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This page offers a description of the ground radiometric instruments and measurements available during the campaign. | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
SOLAR RANGE GROUND RADIOMETRIC MEASUREMENTS Instrumentation • ASD FieldSpect Pro FR Spectroradiometer The FieldSpec Pro (Fig.5.2) is a highly portable, general-purpose spectroradiometer. A fiber optic bundlefor light collection. Inside the instrument, light is projected from the fiber optics onto a holographic diffraction grating where the wavelength components are separated and reflected for independent measurement by the detectors. The response of each detector is digitised to 16-bit precision. The Visible/Near Infrared (VNIR) portion of the spectrum, the 350-1050 nanometer wavelength domain, is measured by a 512-channel silicon photodiode array. Each channel is geometrically positioned to receive light within a narrow (1.4 nm) bandwidth. The VNIR spectrometer has a spectral resolution (FWHM of a single emission line) of approximately 3 nm at around 700 nm. The Short-Wave Infrared (SWIR), also called Near Infrared (NIR), portion of the spectrum is acquired with two scanning spectrometers. These differ from the array used in the VNIR in that they measure wavelengths sequentially, rather than simultaneously. Each spectrometer consist of a concave holographic grating and a single thermoelectrically cooled indium gallium arsenide (InGaAs) detector. The gratings are mounted about a common shaft that oscillates with a period of about 200 milliseconds (100 ms/scan). Unlike the VNIR, each SWIR spectrometer has only one detector, which is exposed to different wavelengths of light as the grating oscillates. The first spectrometer (SWIR1) measures light between about 900 – 1850 nm; the second (SWIR2) covers the region between about 1700 – 2500 nm. The sampling interval for each SWIR region is about 2 nm, and the spectral resolution varies between 10 nm and 12 nm, depending on the scan angle at that wavelength. Light may be collected with a bare fiber optic, that has a field of view (FOV) of 25º, or with the use of fore-optic devices, that provide FOV of 8º or 1º, and Remote Cosine Receptors (RCR) for full-hemisphere albedo measurements. Figure 5.1. ASD FieldSpect Pro-FR Spectroradiometer.
• GER 3700 Spectroradiometer The GER 3700 Spectroradiometer (fig.5.3), with a spectral range of 300 to 2500 nm, has 704 measurement channels. Spectral resolution of 1.5 nm from 300 to 1050 nm, 6.5 nm from 1050 to 1900 nm and 9.5 nm from 1900 to 2500 nm. Their scan time is 50 ms and it has a field of view (FOV) of 6º circular. Spectrum averaging is selectable from 4 to 9. Figure 5.2. GER 3700 Spectroradiometer
Physical Properties:
• Transmittance/Radiance images using electronic tunable filters. Hiperspectral images of leaves and canopy in the VIS and NIR regions are to be acquired using the two main technologies for electronic tunable filters: Liquid Crystal Tunable Filters (LCTF) and Acousto-Optic Tunable Filters (AOTF). • Description of OKSI LCTF A LCTF is formed by a stack of polarizers and tunable retardation liquid crystal plates. Combining the transmission of all the plate only a narrow band can be transmitted. Changing the bandpass is very fast (~50 msec). We are using the OKSI hypersepctral camera, which uses two VarisPec Tunable Imaging Filter from Cambridge Research, Inc., one covers the VIS range and the second one the NIR.
Figure 5.3.VIS filter and the VIS/NIR control units. • Description of Brimrose AOTF. The “AOTF Camera Video Adapter CVA-100” from Brimrose is a sealed unit that contains AOTF modular, relay optics, zero-order stop and CCD camera interface. It has a front aperture and a back aperture to connect, respectively, a camera objective and a optical sensor. The optical device is controlled by a AOTF Driver with a frequency range from 69 MHz to 219 MHz. This equipment has the following specifications: –Aperture size: 10x10 mm. • Camera The camera used to acquire the spectral bands is a 12-bit resolution
Qimaging Retiga EX with the following features:
• Illumination. An illumination box has been built in order to generate a suitable light source for reflectance and transmittance measurements. Halogen lamps, with DC supply, are used. Diffuse lighting is achieved by using both a wide band diffuser and a proper lamp layout that mimics an integration sphere.
Measurement plan Optical radiometric measurements will be performed with three objectives in mind: - Radiometric calibration of air and spaceborne sensors imagery. For calibration purposes appropriate homogeneous fields will be identified
for measurements in a time-span of one hour before and after the overpass
of sensors, in a daily basis. For the characterization of vegetation, a number of significant crops
will be determined in coordination with the teams in charge of vegetation
measurements. In them separate measurements will take place of soil and
canopy under sun and shadows conditions.
