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Spectral observations When operating in the spectral
domain, as it is possible with airborne scanners and satellite
imagery, it is of interest to be able to characterize properties
like down- and up-welling radiance, attenuation and reflectance in
the spectral domain as well. In the following, the radiometric
definitions are briefly described. For a more in depth description
of the various terms, please refer to (Kirk, 1994). Radiant flux is the amount of radiation coming from a source per unit time. Unit: W Radiant intensity is the radiant flux leaving a point on the source per unit solid angle of space surrounding the point. Unit: W sr-1 Radiance is the radiant intensity emitted (or scattered) by a unit area of source (surface). Unit: W m-2 sr-1 Irradiance is the radiant flux incident on a receiving surface from all direction per unit of area. Unit: W m-2 nm-1. Reflectance is the fraction of incident flux that is reflected by a surface. All the above mentioned terms may have the prescript spectral added in which case the units are per wavelength unit, e.g. nm.
Measurements
Spectral radiance The spectral radiance is commonly measured by pointing the tip of the optic fibre towards the target. The solid angle of observation may be adjusted by attaching specific calibrated fore-optics.
Spectral irradiance The spectral irradiance may be measured directly by attaching a cosine receptor to the spectroradiometer and pointing the receptor parallel to the surface for which the irradiance is to be measured. In the case of measuring down-welling solar irradiance the sensor head is pointed upwards and kept horizontal. An indirect way of measuring irradiance is to point the fibre optic (without cosine receptor) vertical down on a perfect lambertian reflector placed horizontal. The method requires the measured radiance to be multiplied by 2 p to convert to irradiance. A Spectralon panel may be used as an almost perfect lambertian reflector. Spectral reflectance Ideally the reflectance is measured / calculated based on simultaneous measurement of radiant flux towards and away from the target. This does however require a dual sensor set-up, which is far more expensive than single sensor. In the single sensor set-up spectral reflectance is instead measured by first pointing the tip of the optic fibre vertical down towards a target of known reflectance, e.g. a Spectralon panel. This measurement is called the white reference. The following measurements are then made as relative to the white reference. The post-processing then involves the correction for the non-perfect reflectance of the white reference panel. In the case of reflectance measurements over or even below the water surface the differences in radiance levels may require that different integration times are applied for the white reference and the target to be observed. In this case the reflectance in not measured directly but rather calculated from observations of radiance or irradiance. In any case where the single sensor set-up is used it is a natural pre-requisite that the illumination is constant over the time of measurements. Be careful to measure the down-welling radiance both prior to and after the measurements of targets. Parameters to observe If possible the following measurements should be taken in parallel with over-flight or close to over-flight. The purpose of the spectroradiometric measurements is to characterise the actual illumination situation and the vertical beam attenuation of the water as the composition is at the time of image acquisition. Downwards illumination The downward illumination may be described briefly by two signature types: the downwards spectral irradiance and the diffuse proportion of the downwards spectral irradiance. The downwards spectral irradiance measurement is made as a radiance measurement of the radiance reflected by a horizontal Spectralon panel as described above, the measurements should are taken above the surface. The diffuse proportion of the downward irradiance may be estimated by a reflectance measurement using a bare tip of the fibre optic. The fibre tip is pointed towards a position in the sky which 90 degrees away from the sun and in the sun-observer zenith plane. Vertical beam attenuation of the water Spectral downward irradiance measurements at various depths are used for determining the vertical beam attenuation. It is in general assumed that the downward irradiance available at a given depth can be described as: Ed = E0 e-k d E0 is the irradiance just below the surface and Ed is the irradiance at depth d, k is the vertical beam attenuation coefficient. Spectral reflectance signatures of the bottom features The spectral reflectance signatures should in the ideal world be independent of the illumination situation, it is however always preferential to measure the spectral reflectance signatures at conditions similar to the situation when the image data are acquired. Observations needed to calculate the reflectance signatures are up- and down-welling irradiance just above the target in question. Observations for reflectance
signatures should be made over a variety of surfaces, where e.g. the
water depth and density of vegetation vary. |
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