四颗射电源在依巴谷和PPM星表中的光学定位

利用北京天文台施密特望远镜的CCD巡天资料（BATC）中的20次观测,用IRAF软件处理得到星象中心位置,以依巴谷星表和PPM星表作为参考星表,用底片常数法进行处理,得到4颗河外射电源0851 202,1228 126,1442 101,1749 701的光学位置。文中还对所得到的位置与射电位置作了比较。     

射电源0851 202,1228 126,1749 701的光学定位

利用北京天文台施密特望远镜ＣＣＤ类星体多色测光巡天中的１５次观测,以ＮＰＭ星表作为参考星表和底片常数法进行处理,得到３颗河外射电源０８５１＋２０２,１２２８＋１２６,１７４９＋７０１的光学位置。文中分析比较了ＩＲＡＦ软件中计算星象中心的三种方法;同时提出应根据待测星的星等（或星象的半峰宽度）选择合适的采样范围。     

射电源0851＋202,1228＋126,1749＋701的光学定位

利用北京天文台施密特望远镜ＣＣＤ类星体多色测光巡天中的１５次观测,以ＮＰＭ星表作为参考星表和底片常数法进行处理,得到３颗河外射电源０８５１＋２０２,１２２８＋１２６,１７４９＋７０１的光学位置,文中分析比较了ＩＲＡＦ软件中计算星象中心的三种方法;同时提出应根据待测星的星等（或星象的半峰宽度）选择合适的采样范围。     

佘山40cm折射望远镜的天体测量检验

本对已经使用九十年，位于上海西郊佘山的40cm折射望远镜，利用近期拍摄的三张昴星团区域底片，在PDS上量测星象坐标，再利用天体测量标准星场：Eichhorn,H.et al的昴星团区域恒星精确位置，作为底片上星象位置的比较标准，采用作常数、三镒底片归算模型求得在底片中心周围40′×40′的象场范围内定位转换精度达0″.03，对于50′×50′和1°×1°范围，分别达0.″04和0.″05－0.″06。底片常数中相应于彗差项系数达10^－5－10^－6量级，畸变项系数达10^－8量级，这些结果表明：架望远镜的光学和装上光电导星装置的机械传动系统，仍能满足高精度的天体测量工作的要求。     

观测过程中较差大气折射引起的星象移动的计算和研究

本文给出了一种计算观测过程中较差大气折射引起的星象移动的方法，包括焦面最佳转动的确定．算法中除大气折射公式外，都是严格的．本文用这种方法详细计算了我国即将研制的大天区面积多目标光纤光谱望远镜（ＬＡＭＯＳＴ）中较差大气折射引起的星象移动，文中详细计算了望远镜安放在纬度４０．４°，观测天区－１０°δ＋９０°，天体过子午圈前后１．５小时，视场直径５°情况下，星象移动的结果，并得到星象的最大位移为０．８５９″，ＬＡＭＯＳＴ中光纤的直径是３．３″，光纤定位系统可不作校正．本文提出了实现焦面最佳转动的导星方法：在导星元件是ＣＣＤ的情况下，可任选一颗星来引导焦面旋转，只要使星象在ＣＣＤ靶面上作切向位移，其值等于按本文方法计算得到的值，若采用赤径、赤纬分角线方向（四个４５°方向）的星来引导旋转，也可近似地得到焦面的最佳转动．本文提出的算法和导星方法，可应用于任何天区，任意的观测时间和任何形式的焦面可旋转的望远镜．     

紫金山天文台1955年小行星、彗星位置的照相观测

下表所载小行星、彗星的位置(包括两次冥王星的位置)是在1955年全年内所做的照相观测。用以观测的远镜是口径60厘米,焦距300厘米的返射望远镜和口径15厘米焦距150厘米的折光远镜,它们在下表底片序号一栏中相当地以N号和T号表明。每次观测所用比较星通常先自摄影星表,其中也有一部分选自Yale星表和A.G.星表,应用后两种星表的观测,大都利用了以四个底片常数归算星体位置的方法,     

紫金山天文台1956年小行星、彗星位置的照相观测

下表所载小行星、彗星的位置是在1956年全年内所做的照相观测.用以观测的望远镜是口径60厘米,焦距300厘米的返射望远镜和口径15厘米,焦距150厘米的折光望远镜,它们在下表底片号数一栏中相当地以 N 号和 T 号表明.表中观测与计算之差一栏,系与苏联理论天文研究所出版的小行星星历表比较而得的数值.有时观测日期     

人造卫星的视轨迹和人造卫星照相机跟踪机架的论证

一、前言大家知道,人造卫星在天球上运动很快,利用固定装置的人造卫星照相机拍摄,有效露光时间 T 极短,大大限制了拍摄人造卫星的能力.T=d/Fω=d/v其中,d 是底片上星象弥散(圆)直径;F 是照相机的焦距;ω是卫星相对仪器的运动角速度;v 是卫星星象在底片上的运动线速度.     

