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1.
现代日晕光度计是用于精确测定监测址点的多种大气参量的精密仪器,它已列为我国西部太阳设备选址工作中的重要设备。利用同一架日晕光度计首先对昭通大山包进行了多波段数据采集。在仔细分析初步测光结果的基础上,进一步完善日晕光度计的光学系统。使用改进后的设备对昆明凤凰山址点进行了多次数据采集,都获得了理想数据。这表明日晕光度计的多波段测光系统已能够用于西部太阳选址工作中。  相似文献   

2.
埃文斯目视日晕光度计(Evans Visual Sky Photometer,EVSP)是应用于日冕仪选址的重要仪器,从20世纪40年代一直使用至今,它为现代日晕光度计的定标提供了参考标准。通过使用云南天文台现存的一架EVSP研究了它的工作原理,并重点介绍了所利用的简易定标方法。给出了国际现有的多台EVSP日晕亮度定标曲线。由于EVSP内部光学元件反射率和透过率,以及中性渐变光楔的光学密度等存在未知的时间缓变特点,因此利用这种新定标手段可以高效经济地获得各自的定标曲线。  相似文献   

3.
兴隆1m光学望远镜杂散光效应研究   总被引:1,自引:0,他引:1  
兴隆1m光学望远镜采取了加装挡板等基于经验和定性分析的杂散光抑制措施。用Tracepro光学分析软件对圆顶内1m望远镜的杂散光传播路径做了计算和分析,提出了对1m望远镜的杂散光抑制的改进措施,通过在Tracepro中计算的系统杂散光"归一化点源辐照度透过率(PSNIT)"函数对改进措施进行了评价。计算结果表明:对于有效视场外30°范围的杂散源,改进措施可使得1m望远镜的PSNIT全部下降到10-10;模拟1m望远镜在满月条件下对偏月25°的天体观测(R波段、15等星、t=15~150s),1m望远镜观测信噪比可提高约147%。  相似文献   

4.
1 m新真空太阳望远镜的成像系统包括Hα,Ca Ⅱ和He Ⅰ三个窄带成像通道,三者均使用里奥滤光器系统进行单色像观测。以Hα通道实测图像为例,探讨了在线心-线翼的偏带观测出现的太阳像亮度空间分布不均匀问题的原因。该不均匀性不同于杂散光,其空间分布形式与变化程度随观测波长点的不同而不同。通过对多组实测数据的分析认为,出现亮度不均现象的根本原因是滤光器的视场效应,视场边缘区域的工作波长相对中心区域发生频率漂移。频漂的程度和空间分布特征与光路装调密切相关,通过分析对比2017年3月光路调整前后频漂情况得出结论:在目前Hα成像通道2.2'的视场范围内,视场频漂量最大为0.005 nm,小于透过带带宽,且仅出现在视场左下角边缘。  相似文献   

5.
杂散光由于光学表面散射和地球大气散射引起,降低了光谱图像的空间分辨率。光学系统都存在杂散光,要获得高分辨的光谱图像需要对杂散光进行抑制。多波段光谱仪的杂散光分为两类:(1)光谱桶内由于光机结构引起的杂射光;(2)混在成像光路中并参与色散的杂散光。第1种杂散光可直接测量,约占光谱能量的3%左右。第2种杂散光由于受多种因素影响,所以很难精确测量。从日食光谱测量中测得在观测目标周围对目标产生的杂散光的下限约为10%,并对空间方向的点扩散函数进行测量,为光谱的高分辨重建提供参考。  相似文献   

6.
遮光筒会影响主镜上方的空气流动,不利于主镜表面与周围空气的热交换。以兴隆基地50 cm望远镜为例,应用CFD软件分析了两种消杂散光装置(遮光筒和独立挡光环结构)对主镜区域气流运动和温度的影响。同时根据温度数据计算主镜视宁度。分析结果表明,遮光筒会造成温度分布不均匀、湍流影响范围大、非对称的漩涡绕流等影响。独立挡光环结构的情况下,主镜视宁度减小74%。由此说明,在主镜散热和空气流通方面,主镜遮光筒有较大弊端。将该分析方法与杂散光分析结合,可合理选择杂散光抑制方案,对望远镜设计及改造具有一定参考和应用价值。  相似文献   

7.
一个巨型望远镜方案   总被引:4,自引:0,他引:4  
提出一个有特色的巨型望远镜(FGT)方案.其主镜口径为30米,主焦比为1.2,由1095块圆环形子镜构成.采用地平式装置.光学系统包括Nasmyth系统、折轴(Coude)系统和一个大视场系统.提出一个由4个镜面组成的新的Nasmyth系统,在约10′的视场范围内像斑小于爱里斑,达到衍射极限.比传统的Nasmyth系统的衍射极限视场大得多.可在这样的大视场内同时作好几个小区域的衍射极限的观测.当由Nasmyth系统转换到折轴系统和大视场系统时,采用主动光学技术改变子镜的面形、倾斜和平移,产生一个新的主镜面形,使折轴系统和大视场系统都能得到很好的像质.大视场系统的视场直径25′,场曲轻微,并有可能校正大气色散.给出了子镜面形和位置的公差,并讨论了望远镜的装置和结构,方案中的特色和创新对未来大望远镜的研制有普遍意义.  相似文献   

