高空低气压下电晕放电电磁脉冲辐射特性模拟实验

为研究高空低气压下飞行器表面电晕放电电磁脉冲辐射特性,以尖端导体电晕放电为研究对象,进行了低气压下电晕放电电磁脉冲辐射特性模拟实验,给出了辐射电场幅值与气压的关系表达式,并基于气体放电和电磁场理论总结了电晕放电电磁脉冲辐射特性随电压极性、气压以及测试距离的变化规律。结果表明:电晕放电电磁脉冲辐射电场时域波形呈衰减振荡形式,持续时间约为600 ns,首脉冲方向随电压极性的不同而不同,且辐射电场分量主要集中在与放电针相同的极化方向;辐射电场频谱主要分布在500 MHz以内,在35 MHz和170 MHz处出现稳定的波峰;在气压为4~30 kPa范围内,随着气压的降低,放电电磁脉冲辐射电场增强;随着测试距离的增加,电晕放电电磁脉冲辐射电场逐渐衰减。该研究结论可为低气压下飞行器电晕放电电磁脉冲辐射特性研究提供有益参考。     

涡扇发动机轴对称引射收敛喷管红外辐射特性

数值研究了涡扇发动机轴对称引射收敛喷管的红外辐射特性.排气系统的流场计算采用商用数值模拟软件,红外辐射特性计算采用自主开发的软件NUAA-IR,计算分析了轴对称收敛喷管和引射收敛喷管在3~5μm波段红外辐射特性以及喷管内不同固体壁面在探测方向上的红外辐射贡献.结果表明:引射收敛喷管的红外抑制作用主要在于引射加强了尾喷流与环境大气的掺混,减小了尾喷流的长度,降低了燃气流的红外辐射;引射收敛喷管对喷管内固体壁面的遮挡以及降温作用很小,只在方位角为20°方向上对内涵壁面、外涵内壁等中低温壁面有效;引射收敛喷管的总积分辐射强度在方位角为0°~15°范围内与收敛喷管几乎相等,在其他方位角范围内均小于收敛喷管,且在方位角为40°方向上降低幅度达到最大,约为34%.      

红外窗口材料的热辐射特性测量方法

飞行器在大气层内高超声速飞行时,高温窗口迅速成为气动热辐射效应的主要因素,气动热辐射效应会降低甚至破坏红外(IR)探测系统的性能.通过分析红外探测窗口热辐射传输特性,提出一种红外窗口材料的热辐射特性测量方法,并测量了应用于中波红外(MWIR)探测系统的某蓝宝石红外窗口材料在高温状态下的透过率和自身辐射等热辐射数据.结果表明:在100~350℃范围内,0.1mm厚蓝宝石材料薄层在中波红外3.7~4.8μm波段的热辐射特性与温度近似呈3次方关系,温度越高,蓝宝石透过率越小,自身辐射越大.强烈的自身辐射极易导致红外探测器局部饱和现象,对探测系统造成的影响比透过率引起的信噪比(SNR)下降要大得多.      

航天员受银河宇宙线辐射的剂量计算

在近地空间(LEO)和深空探测中,航天员遭受的辐射风险主要来自于银河宇宙线(GCR)照射.银河宇宙线的辐射剂量是航天员辐射风险评价的基础.国际放射防护委员会(ICRP)于2013年提出了新的航天员空间辐射剂量估算方法,以更准确给出空间重离子辐射的剂量.基于此方法,开发了宇宙线粒子在物质中输运的蒙特卡罗程序,并在程序中实现用中国成年男性人体数字模型来仿真航天员.采用该程序计算了粒子(Z=1~92)各向同性照射航天员时器官的通量-器官剂量转换因数,并估算出航天员在近地轨道空间受银河宇宙线辐射的剂量.     

反演航天器在轨瞬态外热流的导热反问题

获得航天器在轨飞行过程中的外热流数据对于研究热控涂层在轨退化规律、各种空间因素对热控产品的影响以及航天器姿轨控发动机羽流热效应都有非常重要的意义,然而直接测量热流存在很多困难,因此可以通过求解导热反问题得到满足一定精度的结果.首先,通过研究利用航天器设备在轨遥测温度值反演出航天器在轨瞬态外热流的导热反问题方法,建立了反演航天器在轨瞬态外热流的数学模型,采用共轭梯度法求解导热反问题并从物理概念角度改进了共轭梯度法的迭代过程以增加其抗不适定性;然后构造了两组能够代表目前大多数地球轨道航天器以及深空探测航天器在轨吸收外热流变化的数值试验对共轭梯度法的反演效果进行了检验.除阶跃变化位置以外反演值与真实值的最大相对偏差为2.9%,反演效果非常好;对于阶跃变化位置的吸收外热流在对反演结果进行分析处理后也能够得到较好的反演结果.      

