| Pattern
zIN, W.
on multi
ering &
solution
streets.
1): 867-
e meter
hives of
traction
mmetric
> UM,
ches for
sensing,
national
Remote
ological
natic, 2:
entation
satellite
sensing,
> image
Sensing,
ul 2004
METHOD OF THE HIGH ACCURACY RESOLVING
RANGE/VELOCITY UNCERTAINTY FOR THE LASER SCANNER
WITH LINEAR FM
V. M. Lisitsyn, S. V. Tikhonova
7, Victorenko Street, 125319, Moscow, Russian Federation - lvm@gosniias.ru
———ÁRÀ—————
Commission I, WG I/3
KEY WORDS: Laser scanning, Infrared, Method, Measurement, Real-time, Algorithms, Precision, Modelling
ABSTRACT
The laser scanning system on basis of CO, laser with continuous radiation with 10.6 uum wavelength situated onboard of aircraft is
considered. The system is intended for remote sensing of surface ahead of aircraft. Simultaneously distance image of observed scene
has to be formed and vehicle own velocity has to be measured. The system operates in a mode of azimuthal one-line scanning across
a trajectory of flight. For distance measurement linear-frequency modulation with pulse compression is used. Pulse compression is
produced with dispersive acoustic delay line. Mathematical expressions are known that permit to resolve distance/speed uncertainty
in this case. These expressions need two sensing of each element of a surface. However in reality scanning is carried out
continuously, so two neighbor sensings is made on different elements of surface.
Suggested method permit to increase noticeably the accuracy of vehicle own velocity measurement while permitting to measure
distance to each element of surface in case of continuous scanning. For this purpose the fact is used, that value of the carrier own
velocity is slowly varying function. So, averaging and extrapolation of the information is made line by line to increase accuracy of
vehicle own velocity measurement. For each sensing, distance is calculated based on the extrapolated velocity value.
INTRODUCTION
The laser scanning system on basis of CO, laser with
continuous radiation with 10.6 um wavelength situated onboard
of aircraft is considered. The system is intended for remote
sensing of surface ahead of aircraft. Simultaneously distance
image of observed scene has to be formed and vehicle own
velocity has to be measured. The system operates in a mode of
azimuthal one-line scanning across a trajectory of flight. For
distance measurement linear-frequency modulation with pulse
compression is used. Pulse compression is produced with
dispersive acoustic delay line [Stephan, B., 1085- Dansac, 1,
Meyzonnette, J. L., 1985].
In the system realizing such kind of modulations (fig. 1), almost
all laser output power goes to acoustic-optical modulator
(AOM) where radiation gets linear FM with the triangular law
of change of frequency. The modulated laser beam goes through
optics and the scanner and is radiated in space, and the part of
not modulated radiation branches off to the photodetector where
it mixes up with the received reflected signal. As a result of this
mixing optical heterodyning of received laser signal is carried
out, and linear FM is transferred to intermediate frequency. At
presence of vehicle own velocity frequency of the reflected
signal is increased by the Doppler shift value. As vehicle own
velocity can vary considerably, radio oscillator is used (unlike
to [Stephan, B., 1985]) to maintain a necessary dynamic range
on frequency.
Further the signal goes to a dispersive acoustic delay line
(DADL) where it is compressed in the number of times equal to
product of frequency deviation AF and linear FM half-cycle to.
An output of DADL is series of short pulses going with
frequency that is equivalent of double modulation frequency of
laser. The generated pulses are received by the counter which
measures a time delay /44 between the compressed pulses and
clock pulses marking the beginning of sensing.
Measured delay times goes to the processor of preliminary
processing of the information. A task of the processor is
range/velocity uncertainty resolution, radio oscillator
management in real time and transformation of distance
measurements to a kind convenient for the further processing.
We shall accept periodicity of sensing equal to tg, = 20 ps, that
corresponds to one linear section of triangular linear FM with
deviation of frequency of radiation AF = 40 MHz. One sensing
gives one element of distance image.
By results of double sensing slant-distance up to probed surface
that is perpendicular to axis of beam (R) and a radial component
of vehicle velocity (V) can be accordingly determined as [2, 3]:
CT.
R= 4 " + Eu
pull dl in (1)
dr del del
dev
where c is the velocity of light; À is the radiation wave-length;
+ : : > - ^ S ;
(4, is delay time of the compressed pulse for increasing
section of linear FM of the reflected signal; 7 4, is delay time of
the compressed pulse for decreasing section of linear FM of the
reflected signal, AF is the deviation of radiation frequency, /a«
is the linear FM half-cycle.
Delay time is expressed as:
2. U dev
d Cea =D; A e te +, (2)
where D is slant-distance;