8.
该文概述了近十余年来得到较多研究和发展的孔径阵列技术及其在射电天文中的应用,如高效馈源照明、扩大单反射面射电望远镜的视场、高效多波束、射频干扰抑制、对射电望远镜反射面缺陷的补偿等.随着孔径阵列(Aperture Array Tiles,简称 AAT)技术的日益成熟和成本的降低,AAT技术有可能成为全新一代射电望远镜(例如无反射面射电望远镜和软件射电望远镜)的基石.  相似文献   

9.
我们和北京天文台恒星室的同志于1975年8月16日(离新星爆发极大前15天左右)使用北京天文台40/200 cm双筒天体照相仪拍摄了NGC 7000区域.由于视场为8°×8°,正巧把新星拍在象场边缘附近.观测时左右筒同时露光,使用柯达103a-0底片,未加滤光片.为了定出新星在这一时刻的星等,  相似文献   

10.
近地天体望远镜由SI600S (4k×4k) CCD升级为STA1600LN (10k×10k) CCD后,观测视场由4 deg~2增至9 deg~2,可用视场直径由望远镜原设计视场的3.14°增至4.28°,超出原设计36%,同时作为CCD密封窗的场镜增厚8.75 mm;两个因素导致10k CCD成像的轴外像差增大,视场外围的像质变差.依据望远镜原始设计光学参数,借助光学设计软件ZEMAX进行像质改善尝试,最终选择在10k CCD场镜前插入一个由两片球面透镜组成的场改正镜,使10k CCD的轴外像差得到校正.同时还提出了一个进一步拓展近地天体望远镜观测能力的设计方案,将望远镜的可用视场从目前的14.38 deg~2扩展至28.27 deg~2.  相似文献   

11.
For the future development of Chinese Giant Solar Telescope (CGST) in Western China, a new sky brightness monitor (SBM) has been produced for the site survey for CGST. To critically examine the performance and sensitivity of SBM, we used it in the observation of the annular solar eclipse in Dali City, Yunnan, on 15 January 2010. The observation met good weather conditions with an almost clear sky during the eclipse. The SBM measurement translates into the solar illuminance changes at a level of 2.4×10?4 I?s?1 during the eclipse. The time of the minimal sky brightness in the field of view (FOV) is found consistent with the time of maximum eclipse. Two local sky regions in the FOV are chosen to make a time series of the calibrated skylight profiles. The evolution of the sky brightness thus calibrated also shows good consistency with the eclipse, particularly between the second and the third contacts. The minimal sky brightness in each local sky region took place within half a minute from the corresponding predicted contact time. Such small time delays were mainly caused by occasional cirri. The minimal sky brightness measured during the eclipse is a few millionths of I ?? with standard deviation of 0.11 millionths of I ??. The observation supports that the single-scattering process (optically thin conditions) is the main contributor to the atmospheric scattering. We have demonstrated that many important aerosol optical parameters can be deduced from our data. We conclude that the new SBM is a sensitive sky photometer that can be used for our CGST and coronagraph site surveys.  相似文献   

12.
LaBonte  Barry 《Solar physics》2003,217(2):367-381
Measurements of the brightness of the clear daytime sky at Haleakala, Maui are presented for the interval 1955 through 2002. The observations are made near the direction of the Sun, where forward scattering off aerosols dominates the sky brightness. The Haleakala summit at 3054 m is normally above the inversion layer. The Haleakala sky is dark; the observed brightness per airmass has a median of 10 millionths of the solar disk and a mode of 5 millionths, with Rayleigh scattering contributing 1 millionth. There is no demonstrable long-term trend in the data.  相似文献   

13.
现代日晕光度计(Sky Brightness Monitor,SBM)是一种测定天文址点白昼大气参量的精密仪器,它已成为国际上太阳选址工作的重要设备之一。与国外同类设备不同的是,云南天文台研制的现代日晕光度计上的CCD相机系统可以被简单拆卸并保存,有利于选址踏勘阶段的携带和运输。为获取组装现代日晕光度计设备时可能存在的CCD离焦所导致的测量误差,于2011年6月在新疆奇台县和宁夏石嘴山市利用当地稳定的日照条件做了多次CCD大离焦量快变试验。统计结果表明,现代日晕光度计的CCD显著离焦可造成的相对测量误差约在6%之内。在正常情况下,即观测者基本按照物镜旋筒刻线标志在望远镜上安装CCD设备时,日晕测量的相对误差一般远小于6%。因此认为这种系统误差对优良址点的测量影响基本可以忽略。  相似文献   

