{"title":"A Multiple-receiver Synthetic-aperture Active Sonar Imaging System","authors":"B. L. Douglas, Hua Lee, C.D. Loggins","doi":"10.1109/OCEANS.1992.612706","DOIUrl":null,"url":null,"abstract":"Synthetic aperture iechniqucs have not been widely used in sonar imaging duc to problcms with son:u platform motion, slow mapping iatc, ;ind lncdiuln instnhility. A time-varying medium or nonuniform son:bplntform trajectory will cause ph:ise errors in the soi i ;~ ' rct1111is th:lt dcgradc image quali(y. In :I sufficicntly stA>lc rnctfiuin and with motion compcnsntion. Ihc m:isiinurn possihlc unambiguous mapping rate o f ;I single rcccivcr systcln is approximatcly cqu:rl to one-fourth the propag;ition spccil i n [he medium tinics the width o f the tr:insiniltcr. Even :if this rate, the resulting synthetic :ipcrtiirc im:igcs suffer from specular noise. We present a multiple rcccivcr syslcm for synthetic apcilure sonar imaging nnd :I rohusl algorithm th:ll c:iil pcrfonn thc ncccsssry cstiinalion ml col-rcclion ol' motion emors and phasc errors ;ind c:in map ;it :I faster rate than ;i single receiver syslciri. The synlhclic apcilrirc imaging system consists of a lii~ti-rcsol~itioii s dcsc:in s y tcm which has been rnotlitictl to timiismit over :I n;u-row apei-rure, resulting i n a broader hcaiiiwidlh. which innkcs synthetic apcrture imlging possible. Thc ;rlgorithm u t i lizcs the acoustic returns at niulliplc receivers to foim ;I coin plex val ue d prcl i in i nary i m:igc for c:ic t i trans in i t h u I'S I. Each prclirninary i m q c is translated and rot:itcd relntivc to the previous one by an :tmount detcrmincd by the motion of the s o n x pkitforin. Pcilurlxitions o f thc sonar plntform velocity also C:IUSC i-an?c-tlcpcndcnt phxc errors hctween successive preliminary irnligcs. Translation nnd rotation arc estiimtcd Ihrouyh coi-rcl:ition Ixisctl tcchniqucs, then comectcd Ihrougli i m q c rcgistr:ifioii, The rcgislcrcd images are [hen aligned i n ph;isc h y applying :I rxigcdependent phasc correction. Fin:illy the registered pti:isc corrected imagcs x e coticrcntly superimposed to lorin ;I high-resolution synthetic apcrtirrc s o i w iiiwgc. t Chest cr laggin s i s wait t i Son nl ecli , I11 c.. S;in I n I3a I-IXIIII. ('n I i 10 iii i ;i 93111. The tcchniquc involved i n forming the complexv:ilucd preliminary iixigcs :ind the motion compensation :ind p h x c con'cction :ilgorithms will be presented. The rclnlivc tr:tdc-offs hclwccn coherent superposition to form high-resolution synlliclic :rpcrturc images with specular noise. ant1 magnitude siipcrposilion to foim multiple-look physical :ipcilur-c im:rgcs with less specular noise, will be discussed. We present results of cxperiinents at sea with the prolotypc syiiltictic :ipcrtiirc soii'x system.","PeriodicalId":158109,"journal":{"name":"OCEANS 92 Proceedings@m_Mastering the Oceans Through Technology","volume":"28 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1992-10-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"7","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"OCEANS 92 Proceedings@m_Mastering the Oceans Through Technology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/OCEANS.1992.612706","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 7
Abstract
