1,543 research outputs found
Photophoresis boosts giant planet formation
In the core accretion model of giant planet formation, a solid protoplanetary
core begins to accrete gas directly from the nebula when its mass reaches about
5 earth masses. The protoplanet has at most a few million years to reach
runaway gas accretion, as young stars lose their gas disks after 10 million
years at the latest. Yet gas accretion also brings small dust grains entrained
in the gas into the planetary atmosphere. Dust accretion creates an optically
thick protoplanetary atmosphere that cannot efficiently radiate away the
kinetic energy deposited by incoming planetesimals. A dust-rich atmosphere
severely slows down atmospheric cooling, contraction, and inflow of new gas, in
contradiction to the observed timescales of planet formation. Here we show that
photophoresis is a strong mechanism for pushing dust out of the planetary
atmosphere due to the momentum exchange between gas and dust grains. The
thermal radiation from the heated inner atmosphere and core is sufficient to
levitate dust grains and to push them outward. Photophoresis can significantly
accelerate the formation of giant planets.Comment: accepted in Astronomy and Astrophysics, 201
Protostellar Disk Evolution Over Million-Year Timescales with a Prescription for Magnetized Turbulence
Magnetorotational instability (MRI) is the most promising mechanism behind
accretion in low-mass protostellar disks. Here we present the first analysis of
the global structure and evolution of non-ideal MRI-driven T-Tauri disks on
million-year timescales. We accomplish this in a 1+1D simulation by calculating
magnetic diffusivities and utilizing turbulence activity criteria to determine
thermal structure and accretion rate without resorting to a 3-D
magnetohydrodynamical (MHD) simulation. Our major findings are as follows.
First, even for modest surface densities of just a few times the minimum-mass
solar nebula, the dead zone encompasses the giant planet-forming region,
preserving any compositional gradients. Second, the surface density of the
active layer is nearly constant in time at roughly 10 g/cm2, which we use to
derive a simple prescription for viscous heating in MRI-active disks for those
who wish to avoid detailed MHD computations. Furthermore, unlike a standard
disk with constant-alpha viscosity, the disk midplane does not cool off over
time, though the surface cools as the star evolves along the Hayashi track. The
ice line is firmly in the terrestrial planet-forming region throughout disk
evolution and can move either inward or outward with time, depending on whether
pileups form near the star. Finally, steady-state mass transport is a poor
description of flow through an MRI-active disk. We caution that MRI activity is
sensitive to many parameters, including stellar X-ray flux, grain size,
gas/small grain mass ratio and magnetic field strength, and we have not
performed an exhaustive parameter study here.Comment: Accepted for publication in Astrophysical Journal. 19 pages,
including 8 figure
H-alpha Activity of Old M Dwarfs: Stellar Cycles and Mean Activity Levels For 93 Low-Mass Stars in the Solar Neighborhood
Through the McDonald Observatory M Dwarf Planet Search, we have acquired
nearly 3,000 high-resolution spectra of 93 late-type (K5-M5) stars over more
than a decade using HET/HRS. This sample provides a unique opportunity to
investigate the occurrence of long-term stellar activity cycles for low-mass
stars. In this paper, we examine the stellar activity of our targets as
reflected in the H-alpha feature. We have identified periodic signals for 6
stars, with periods ranging from days to more than 10 years, and find long-term
trends for 7 others. Stellar cycles with P > 1 year are present for at least 5%
of our targets. Additionally, we present an analysis of the time-averaged
activity levels of our sample, and search for correlations with other stellar
properties. In particular, we find that more massive, earlier type (M0-M2)
stars tend to be more active than later type dwarfs. Furthermore,
high-metallicity stars tend to be more active at a given stellar mass. We also
evaluate H-alpha variability as a tracer of activity-induced radial velocity
(RV) variation. For the M dwarf GJ 1170, H-alpha variation reveals stellar
activity patterns matching those seen in the RVs, mimicking the signal of a
giant planet, and we find evidence that the previously identified stellar
activity cycle of GJ 581 may be responsible for the recently retracted planet f
(Vogt et al. 2012) in that system. In general, though, we find that H-alpha is
not frequently correlated with RV at the precision (typically 6-7 m/s) of our
measurements.Comment: Submitted to ApJ. Reflects comments from a positive refere
Hiding in the Shadows: Searching for Planets in Pre--transitional and Transitional Disks
Transitional and pre--transitional disks can be explained by a number of
mechanisms. This work aims to find a single observationally detectable marker
that would imply a planetary origin for the gap and, therefore, indirectly
indicate the presence of a young planet. N-body simulations were conducted to
investigate the effect of an embedded planet of one Jupiter mass on the
production of instantaneous collisional dust derived from a background
planetesimal disk. Our new model allows us to predict the dust distribution and
resulting observable markers with greater accuracy than previous work.
Dynamical influences from a planet on a circular orbit are shown to enhance
dust production in the disk interior and exterior to the planet orbit while
removing planetesimals from the the orbit itself creating a clearly defined
gap. In the case of an eccentric planet the gap opened by the planet is not as
clear as the circular case but there is a detectable asymmetry in the dust
disk.Comment: Accepted to ApJL 25th September 2013. 4 figures, 1 tabl
Molecular evidence for sediment nitrogen fixation in a temperate New England estuary
Primary production in coastal waters is generally nitrogen (N) limited with denitrification outpacing nitrogen fixation (N2-fixation). However, recent work suggests that we have potentially underestimated the importance of heterotrophic sediment N2-fixation in marine ecosystems. We used clone libraries to examine transcript diversity of nifH (a gene associated with N2-fixation) in sediments at three sites in a temperate New England estuary (Waquoit Bay, Massachusetts, USA) and compared our results to net sediment N2 fluxes previously measured at these sites. We observed nifH expression at all sites, including a site heavily impacted by anthropogenic N. At this N impacted site, we also observed mean net sediment N2-fixation, linking the geochemical rate measurement with nifH expression. This same site also had the lowest diversity (non-parametric Shannon = 2.75). At the two other sites, we also detected nifH transcripts, however, the mean N2 flux indicated net denitrification. These results suggest that N2-fixation and denitrification co-occur in these sediments. Of the unique sequences in this study, 67% were most closely related to uncultured bacteria from various marine environments, 17% to Cluster III, 15% to Cluster I, and only 1% to Cluster II. These data add to the growing body of literature that sediment heterotrophic N2-fixation, even under high inorganic nitrogen concentrations, may be an important yet overlooked source of N in coastal systems
Saturn Forms by Core Accretion in 3.4 Myr
We present two new in situ core accretion simulations of Saturn with planet
formation timescales of 3.37 Myr (model S0) and 3.48 Myr (model S1), consistent
with observed protostellar disk lifetimes. In model S0, we assume rapid grain
settling reduces opacity due to grains from full interstellar values (Podolak
2003). In model S1, we do not invoke grain settling, instead assigning full
interstellar opacities to grains in the envelope. Surprisingly, the two models
produce nearly identical formation timescales and core/atmosphere mass ratios.
We therefore observe a new manifestation of core accretion theory: at large
heliocentric distances, the solid core growth rate (limited by Keplerian
orbital velocity) controls the planet formation timescale. We argue that this
paradigm should apply to Uranus and Neptune as well.Comment: 4 pages, including 1 figure, submitted to ApJ Letter
Response of Daphnia Magna to Episodic Exposures of Several Types of Suspended Clay
2008 S.C. Water Resources Conference - Addressing Water Challenges Facing the State and Regio
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