
Major, G., 1992: Estimation of the error caused by the circumsolar radiation when measuring global
4
radiation as a sum of direct and diffuse radiation. Solar Energy, 48. (See Table 4.1 for common
combinations of pyrheliometers and pyranometers.)
Bush, B.C., F.P.J. Valero and A.S. Simposn, 2000: Characterization of thermal effects in pyranometers: A
5
data correction algorithm for improved measurement of surface insolation. Jour. Atmos. Ocean. Tech., 17,
165 - 175.
11
A solar tracker with an accuracy of ±0.10° or better, is needed to accommodate the
pyrheliometer, the ACR and, during calibrations, a second ACR. It is recommended that the
tracker pointing be monitored using a four-quadrant sensor because pointing accuracy is
important in determining the quality of the direct beam measurement. The sampling rate should
be the same as that of the instruments attached to the tracker. A variety of high-quality trackers
are now available that use four-quadrant sensors for actively positioning the tracker on the solar
beam during periods of high irradiance and a solar position algorithm during low intensity
conditions.
The parameters to be monitored are: output of the pyrheliometer thermopile; outputs of the ACR
(U, I or thermopile signals for a passive instrument); body temperatures of the pyrheliometer and
ACR; output of the four-quadrant sensor. Only the values associated with the calculated
irradiance (mean, maximum, minimum and standard deviation) are required by the BSRN archive.
All other raw data should be archived at the centre responsible for the measurements.
2.2.1.2 Diffuse Radiation
The original instrument configuration associated with the BSRN target uncertainty of 4% (5 W m )
-2
was a ventilated pyranometer with a sensor to monitor the instrument thermopile temperature (to
be used to correct for temperature-related changes in thermopile responsivity and thermal
offset). Shading of the instrument from the direct sun was to be by a shading disk. The shade
geometry of the combination of the sensor and the disk was to replicate the geometry of the direct
beam sensor when pointing toward the zenith (5° full-angle from the centre of the detector) . The
4
instrument’s sensor and dome must be completely shaded. Incorrect geometry alone can lead to
errors of up to 5 W m depending on instrumentation and atmospheric conditions.
-2
A relationship has been shown between pyranometer thermal offsets and diffuse irradiance that
can significantly affect the quality of the measurement . A possible solution to overcome the offset
5
problem is to use a ‘black and white’ type pyranometer (B&W) for the measurement of diffuse
radiation. This type of instrument does not exhibit the thermal offset of ‘black’ thermopile
instruments because both hot and cold junctions are exposed to the same thermal regime. B&W
instruments, currently, do not have the same optical qualities (spectral and directional) as the
black thermopile instruments recommended for use at BSRN stations and cannot be used for the
measurement of global radiation. Using a B&W instrument for the measurement of diffuse
irradiance would therefore mean a second type of instrument would have to be used for the global
irradiance measurement, which may increase the overall uncertainty of the three-component
measurements.
Research is presently ongoing to determine whether a correction factor can be applied to the
‘black’ pyranometer thermal offset. In Section 9.2.2 experimental methods of correcting this offset
are presented. Further research continues into the design of a ‘black’ pyranometer that does not
exhibit thermal offset. Several instruments that use other technologies (e.g., PRT) are available
that do not exhibit offset problems associated with radiative cooling.
The BSRN has yet to recommend a standard method of correcting for thermal offset or selecting
a particular type of instrument for measuring diffuse irradiance. A careful uncertainty analysis of
any diffuse system will determine the quality of the measurement if each component is properly
addressed.
The parameters to be acquired are: output of pyranometer thermopile; pyranometer body
temperature. Only the values associated with the calculated irradiance (mean, maximum,
minimum and standard deviation) are required by BSRN archive. All other raw data should be
archived at the centre responsible for the measurements.
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