14.
本文从日冕观测和研究的意义出发,叙述了用外遮档及小孔减光测量日晕光度的方法以及在云南和新疆若干选点的初步观测结果。  相似文献   

15.
The Advanced Technology Solar Telescope site survey Sky Brightness Monitor simultaneously images the solar disk and the sky to about 8 solar radii in four wavelengths at 450, 530, 890 and 940 nm. One day of data from Mees Solar Observatory on Haleakala and from the National Solar Observatory at Sacramento Peak (Sunspot, New Mexico) are analyzed. Both sites show strong Rayleigh extinction, but while Haleakala shows a larger aerosol component, Sunspot shows a large variation in the aerosol component. Overall the Haleakala extinction varies as –2 whereas the Sunspot extinction changes from about –3.5 to about –2, suggesting an increasing aerosol component during the day. Water vapor absorption measurements from both sites are similar, though Sunspot shows larger time variations than Haleakala. The instrument-corrected sky brightness from both sites show comparable values, and again the Sunspot data show more variations. The sky brightness values show a radial dependence of sky brightness of r –0.1 at Haleakala, but a dependence of r –1.0 at Sunspot. The wavelength variation of the sky brightness at Haleakala is relatively constant at –1.5 but varies at Sunspot from –1.5 to –0.1 again suggesting an increasing aerosol contribution during the day at Sunspot. Finally, dust measurements near the ground are compared with the extinction wavelength exponent for data taken at Haleakala on 24 Feb. 2003. The measurements suggest more large dust particles are present near the ground than averaged over the whole air column.  相似文献   

16.
Photoelectric observations of night sky brightness at different zenith distances in blue, yellow and red colours have been carried out at Abu-Simbel site. Variations in the night sky brightness and (B-V) colour index with time are detected. These variations have been explained by the change of the galactic latitude of the observed point with time. The deduced results of night sky brightness have been compared with that obtained before at other sites. It has been found for both blue and yellow colours, that Abu-Simbel is the darkest site especially for zenith distances equal or greater than 60°. The present values of night sky brightness and colour have been obtained for the first time at Abu-Simbel site. The average night sky brightness at the galactic plane is 22.58 mag/arc sec2 for blue and 21.66 mag/arc sec2 for yellow. This revised version was published online in August 2006 with corrections to the Cover Date.  相似文献   

17.
Photoelectric measurements have been carried out at Kottamia Observatory site to study night sky brightness and the atmospheric extinction at different wavelengths. The results show that the mean extinction coefficients are k = 0.41, k = 0.28< and k = 0.17 mag/air mass during autumn season. These values are almost the same as that obtained by Mikhail (1979) at the same site during the same season. Results of night sky brightness at different altitudes above the horizon have been obtained. Complete scan each five degrees step in azimuth have been done at altitudes 50°, 60° and 70° to complete the previous measurements given by Nawar et al. (1995). Far from the diffuse galactic light, slight variations in night sky brightness with azimuth have been detected. This revised version was published online in August 2006 with corrections to the Cover Date.  相似文献   

18.
The absolute brightness of the zenith sky was measured using a simple calibrated spectrometer during the annular solar eclipse event on May 21, 2012 in Fujioka City, Japan (36.2924°N, 139.0823°E). The sensitivity of the spectrometer was calibrated as a function of wavelength between 400 and 700 nm with an integral sphere. The brightness of the sky decreased to 6 % of its usual condition at the maximum magnitude of the annular eclipse of 0.95 for all wavelengths. The curve describing the variation of sky brightness accords well with the total luminosity of the solar disk estimated by a simple model that accounts for the limb darkening effect. This study provides zenith sky radiance as a function of wavelength and solar elevation angle, which is useful for the investigation of new optical instruments for atmospheric studies.  相似文献   

19.
The sky brightness is a critical parameter for estimating the coronal observation conditions for a solar observatory. As part of a site-survey project in Western China, we measured the sky brightness continuously at the Lijiang Observatory in Yunnan province in 2011. A sky brightness monitor (SBM) was adopted to measure the sky brightness in a region extending from 4.5 to 7.0 apparent solar radii based on the experience of the Daniel K. Inouye Solar Telescope (DKIST) site survey. Every month, the data were collected manually for at least one week. We collected statistics of the sky brightness at four bandpasses located at 450, 530, 890, and 940 nm. The results indicate that aerosol scattering is of great importance for the diurnal variation of the sky brightness. For most of the year, the sky brightness remains under 20 millionths per airmass before local Noon. On average, the sky brightness is less than 20 millionths, which accounts for 40.41% of the total observing time on a clear day. The best observation time is from 9:00 to 13:00 (Beijing time). The Lijiang Observatory is therefore suitable for coronagraphs investigating the structures and dynamics of the corona.  相似文献   

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