Analysis of radiometer effect on proof mass in purely gravitational orbit

Spacecrafts with the pure gravity environment are of great significance in precision navigation,gravity field measurement for celestial bodies,and basic physics experiments.The radiometer effect is one of the important interfering factors on the proof mass in a purely gravitational orbit.For the gravity field measurement system based on the inner-formation flying,the relationship between the radiometer effect on the innersatellite and the system parameters is studied by analytical and numerical methods.An approximate function of the radiometer effect suitable for the engineering computation and the correction factor are obtained.The analytic results show that the radiometer effect on the inner-satellite is proportional to the average pressure while inversely proportional to the average temperature in the outer-satellite cavity.The radiometer effect increases with the temperature difference in the cavity,and its minimum exists when the cavity radius increases.When the minimum of the radiometer effect arrives,the ratio of the cavity radius to the inner-satellite radius is 1.189 4.This constant is determined by the spherical cavity configuration and independent of the temperature and pressure distributions.When the ratio of the cavity radius to the inner-satellite radius is more than 10,it is believed that the cavity is large enough,the radiometer effect is approximately proportional to the square of the inner-satellite radius,and the influence of the outer-satellite cavity radius on the radiometer effect can be ignored.     

硅陷阱探测器在350—1064 nm波段的绝对光谱响应度定标

介绍了利用钛宝石可调谐激光器、倍频器和单波长激光器作为光源,在24个波长分立点定标了三个硅陷阱探测器的绝对光谱响应度,解决了红外激光的精确定位与调整、窗口透过率模拟定标等关键技术.结果显示：在激光波长为412—800nm时,三个陷阱探测器定标的不确定度约低于0.05％;当激光波长大于800nm以及低于355nm时,获得的陷阱探测器的定标不确定度约低于0.065％.硅陷阱探测器可以作为空间各类遥感器在350—1064nm波段定标的传递标准探测器. 关键词： 陷阱探测器 低温辐射计 光谱响应度 辐射定标     

辐射探测芯片吸收膜理论设计及镍磷黑膜制备

对新型条形辐射探测芯片的吸收膜层进行了理论分析,并且在金刚石材质的探测芯片上采用电镀方法制备了镍磷黑吸收膜.辐射探测芯片的膜层吸收分析表明,芯片吸收膜层的吸收率正比于表面粗糙度.通过对辐射吸收膜层设计与制作工艺的研究,制备出一种用于条形辐射探测芯片的镍磷黑吸收膜,通过测量其表面形貌结构,表明该膜层具有50nm—1.5μm范围的微结构;红外吸收测试表明其吸收率在1.4—8μm波段为0.989以上,从而提高了辐射探测芯片的性能.     

激光二极管泵浦的重复频率大能量低温Yb:YAG激光器设计

为实现重复频率大能量激光输出,基于Yb:YAG激光介质低温下良好的热特性和激光特性,设计了12kW高功率激光二极管(LD)阵列泵浦的V型腔低温Yb:YAG激光器(液氮温度)。对于泵浦耦合系统和散热结构两个关键点,分别使用光线追迹方法和有限元方法进行了分析,提出了楔形真空窗口和低温热管等解决方案。模拟结果表明,该设计的激光器热效应较低,可实现重复频率大能量输出。     

高真空多层绝热低温容器真空丧失的实验研究

突然的、完全的真空丧失是一种可能发生在高真空多层绝热容器上的严重事故。为了保证高真空多层绝热容器的安全使用,真空丧失后的漏热量是进行高真空多层容器设计的一个重要参数。利用一个工业化高真空多层绝热低温量热器,以液氮为介质研究了其真空丧失前以及内筒壁及外筒壁泄露后的传热。结果表明,真空丧失后排放率及漏热量都会急剧增加,但是多层绝热材料仍然起到了一定的保温作用。由于空气中的部分气体在绝热层内部的凝结,导致低温容器外壁泄露后的漏热量远高于内壁泄露后的漏热量。     

