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101.
In this article the charged analogues of recently derived Buchdahl’s type fluid spheres have been obtained by considering a particular form of electric field intensity. In this process, Einstein–Maxwell field equations yield eight different classes of solutions, joining smoothly with the exterior Reissner–Nordstrom metric at the pressure free intersurface. Out of the eight solutions only seven could be utilized to represent superdense star models with ultrahigh surface density of the order 2×1014 gm cm−3. The maximum masses of the star models were found to be 8.223931MΘ and 8.460857MΘ subject to strong and weak energy conditions, respectively, which are much higher than the maximum masses 3.82MΘ and 4.57MΘ allowed in the neutral cases. The velocity of sound seen to be less than that of light throughout the star models. 相似文献
102.
Using a large sample of 78 well-observed double quasars, we have investigated several consequences of the relativistic beaming
model. In this model the ratio of the strengths of the central component and outer lobes of a double source depends on whether
the jet axis lies close to or away from the line of sight, If this is the actual situation, the fraction of emission from
the core,f
c, may be used as a statistical measure of the orientation of the source and should be correlated with other source parameters
which also depend on the inclination of the jet axis to the line of sight.
We findf
c to be anticorrelated with the overall projected linear size of the extended emission but to exhibit a positive correlation
with both the observed degree of misalignment from a collinear double structure, and the ratio of separations of the outer
hotspots from the central component. As might be expected from these relationships, we also find sources of smaller projected
linear sizes to appear more misaligned and the degree of misalignment to be correlated with the ratio of separations of the
outer hotspots. All these correlations are consistent with the predictions of the relativistic beaming model. 相似文献
103.
G.?Dubosclard F.?DonnadieuEmail author P.?Allard R.?Cordesses C.?Hervier M.?Coltelli E.?Privitera J.?Kornprobst 《Bulletin of Volcanology》2004,66(5):443-456
Besides their common use in atmospheric studies, Doppler radars are promising tools for the active remote sensing of volcanic eruptions but were little applied to this field. We present the observations made with a mid-power UHF Doppler radar (Voldorad) during a 7-h Strombolian eruption at the SE crater of Mount Etna on 11–12 October 1998. Main characteristics of radar echoes are retrieved from analysis of Doppler spectra recorded in the two range gates on either side of the jet axis. From the geometry of the sounding, the contribution of uprising and falling ejecta to each Doppler spectrum can be discriminated. The temporal evolution of total power backscattered by uprising targets is quite similar to the temporal evolution of the volcanic tremor and closely reproduces the overall evolution of the eruption before, during and after its paroxysm. Moreover, during the sharp decrease of eruptive activity following the paroxysm, detailed analysis of video (from camera recording), radar and seismic measurements reveals that radar and video signals start to decrease simultaneously, approximately 2.5 min after the tremor decline. This delay is interpreted as the ascent time through a magma conduit of large gas slugs from a shallow source roughly estimated at about 500 m beneath the SE crater. Detailed analysis of eruptive processes has been also made with Voldorad operating in a high sampling rate mode. Signature of individual outburst is clearly identified on the half part of Doppler spectra corresponding to rising ejecta: temporal variations of the backscattered power exhibit quasi periodic undulations, whereas the maximum velocity measured on each spectrum displays a sharp peak at the onset of each outburst followed by a slow decay with time. Periodicity of power variations (between 3.8 and 5.5 s) is in agreement with the occurrence of explosions visually observed at the SE vent. Maximum vertical velocities of over 160 m s–1 were measured during the paraoxysmal stage and the renewed activity. Finally, by using a simplified model simulating the radar echoes characteristics, we show that when Voldorad is operating in high sampling rate mode, the power and maximum velocity variations are directly related to the difference in size and velocity of particles crossing the antenna beam.Editorial responsibility: A. Woods 相似文献
104.
The effect of transient eddy on interannual meridional displacement of summer East Asian subtropical jet 总被引:3,自引:0,他引:3
Using ERA-40 reanalysis daily data for the period 1958-2002,this study investigated the effect of transient eddy(TE) on the interannual meridional displacement of summer East Asian subtropical jet(EASJ) by conducting a detailed dynamical diagnosis.The summer EASJ axis features a significant interannual coherent meridional displacement.Associated with such a meridional displacement,the TE vorticity forcing anomalies are characterized by a meridional dipole pattern asymmetric about the climatological EASJ axis.The TE vorticity forcing anomalies yield barotropic zonal wind tendencies with a phase meridionally leading the zonal wind anomalies,suggesting that they act to reinforce further meridional displacement of the EASJ and favor a positive feedback in the TE and time-mean flow interaction.However,The TE thermal forcing anomalies induce baroclinic zonal wind tendencies that reduce the vertical shear of zonal wind and atmospheric baroclinicity and eventually suppress the TE activity,favoring a negative feedback in the TE and time-mean flow interaction.Although the two types of TE forcing tend to have opposite feedback roles,the TE vorticity forcing appears to be dominant in the TE effect on the time-mean flow. 相似文献
105.
