412 research outputs found
The effect of temperature and pressure on the distribution of iron group elements between metal and olivine phases in the process of differentiation of protoplanetary material
The distribution patterns of Ni, Co, Mn, and Cr were studied in olivines of various origins: from meteorites (chondrites, achondrites, pallasites), which are likely analogs of the protoplanetary material, to peridotite inclusions in kimberlite pipes, which are analogs of mantle material. According to X-ray microanalysis data, nickel is concentrated in peridotite olivines, while manganese is concentrated in meteoritic olivines. The maximum chromium content was found in ureilites, which were formed under reducing conditions. Experiments at pressures of 20 to 70 kbar and temperatures of 1100 to 2000 C have shown that in a mixture of olivine and Ni metal or NiO, nickel enters the silicate phase, displacing Fe into the metallic phase. Equilibrium temperatures were estimated from the Fe, Ni distribution coefficients between the metal and olivine: 1500 K for pallasites, 1600 K for olivine-bronzite H6 chondrites, 1200 K for olivine-hypersthene L6, 900 K for LL6, and 1900 K for ureilites (at P = 1 atm). The equilibrium conditions of peridotites are close to T = 1800 K and P over 100 kbar. It is concluded that there is a sharp difference between the conditions of differentiation of the protoplanetary material at the time meteorites were formed and the conditions of differentiation of the planets into concentric layers
Accretion and outflow activity on the late phases of pre-main-sequence evolution. The case of RZ Piscium
RZ Psc is an isolated high-latitude post-T Tauri star that demonstrates a UX
Ori-type photometric activity. The star shows very weak spectroscopic
signatures of accretion, but at the same time possesses the unusual footprints
of the wind in Na I D lines. In the present work we investigate new
spectroscopic observations of RZ Psc obtained in 2014 during two observation
runs. We found variable blueshifted absorption components (BACs) in lines of
the other alcali metals, K I 7699 \AA\ and Ca II IR triplet. We also confirmed
the presence of a weak emission component in the H line, which allowed
us to estimate the mass accretion rate on the star as Msun yr. We could not reveal any clear periodicity in the
appearance of BACs in sodium lines. Nevertheless, the exact coincidence of the
structure and velocities of the Na I D absorptions observed with the interval
of about one year suggests that such a periodicity should exist
CompHEP-PYTHIA interface: integrated package for the collision events generation based on exact matrix elements
CompHEP, as a partonic event generator, and PYTHIA, as a generator of final
states of detectable objects, are interfaced. Thus, integrated tool is proposed
for simulation of (almost) arbitrary collision processes at the level of
detectable particles. Exact (multiparticle) matrix elements, convolution with
structure functions, decays, partons hadronization and (optionally) parton
shower evolution are basic stages of calculations. The PEVLIB library of event
generators for LHC processes is described.Comment: Standard LaTeX, 4 pages. To appear in the proceedings of the Seventh
International Workshop on Advanced Computing and Analysis Technics in Physics
Research (ACAT2000, Fermilab, October 16-20, 2000
B fields in OB stars (BOB): Detection of a magnetic field in the He-strong star CPD-57{\deg} 3509
We report the detection of a magnetic field in the helium-strong star CPD-57
3509 (B2 IV), a member of the Galactic open cluster NGC3293, and characterise
the star's atmospheric and fundamental parameters. Spectropolarimetric
observations with FORS2 and HARPSpol are analysed using two independent
approaches to quantify the magnetic field strength. A high-S/N FLAMES/GIRAFFE
spectrum is analysed using a hybrid non-LTE model atmosphere technique.
Comparison with stellar evolution models constrains the fundamental parameters
of the star. We obtain a firm detection of a surface averaged longitudinal
magnetic field with a maximum amplitude of about 1 kG. Assuming a dipolar
configuration of the magnetic field, this implies a dipolar field strength
larger than 3.3 kG. Moreover, the large amplitude and fast variation (within
about 1 day) of the longitudinal magnetic field implies that CPD-57 3509 is
spinning very fast despite its apparently slow projected rotational velocity.
The star should be able to support a centrifugal magnetosphere, yet the
spectrum shows no sign of magnetically confined material; in particular,
emission in H{\alpha} is not observed. Apparently, the wind is either not
strong enough for enough material to accumulate in the magnetosphere to become
observable or, alternatively, some leakage process leads to loss of material
from the magnetosphere. The quantitative spectroscopic analysis of the star
yields an effective temperature and a logarithmic surface gravity of 23750+-250
K and 4.05+-0.10, respectively, and a surface helium fraction of 0.28+-0.02 by
number. The surface abundances of C, N, O, Ne, S, and Ar are compatible with
the cosmic abundance standard, whereas Mg, Al, Si, and Fe are depleted by about
a factor of 2. This abundance pattern can be understood as the consequence of a
fractionated stellar wind. CPD-57 3509 is one of the most evolved He-strong
stars known.Comment: 15 pages, 11 figures. Accepted for publication in A&
Magnetic field geometry and chemical abundance distribution of the He-strong star CPD -57 3509
The magnetic field of CPD -57 3509 was recently detected in the framework of
the BOB (B fields in OB stars) collaboration. We acquired low-resolution
spectropolarimetric observations of CPD -57 3509 with FORS2 and high-resolution
UVES observations randomly distributed over a few months to search for
periodicity, to study the magnetic field geometry, and to determine the surface
distribution of silicon and helium. We also obtained supplementary photometric
observations at a timeline similar to the spectroscopic and spectropolarimetric
observations. A period of 6.36d was detected in the measurements of the mean
longitudinal magnetic field. A sinusoidal fit to our measurements allowed us to
constrain the magnetic field geometry and estimate the dipole strength in the
range of 3.9-4.5kG. Our application of the Doppler imaging technique revealed
the presence of He I spots located around the magnetic poles, with a strong
concentration at the positive pole and a weaker one around the negative pole.
