1987
DOI: 10.1364/ao.26.001201
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Fibers for low-temperature radiometric measurements

Abstract: Theoretical calculations are presented for the performance of a fiber-optic radiometer which makes use of infrared transmitting fibers to measure low temperatures (near room temperature). We calculate the radiometer spatial resolution, the dependence of the radiometer signal on the surface temperature, and the minimum resolvable temperature difference (MRDeltaAT) of the radiometer. The performance of the fiber-optic radiometer is compared with a conventional optical (thin lens) radiometer.

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Cited by 35 publications
(12 citation statements)
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“…The mean values and corresponding standard deviations from the three calibrations are shown in Figure A. The BBR signals from the three calibrations are insensitive to the distance, which is consistent with previous theoretical studies that a fiber radiometric thermometer is insensitive to the distance between the fiber end to a thermal surface . The mean values can be fitted by a power function very well as indicated by the correlation coefficient, R .…”
Section: Resultssupporting
confidence: 87%
“…The mean values and corresponding standard deviations from the three calibrations are shown in Figure A. The BBR signals from the three calibrations are insensitive to the distance, which is consistent with previous theoretical studies that a fiber radiometric thermometer is insensitive to the distance between the fiber end to a thermal surface . The mean values can be fitted by a power function very well as indicated by the correlation coefficient, R .…”
Section: Resultssupporting
confidence: 87%
“…Therefore, it is important to quantify the BBR due to temperature at different working distances. Theoretically, BBR is independent of the working distance and the angle between the fiber and the tissue surface, but proportional to the numerical aperture and the fiber diameter [26]. We measured the BBR over a temperature range of 65-110°C with the fiber tip positioned at 1, 2, and 3 mm above the dry bath surface.…”
Section: Blackbody Radiation Measurement At Different Working Distancesmentioning
confidence: 99%
“…The end face of transmitting fiber Φ can be denoted as ⊙O T . Every point on ⊙O T forms a normal light cone, and all light emitted from the emitting point is within the normal cone [18]. The light intensity distribution on the plane of receiving fiber Ψ is a linear superposition of all light cones reflected on the finite plate P from all emitting points on the end face of transmitting fiber Φ.…”
Section: Mathematical Modelingmentioning
confidence: 99%
“…Normally, light exits an end-emitter fiber in a hypothetical cone of light defined by the numerical aperture (NA) of the fiber, and every light point on the end face of transmitting fiber brings about a local light cone which would be combined to form the whole emitting light [18]. The light intensity distribution on the end face of transmitting fiber is considered as Gauss distribution, as well as the light intensity distribution on every section of local light cone.…”
Section: Introductionmentioning
confidence: 99%