peer revie
Collisional heating of icy planetesimals. I. Catastrophic collisions
Planetesimals in the primordial disc may have experienced a collisional
cascade. If so, the comet nuclei later placed in the Kuiper belt, scattered
disc, and Oort Cloud would primarily be fragments and collisional rubble piles
from that cascade. However, the heating associated with the collisions cannot
have been strong enough to remove the hypervolatiles that are trapped within
more durable ices, because comet nuclei are rich in hypervolatiles. This places
constraints on the diameter of the largest bodies allowed to participate in
collisional cascades, and limits the primordial disc lifetime or population
size. In this paper, the thermophysical code NIMBUS is used to study the
thermal evolution of planetesimals before, during, and after catastrophic
collisions. The loss of CO during segregation of mixtures
and during crystallisation of amorphous is calculated, as well
as mobilisation and internal relocation of . If an amorphous
host existed, and was protected by a heat
sink, only diameter (inner disc) and
(outer disc) bodies could have been involved in a collisional cascade. If
was the only CO host, the critical diameters drop to
-. Avoiding disruption of larger bodies requires a
primordial disc lifetime of at and
- at . Alternatively, if a
disc lifetime is required to associate the primordial disc
disruption with the Late Heavy Bombardment, the disc population size must have
been 6-60 times below current estimates.Comment: 20 pages, 11 figures. This is a pre-copyedited, author-produced PDF
of an article accepted for publication in MNRAS following peer revie
Application of the Panzar-Rosse Model: An Analysis of the Brewery Industry in the U.S.
Waves of mergers and acquisitions has left the brewery industry in the United States considerably concentrated. The top two firms, Anheuser-Busch InBev and MillerCoors control more than 60% of the market share. It has become very important to assess the level of competition within the industry. The Panzar-Rosse model is an assessment of competitive conduct that has been widely used to study the competitiveness of the banking industry. The associated measure of competition, called the H-statistic, is obtained as the sum of elasticities of gross revenue with respect to input prices. For this study, the Panzar-Rosse model will be applied to the United States brewery industry and finds that the H-statistic has a negative value, meaning the industry operates under a neoclassical monopolist style or a collusive oligopoly
Secondary gas in debris discs released following the decay of long-lived radioactive nuclides, catastrophic or resurfacing collisions
Kuiper-like belts of planetesimals orbiting stars other than the Sun are most
commonly detected from the thermal emission of small dust produced in
collisions. Emission from gas, most notably CO, highlights the cometary nature
of these planetesimals. Here we present models for the release of gas from
comet-like bodies in these belts, both due to their thermophysical evolution,
most notably the decay of long-lived radioactive nuclides and collisional
evolution, including catastrophic and gentler resurfacing collisions. We show
that the rate of gas release is not proportional to the rate of dust release,
if non-catastrophic collisions or thermal evolution dominate the release of CO
gas. In this case, care must be taken when inferring the composition of comets.
Non-catastrophic collisions dominate the gas production at earlier times than
catastrophic collisions, depending on the properties of the planetesimal belt.
We highlight the importance of the thermal evolution of comets, including
crucially the decay of long-lived radioactive nuclides, as a source of CO gas
around young (<50Myr) planetary systems, if large (10-100s kms) planetesimals
are present.Comment: Submitted to MNRAS, 16 page
Short-term variability of a sample of 29 trans-Neptunian objects and Centaurs
We present results of 6 years of observations, reduced and analyzed with the
same tools in a systematic way. We report completely new data for 15 objects,
for 5 objects we present a new analysis of previously published results plus
additional data and for 9 objects we present a new analysis of data already
published. Lightcurves, possible rotation periods and photometric amplitudes
are reported for all of them. The photometric variability is smaller than
previously thought: the mean amplitude of our sample is 0.1mag and only around
15% of our sample has a larger variability than 0.15mag. The smaller
variability than previously thought seems to be a bias of previous
observations. We find a very weak trend of faster spinning objects towards
smaller sizes, which appears to be consistent with the fact that the smaller
objects are more collisionally evolved, but could also be a specific feature of
the Centaurs, the smallest objects in our sample. We also find that the smaller
the objects, the larger their amplitude, which is also consistent with the idea
that small objects are more collisionally evolved and thus more deformed.