Synthetic aperture iechniqucs have not been widely used in sonar imaging duc to problcms with son:u platform motion, slow mapping iatc, ;ind lncdiuln instnhility. A time-varying medium or nonuniform son:bplntform trajectory will cause ph:ise errors in the soi i ;~ ' rct1111is th:lt dcgradc image quali(y. In :I sufficicntly stA>lc rnctfiuin and with motion compcnsntion. Ihc m:isiinurn possihlc unambiguous mapping rate o f ;I single rcccivcr systcln is approximatcly cqu:rl to one-fourth the propag;ition spccil i n [he medium tinics the width o f the tr:insiniltcr. Even :if this rate, the resulting synthetic :ipcrtiirc im:igcs suffer from specular noise. We present a multiple rcccivcr syslcm for synthetic apcilure sonar imaging nnd :I rohusl algorithm th:ll c:iil pcrfonn thc ncccsssry cstiinalion ml col-rcclion ol' motion emors and phasc errors ;ind c:in map ;it :I faster rate than ;i single receiver syslciri. The synlhclic apcilrirc imaging system consists of a lii~ti-rcsol~itioii s dcsc:in s y tcm which has been rnotlitictl to timiismit over :I n;u-row apei-rure, resulting i n a broader hcaiiiwidlh. which innkcs synthetic apcrture imlging possible. Thc ;rlgorithm u t i lizcs the acoustic returns at niulliplc receivers to foim ;I coin plex val ue d prcl i in i nary i m:igc for c:ic t i trans in i t h u I'S I. Each prclirninary i m q c is translated and rot:itcd relntivc to the previous one by an :tmount detcrmincd by the motion of the s o n x pkitforin. Pcilurlxitions o f thc sonar plntform velocity also C:IUSC i-an?c-tlcpcndcnt phxc errors hctween successive preliminary irnligcs. Translation nnd rotation arc estiimtcd Ihrouyh coi-rcl:ition Ixisctl tcchniqucs, then comectcd Ihrougli i m q c rcgistr:ifioii, The rcgislcrcd images are [hen aligned i n ph;isc h y applying :I rxigcdependent phasc correction. Fin:illy the registered pti:isc corrected imagcs x e coticrcntly superimposed to lorin ;I high-resolution synthetic apcrtirrc s o i w iiiwgc. t Chest cr laggin s i s wait t i Son nl ecli , I11 c.. S;in I n I3a I-IXIIII. ('n I i 10 iii i ;i 93111. The tcchniquc involved i n forming the complexv:ilucd preliminary iixigcs :ind the motion compensation :ind p h x c con'cction :ilgorithms will be presented. The rclnlivc tr:tdc-offs hclwccn coherent superposition to form high-resolution synlliclic :rpcrturc images with specular noise. ant1 magnitude siipcrposilion to foim multiple-look physical :ipcilur-c im:rgcs with less specular noise, will be discussed. We present results of cxperiinents at sea with the prolotypc syiiltictic :ipcrtiirc soii'x system.
合成孔径技术在声纳成像中存在平台运动缓慢、成像速度慢、成像质量低等问题,尚未得到广泛应用。随时间变化的介质或不均匀的平面轨迹会在地面上引起误差,从而影响图像质量。在:I充分连接和运动协调。在单接收机系统中,可能的无二义映射率约为传播速率的1 / 4到1 / 4,特别是在介质中,信号的宽度为1 / 4。即使是这样的速率,合成的模糊图像也会受到镜面噪声的影响。本文提出了一种用于合成声纳成像的多接收机系统,并提出了一种算法,该算法能够有效地处理图像中不同位置的运动误差和相位误差,其速度比单接收机系统快。该同步成像系统是由一种高分辨率、低分辨率、高分辨率的红外成像系统组成的,这种高分辨率、低分辨率、低分辨率的红外成像系统已经被广泛应用于红外成像领域。这使得合成孔径成为可能。该算法将原始接收机处的声波回波进行分类,输入复合值,并将其转换为初始值,然后将其转换为初始值,再将其转换为初始值,然后将其转换为初始值,每个初始值都被转换并相对于前一个值进行转换,其数量由初始值的运动决定。声纳平台的速度也有C:IUSC - i和?连续的初始序列之间的PHXC错误。首先利用共轭相位校正技术对图像进行平移和旋转估计,然后利用共轭相位校正技术对图像进行拼接,然后利用共轭相位校正技术对图像进行共轭相位校正。最后,将配准后的图像正确地叠加到图像上,得到高分辨率的合成图像。如果胸部落后了,那就等着我的儿子来吧。3 . in I;in I;(I I I 10 I I; I 93111.)本文还将介绍形成该复合体所涉及的技术,并对运动补偿和运动补偿算法进行了初步的阐述。该方法通过相干叠加形成高分辨率的具有镜面噪声的合成图像。我们将讨论如何用较少的镜面噪声来形成多视物理光场。我们介绍了在海上试验的结果,该系统是典型的典型土壤系统。