共查询到18条相似文献，搜索用时 171 毫秒
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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
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基于彭秋和等1978年得到的无扰动有限厚盘引力势,根据两个引力势参数(h_(z1)= 0．001kpc,h_(z2)=0．325 kpc)和两个速度分布参数(σ_(v1)=115km/s,σ_(v2)=200 km/s)组合的4种情况,对4×10~5颗脉冲星做了三维蒙特卡洛模拟．4×10~5颗脉冲星按着10~8年间隔被分成20组,计算了每组“逃逸”脉冲星所占比例．对每组中“未逃逸”脉冲星,分别在0＜r＜25kpc和5＜r＜11kpc两个区域中对|z|分布做了统计,研究了“未逃逸”脉冲星在这两个区域中的分段标高和累积标高的演化特征．“未逃逸”脉冲星的分段标高在一定空间范围内的变化不规则,但累积标高的变化却比较平滑．在相对长的时间里(＞10~8年),银盘厚度对脉冲星累积标高演化有显著的复杂影响；在相对短的时间中(＜2×10~7年),这种效应很小,而且累积标高对时间的依赖关系是线性的．在长时间里,初始速度分布对累积标高也有显著影响．在引力势h_(z2)=0．325 kpc的条件下,在径向范围5＜r＜11kpc和时间t=9．22×10~6年以及σ_(v2)=200km/s的情况下,模拟的累积标高是0．596±0．005 kpc． 相似文献
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ＳＬ９慧星撞击木星类似于大气中陨落的流星现象，是替星与木星大气相互作用的过程．慧星碎块的质量取为１０（１２）、１０（１３）和１０（１４）ｋｇ，其密度分别为３．０、１．０、０．８、０．５和０．２ｇ／ｃｍ３．结果表明：这些慧星碎块能穿透木星大气的氨云层，在接近１ｂａｒ的地方爆炸，这与文［１］的模拟结果一致． 相似文献
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本文从高斯型的初始质量密度扰动出发,采用球对称演化模型计算了星系大尺度本动速度随尺度的分布。采用这样一种模型可以避免通常流体模型中线性增长以及窗函数的假设,对不同的宇宙物质主导成分的讨论表明,在各种情况下本动速度的期待值v_p在大尺度上的分布是随着尺度的增大而逐渐减小,这与流体模型以及宇宙弦模型下的趋势是一致的,但对所有参数的可能取值所作的计算表明,理论结果很难解释Dressler等人在r～60h~(-1)Mpc的尺度上观测到的大的本动速度,这很可能是由于在本星系群(LG)之外r 60h~(-1)Mpc的远处存在着一个大质量的物质凝聚区域。 相似文献
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伽利略探测器对木星深部的大气测量，进一步增加了木星大气的平均带状交替快速环流是由其深部大气运动产生的可能性。由于木星高速自转，所以此带状流的基本动力学特征是地转流，即主要动力学平衡是科里奥利力和压力。基于近两维和非轴对称地转慢波的非线性相互作用，描述了一个新的带状交替环流的分析理论，并给出了地转波动的一个显函数关系分析表达式，以及它对应于弱非线性问题的首阶解。对考虑非线性效应的高阶解问题，推导出了一个运动方向交替的快速环流的分析表达式。也对该理论在木星和其他行星的大气动力学研究方面作了讨论。 相似文献
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岳曾元 《中国天文和天体物理学报》1983,(2)
本文将指出,为得到有限厚度旋涡星系中平均扰动引力势φ_1(r)与扰动面密度σ_1(r)的渐近关系,以及对称面上的扰动引力势φ_1(r,0)与σ_1(r)的渐近关系,我们不一定要从相应的三维渐近关系出发,而可以用二重级数展开方法直接地、十分简单地导出。所得结果对于紧卷性准确到m~2(kr)~(-2)量级,对于厚度效应准确到 k〈|z|〉量级,其中m为旋臂数,k为径向波数,r为到星系中心的径向距离,〈|z|〉为星到对称面距离的平均值。这样的精度对于讨论有限厚度扁盘状星系中密度波模式及其增长率通常是足够的。本文结果表明:在上述精度下,如采用〈|z|〉表征厚度,则不同纵向密度剖面下的φ_1(r,0)～σ_1(r)渐近关系可表为统一形式;如采用二星纵向平均距离〈|z-z’|〉表征厚度,则不同纵向密度剖面下的φ_1(r)～σ_1(r)渐近关系可表为统一形式。只有比值〈|z-z’|〉/〈|z|〉才是纵向密度剖面的泛函。对于符合物理意义的通常各种不同密度剖面,此比值都甚接近:对于高斯型纵向密度剖面,此比值为2~(1/2);对于 sech~2(z/z_1(r))型剖面,此比值为 1/In2=1.443;对于 exp[-|z|/z_1(r)]型剖面,此比值为1.5。 相似文献
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《天文学报》2015,(4)
结合最新的哈勃参量H(z)观测数据、重子声学振荡(BAO)数据与普朗克卫星观测得到的宇宙微波背景辐射(CMB)数据,利用马尔柯夫链蒙特卡洛算法(MCMC)对一种相互作用暗能量模型进行了观测限制.这3种数据联合限制得到的各参数的最佳拟合值及1σ误差范围分别为:物质能量密度参数?m=0.266+0.028-0.028,相互作用因子γ=0.090+0.100-0.098,暗能量状态方程参数wX=-1.307+0.263-0.269,哈勃常数H0=74.20+4.66-4.56.相互作用耦合参数γ0表明能量正在从暗物质转移到暗能量.然而,宇宙学常数模型中的巧合性问题在1σ误差范围内依然可以轻微缓解.为了更好地做出比较,还利用BAO+CMB组合数据及单独的H(z)数据对该模型进行了考察,得到的结果如下:(1)H(z)数据能对相互作用参数γ给出更好的限制结果;(2)ΛCDM模型仍然是与观测数据符合得最好的模型,耦合参数γ与其它模型参数(?m,H0)相互关联;(3)在考虑了暗能量与暗物质间的相互作用之后,超新星局域距离阶梯测量与普朗克观测对H0限制结果的冲突问题能够得到一定程度的缓解. 相似文献
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A linear model of Comet Shoemaker-Levy 9's collision with Jupiter ispresented, in which the Jovian atmosphere is taken to be a stratified, incompressible and inviscid fluid layer and the gravity wave associated with the impacts is caused by an initial impulse. Instead of adopting an initial surface deformation, we take an initial impulsive pressure P(r, z, 0) as the initial condition. It is found that this approach is more convenient for the mathematical formulation of the problem, especially for the computation of the vertical displacement of the fluid particles and the perturbation potential energy which can then be expressed by finite Fourier sine and cosine transform of P(r, z, 0).
