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 共查询到19条相似文献,搜索用时 296 毫秒
1.
包纲  陈道汉  马月华 《天文学报》2004,45(3):279-287
苏梅克-列维9号彗星(SL9)与木星相撞后,在木星上观测到的以常速度(~450m/s)向外扩展的圆环意味着这是碰撞在木星大气中引起的线性波动.我们选取:非旋转、无粘性、密度分层、不可压缩的木星大气模型,而且木星大气以水平速度U=b az运动;给出初始扰动压力P(r;0)作为碰撞的初始条件,用流体力学方程组求解了彗木相撞中的惯性引力波.结果表明:当木星大气以速度U=U0(~170m/s)运动时,彗星碎片的大部分能量都用来产生内波,同时还得到彗星碎片的撞击深度H与水平相速Vp的关系式.当木星大气以速度为U=b az运动时,木星大气的扰动能量不再是在动能和势能间均分。  相似文献   

2.
本文介绍了1994年7月SL-9彗星撞击木星期间3.6cm和12cm射电连续谱观测的结果.在3.6cm波长上,撞击事件无明显的视效应,在12cm波长上,木星的射电平均视流量增加约20%.  相似文献   

3.
Shoemaker-Levy9号童星于1994年7月与木星碰撞己成为事实.本文依据众多碰撞时刻的观测报道,并结合碰撞预报,对其进行了系统研究.分析了用不同观测技术和观测手段所给出的碰撞时刻的报道,强调了碰撞物理过程的重要性.最后,按照统一的物理模式初步确定了各个碎核的碰撞时刻.并归算出木星南纬碰撞带区的自转速度约为9h55min-周,说明它没有受到营核连续撞击的影响.本文还将各管核撞击点在水面上的位置与预报做了比较.  相似文献   

4.
1994年7月16日─22日,苏梅克-列维9号周期慧星的21颗碎片连续撞击木星事件是一次极为罕见的天文现象.文中概括介绍了我国天文学家对慧木相撞事件的光学和射电观测网点、课题设置以及所取得的主要观测结果.  相似文献   

5.
在SL-9彗星撞击木星期间,用上海天台佘山观测站的1.56m望远镜和CCD照相机,观测木星卫星在接击期间的亮度变化,由此测定了六块碎片的撞击时间。  相似文献   

6.
本介绍了1994年7月SL-9彗星撞击木星期间3.6cm和12cm射电连续谱观测的结果。在3.6cm波长上,撞击事件无明显的视效应,在12cm波长上,木星的射电平均视流量增加约20%。  相似文献   

7.
K.ZHANG  陈道汉  C.Jones 《天文学报》2004,45(2):176-185
提出了一个彗木相撞的线性模型.在这个模型中,将木星大气看作是一个分层的、不可压缩和无粘滞的流体层,而与撞击相联的引力波则由一个初始冲力所造成.采用初始冲压P(r,z,0)代替初始表面形变作为初始条件.发现这种做法使得问题的数学处理更加方便,特别是在计算流体粒子的垂直位移和摄动势能方面,后者可以表为P(r,z,0)的有限傅立叶正弦和余弦变换.导出了一个联系彗星碰撞参数、木星大气参数和所设初始冲力之间的关系式.还对两种P(r,z,0)的假设形式分析地导出表面波波高.  相似文献   

8.
天文奇观:彗星联珠撞木星法平今年7月17日~22日发生的苏梅克一利维9号(简称SL9)慧星与木星联珠撞击,吸引了世界天文学界,全球上百座天文台(站)的数以千计的天文学家作了各种观测,取得了丰硕的成果。据各有关报道,SL9慧星碎裂的21块慧核接连与木星...  相似文献   

9.
2019年11月3日,美国航天局(NASA)的木星探测器——朱诺号(Juno)第22次飞掠木星时,在木星的南极地区探测到一个新的巨型风暴。当朱诺号在2016年7月初次抵达木星时,它在木星的两极上方发现了几个红外和可见光波段可见的巨大气旋—其中有9个在北极地区,6个在南极地区。  相似文献   

10.
《天文爱好者》2014,(11):8-9
15日 视直径:41.45″亮度:-2.3^m 木星 在狮子座运行,9日木星留后由顺行变为逆行。日出时位于西南方天空,升起时间进一步提前到夜晚约21时10分,亮度约-2.3等,观测条件不错。12日12时木星合月,木星位于月亮之北5°。  相似文献   

11.
An important feature observed in the wake of the Jupiter-comet clash was the appearance of the ring structure axisymmetrically positioned around the center of the impact. The persistent expansion of the dark rings and its speed indicated an outward propagating gravity wave (Benka, 1995). We employ an analytical model of constant density, uniform finite depth and inviscid fluid layer to investigate the wave motion produced by the impact of Comet Shoemaker-Levy 9 on the Jovian atmosphere. The relevant thermal effects are neglected and an explosion resulting from the collision is then described by an initial impulsive pressure at the surface of the Jovian atmosphere. Under the assumption that all the kinetic energy of a comet fragment is completely converted into the energy of wave motions in the Jovian atmosphere, an analytical formula describing the relationship between the resulting wave motion in the atmosphere and the parameters of a comet fragment (the radius, density and speed) is derived. Results from the present simple analytical model give a qualitative agreement with observations regarding the distance and speed of the waves.  相似文献   

