PDS_VERSION_ID = PDS3 RECORD_TYPE = STREAM OBJECT = SPACECRAFT_INSTRUMENT SPACECRAFT_ID = "IRAS" INSTRUMENT_ID = "FPA" OBJECT = INSTRUMENT_INFORMATION INSTRUMENT_NAME = "FOCAL PLANE ARRAY" INSTRUMENT_TYPE = "DETECTOR ARRAY" INSTRUMENT_DESC = " The IRAS Focal Plane Array was located at the focal plane of the IRAS Ritchey-Chretien telescope. The mirror surfaces were beryllium, and the baffles were aluminum coated with Martin Optical black. The telescope had an entrance pupil diameter of 57 cm, and a central obscuration diameter of 24 cm, for an effective collecting area of 2019 cm+2. The measured system focal length was 545 cm and the system F/number was 9.56. The measured plate scale at the focal plane was 1.585 mm/arcminute. Imaging was diffraction limited at 25, 60 and 100 microns, but not at 12 microns. The telescope was cooled by contact with the superfluid helium tank to temperatures ranging from 2 to 5 K. The operating temperature of the FPA was 2.6 K. The FPA contains 62 infrared detectors, divided into eight parallel modules, two for each color band. Each module contains either seven or eight detectors. The layout of the detectors is given in the IRAS Explanatory Supplement. The detectors were rectangular with their narrow dimension arrayed parallel to the scan path of infrared sources. The design was such that the image of a real source would cross a detector in one module and subsequently cross another detector of the same band in the second module, providing a 'seconds-confirmation'. This allows for the discrimination between real and spurious sources, such as cosmic rays. The infrared detectors were sampled at 16, 16, 8, and 4 Hz at 12, 25, 60, and 100 microns, respectively. The response functions of the 4 spectral bands used in the focal plane array are given in the IRAS Spectral Response dataset distributed through PDS and are listed in the IRAS Explanatory Supplement. Output from FPA detectors is typically reported in units of flux density (Jansky, where 1 Jy = 1.e-26 Watt/(meter^2)/Hz), calculated from inband flux (Watts/meter^2) assuming the external source function to be proportional to 1/frequency. Jy (BD) is converted to Watt/(meter^2) (IB) by the relation BD*K=IB, where K is given in MOSHIRETAL1989 and is listed below: Wavelength K 12 1.348e-13 25 5.155e-14 60 2.577e-14 100 1.000e-14 for more information see BEICHMANETAL1988. " END_OBJECT = INSTRUMENT_INFORMATION OBJECT = INSTRUMENT_REFERENCE_INFO REFERENCE_KEY_ID = "BEICHMANETAL1988" END_OBJECT = INSTRUMENT_REFERENCE_INFO OBJECT = INSTRUMENT_REFERENCE_INFO REFERENCE_KEY_ID = "MOSHIRETAL1989" END_OBJECT = INSTRUMENT_REFERENCE_INFO END_OBJECT = SPACECRAFT_INSTRUMENT END