Average rotation rates from our work are 7.5h for the whole sample, 7.6h for
the TNOs alone and 7.3h for the Centaurs. All of them appear to be somewhat
faster than what one can derive from a compilation of the scientific literature
and our own results. Maxwellian fits to the rotation rate distribution give
mean values of 7.5h (for the whole sample) and 7.3h (for the TNOs only).
Assuming hydrostatic equilibrium we can determine densities from our sample
under the additional assumption that the lightcurves are dominated by shape
effects, which is likely not realistic. The resulting average density is
0.92g/cm^3 which is not far from the density constraint that one can derive
from the apparent spin barrier that we observe.Comment: Accepted for publication in A&
Implications of the Small Spin Changes Measured for Large Jupiter-Family Comet Nuclei
Rotational spin-up due to outgassing of comet nuclei has been identified as a possible mechanism for considerable mass-loss and splitting. We report a search for spin changes for three large Jupiter-family comets (JFCs): 14P/Wolf, 143P/Kowal-Mrkos, and 162P/Siding Spring. None of the three comets has detectable period changes, and we set conservative upper limits of 4.2 (14P), 6.6 (143P) and 25 (162P) minutes per orbit. Comparing these results with all eight other JFCs with measured rotational changes, we deduce that none of the observed large JFCs experiences significant spin changes. This suggests that large comet nuclei are less likely to undergo rotationally-driven splitting, and therefore more likely to survive more perihelion passages than smaller nuclei. We find supporting evidence for this hypothesis in the cumulative size distributions of JFCs and dormant comets, as well as in recent numerical studies of cometary orbital dynamics. We added 143P to the sample of 13 other JFCs with known albedos and phase-function slopes. This sample shows a possible correlation of increasing phase-function slopes for larger geometric albedos. Partly based on findings from recent space missions to JFCs, we hypothesise that this correlation corresponds to an evolutionary trend for JFCs. We propose that newly activated JFCs have larger albedos and steeper phase functions, which gradually decrease due to sublimation-driven erosion. If confirmed, this could be used to analyse surface erosion from ground and to distinguish between dormant comets and asteroids
A micronised, dispersible ferric pyrophosphate with high relative bioavailability in man
Ferric pyrophosphate is a water-insoluble Fe compound used to fortify infant cereals and chocolate-drink powders as it causes no organoleptic changes to the food vehicle. However, it is only of low absorption in man. Recently, an innovative ferric pyrophosphate has been developed (Sunactive Fe™) based on small-particle-size ferric pyrophosphate (average size 0·3 μm) mixed with emulsifiers, so that it remains in suspension in liquid products. The aim of the present studies was to compare Fe absorption of micronised, dispersible ferric pyrophosphate (Sunactive Fe™) with that of ferrous sulfate in an infant cereal and a yoghurt drink. Two separate Fe absorption studies were made in adult women (ten women/study). Fe absorption was based on the erythrocyte incorporation of stable isotopes (57Fe and 58Fe) 14 d after the intake of labelled test meals of infant cereal (study 1) or yoghurt drink (study 2). Each test meal was fortified with 5 mg Fe as ferrous sulfate or micronised, dispersible ferric pyrophosphate. Results are presented as geometric means. There was no statistically significant difference between Fe absorption from micronised, dispersible ferric pyrophosphate- and ferrous sulfate-fortified infant cereal (3·4 and 4·1 % respectively; P=0·24) and yoghurt drink (3·9 and 4·2 % respectively; P=0·72). The results of the present studies show that micronised, dispersible ferric pyrophosphate is as well absorbed as ferrous sulfate in adults. The high relative Fe bioavailability of micronised, dispersible ferric pyrophosphate indicates the potential usefulness of this compound for food fortificatio
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