12.
The impact of comet Shoemaker-Levy 9 (SL-9) with Jupiter occurred within a period marking the change over from solar maximum to solar minimum activity in solar cycle 22. In consequence, co-rotating interaction regions, flare-related disturbances, and coronal mass ejections potentially perturbed the Jovian magnetosphere during the period of cometary impact. SOLTIP (Solar Connection with Transient Interplanetary Processes) has called a World Interval, SOLTIP Interval IV, suitably bridging the predicted period of arrival of dust and significant cometary fragments at the planet and, within this time span, 9 May – 9 October, 1994, multi-disciplinary space-based and ground-based solar observations are in process of being formally coordinated, analyzed and made available to observers of the SL-9/Jupiter encounter. In this way, diverse aspects of the circumstances and consequences of the impact of comet Shoemaker-Levy 9 with the Jovian magnetosphere can be interpreted against the background of whatever solar-related interplanetary activity concomitantly occurred.  相似文献   

13.
张璞  陈道汉  马月华 《天文学报》2007,48(2):190-199
提出一个彗木相撞的修正了的线性模型.在这个模型中,将木星大气视为一个转动的、分层的、可压缩和无粘滞的流体层.结果表明,虽然大部分撞击能量仍然转换成内波能量,但不能忽视可压缩效应.  相似文献   

14.
Gajdoš  Š.  Zigo  P.  Kostecký  P.  Taubinger  K. 《Earth, Moon, and Planets》1995,68(1-3):283-287
A report about observations of collision of the comet Shoemaker-Levy 9 with Jupiter is presented. The observations were made both in optical and radio wavelengths. Some consequences of impacts of individual fragments of the comet were detected visually in the 20-cm refractor. 21 days prolonged series of records on a video tape was taken in the focus of the 60-cm reflector, too. 13 serious events from July 16, 1994 to July 23, 1994 on 42.7 MHz radio wavelengths were registered. Its coherence with the pair Shoemaker-Levy 9 and Jupiter in the interaction is the subject of further investigation. More comprehensive results will be published after collecting information about similar observations on radio waves all over the world.  相似文献   

15.
A revised linear model is presented to explain the waves from the collisions of Comet Shoemaker-Levy 9 with Jupiter, in which the Jovian atmosphere is taken as a rotating stratified, compressible and inviscid fluid layer. It is shown that the effect of compressibility can not be ignored, although most of the impacting energy is still converted into the energy of internal waves.  相似文献   

16.
17.
Positional and photometric CCD observations of the comet Shoemaker-Levy 9 fragments were carried out at the Abastumani Astrophysical Observatory. Up to 15 named fragments were detected and their equatorial coordinates and magnitudes are reported. CCD frames were processed using DAOPHOT II. The internal precision of reference star positions down to 18m is 0.″7 and the mean error of photometry does not exceed ±0.3 mag.  相似文献   

18.
In this article we report the peculiar oscillations in the intensity of microwave (4.15 GHz) emission seen during the impact of K fragment of comet Shoemaker-Levy 9 on July 19, 1994. The oscillations begin at 10h 13m 25s UT suddenly with a frequency of ~0.3 Hz and gradually the frequency of these oscillations increases to ~ 1 Hz. The oscillations are not due to local atmosphere or the radio interference from signals of geostationary satellite. They are intrinsic to the microwave emission from Jupiter during the impact of K fragment. Peak-to-peak amplitude of the oscillations is about 34% of the total microwave emission from Jupiter. If we assume that only 50% of the microwave emission is non-thermal and only the non-thermal emission suffered oscillations, then the oscillations are about 68% of the non-thermal emission from Jupiter. The observations also indicate that there are three continuum enhancements during this event and periodic oscillations almost all through. The third enhancement was the largest and during this enhancement there were some additional aperiodic variations. The aperiodic variations were of the order of few minutes and were possibly generated by the gravity waves. The periodic oscillations could be synchrotron emission modulated by the plasma oscillation in the outer magnetosphere. kg]Key words  相似文献   

19.
This article reports the observations of microwave emission from Jupiter during the impact of K, N, P2 and S fragments of the comet Shoemaker-Levy 9. The comparison of microwave bursts intensities produced by these impacts with the impact class and the size of the impactors reveals no correlation. This is in conformity with other observations at microwave frequencies and indicates that the process of burst emission is very complex. The impacts K and N produced three microwave bursts which could possibly be due to further fragmentation of these fragments. The results are discussed in the perspective of synchrotron emission from Jupiter and possible enhancements due to an increase in the radial diffusion coefficient. However, this model does not fully explain the observations.  相似文献   

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