All measurements will be acquired in radiances, and later processed into
reflectances when needed. UCL Leaf Reflectance/Transmittance and Top-of-Canopy Reflectance Measurements Plan
Instrumentation • CIMEL 312-1 radiometer The CIMEL CE-312-1 is a radiance-based thermal-infrared radiometer composed
of two major components: an optical head containing the detector and optics,
and the electronic unit that performs the data storage. The detector includes
one broad-band filter, 8-13 µm, and three narrower filters, 8.2
– 9.2 µm, 10.5 – 11.5 µm and 11.5 – 12.5
µm (Table 5.1). A external temperature probe can be added by the
user into the control unit. It allows collecting the temperature of an
external blackbody especially for the estimation of absolute emissivity.
A set of different scenarios is available to collect data depending on
the user desires. Table 5.1. Thermal Infrared radiometer CIMEL CE312 specifications
• CIMEL 312-2 ASTER radiometer The CIMEL CE-312-2 ASTER is a radiance-based thermal-infrared radiometer composed of two major components: an optical head containing the detector and optics, and the electronic unit that performs the data storage. The detector includes 6 bands, a wide one, 8-13 µm, and five narrower filters, 8.1 – 8.5 µm, 8.5 – 8.9 µm, 8.9 – 9.3 µm, 10.3 – 11 µm and 11 – 11.7 µm (Table 5.2). A external temperature probe can be added by the user into the control unit. It allows collecting the temperature of an external blackbody especially for the estimation of absolute emissivity. A set of different scenarios is available to collect data depending on the user desires. Table 5.2. Thermal Infrared radiometer CIMEL CE312 specifications
• EVEREST 3000.4ZLC Infrared temperature transducer The Everest thermometer, model 3000.4ZLC single band 8 – 14 µm collect the infrared radiation from the sample converting it into electrical signal. With the suitable calibration process, the electrical signal is converted to a signal in terms of temperature. It is scaled from – 40ºC to 100ºC with a resolution of 0.1 K, an accuracy of ±0.5 K and a repeatibility of ±0.1K. The Field of View -FOV- is 4º. It has an adjustable emissivity equal to unity. The output signal is in mV (10 mV/º), and the power requirements is 5V to 26V DC. Power supply was provided by an auxiliary Einhell power station. Table 5.3. EVEREST 3000.4ZLC transducer specifications.
• RAYTEK ST8 Infrared radiometer A portable RAYTEK, model ST8 single band 8–14 µm, with a FOV of 8 degrees, and with adjustable emissivity operation mode will be used. It ranges up to 100ºC with a sensitivity of 0.1 K and an accuracy of 0.5K. It has a laser beam that helps to locate the target for the measurements. • RAYTEK Thermalert MID radiometers The Raytek Thermalert MID radiometer is an infrared sensor with a single band 8–14 µm, with a FOV of 20 degrees, and with adjustable emissivity operation mode. It ranges up to 600ºC with a sensitivity of 0.1 K and an accuracy of 0.5K.
A calibration source EVEREST model 1000 will be used to calibrate the radiometers. Its operating range is from 0ºC to 60ºC, with a resolution of 0.1K, with an absolute accuracy of 0.3 K over entire range. • GALAI 204-P calibration source (from the ULP) A calibration source GALAI model 204-P will be used to calibrate the radiometers.
Four different Licor LI-1000 dataloggerss will be used to storage data from both radiometers and thermocouples. CAMPBELL CR21 Micrologger (from the ULP) • Goniometer motorized system
Details of the instruments are given in Table 5.4. Table 5.4. Thermal Infrared instrument settings.
A set of thermal radiometric measurements will be carried out in the
framework of the SPARC-2004 experimental field campaign. The retrieval
of bio geophysical parameters such as land surface emissivity and temperature
is the main aim of these measurements. To this end, radiometric measurements
will be carried out in the thermal infrared region with various instruments
that include fixed FOV and single band or multi bands radiometers. In
addition, a thermocouple for thermometric temperatures measurements and
black bodies (calibration sources) for calibration purposes will be used.
Table 5.5. Field work foreseen by Global Change Unit during SPARC-2003. TBD: - All days, brightness temperature transects simultaneously with flight/satellite overpass will be carried out (AHS, AATSR, ASTER, SEVIRI, LANDSAT, AIRFLEX). - All the samples in the table 5.5 are named according to the classification crop map corresponding to 2004. PLANNED ACTIVITIES: Table 5.5. Planned activities for the Mission 1 of SEN2FLEX campaign.
![]() Goniometer system EVEREST 3000.4ZLC Infrared temperature transducer CIMEL 312-1 radiometer RAYTEK ST6 Infrared radiometer Thermal camera Irisys-Iri1001 EVEREST 1000 calibration source
RAYTEK Thermalert MID radiometers GALAI 204-P calibration source (from the ULP) Thermocouple Type K Goniometer motorized system
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by GPDS Group University of Valencia (Spain) |
Last Updated: July
29th - 14:40h LT |