低温辐射计黑体腔吸收率分析

低温辐射计是目前国际上光辐射功率计量中准确度最高的测量系统,其光辐射测量不确定度可达10-5量级,目前国内仅有少数研究机构从国外引进低温辐射计开展计量研究,亟待发展国产低温辐射计替代进口产品。由于低温辐射计采用低温超导状态下的电替代测量原理进行光辐射功率测量,发展低温辐射计的难点之一在于研制黑体吸收腔这一核心光辐射接收器件,并要求黑体腔在各波长下的吸收率都要达到0.999 9以上。为研制超高光谱吸收率的黑体吸收腔,系统性分析了各影响黑体腔光谱吸收率因素,在此基础上利用蒙特卡罗光线追迹方法重点研究了光谱波长、腔体长度、黑材料漫反射系数、黑材料吸收率和入射光空间位置等对斜底黑体腔光谱吸收率的影响。研究结果表明：在300～1 100 nm波长范围内黑体腔吸收率与其内壁涂黑材料的吸收率呈正相关,且在300～1 000 nm范围内的吸收率都达到了0.999 9以上,其中在700 nm处的吸收率取得最大值0.999 941 5,表明采用该类型黑材料的黑体腔只在300～1 000 nm范围内满足低温辐射计设计要求,后续需要根据仿真和测试结果对低温辐射计在不同波长下的光电不等效性进行修正;在黑体腔结构和口径确定的情况下,黑体腔吸收率将随腔长增加而逐渐升高,在40 mm后变化趋缓,并在65 mm后逐渐趋于平衡,考虑到低温辐射计低温舱对腔体尺寸的限制,认为腔体长度与口径之比为6.5时较为合适;黑体腔吸收率还受黑材料的漫反射系数影响,随着黑材料漫反射系数的提高,腔体吸收率呈现近似线性下降,所以在选择黑体腔涂黑材料时,在吸收率等指标相同的情况下应尽量选择镜面吸收黑;黑材料吸收率从0.8到1的变化过程中,腔体吸收率提升了0.05个百分点,且黑材料吸收率为0.92时腔体吸收率可达到0.999 9以上,表明黑材料在其有效工作波长范围内任一点的光谱吸收率都要大于0.92;腔体吸收率还受入射光投射的空间位置影响,光线位置越靠近斜底腔顶点处,腔体吸收率越高,但整体吸收率变化不明显,光线位置对腔体吸收率影响只有不到0.004个百分点,几乎可以忽略,认为斜底腔不同位置处的吸收率是均匀的。研究结果对低温辐射计黑体腔研制有一定参考价值。     

The void nucleation mechanism within lead phase during spallation of leaded brass

The incipient spall behaviours of Cu-34%Zn-3%Pb leaded brass samples with annealed and cryogenic-treated conditions were loaded using one-stage light gas gun experiments. The effect of Pb-phase on dynamic damage nucleation in leaded brass specimens was investigated by means of optical microscopy, scanning electron microscopy and x-ray computer tomography. It was found that the voids of incipient spall were mainly nucleated in the interior of the lead (no tensile stress would be produced within lead according to the impact theory) instead of nucleated at the phase interface as expected by quasi-static damage fracture theory. A nucleation model is proposed in the present work that is the asymmetry high compression zones in the centre of the lead-phase were formed by the rarefaction wave convergence effects of matrix/quasi-spherical lead interface, which caused adiabatic temperature rise that exceeded melting point of lead due to severe plastic deformation, finally led to local melting and void nucleation. In addition, the spall strength and damage rate increased with the increase in the Pb-phase number.     

冷冻靶校准误差和烧蚀层粗糙度对氘氚层均匀性的影响

 理论分析了氘氚层外表面的温差与其粗糙度间的关系;以法国兆焦激光装置LMJ为原型,利用计算流体力学程序Fluent,分别模拟了靶丸轴向偏离黑腔中心不同尺度和烧蚀层存在不同大小的非均匀厚度对氘氚层温度分布的影响,求得了这两种误差引起氘氚层厚度的非均匀度。结果表明：为了满足点火靶的要求,靶丸轴向偏离腔体中心的尺度须在8.5 μm内,烧蚀层轴向粗糙度则应控制在0.72 μm内。     

Serrated magnetic properties in metallic glass by thermal cycle

Fe-based metallic glasses(MGs) with excellent soft magnetic properties are applicable in a wide range of electronic industry. We show that the cryogenic thermal cycle has a sensitive effect on soft magnetic properties of Fe_(78)Si_9B_(13) glassy ribbon. The values of magnetic induction(or magnetic flux density) B and H_c coercivity c show fluctuation with increasing number of thermal cycles. This phenomenon is explained as thermal-cycle-induced stochastically structural aging or rejuvenation which randomly fluctuates magnetic anisotropy and, consequently, the magnetic induction and coercivity. Overall,increasing the number of thermal cycles improves the soft magnetic properties of the ribbon. The results could help understand the relationship between relaxation and magnetic property, and the thermal cycle could provide an effective approach to improving performances of metallic glasses in industry.     

Design and Implementation of Comprehensive Gas Chromatography with Cryogenic Modulation

Comprehensive gas chromatography is the realization of true continuous multidimensional (dual column) gas chromatography. The key requirement in the comprehensive GC experiment is that the second dimension analysis is completed in a rapid time‐frame compared to the elution of components in the first dimension, and that the two coupled dimensions represent ‘orthogonal’ analyses towards the analytes to be separated. The former normally necessitates pulsing of contiguous segments of each chromatographic band from the first to the second dimensions. The two dimensions should be in fluid communication. The comprehensive GC×GC experiment passes all the column flow from the first column to the second column, leading to no sample loss, but this also requires a suitable method for time‐ or zone‐compression of the band to be pulsed to the second column. The final pulse should be narrow, and should be delivered to the second column quickly. A simple procedure can achieve this using the cryogenic modulator that has been recently described by this group. The system uses a cryogenic trap which can be moved away from the cooled zone of the column faster than 10 ms. A fast‐acting pneumatic ram achieves this performance. The cooled column heats up to the prevailing oven temperature within 10–15 ms. Molecules as volatile as C5 alkanes or small aromatics will be fully retained by the trap within the period of modulation used for GC×GC. The technique is simple to implement and requires no special column connections. Using a gas chromatograph which allows control of external events and can acquire from a detector at 50 Hz or faster, and a timing controller for modulation, the comprehensive result can easily and effectively be achieved.