日盲紫外探测技术在空间预警中的应用

天基紫外预警是反弹道导弹武器的重要手段。文章从地球日盲紫外空间背景和导弹紫外辐射特性两方面进行分析,论证天基紫外空间预警系统可以获得较高的信噪比和信杂比,能够实现低虚警率的空间预警。同时提出了天基紫外空间预警系统可能的3种工作体制：单一基于紫外波段的天基预警系统存在发现目标较晚的问题;紫外—红外双波段天基预警系统可以实现更低的空间预警虚警率;红外—紫外光谱复合天基预警系统可通过紫外光谱观测辨别导弹种类。最后,文章对现有紫外探测技术进行分析,论证了AlGaN和SiC探测器用于天基紫外预警的可行性,并对其工作模式进行了分析。     

Space Life Science of China in 2013

In the past two years, space life science research in China is characterized by a wide area of basic researches for providing foundation for the future China Space Station. The effect of microgravity and radiation was further studied from physiology phenomena to the level of bio-molecule mechanisms. Chinese space life science is maturing in a new era of comprehensive development. Here, we review and summarize researches on space life sciences which were contributed by Chinese scientists.      

Thick galactic cosmic radiation shielding using atmospheric data

NASA is concerned with protecting astronauts from the effects of galactic cosmic radiation and has expended substantial effort in the development of computer models to predict the shielding obtained from various materials. However, these models were only developed for shields up to about 120 g/cm² in mass thickness and have predicted that shields of this mass thickness are insufficient to provide adequate protection for extended deep space flights. Consequently, effort is underway to extend the range of these models to thicker shields and experimental data is required to help confirm the resulting code. In this paper empirically obtained effective dose measurements from aircraft flights in the atmosphere are used to obtain the radiation shielding function of the Earth's atmosphere, a very thick, i.e. high mass, shield. Obtaining this result required solving an inverse problem and the method for solving it is presented. The results are shown to be in agreement with current code in the ranges where they overlap. These results are then checked and used to predict the radiation dosage under thick shields such as planetary regolith and the atmosphere of Venus.     

Analytical-HZETRN model for rapid assessment of active magnetic radiation shielding

The use of active radiation shielding designs has the potential to reduce the radiation exposure received by astronauts on deep-space missions at a significantly lower mass penalty than designs utilizing only passive shielding. Unfortunately, the determination of the radiation exposure inside these shielded environments often involves lengthy and computationally intensive Monte Carlo analysis. In order to evaluate the large trade space of design parameters associated with a magnetic radiation shield design, an analytical model was developed for the determination of flux inside a solenoid magnetic field due to the Galactic Cosmic Radiation (GCR) radiation environment. This analytical model was then coupled with NASA’s radiation transport code, HZETRN, to account for the effects of passive/structural shielding mass. The resulting model can rapidly obtain results for a given configuration and can therefore be used to analyze an entire trade space of potential variables in less time than is required for even a single Monte Carlo run. Analyzing this trade space for a solenoid magnetic shield design indicates that active shield bending powers greater than ∼15 Tm and passive/structural shielding thicknesses greater than 40 g/cm² have a limited impact on reducing dose equivalent values. Also, it is shown that higher magnetic field strengths are more effective than thicker magnetic fields at reducing dose equivalent.     

Method for the prediction of the effective dose equivalent to the crew of the International Space Station

This paper describes a methodology for assessing the pre-mission exposure of space crew aboard the International Space Station (ISS) in terms of an effective dose equivalent. In this approach, the PHITS Monte Carlo code was used to assess the particle transport of galactic cosmic radiation (GCR) and trapped radiation for solar maximum and minimum conditions through an aluminum shield thickness. From these predicted spectra, and using fluence-to-dose conversion factors, a scaling ratio of the effective dose equivalent rate to the ICRU ambient dose equivalent rate at a 10 mm depth was determined. Only contributions from secondary neutrons, protons, and alpha particles were considered in this analysis.