亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        Length estimation of extended targets based on bistatic high resolution range profile

        2015-04-22 07:49:20QUQuanyou屈泉酉GUOKunyi郭琨毅SHENGXinqing盛新慶

        QU Quan-you(屈泉酉), GUO Kun-yi(郭琨毅), SHENG Xin-qing(盛新慶)

        (School of Information and Electronics, Beijing Institute of Technology, Beijing 100081, China)

        ?

        Length estimation of extended targets based on bistatic high resolution range profile

        QU Quan-you(屈泉酉), GUO Kun-yi(郭琨毅), SHENG Xin-qing(盛新慶)

        (School of Information and Electronics, Beijing Institute of Technology, Beijing 100081, China)

        The approach to estimate the length of extended targets by using the bistatic high resolution range profile (HRRP) is analyzed in this paper. The relationship between the bistatic HRRP and the monostatic HRRP of extended targets are investigated. It is demonstrated by simulations that the target length measured by the bistatic HRRP is more meaningful and accurate than that by the monostatic HRRP, though the monostatic HRRP has been well developed and widely used in target recognizing and classification. The estimation results of a cone shaped target are present and compared at the end of the paper. To assure the reliability of the simulation, the bistatic HRRP is obtained through the scattering field data calculated by a full-wave numerical method, FE-BI-MLFMA.

        bistatic radar; high resolution range profile (HRRP); full-wave numerical method; length estimation

        A bistatic radar system employs separate transmit and receive platforms by a large distance in space. It has many advantages compared with a monostatic radar system[1-4]. In a bistatic system, one or more receivers work cooperatively with a higher cost transmitting platform at a safe standoff distance, and the receivers provide multiple aspect looks of the target , which include more geometric information for target identification than a monostatic radar does[5-6]. In recent years, wideband bistatic imaging has become a research focus and has been widely used in target reorganization and classification. The high resolution range profile (HRRP) plays an important role in radar imaging and automatic target reorganization. The bistatic HRRP of point targets are used to extract the length of a target[7]. Length estimation of extended targets with the bistatic HRRP, however, has not been studied thoroughly.

        In this paper, the bistatic HRRP of extended targets is investigated and compared with the monostatic HRRP. It is demonstrated that although the bistatic and monostatic HRRPs have similar forms, the range resolution is quite different. The bistatic HRRP shows the bistatic scattering information along the bisector of the bistatic angle.

        The bistatic HRRP is simulated using the scattering field computed with the full-wave numerical method, the hybrid FE-BI-MLFMA[8-11]. The precise of this method has been well validated. The estimation result demonstrated that the target length measured by the bistatic HRRP is more meaningful and accurate than the monostatic HRRP.

        1 Analysis of the bistatic HRRP

        1.1 Geometry and signal model

        Fig.1 Geometry of the bistatic radar

        Set the geometric center of the chosen target be the origin of the coordinate, and the ranges ofTrandReare denoted asRTandRR. The vectors of RTand RRcan be expressed by

        (1)

        (2)

        (3)

        S(f)=

        (4)

        Thebistatichighresolutionrangeprofile(bi-HRRP)canbegottenbydoinginverseFouriertransformofEq.(4),andbeexpressedas

        (5)

        (6)

        whererdescribes the range variable along the incident direction. Therefore,Pmcan represent the scattering centers distribution along the incident direction.

        1.2 Bistatic and monostatic HRRPs

        According to the scattering center theory[12], the high-frequency scattering response of an extended target can be approximated as the sum of responses from individual scattering centers. Therefore, we model the scattering response by the individual scattering centers as

        (7)

        (8)

        (9)

        wherβis the bistatic angle of the bistatic radar system. Submitting Eq.(9) to Eq.(7), and Eq.(7) can be rewritten as

        (10)

        (11)

        Thenthebi-HRRPcanbedescribedas

        (12)

        Similarly,wecangetthemon-HRRPofmultipleindividualscatteringcentersas

        (13)

        (14)

        whereBis the band width of the bistatic radar system,c/(2B) is the range resolution of the monosatic radar. Eq.(14) shows that the bistatic range resolution Δrbiis closely related to the bistatic angle. This conclusion is apparently valid for measuring the ranges between isotropic scattering centers using the bistatic HRRP, as the scattering intensities are evenly distributed in the whole space. To measure the extended targets length using the HRRP is first to count the total number of the bistatic scattering centers demonstrated in a bi-HRRP image

        (15)

        (16)

        wherern,r1are the coordinate of thenth and the 1st SC.

        2 Results

        In this section, a perfectly conducting ballistic missile warhead is studied,and the dimensions are shown in Fig.2. The spectra of bistatic HRRPs are shown in Fig.3. Because the range resolution of bistatic radar varies with the bistatic angle, the spectra are modified through interpolation. And it is obvious that the curve blurs in large bistatic angles. The incident elevation angles are 0°, 30°, 50° and 100° in Fig.3a-Fig.3d, and the receive elevation angles change with step of 2°.Because the target is rotationally symmetric, both the incident and receive azimuth angles are chosen to be same and unchanged. To avoid the forward scattering, the bistatic angles change from 0° to 160°. The spectra of monostatic HRRPs are shown in Fig.4. The incident angleθTvaries from 0° to 180° with step of 1°.