In contrast, high concentration Si III spots are located close to the magnetic
equator. Further, our analysis of the spectral variability of CPD -57 3509 on
short time scales indicates distinct changes in shape and position of line
profiles possibly caused by the presence of beta Cep-like pulsations. A small
periodic variability in line with the changes of the magnetic field strength is
clearly seen in the photometric data.Comment: 11 pages, 5 tables, 7 figures, accepted for publication in MNRA
Автомобильный абсорбционный кондиционер
The purpose of this study is to develop a circuit for an automobile air conditioner, which will reduce the consumption of power developed by the engine. This paper proposes the design of an automobile absorption air conditioner. A description of the principle of operation of an automobile absorption air conditioner operating on a cycle of a one-stage absorption refrigeration machine has been given in the paper. It consists of a stripper (generator), a condenser, an absorber, an evaporator. Lithium bromide (LiBr) solution has been used as an absorbent, which has a low boiling point, is non-toxic and safe. 3D-models of the absorber and generator of an automobile absorption air conditioner has been developed in the course of the research. The absorber is designed to form a weak absorbent solution. This solution is supplied to the generator heat exchanger using a liquid pump. There it is heated by the exhaust gases to the boiling point. The solution evaporates and water vapor enters the condenser (evaporator). In the generator, the solution is concentrated from 52 to 60 %. After that, water vapor is supplied to the absorber from the condenser, and a concentrated absorbent solution is supplied from the generator. It should be noted that the generator is a key element of an automobile absorption air conditioning system. Inside it is a strong LiBr solution that feeds the absorber. The design of the air conditioning system does not provide for the use of a compressor and allows to reduce the power loss of the power plant to the drive of the liquid pump. According to calculations, the pump drive power was 0.17 kW. For comparison, the compressor of a modern car air conditioner consumes 7–11 kW. An absorption car air conditioner provides the following advantages: additional engine cooling, environmental friendliness, fuel economy, efficient use of the heat of vehicle exhaust gases. A distinctive feature of this design is that it is proposed to use the heat of the exhaust gases for the process of heating the absorbent. This design can fully compete with the existing modern car air conditioners.Целью исследования являлась разработка схемы автомобильного кондиционера, позволяющего снизить потребление развиваемой двигателем мощности. Предложена конструкция и приведено описание принципа действия автомобильного абсорбционного кондиционера, работающего по циклу одноступенчатой абсорбционной холодильноймашины. Она состоит из десорбера (генератора), конденсатора, абсорбера, испарителя. В качестве абсорбента использовали раствор бромида лития (LiBr), который имеет низкую температуру кипения, не токсичен и безопасен. В процессе исследования разработаны 3D-модели абсорбера и генератора абсорбционного автомобильного кондиционера. Абсорбер предназначен для образования слабого раствора абсорбента, который при помощи жидкостного насоса поступает в теплообменник генератора, где нагревается отработавшими газами до температуры кипения. Раствор испаряется, и пар идет в конденсатор (испаритель). В генераторе раствор концентрируется от 52 до 60 %. После этого в абсорбер из конденсатора поступает водяной пар, а из генератора – концентрированный раствор абсорбента. Следует заметить, что генератор является ключевым элементом системы абсорбционного автомобильного кондиционера. Внутри него находится крепкий раствор LiBr, питающий абсорбер. Конструкция системы кондиционера не предусматривает использование компрессора и позволяет снизить потери мощности силовой установки на привод жидкостного насоса. Согласно расчетам, мощность привода насоса составила 0,17 кВт. Для сравнения, компрессор современного автомобильного кондиционера потребляет 7–11 кВт. Абсорбционный автомобильный кондиционер имеет следующие преимущества: дополнительное охлаждение двигателя, экологичность, экономию топлива, эффективное использование теплоты выхлопных газов автомобиля. Отличительная особенность данной конструкции в том, что для процесса нагрева абсорбента используется теплота отработавших газов. Такая конструкция может составить полноценную конкуренцию имеющимся современным автомобильным кондиционерам
Spectroscopic signatures of magnetospheric accretion in Herbig Ae/Be stars. I. The case of HD101412
Models of magnetically-driven accretion and outflows reproduce many
observational properties of T Tauri stars. This concept is not well established
for the more massive Herbig Ae/Be stars. We intend to examine the
magnetospheric accretion in Herbig Ae/Be stars and search for rotational
modulation using spectroscopic signatures, in this first paper concentrating on
the well-studied Herbig Ae star HD101412. We used near-infrared spectroscopic
observations of the magnetic Herbig Ae star HD101412 to test the magnetospheric
character of its accretion disk/star interaction. We reduced and analyzed 30
spectra of HD101412, acquired with the CRIRES and X-shooter spectrographs
installed at the VLT (ESO, Chile). The spectroscopic analysis was based on the
He I lambda 10,830 and Pa gamma lines, formed in the accretion region. We found
that the temporal behavior of these diagnostic lines in the near-infrared
spectra of HD101412 can be explained by rotational modulation of line profiles
generated by accreting gas with a period P = 20.53+-1.68 d. The discovery of
this period, about half of the magnetic rotation period P_m = 42.076 d
previously determined from measurements of the mean longitudinal magnetic
field, indicates that the accreted matter falls onto the star in regions close
to the magnetic poles intersecting the line-of-sight two times during the
rotation cycle. We intend to apply this method to a larger sample of Herbig
Ae/Be stars.Comment: 8 pages, 1 table, 7 figures, accepted for publication in A&
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