首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 140 毫秒
1.
利用浅水模型研究热木星属性参数对其大气环流平衡图案及相曲线相位的影响,分别考虑了热木星半径、自转速率、表面重力加速度这3个参数变化产生的影响.应用热木星HD 189733b的属性参数进行模拟,结果显示:半径、表面重力加速度变化对于热木星大气环流平衡图案及红外相曲线相位的影响也可以忽略.但自转速率变化对于热木星大气环流平衡图案以及红外相曲线相位的影响较大.进而可以推测,在热木星红外相曲线的长期观测中,若极大值和极小值的相位发生了明显变化,则热木星的自转速率改变有可能是原因之一.  相似文献   

2.
本文讨论人造宇宙飞行器的变阻力大气摄动问题,给出摄动的分析解,并与常阻力大气摄动问题进行比较,得到了两个方面的主要结论,一是变阻力大气摄动保留了常阻力大气摄动的基本特征,另一个是变阻力大气摄动的解与帆板的定向有关.  相似文献   

3.
探测系外行星的最终目的是为了寻找系外生命和宣居行星,而系外行星大气是人们了解行星宜居特性的窗口,所以系外行星大气的研究至关重要。近10年来,系外行星大气的理论研究和观测都发展迅速。受观测技术限制,目前观测到大气的系外行星主要是用凌星法探测到的热木星和超级地球,还有用直接成像法探测到的离主星较远的年轻气态巨行星。力求在系外行星大气领域飞速发展之际,对该领域研究现状做简明介绍。首先介绍系外行星大气的观测方法,随后介绍热木星和超级地球的大气概况和研究现状,最后对系外行星大气探测的有关项目进行简要介绍,以展示未来系外行星大气研究的前景。  相似文献   

4.
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   

5.
本顾及湍流外尺度的影响导出了星像抖动频谱的普遍表达式,在均匀光路的情况下得到了分析表达式。理论结果与实验数据相当一致,同时讨论了测量星像抖动所需要的频带宽度以及有限带宽所产生的测量误差。  相似文献   

6.
本文顾及湍流外尺度的影响导出了星像抖动频谱的普遍表达式,在均匀光路的情况下得到了分析表达式。理论结果与实验数据相当一致。同时讨论了测量星像抖动所需要的频带宽度以及有限带宽所产生的测量误差。  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.
卫星圆轨道假设对GPS无线电掩星反演地球大气参数的影响   总被引:3,自引:0,他引:3  
蒋虎 《天文学报》2001,42(3):243-247
给出GPS无线电掩星反演地球大气参数过程中计算大气折射角的解析表达式,以圆轨道假设下的大气折射角计算值为先验约束,采用迭代法对不引入圆轨道假设情况的大气折射角进行归算,在此基础,利用反演方法得到了引入和不引入圆轨道假定两种情况下大气参数(气压和温度)的差分序列,结果表明:卫星圆轨道假设对GPS无线电掩星反演大气参数的影响,在气压方面为1mbar左右,而在气温方面为1K左右,这一结果支持了目前无线电掩星定性误差估计研究中通常引入卫星圆轨道假设这个近似处理方法的合理性,同时也表明:若在高精度反演地球大气参数时,摒弃圆轨道是必要的。  相似文献   

9.
陈道汉  包纲 《天文学报》2003,44(4):337-341
1994年7月18日至24日期间,彗星苏梅克-列维9(SL-9)的超过20块碎片与木星发生了相撞.哈勃空间望远镜(HST)拍摄到的图像揭示了木星大气对撞击的动力学响应.具有重要意义的是观测到5个撞击点周围的圆环,它们以450米/秒的常速度向外运动.环的圆形性表明它们是波.因为对于不同大小的撞击,波速是常量,可以推断出传播速度与爆炸能量无关.这意味着这些波动是线性波.评述现行理论所使用的3类候选波,亦即惯性引力波、声波和地震波,介绍的重点是前面两种.  相似文献   

