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Performance and Progress Report - John Doe FIX: put in the authors ...

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The collection of new sediment samples <strong>and</strong> SPI images <strong>in</strong> August 2006 (with gra<strong>in</strong> size<br />

analysis <strong>in</strong> 0.5 phi steps) roughly at <strong>the</strong> same time as a new multibeam survey will allow<br />

for a better correlation between backscatter <strong>and</strong> gra<strong>in</strong> size <strong>and</strong> also <strong>the</strong> determ<strong>in</strong>ation of<br />

to what extent gra<strong>in</strong> size extracted from profile images is a reliable parameter. Sediment<br />

analyses are underway. When <strong>the</strong>se are complete, <strong>the</strong> ARA analyses will be done <strong>and</strong> <strong>the</strong><br />

results compared with <strong>the</strong> gra<strong>in</strong> size analysis <strong>and</strong> SPI images. The ARA model will be<br />

applied <strong>in</strong> <strong>the</strong> st<strong>and</strong>ard mode with a fixed number of p<strong>in</strong>gs over <strong>the</strong> entire swath of each<br />

multibeam l<strong>in</strong>e <strong>and</strong> also <strong>in</strong> <strong>the</strong> supervised segmentation mode (described above), where<br />

<strong>the</strong> mosaic is first segmented <strong>in</strong> classes <strong>and</strong> <strong>the</strong>n <strong>the</strong> ARA model is applied for <strong>the</strong> each<br />

segmented <strong>the</strong>me <strong>in</strong>dependently.<br />

LIDAR Waveform Analysis: F<strong>in</strong>ally, we cont<strong>in</strong>ue our efforts to explore <strong>the</strong> potential of<br />

LIDAR data as a means to characterize <strong>the</strong> shallow coastal seafloor. Shachack Peeri who<br />

has recently been promoted to Research Scientist has led this effort which has <strong>in</strong>cluded<br />

<strong>the</strong> <strong>in</strong>vestigation of <strong>the</strong> use of special characteristics of <strong>the</strong> Raman waveform for <strong>the</strong><br />

robust identification of returns from very shallow waveforms. Peeri has noticed that <strong>in</strong><br />

very shallow water, <strong>the</strong> head <strong>and</strong> rise of <strong>the</strong> waveform shape are <strong>the</strong> same as <strong>the</strong> basic<br />

Raman waveform, but along with a decrease <strong>in</strong> <strong>the</strong> digital number values of <strong>the</strong> tail <strong>and</strong><br />

<strong>the</strong> fall, <strong>the</strong> peak shifts toward <strong>the</strong> head of <strong>the</strong> waveform <strong>and</strong> decreases. In support of<br />

this research as well is <strong>in</strong> support of <strong>the</strong> upcom<strong>in</strong>g Shallow Survey 2008 Conference (see<br />

below), we have, <strong>in</strong> collaboration with NOAA, <strong>the</strong> Army Corps of Eng<strong>in</strong>eers, <strong>and</strong> our<br />

<strong>in</strong>dustrial partners LADS/TENIX, collected three new LIDAR datasets <strong>in</strong> <strong>the</strong> Portsmouth<br />

Harbor region. These data sets <strong>in</strong>clude SHOALS 1000, SHOALS 3000 <strong>and</strong> LADS II<br />

data <strong>and</strong> will play an important role <strong>in</strong> future study explor<strong>in</strong>g <strong>the</strong> capabilities of LIDAR<br />

as a hydrographic tool.<br />

Also <strong>in</strong> support of this research, a LIDAR simulator project has been <strong>in</strong>itiated. The<br />

objective of this study is to simulate both a bathymetric LIDAR system <strong>and</strong> <strong>the</strong> realistic<br />

environmental factors that might be present <strong>in</strong> various coastal areas. By conduct<strong>in</strong>g this<br />

study <strong>in</strong> a laboratory environment, <strong>the</strong> relative importance of <strong>the</strong> various scatter<strong>in</strong>g<br />

components on LIDAR waveforms can be <strong>in</strong>vestigated <strong>in</strong>dividually. It is important to<br />

note that this study is focus<strong>in</strong>g on both <strong>the</strong> elastic (Mie) <strong>and</strong> <strong>in</strong>elastic (Raman <strong>and</strong><br />

fluorescence) scatter<strong>in</strong>g regimes <strong>and</strong> <strong>the</strong> ability to leverage <strong>the</strong> excitation of <strong>the</strong> different<br />

scatter<strong>in</strong>g phenomena. This research will provide <strong>the</strong> basis for us<strong>in</strong>g airborne LIDAR<br />

systems to make quantitative measurements of a variety of environmental factors <strong>in</strong> <strong>the</strong><br />

coastal areas <strong>in</strong> addition to <strong>the</strong> bathymetry.<br />

The first step of this study is configur<strong>in</strong>g <strong>the</strong> LIDAR simulator. At <strong>the</strong> moment we are<br />

us<strong>in</strong>g a surplus Copper Vapor Laser (511 nm) that that is similar to but is not precisely<br />

<strong>the</strong> 532 nm Nd: YAG green laser used for bathymetric applications. To date, we have<br />

conditioned <strong>the</strong> laser <strong>and</strong> conducted two feasibility tests. These tests aid us <strong>in</strong><br />

underst<strong>and</strong><strong>in</strong>g what types of <strong>in</strong>strumentation are needed <strong>and</strong> <strong>the</strong> configurations needed<br />

for each type of experiment. The prelim<strong>in</strong>ary results of <strong>the</strong> tests show that <strong>the</strong> spread<strong>in</strong>g<br />

of laser beam through <strong>the</strong> very clear water is l<strong>in</strong>ear <strong>and</strong> that <strong>the</strong> tank’s bottom scatters<br />

light <strong>in</strong> a manner that upwell<strong>in</strong>g was not noticed by <strong>the</strong> naked eye. When plac<strong>in</strong>g a mirror<br />

on <strong>the</strong> tank’s bottom, <strong>the</strong> upwell<strong>in</strong>g radiation was visible. The laser beam was captured<br />

JHC <strong>Performance</strong> <strong>Report</strong> 42 30 January 2007

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