物理学报
物理學報
물이학보
2013年
9期
242-248
,共7页
狄慧鸽*%华灯鑫%王玉峰%闫庆
狄慧鴿*%華燈鑫%王玉峰%閆慶
적혜합*%화등흠%왕옥봉%염경
激光雷达%标定%重叠因子%消光系数
激光雷達%標定%重疊因子%消光繫數
격광뢰체%표정%중첩인자%소광계수
lidar%correction%overlap factor%extinction coeffients
由于激光雷达光轴夹角的存在和光束质量分布的非均匀性,导致理论回波信号与实际回波信号有较大差别,需要对其进行校正.基于数学推导和软件仿真,给出了激光雷达重叠因子的数学表达式,分析了光轴夹角导致的系统重叠因子在全程探测空间的变化情况;分析了光束分布为高斯分布和均匀分布时的重叠因子变化情况;对激光雷达的距离校正信号和Klett算法公式进行了重叠因子修正,最后在对激光雷达系统参数标定的基础上,在重叠区域利用修正的Klett公式对其所测得到的回波信号进行了修正,在探测盲区利用斜率法修正距离校正信号,进而得到了符合理论与实际情况的激光雷达在全程上校正的消光系数曲线.
由于激光雷達光軸夾角的存在和光束質量分佈的非均勻性,導緻理論迴波信號與實際迴波信號有較大差彆,需要對其進行校正.基于數學推導和軟件倣真,給齣瞭激光雷達重疊因子的數學錶達式,分析瞭光軸夾角導緻的繫統重疊因子在全程探測空間的變化情況;分析瞭光束分佈為高斯分佈和均勻分佈時的重疊因子變化情況;對激光雷達的距離校正信號和Klett算法公式進行瞭重疊因子脩正,最後在對激光雷達繫統參數標定的基礎上,在重疊區域利用脩正的Klett公式對其所測得到的迴波信號進行瞭脩正,在探測盲區利用斜率法脩正距離校正信號,進而得到瞭符閤理論與實際情況的激光雷達在全程上校正的消光繫數麯線.
유우격광뢰체광축협각적존재화광속질량분포적비균균성,도치이론회파신호여실제회파신호유교대차별,수요대기진행교정.기우수학추도화연건방진,급출료격광뢰체중첩인자적수학표체식,분석료광축협각도치적계통중첩인자재전정탐측공간적변화정황;분석료광속분포위고사분포화균균분포시적중첩인자변화정황;대격광뢰체적거리교정신호화Klett산법공식진행료중첩인자수정,최후재대격광뢰체계통삼수표정적기출상,재중첩구역이용수정적Klett공식대기소측득도적회파신호진행료수정,재탐측맹구이용사솔법수정거리교정신호,진이득도료부합이론여실제정황적격광뢰체재전정상교정적소광계수곡선.
There has been great difference between the theoretical signals of the lidar’s echo and its actual signals, due to the angles between the laser beam and its receiving optical axis, and the laser intensity distribution being asymmetrical. So the correction of the echo signal is necessary. According to the mathematical derivation and the software simulation, the mathematical expression of the lidar’s overlap factor is given, and the overlap factor curves with detection range are drawn which express the characters over the total detection range, then the best angle between lidar’s emitting axis and the receiving axis is obtained. The overlap factors are analyzed when the laser is Gaussian with a uniform intensity distribution. The lidar distance correction signal and Klett formula are corrected by the overlap factor, and the instrument parameters of the lidor are measured. In the range where the overlap factor is not zero, its correction echo signals and extinction coefficients can be obtained by using the corrected Klett formula. While in the range of the lidar’s blind zone, the signals can be derived by a slope method. Finally, the total correction curve of the extinction coefficients is gained, and it is in accordance with the actual one correction cuive.