10.
地球自转、大气角动量和太阳活动的30—60天波动特征   总被引:1,自引:0,他引:1  
本分析了十三年的日长变化、大气角动量和太阳黑子相对数资料,研究了这三种资料序列中30-60天波动过程,用统计分析和检验方法证实这种波动过程在时间尺度上具有随机游动的特性,定量分析表明,在此时间尺度上,大气环流中带风的作用对日长变化的贡献约为87%。如果太阳活动对地球自转中30-60天波动存在激发作用,其作用过程不能完全证明是直接通过大气影响地球自转的。可能存在其他媒介,如通过海洋再作用于大气和固体地球。  相似文献   

11.
Measurements by the Galileo probe in Jupiter's deep atmosphere support the possibility that the mean zonal multiple-jet flows in Jupiter's atmosphere are deep rooted. As a consequence of Jupiter's high rotation rate, the primary dynamics of the zonal flows must be geostrophic, i.e., the dynamic balance is largely between the Coriolis and pressure forces. This paper describes a new analytical theory for the generation of zonal multiple-jet flows on the basis of the nonlinear interaction of slowly traveling, nearly two-dimensional and non-axisymmetric geostrophic waves. An explicit analytical expression for the geostrophic waves is obtained as the leading-order solution of the weakly nonlinear problem. In the high-order problem taking into account of nonlinear effects, an analytical expression for an alternating multiple-jet flow is derived. Implications of the theory for Jupiter and other planets are discussed.  相似文献   

12.
Measurements from the Galileo probe suggest that the zonal winds are deep rooted. Jupiter's high rotation rate makes it likely that the whole outer molecular H/He layer is involved in these long-lived jet flows. Assuming that the primary flows are geostrophic, and that the banded surface structure stretches right through the molecular H/He layer, we examine the conditions for such flows to be stable. As a first step, the linear stability of some prescribed banded zonal flows in a rotating spherical shell is explored. Incompressibility is assumed for simplicity, and the boundary condition is stress-free. We compare solutions for two aspect ratios, appropriate for the molecular H/He layers of Jupiter and Saturn, and two Ekman numbers (E=10−2 and E=10−4). Convective and shear flow instabilities compete in our system. The convective instabilities are of the well-known columnar structure. Shear flow instabilities for the larger Ekman number are similar to the Taylor-Couette instability in rotating annuli. At the lower Ekman number, shear flow instabilities adopt a geostrophic character, assuming the form of rotating columns, similar to the convective instabilities. While the convective instability always sets in outside the tangent cylinder, shear instability can become unstable inside the tangent cylinder. If even a weak zonal flow is present inside the tangent cylinder, the flow is unstable to shear instability. This offers an explanation why the jovian zonal jet structure is much weaker at the higher latitudes that correspond to locations inside the tangent cylinder.  相似文献   

13.
V. Ramanathan  R.D. Cess 《Icarus》1975,25(1):89-103
A dynamical model is presented for the observed strong zonal circulation within the stratosphere of Venus. The model neglects rotational effects and considers a compressible and radiating atmosphere. It is shown that diurnal radiative heating is negligible within the lower stratosphere, a region below 85km, while observational evidence for the strong zonal circulation pertains to the lower stratosphere within which a direct thermal driving for the circulation is absent. The analysis, however, suggests that propagating internal gravity waves generated by diurnal solar heating of the upper stratosphere induce mean zonal velocities within the upper and lower stratosphere.Considering the linearized equations of motion and energy, and following Stern's (1971) analysis for an analogous problem, it is shown that the zonal velocity induced by internal gravity waves is retrograde in direction, a result which is in agreement with observation. The nonlinear equations of motion and energy are then solved by an approximate analytical method to determine the magnitude of the zonal velocity. This velocity increases from zero at the tropopause to about 200 msec?1 at the 85 km level. The velocity near the uv-cloud level compares favorably with the observed value of 100 msec?1.  相似文献   

