Spectral Unmixing Applied to Desert Soils for the - Naval ...
Spectral Unmixing Applied to Desert Soils for the - Naval ...
Spectral Unmixing Applied to Desert Soils for the - Naval ...
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Specimens were sampled during <strong>the</strong> time periods of 0930–1130 and 1300–1500,<br />
falling within <strong>the</strong> +/- 2 hours of solar noon described by (Roberts and Herold, 2004).<br />
Collected spectra were <strong>the</strong>n converted <strong>to</strong> reflectance using spectral math. The spectral<br />
math equation used was s1/s2 where s2 was <strong>the</strong> average white reference spectrum and s1<br />
was one of <strong>the</strong> field collected spectra. This process was conducted on each individual<br />
spectrum from each collection site, and utilized <strong>the</strong> site specific white reference spectrum<br />
<strong>for</strong> a given calculation. One of <strong>the</strong> results of this process can be seen in Figure 19. Once<br />
<strong>the</strong> spectra were in units of reflectance, <strong>the</strong>y were examined <strong>for</strong> proof of concept with<br />
respect <strong>to</strong> detecting soil disturbance using reflectance spectroscopy and <strong>the</strong> continuum<br />
removal method. To verify if differences were significant enough <strong>to</strong> be considered<br />
spectrally extreme, band depths were analyzed between both <strong>the</strong> ASD collected spectra<br />
and <strong>the</strong> imagery derived endmembers using <strong>the</strong> following equations (5) and (6) described<br />
by Kokaly and Clark, (1999) and Kokaly (2001). Equation (5) calculates <strong>the</strong> continuum<br />
removed reflectance required <strong>to</strong> <strong>the</strong>n calculate <strong>the</strong> band depth using equation (6) (Kokaly<br />
and Clark, 1999; Kokaly (2001).<br />
where:<br />
is <strong>the</strong> continuum removed reflectance at <strong>the</strong> absorption feature,<br />
feature.<br />
where:<br />
is <strong>the</strong> <strong>the</strong> reflectance at <strong>the</strong> base of <strong>the</strong> absorption feature, and<br />
is <strong>the</strong> reflectance of <strong>the</strong> fitted continuum line that corresponds <strong>to</strong> <strong>the</strong> absorption<br />
is <strong>the</strong> calculated band depth of <strong>the</strong> continuum removed absorption feature and<br />
is <strong>the</strong> previously calculated continuum removed reflectance from equation (5).<br />
39<br />
(5)<br />
(6)