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矢量跟踪是一种将全球导航卫星系统(GNSS)接收机的信号跟踪与导航解算融为一体的跟踪算法。传统的基于矢量延迟/频率锁定环(VDFLL)的跟踪算法普遍采用延迟锁定环(DLL)和锁频环(FLL)鉴别器计算伪距和伪距率偏差观测量,由于锁频环鉴别器存在近似误差和一步延迟效应,在高动态环境下容易造成环路失锁。从直接估计卫星信号特征参数的角度出发,基于中频信号模型构建码相位和载波多普勒的极大似然代价函数,采用非迭代估计算法得到各通道码相位和多普勒频移的估计偏差,转换为卡尔曼滤波器的观测矢量,提出一种基于极大似然估计器(MLE)的矢量跟踪算法。理论分析和仿真结果表明:新算法结合了极大似然估计和矢量跟踪的优点,克服了FLL的延迟效应,与基于VDFLL的矢量环路相比,高动态环境下的跟踪稳定性更好,可以对被遮挡的卫星保持持续的跟踪。 相似文献
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以Harris Sheet作为初始条件, 使用数值模拟的方法, 研究了二级磁岛不稳定重联的一些性质. 在模拟中随着初始扰动的加入, Harris Sheet将演化到非线性阶段, 形成更薄的有剪切速度的电流片, 并伴有一级磁岛产生. 当Lundquist数大于或等于105时, 非均匀剪切速度的Sweet-Parker电流片开始不稳定, 并有二级磁岛出现. 不稳定Sweet-Parker电流片对应的临界长宽比为65. Lundquist数越大, 演化形成的Sweet-Parker电流片越薄, 更多的二级磁岛将出现, 且沿电流片两边向外喷出, 随时间变大, 相互合并. 二级磁岛的出现使重联率增大, 并与Lundquist数之间不再满足S-1/2的关系, 而似乎对它的依赖关系不明显. 相似文献
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Numerical simulations of unsteady flow problems with moving boundaries commonly require the use of geometric conservation law(GCL).However,in cases of unidirectional large mesh deformation,the cumulative error caused by the discrete procedure in GCL can significantly increase,and a direct consequence is that the calculated cell volume may become negative.To control the cumulative error,a new discrete GCL(D-GCL)is proposed.Unlike the original D-GCL,the proposed method uses the control volume analytically evaluated according to the grid motion at the time level n,instead of using the calculated value from the D-GCL itself.Error analysis indicates that the truncation error of the numerical scheme is guaranteed to be the same order as that obtained from the original D-GCL,while the accumulated error is greatly reduced.For validation,two challenging large deformation cases including a rotating circular cylinder case and a descending GAW-(1)two-element airfoil case are selected to be investigated.Good agreements are found between the calculated results and some other literature data,demonstrating the feasibility of the proposed D-GCL for unidirectional motions with large displacements. 相似文献
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跨声速风洞斜孔壁非线性流动试验 总被引:1,自引:0,他引:1
为分析跨声速风洞斜孔壁近壁区域的流动特性,评估气流偏角-压力系数的非线性关联,在0.6 m跨超声速风洞中开展了基于七孔探针的流动特性测量试验。通过气流偏角和压力系数分布分析了斜孔壁流动的差阻特性,以及马赫数、模型升力对斜孔壁流动的影响,最后基于试验结果发展了计算斜孔壁特性参数的微分法,并与经验方法结果进行对比。结果表明,斜孔壁流动呈现出明显的差阻性和非线性,在负压差范围内,近壁流动仍以出流为主;高亚声速时,空风洞模型区孔壁流动特性趋于实壁;安装模型后,随着升力的增大,升力面对应的孔壁区域流动向入流发展,孔壁流动特性趋于开口边界。 相似文献