14.
A cloudy planetary atmosphere at rest is shown to be unstable to disturbances of large horizontal scale. The energy source for the instability is the change in radiative heat flux associated with vertical displacement near the emitting level. A simple model is described in which Qδz, where Q is the net heating rate in the cloud and δz is vertical displacement. The constant of proportionality may be either positive or negative. Disturbances may take the form of either quasi-steady geostrophic motions or amplified inertia-gravity waves. The model is applied to Jupiter's zonal winds and to motions near the Venus cloud tops, and provides a possible explanation for many important features of these two flows.  相似文献   

15.
In the present work, the generation of large-scale zonal flows and magnetic field by short-scale collision-less electron skin depth order drift-Alfven turbulence in the ionosphere is investigated. The self-consistent system of two model nonlinear equations, describing the dynamics of wave structures with characteristic scales till to the skin value, is obtained. Evolution equations for the shear flows and the magnetic field is obtained by means of the averaging of model equations for the fast-high-frequency and small-scale fluctuations. It is shown that the large-scale disturbances of plasma motion and magnetic field are spontaneously generated by small-scale drift-Alfven wave turbulence through the nonlinear action of the stresses of Reynolds and Maxwell. Positive feedback in the system is achieved via modulation of the skin size drift-Alfven waves by the large-scale zonal flow and/or by the excited large-scale magnetic field. As a result, the propagation of small-scale wave packets in the ionospheric medium is accompanied by low-frequency, long-wave disturbances generated by parametric instability. Two regimes of this instability, resonance kinetic and hydrodynamic ones, are studied. The increments of the corresponding instabilities are also found. The conditions for the instability development and possibility of the generation of large-scale structures are determined. The nonlinear increment of this interaction substantially depends on the wave vector of Alfven pumping and on the characteristic scale of the generated zonal structures. This means that the instability pumps the energy of primarily small-scale Alfven waves into that of the large-scale zonal structures which is typical for an inverse turbulent cascade. The increment of energy pumping into the large-scale region noticeably depends also on the width of the pumping wave spectrum and with an increase of the width of the initial wave spectrum the instability can be suppressed. It is assumed that the investigated mechanism can refer directly to the generation of mean flow in the atmosphere of the rotating planets and the magnetized plasma.  相似文献   

16.
The GalileoJupiter atmospheric entry probe was launched along with the Galileoorbiter spacecraft from Cape Canaveral in Florida, USA, on October 18, 1989. Following a cruise of greater than six years, the probe arrived at Jupiter on December 7, 1995. During its 57-minute descent, instruments on the probe studied the atmospheric composition and structure, the clouds, lightning, and energy structure of the upper Jovian atmosphere. One of the two radio channels over which the experiment data was transmitted to the orbiter was driven by an ultrastable oscillator. All motions of the probe and orbiter, including the speed of probe descent, Jupiter's rotation, and the atmospheric winds, contributed to a Doppler shift of the probe radio frequency. By accurately measuring the frequency of the probe radio signal, an accurate time history of the probe–orbiter relative motions could be reconstructed. Knowledge of the nominal probe and orbiter trajectories allowed the nominal Doppler shift to be removed from the probe radio frequency leaving a measurable frequency residual arising primarily from the zonal winds in Jupiter's atmosphere, and micromotions of the probe arising from probe spin, swing under the parachute, atmospheric turbulence, and aerodynamic effects. Assuming that the zonal horizontal winds dominate the residual probe motion, a profile of frequency residuals was generated. Inversion of the frequency residuals resulted in the first in situ measurements of the vertical profile of Jupiter's deep zonal winds. It is found that beneath 700 mb, the winds are strong and prograde, rising rapidly to 170 m/s between 1 and 4 bars. Beneath 4 bars to 21 bars, the depth at which the link with the probe was lost, the winds remain constant and strong. When corrections for the high temperatures encountered by the probe are considered, there is no evidence of diminishing or strengthening of the zonal winds in the deepest regions explored by the Galileoprobe. Following the wind recovery, the frequency residuals offer tantalizing clues to microstructure in the atmospheric dynamics, including turbulence and wave motion.  相似文献   

