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The principle and procedure of laser range detection using two methods: lunar laser ranging experiment and intensity-based method. The lunar laser ranging experiment involves measuring the time it takes for a laser beam to bounce off retroreflectors on the moon and return to earth to determine the distance between the earth and moon. The intensity-based method measures the intensity of the reflected laser beam to determine the distance to a target. The setup of the apparatus, the principle behind the method, and the procedure for conducting the experiment with aluminum, wood, paper, and steel targets.
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surgery, nuclear fusion, material processing, microscopy, laser communication and in many more applications. One of its uses is in an important application that is range detection. Military use it for ranging and target designation etc. There are many experiments to measure some specific range using laser.
One of these is Lunar Laser Experiment. It also has use in LIDAR for range detection. When the Apollo astronauts visited the moon, they planted retro reflector arrays to make possible the Lunar Laser Ranging Experiment. Laser beams are focused through large telescopes on Earth aimed toward the arrays, and the time taken for the beam to be reflected back to Earth measured to determine the distance between the Earth and Moon with high accuracy.
Another method used for range detection is laser pulse time-of-flight distance measurement. Principle of this method is very simple. A laser pulse is projected in the scene and the time the pulse takes to hit the target, reflect and reach the detector is measured. If d is the distance to the target, t is the echo time, and c is the speed of light, then 2d = ct
relation gives distance of detector and target. In this case time t should be greater than pulse width.
There are many other methods which are used for distance or range finding. In our experiment we used a simpler method which depends on intensity of reflected beam.
etc,
passes through beam splitter and lenses, for collimation and converging, and falls on target. The alignment should be made such that reflected part of beam from target falls on beam splitter and then on detector. Detector is placed on opposite side of beam splitter, i.e. partial beam of laser beam, reflected from beam splitter is reflected on one side while detector is on other side and reflected light from target falls on detector. A converging lens is placed after beam splitter, which focuses light of laser.
After laser source collimation lenses are placed. First converging lens is of small focal f 1 length so it diverge light after its focal point and a second lens of larger focal length f 2 is placed at distance d= f 1 +f 2 from first lens. This will produces collimated beam. Beam splitter is placed between the collimation lenses. Another lens is used after the collimation lenses which converge light. This lens should be of large focal point and target is detected by this lens.
Fig. Setup of apparatus
experiment.
on sliding stand at distance large than focal point. Distance of target from lens is noted and intensity of reflected beam is also measured. Target is slowly changed in position and intensity is measured. Target is brought from far focal point to near lens point and intensity is measured for all positions. This procedure is repeated for many targets. Then position versus intensity plot is taken.
Normalized intensity plots against position of different targets are shown. All targets give maximum reflected intensity at focal point if lens used after for converging of collimated beam.
1. Aluminum:- Aluminum was used as target. Our goal was to detect its position when it was on focal point. It intensity observed at different positions shows that it has maximum intensity reflected at focal point. Its plot is given below. Maximum intensity is reflected at focal point because at that point large intense beam highly focus fall on target so there is a big chance of reflection at this point.
3. Paper:- Third material used as target was paper. Its normalized intensity plot against position of paper is shown. This plot again shows maximum intensity at focal point of lens.
Intensity measured at different position of target paper
Position Intensity Position Intensity Position Intensity Position Intensity
44 50 34 66 24 79 14 52
42 51 32 82 22 68
40 55 30 99 20 61
38 56 28 102 18 57
36 59 26 96 16 53
4. Steel:- Another target used was steel. Its normalized intensity plot against position is given which says maximum intensity corresponds to focal point.
Intensity measured at different position of target paper
Position Intensity Position Intensity Position Intensity Position Intensity
46 52 36 60 26 76 16 55 44 53 34 63 24 65 14 55
42 54 32 80 22 60 40 54 30 99 20 57
38 55 28 96 18 56
point so we can say that we can specify object position that it is at distance f(focal length) from our system and in this way laser is used for range detection. If intensity of reflected light is increasing then we can say that object is behind the focal point and if it is decreasing then we can say that it has crossed focal point.
technology. In missile system it is desired that it should explode at some specific distance above the ground. This can be done by a system fixed at missile firing place but due to weather problems it may not work properly. Another choice is laser based