A relationship among parameters of the impact and the Jovian atmosphereand the assumed initial impulse is deduced. We also derive the wave height of the surface wave analytically for two assumed forms of P(r, z, 0). 相似文献
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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
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《Chinese Astronomy and Astrophysics》2005,29(2):203-212
After the collision of Comet Shoemaker-Levy 9 (SL9) with Jupiter, some ring structures were observed propagating outwards at a constant speed (∼450 m/s) on the Jovian surface. These are thought to be linear waves caused by the collision. A linear model of the collision is presented, in which the Jovian atmosphere is considered as an irrotational, inviscid, stratified and incompressible fluid layer moving at a speed of U = b + az. We take an initial impulsive pressure p(r; 0) as the initial condition and solve the fluid dynamics equations for inertia-gravity waves. It is found that most part of the perturbation energy is used to produce internal waves when Jovian atmosphere moves at a constant speed (U = Uo (∼170 m/s)). A relation between the impact depth H and the horizontal phase speed vp is deduced. Finally, the inertia-gravity waves are discussed for the case U = b + az and it is found that the perturbation energy is then not divided equally between kinetic energy and potential energy because of the effect of a shear. 相似文献
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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
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D.N. Beaumont 《Icarus》1980,41(3):400-409
A baroclinic model of the Jovian atmosphere is assumed. The zonal flow in the neighborhood of the Great Red Spot has been modeled by an unsymmetrical shear layer. The calculated solitary wave flow fields consist of various combinations of regions of closed streamlines and regions of reversed flow. Some of these flows fields closely resemble those observed around the Great Red Spot but the lack of accurate atmospheric data makes it difficult to determine the type of flow field that would be predicted by the theory. 相似文献
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Shin-ya Nitta 《Monthly notices of the Royal Astronomical Society》1999,308(4):995-1005
The aim of this work is to demonstrate the properties of the magnetospheric model around Kerr black holes (BHs), the so-called fly-wheel (rotation driven) model. The fly-wheel engine of the BH–accretion disc system is applied to the statistics of QSOs/AGNs. In the model, the central BH is assumed to be formed at z ∼102 and obtains nearly maximum but finite rotation energy (∼extreme Kerr BH) at the formation stage. The inherently obtained rotation energy of the Kerr BH is released through a magnetohydrodynamic process. This model naturally leads to a finite lifetime of AGN activity.
Nitta, Takahashi & Tomimatsu clarified the individual evolution of the Kerr BH fly-wheel engine, which is parametrized by BH mass, initial Kerr parameter, magnetic field near the horizon and a dimensionless small parameter. We impose a statistical model for the initial mass function (IMF) of an ensemble of BHs using the Press–Schechter formalism. With the help of additional assumptions, we can discuss the evolution of the luminosity function and the spatial number density of QSOs/AGNs.
By comparing with observations , it is found that a somewhat flat IMF and weak dependence of the magnetic field on the BH mass are preferred. The result explains well the decrease of very bright QSOs and decrease of population after z ∼2. 相似文献
Nitta, Takahashi & Tomimatsu clarified the individual evolution of the Kerr BH fly-wheel engine, which is parametrized by BH mass, initial Kerr parameter, magnetic field near the horizon and a dimensionless small parameter. We impose a statistical model for the initial mass function (IMF) of an ensemble of BHs using the Press–Schechter formalism. With the help of additional assumptions, we can discuss the evolution of the luminosity function and the spatial number density of QSOs/AGNs.
By comparing with observations , it is found that a somewhat flat IMF and weak dependence of the magnetic field on the BH mass are preferred. The result explains well the decrease of very bright QSOs and decrease of population after z ∼2. 相似文献
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The actual penetration depth of the Shoemaker-Levy 9 fragments into the Jovian atmosphere is still an open question. From fundamental equations of meteoric physics with variable cross-section, a new analytic model of energy release of the fragments is presented. In use of reasonable parameters, a series of results are calculated for different initial mass of the fragments. The results show that the largest fragment explodes above pressure levels of 3 bars and does not penetrate into the H2O cloud layer of the Jovian atmosphere, and that airburst of smaller fragments occur even above the upper cloud layer. 相似文献
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Martin S. Spergel 《Earth, Moon, and Planets》1977,17(2):123-131
Modeling of the Jovian atmosphere shows that cosmic ray induced albedo neutron decay is inadequate to account for Pioneer 10 and 11 projected electron levels on Jupiter. High energy solar protons must also be excluded as an important neutron decay source. Analysis of neutron flux data near the top of the Jovian atmosphere can lead to the determination of He/H2 and3He/4He ratios for the Jovian atmosphere. 相似文献