17.
Despite several spacecraft encounters and numerous groundbased investigations, we still do not know much about Jupiter's deep atmosphere; in fact, the Galileo probe results were so different than anyone had anticipated, that we understand even less about this planet's atmosphere now than before the Galileo mission. We formulate four basic questions in Section 1.3, which, if solved, would help to better understand the chemistry and dynamics in Jupiter's atmosphere. We believe that three out of the four questions (explanation of NH3 altitude profile, characterization of hot spots, altitude below which the atmosphere is uniformly mixed) may be solved from passive sounding of Jupiter's deep (∼ tens of bars) atmosphere via a radio telescope orbiting the planet. Question nr. 4 (the water abundance in Jupiter's deep atmosphere) has been singled out by the Solar System Exploration Decadal Survey as a key question, since the water abundance in Jupiter's deep atmosphere is tied in with planet formation models. In this paper we investigate the sensitivity of microwave retrievals to the composition of Jupiter's deep atmosphere, in particular the water abundance. Based upon present uncertainties in the ammonia abundance and other known and unknown absorbers, including uncertainties in clouds (density and index of refraction), and uncertainties in the thermal structure and lineshape profiles, we conclude that the retrieval of water at depth from microwave spectra (disk-averaged and locally) will be highly uncertain. We show that, if the H2O lineshape profile would be accurately known (laboratory data are needed!), an atmosphere with a near-solar H2O abundance can likely be distinguished from one with an abundance of 10-20×solar O based upon the difference in their microwave spectra at wavelengths ?50 cm. This would be sufficient to distinguish between some proposed scenarios by which Jupiter acquired its inventory of volatile elements heavier than helium. If, in addition, limb-darkening measurements are obtained (again, the H2O lineshape profile should be known), tighter constraints on the H2O abundance can be obtained (see also Janssen et al., 2004, this issue).  相似文献   

18.
We have investigated the formation of jet scale meridional circulation cells on Jupiter in response to radiative and zonal momentum forcing. In the framework of semi-geostrophic theory, the meridional streamfunction is described by an elliptic equation with a source term dependent on the sum of the latitudinal derivative of the radiative forcing and the vertical derivative of the zonal momentum forcing. Using this equation with analytic terms similar to the assumed forcing on Jupiter, we obtained two set of atmospheric circulations cells, a stratospheric and a tropospheric one. A possible shift in the overturning circulation of the high and deep atmosphere can be induced by breaking the latitudinal alignment of radiative heating with the enforced belt and zones. A series of numerical simulations was conducted with the Jovian GCM OPUS, which was initiated with observational data obtained from the Cassini CIRS temperature cross-section and a corresponding geostrophic zonal wind field. Newtonian forcing of potential temperature as well as zonal momentum was applied respectively towards latitudinally and vertically uniform equilibrium fields. In accordance with the analytic illustrations two rows of jet scale circulation cells were created. The stratospheric circulation showed the distribution of upwelling over zones and downwelling over belts, consistent with cloud observations. The tropospheric cells featured a partial reversal of the downward vertical velocity over the belts and a considerable reduction of the upward movement over the zones in the domain, consistent with recent detections of high water clouds and lightning in belts. We also used the modeled new forcing fields as source terms for the semi-geostrophic Poisson equation to attribute the origin of the modeled secondary circulation. In this analysis, the stratospheric circulation cells observed in the model are primarily generated in response to radiative forcing, while momentum forcing induces the shifted configurations in the deep atmosphere.  相似文献   

19.
20.
Hydromagnetic planetary waves propagating through a zonal flow and a transverse magnetic field both of which are sheared in the vertical direction are studied. It is found that the effect of the transverse magnetic field is to make planetary waves, which characteristically propagate westwards, propagate eastwards in both westerly and easterly zonal flows. It is also shown that at a critical level the rays are guided by the zonal flow only and that the waves are either attenuated or escalated by an exponential factor as they cross a critical level.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号