行星(月球)自转监测望远镜的原理样机地面验证实验

类地行星(月球)自转监测望远镜的科学目标是在行星(月球)表面现场测量行星(月球)自转并研究其内部结构和物理性质.为了验证全新的观测原理和资料处理方法,项目团队设计制造了一套原理样机,在一台商用天文望远镜的光路前端增加3面反射镜组,使其具有同时观测3个视场的能力.自2017年起在地面上开展了观测实验,获得了混合有3视场星象的图像.通过计算星象在前后图像上的位移实现了归属视场识别,使得观测效果与分视场独立观测等同,证明了用一台设备同时观测多视场的可行性.处理图像并通过3个视场中心的指向变化归算地球自转轴的空间指向,与理论值比较偏差平均约1′′,证明了观测原理和数据处理方法有效.对各种观测误差来源进行了分析,包含大气折射、仪器热稳定性和光学分辨能力的影响等,指出采用更长焦距的望远镜可以提高空间分辨率,优化形变控制可以提高观测稳定性.改进多视场同时观测中的光学设计也有助于精度的提高.     

用1.05m望远镜对海尔-波普彗星的照相定位观测

1996年7月和8月间,利用陕西天文台骊山天文观测站1．05m望远镜卡焦照相,对海尔-波普彗星进行了定位观测。该望远镜卡焦焦比为F／10,底片比例尺为20”／mm,无畸变象场约为1平方度天区．用蔡司ASCORECORDE2坐标量度促进行底片测量,归算时采用6常数模型,用PPMsouth星在做参考标准,最终给出在FK5基本系统上（J2000．0历元）各观测时刻海尔-波普彗星的α和δ观测值。     

Acceleration of Numerical Integration of the Equations of Motion of Asteroids

Solar System Research - Finding and studying possible collisions of asteroids approaching the Earth requires a significant amount of computation. This paper describes the R0 program created to...     

A survey of orbits of co-orbitals of Mars

Many asteroids with a semimajor axis close to that of Mars have been discovered in the last several years. Potentially some of these could be in 1:1 resonance with Mars, much as are the classic Trojan asteroids with Jupiter, and its lesser-known horseshoe companions with Earth. In the 1990s, two Trojan companions of Mars, 5261 Eureka and 1998 VF₃₁, were discovered, librating about the L₅ Lagrange point, 60° behind Mars in its orbit. Although several other potential Mars Trojans have been identified, our orbital calculations show only one other known asteroid, 1999 UJ₇, to be a Trojan, associated with the L₄ Lagrange point, 60° ahead of Mars in its orbit. We further find that asteroid 36017 (1999 ND₄₃) is a horseshoe librator, alternating with periods of Trojan motion. This asteroid makes repeated close approaches to Earth and has a chaotic orbit whose behavior can be confidently predicted for less than 3000 years. We identify two objects, 2001 HW₁₅ and 2000 TG₂, within the resonant region capable of undergoing what we designate “circulation transition”, in which objects can pass between circulation outside the orbit of Mars and circulation inside it, or vice versa. The eccentricity of the orbit of Mars appears to play an important role in circulation transition and in horseshoe motion. Based on the orbits and on spectroscopic data, the Trojan asteroids of Mars may be primordial bodies, while some co-orbital bodies may be in a temporary state of motion.     

Graphical representation of periodic motion of the line of nodes of the Moon

In the text-books of astronomy, sections generally related to the Moon deal with the orbital elements of the Earth-Moon system such asa, e, i, , and the time of perigee passage. While the MEAN of the first of the three elements do not vary, mean longitude of the ascending node-mean longitude of the lunar perigee and the time of perigee passage undergoes secular as well as periodic changes due predominantly to the action of the Sun's gravitational attraction. While to a certain degree, explanations related to the calculation of the lunar orbit parameters are given, not a single graphical representation of these short- or long-periodic changes are presented. We allow the number of data related to these periodic changes must cover a large span of time; and if regression of the line of nodes or advances of the line of apses are to be graphically seen, data covering 18.61 and 8.85 yr, respectively, are needed. In this work we particularly aim at the graphical representation of the periodic changes of the line of nodes.     

Equation of state and anisotropy of pressure of magnetars

Magnetars are the neutron stars with the highest magnetic fields up to 10¹⁵–10¹⁶ G. It has been proposed that they are also responsible for a variety of extra-galactic phenomena, ranging from giant flares in nearby galaxies to fast radio bursts. Utilizing a relativistic mean field model and a variable magnetic field configuration, we investigate the effects of strong magnetic fields on the equation of state and anisotropy of pressure of magnetars. It is found that the mass and radius of low-mass magnetars are weakly enhanced under the action of the strong magnetic field, and the anisotropy of pressure can be ignored. Unlike other previous investigations, the magnetic field is unable to violate the mass limit of the neutron stars.     

Observations of the intensity of the penumbra of sunspots

Observations of the penumbral intensity of sunspots in 13 wavelength regions are presented. In 4 wavelength regions 54 sunspots are measured. In the other wavelength regions the number of sunspots considered ranges from 3–19.The penumbral intensity alters with position within the spot. This intensity variation is found to be comparable with the change in intensity from one spot to another. The penumbral intensity is found to be independent of spot size in the sample considered.The penumbra model of Kjeldseth Moe and Maltby (1969) with = 0.055 is supported by the measurements.