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41.
The cometary meteoroid ejection model of Jones and Brown [Physics, Chemistry, and Dynamics of Interplanetary Dust, ASP Conference Series
104 (1996b) 137] was used to simulate ejection from comets 55P/Tempel-Tuttle during the last 12 revolutions, and the last 9 apparitions
of 109P/Swift-Tuttle. Using cometary ephemerides generated by the Jet Propulsion Laboratory’s (JPL) HORIZONS Solar System
Data and Ephemeris Computation Service, two independent ejection schemes were simulated. In the first case, ejection was simulated
in 1 h time steps along the comet’s orbit while it was within 2.5 AU of the Sun. In the second case, ejection was simulated
to occur at the hour the comet reached perihelion. A 4th order variable step-size Runge–Kutta integrator was then used to
integrate meteoroid position and velocity forward in time, accounting for the effects of radiation pressure, Poynting–Robertson
drag, and the gravitational forces of the planets, which were computed using JPL’s DE406 planetary ephemerides. An impact
parameter (IP) was computed for each particle approaching the Earth to create a flux profile, and the results compared to
observations of the 1998 and 1999 Leonid showers, and the 1993 and 2004 Perseids. 相似文献
42.
We present a simple, semianalytic model of the vaporization of H2O and HDO ice from a comet nucleus. We use this model to show that the flux of HDO relative to H2O can be much higher, at times, than would be expected from the D/H ratio in the nuclear ice itself. This effect varies with position in the comet's orbit. It is negligible sufficiently near the Sun but could lead to erroneous interpretations of the primordial D/H ratio in cometary ice if measurements are made in other parts of the cometary orbit. 相似文献
43.
44.
Comet Hale-Bopp was observed with the 2.6-m and 1.25-m telescopes of the Crimean Astrophysical Observatory on March 9 and
11, 1997. We determined the linear and circular polarization in the coma. For the dust coma, the linear polarization varied
from 7.8% to 12.4%. The degree of circular polarization was always negative and did not exceed 0.3% with an accuracy of ±0.04%
on average. The passage of a bright star through the cometary coma was monitored with polarimetry and photometry. The wavelength
dependence and spatial variations of optical thickness of dust are obtained from the stellar occultation.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
45.
46.
1 引言彗核分裂是彗星的最重要特征之一.至1982年止文献记录共观测到22个彗核分裂,33个次核[1].1986年哈雷彗星回归时观测到彗核的分裂[2].1996年紫金山天文台200mm赤道望远镜和青岛观象台同时观测到百武彗星的分裂[3].海尔波普彗星从1995年8月到10月曾爆发5次[4].1996年3月至12月不断有喷流射出,彗核活动日趋剧烈[5].1997年3月4日我们观测到彗核的小规模分裂及喷流特征,3月3日我们观测到海尔波普彗星近核照片上有喷流,这可能是3月4日彗核小块分裂的前奏.3… 相似文献
47.
The September 2007 encounter of Earth with the 1-revolution dust trail of comet C/1911 N1 (Kiess) is the most highly anticipated
dust trail crossing of a known long period comet in the next 50 years. The encounter was modeled to predict the expected peak
time, duration, and peak rate of the resulting outburst of Aurigid shower meteors. The Aurigids will radiate with a speed
of 67 km/s from a radiant at R.A. = 92°, Decl. = +39° (J2000) in the constellation Auriga. The expected peak time is 11:36 ± 20 min
UT, 2007 September 1, and the shower is expected to peak at Zenith Hourly Rate = 200/h during a 10-min interval, being above
half this value during 25 min. The meteor outburst will be visible by the naked eye from locations in Mexico, the Western
provinces of Canada, and the Western United States, including Hawaii and Alaska. A concerted observing campaign is being organized.
Added in proof: first impression of the shower.
Prepared as a contribution to the conference proceedings of “Meteoroids 2007”, to be published in the journal “Earth, Moon,
and Planets”. 相似文献
48.
Our observations of Comet C/2004 Q2 (Machholz) in the range from 1.2 to 4.8 µm indicate that the material outflowed from the cometary surface in the form of fragments that separated into gas and dust under sublimation on time scales of the order of days. The albedo of these fragments in the range under study was wavelength independent, while the dust was heated by the Sun to an equilibrium temperature at a cross section Qλ inversely proportional to the wavelength. 相似文献
49.
Broadband imaging of Comet 67P/Churyumov–Gerasimenko has provided more data on the characterisation of the target of the ESA
Rosetta Mission. The comet monitoring between r
h=2.37 and r
h=2.78 AU postperihelion shows a prominent dust coma which extends up to ≈ 25,000 km from the nucleus, and a long dust structure
in approximately anti-tail direction, reaching at least 230,000 km, identified as a neck-line structure. The non-isotropic
dust emission is detected from the structures in the inner coma, and it is reflected on the slope of linear fits of surface
brightness profiles vs. cometocentric projected distance in log–log representation as m ≈ 0.83−0.941. Besides the long dust spike at position angle of 295°, the morphological study of the dust coma confirms the
presence of two structures at position angles of
95 and
195° where the overabundance of dust can be as high as 50% at ρ ≤ 30,000 km. The A
f ρ parameter derived from our R broadband data is 26.0 and 29.8 cm at r
h=2.37 and 2.48 AU postperihelion. The dust reflectivity S′(λ), a measurement of the dust colour, is 0.061±0.019, a rather neutral colour. 相似文献
50.
Canaves Marcus V. De Almeida Amaury A. Boice Daniel C. Sanzovo Gilberto C. 《Earth, Moon, and Planets》2002,90(1-4):335-347
The chemistry of both nitrogen and sulfur presents interesting problems in comets.In this paper, we use a model of cometary
comae with gas-phase chemical kineticsand gas dynamics to predict molecular abundances in the inner coma region for twoof
the brightest comets in the past 20 years, Hyakutake (C/1996 B2) and Hale–Bopp(C/1995 O1). In this progress report we concentrate
on the gas-phase chemistry of thenitrogen sulfide (NS) radical at a heliocentric distance of 1 AU to study the abundanceof
NS using a detailed photo and chemical reaction network with over 100 species andabout 1000 reactions. The results are compared
with recent observations of CometHale–Bopp and reveal that conventional gas-phase reactions schemes do not produceNS in sufficient
quantities to explain the observations. We plan to continue therefinement of the model to improve agreement with observational
constraints. 相似文献