        Fig.2 Geometry of a cone shaped missile warhead

        Fig.3 Spectra of bistatic HRRPs

        Fig.5 Length measured by bistatic and monostatic HRRPs

        Scattering center 1-3 marked in Fig.2 are shown in Fig.3 and Fig.4 as continuous curves. The vertical bright lines shown in Fig.3 comes from strong reflections of the cone side and bottom surface. The length measured through the HRRPs are actually the range between any two of SC1-3. The measurement results through Fig.3 are shown in Fig.5 with the legend of “bi”. The corresponding results through Fig.4 are shown in Fig.5 with the legend of “mon”. The theoretical ranges between the scattering centers are also shown as criterions. All measured curves are smoothed by omitting the wide value.

        Fig.4 Spectra of monostatic HRRPs

        It is demonstrated in Fig.4 that the bi-length coincides with the mon-length when the bistatic angleβis smaller than 80°, and varies asβincreases. The bi-lengths show different ranges of SC, and have new physical meanings as the receivers could provide different aspect looks of the target which include more geometric information for target identification than the monostatic radar does.

        3 Conclusion

        Bistatic HRRP through the data of a full-wave numerical method is derived in this paper. Relationships between the bistatic HRRP and the monostatic HRRP are studied. Although the monostatic HRRP has been well developed and widely used in target recognizing and classification, it is demonstrated that the target length measured by the bistatic HRRP (bi-length) is more meaningful and accurate. A preliminary study on the location and amplitude of bistatic scattering centers is presented by comparing the results with the monostatic cases.

        [1] Jackson J A, Rigling B D, Moses R L. Canonical scattering feature models for 3D and bistatic SAR[J]. IEEE Transactions on Aerospace and Electronic Systems, 2010, 46(2): 525-541

        [2] Jackson J A, Rigling B D, Moses R L. Parametric scattering models for bistatic synthetic aperture radar[C]∥Radar Conference RADAR’08, IEEE, NY, USA, 2008.

        [3] Kell R E. On the derivation of bistatic RCS from monostatic measurements[J]. Proceedings of the IEEE, 1965, 53(8): 983-988.

        [4] Qu Quanyou, Guo Kunyi, Mu Haijian, et al. Miss distance measurement based on stable scattering centers of extended targets[J]. Systems Engineering and Electronics, 2013, 35(4): 692-699. (in Chinese)

        [5] Jackson J A. Analytic physical optics solution for bistatic, 3D scattering from a dihedral corner reflector[J]. IEEE Transactions on Antennas and Propagation, 2012, 60(3): 1486-1495.

        [6] Qu Quanyou, Guo Kunyi, Sheng Xinqing. Precise target length estimation based on bistatic SC obtained through scattering characteristics analysis[J]. Journal of Beijing Institute of Technology, 2013, 22(Suppl 1): 95-99.

        [7] Ai X, Li Y, Wang X, et al. Some results on characteristics of bistatic high-range resolution profiles for target classification[J]. Radar, Sonar & Navigation, IET, 2012, 6(5): 379-388.

        [8] Guo K Y, Sheng X Q. Simulation research on scattering characteristics by complex targets[J]. Journal of Systems Engineering and Electronics, 2007, 18(4): 685-691.

        [9] Guo K Y, Sheng X Q. A precise recognition approach of ballistic missile warhead and decoy[J]. Journal of Electromagnetic Waves and Applications, 2009, 23(14): 1867-1875.

        [10] Gou Mingjiang, Wu Yueqian, Sheng Xingqing. Efficient solution of 3D electromagnetic scattering from large homogeneous targets[J]. Journal of Beijing Institute of Technology, 2013, 22(4): 524-529.

        [11] Tian Zhongming, Guo Kunyi, Sheng Xinqing. Effects of surface roughness on monostatic RCS of corner reflector[J]. Transaction of Beijing Institute of Technology, 2011, 31(10): 1227-1230. (in Chinese)

        [12] Keller J B. Geometrical theory of diffraction [J]. JOSA, 1962, 52(2): 116-130.

        (Edited by Cai Jianying)

        10.15918/j.jbit1004-0579.201524.0316

        TN 95 Document code: A Article ID: 1004- 0579(2015)03- 0387- 05

        Received 2014- 02- 28

        Supported by the National Natural Science Fundation of China (61001192)

        E-mail: guokunyi@bit.edu.com

        国产自拍三级黄片视频| 亚洲女同一区二区| 性色做爰片在线观看ww| 亚洲熟少妇在线播放999| 狠狠久久精品中文字幕无码| 久久久精品456亚洲影院| 国产成人AⅤ| 国产视频激情视频在线观看| 亚洲性久久久影院| 在线不卡av片免费观看| 8888四色奇米在线观看| 98色花堂国产精品首页| 国产成人亚洲综合无码精品| 麻豆国产AV网站| 亚洲天堂av在线免费看| 国产视频自拍一区在线观看| a级毛片免费观看在线| 中文字幕在线日韩| 看黄色亚洲看黄色亚洲 | 麻豆人妻性色av专区0000| 亚洲国产精品高清一区| 女邻居的大乳中文字幕| 久久AV中文综合一区二区| 国产一区二区在线观看av| 人妻少妇精品专区性色anvn| 国产日产亚洲系列最新| 最近中文字幕视频高清| 国产一级黄色录像| 日本熟妇精品一区二区三区| 女同三级伦理在线观看| 亚洲欧美精品suv| 精品福利视频一区二区三区| jjzz日本护士| 亚洲av午夜福利一区二区国产 | 亚洲 无码 制服 丝袜 自拍| 一区二区高清视频在线观看| 日韩精品一区二区三区影音视频 | 国产精品狼人久久影院软件介绍 | 亚洲av成人无码网站…| a级毛片免费观看视频| 亚洲人成伊人成综合网中文|