渭河流域一次致洪暴雨过程的中尺度滤波分析 总被引:4,自引:3,他引:1
利用常规高空观测资料和NCEP/NCAR 1°×1°的再分析资料以及25点低通滤波技术,对2003年8月28—29日发生在渭河流域的一次致洪暴雨进行了中尺度分析和探讨,分析出中尺度环流演变特征,总结了渭河流域致洪暴雨的概念模型,认为这次暴雨过程中在以西南气流为主的平均气流场上隐藏着尺度较中尺度平均流场小得多的涡旋,其移动方向和发展程度决定了强降水落区及其强度;高空西风风速脉动与低层南风风速脉动耦合形成了中尺度次级环流圈,其上升支为强降水提供了足够的动力抬升机制;而850 hPa低空急流、700 hPa中尺度低涡、南风脉动以及高空西风风速脉动等条件的合理配置是中尺度次级环流形成的必备因素;地面中尺度辐合线是本次暴雨的触发机制。 相似文献
106.
山东一次区域性暴雨中尺度特征分析 总被引:6,自引:0,他引:6
利用常规资料、地面自动站资料、FY2C卫星云图TBB和多普勒天气雷达资料,对2009年5月9—10日发生在山东的春季区域性暴雨进行分析和研究。结果表明:①强降水是在低层冷空气和深厚西南暖湿气流交汇的过程中产生的,副高异常偏强,制约850~700hPa切变线和地面辐合线停滞少动,产生较长时间的降水。②地面辐合线的形成和维持激发了边界层的辐合上升运动,为暴雨区提供了充足的水汽,冷空气从边界层楔入,与暖湿气流汇合并抬升暖湿气流辐合上升,使上升运动加强,降水增幅。③中尺度对流系统是造成暴雨的主要中尺度系统,多个单体更迭并移经同一区域,形成"列车效应"而产生区域性暴雨。④雷达径向速度图中逆风区和不同高度(超)低空急流的大小对短时强降水预报有一定的指示意义。 相似文献
107.
利用1°×1°NCEP再分析资料和探空资料,对2009年6月3日发生在黄淮流域的强飑线天气过程进行诊断分析,并采用WRF模式进行天气过程模拟和进一步研究。结果表明:本次飑线天气是东北冷涡后部横槽引导冷空气南下与南方暖湿气流相遇引发的。地面干线附近是雷暴和飑线的高发区。这次飑线天气发生在高空急流减弱之际、低空急流建立之前。高低空急流的U、V风分量变化对飑线有一定的指示意义。不同阶段的飑线降水和大风出现位置不同。 相似文献
108.
利用卫星云图、 多普勒天气雷达资料、 常规观测资料和MM5模式模拟结果, 分析了2005年12月4日典型冷涡造成山东半岛暴雪的云带变化、 对流单体的生成与发展、 低空急流特征及雷达强回波带的变化特征。结果表明: 冬季冷涡携带强冷空气南下, 经过渤海暖湿下垫面后影响山东半岛时, 卫星云图上从渤海到山东半岛可以清楚地分析出造成暴雪的西南-东北向结构特征的横向云带; 雷达图上, 在渤海到山东半岛形成一强降雪回波带, PPI径向速度图上可清楚地分析出暴雪区的低空急流和中尺度对流的低空辐合, 雷达径向速度垂直剖面反映暴雪产生在零速度线附近和低空急流的存在; MM5模式模拟结果显示: 暴雪发生时山东半岛在1.5 km存在低空急流, 水平风的时间-高度垂直剖面反映暴雪发生时干冷空气经过暖湿的渤海海面在700 hPa以下出现暖平流, 垂直上升运动和散度的低层辐合、 高层辐散与雷达图像反映的强降雪回波是相对应的。 相似文献
109.
110.
The atmospheric stable boundary layer (SBL) with a low-level jet is simulated experimentally using a thermally stratified
wind tunnel. The turbulence structure and flow characteristics are investigated by simultaneous measurements of velocity and
temperature fluctuations and by flow visualization. Attention is focused on the effect of strong wind shear due to a low-level
jet on stratified boundary layers with strong stability. Occasional bursting of turbulence in the lower portion of the boundary
layer can be found in the SBL with strong stability. This bursting originates aloft away from the surface and transports fluid
with relatively low velocity and temperature upward and fluid with relatively high velocity and temperature downward. Furthermore,
the relationship between the occurrence of turbulence bursting and the local gradient Richardson number (Ri) is investigated.
The Ri becomes larger than the critical Ri, Ricr = 0.25, in quiescent periods. On the other hand, the Ri number becomes smaller than Ricr during bursting events. 相似文献