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134
ph
Since the irradiance on the surface by a pyrheliometer adjusted for the horizontal surface F is
the following relation must be kept,
where the subscript d stands for the variable for the diffusometer.
This last equation shows two important aspects concerning the geometry of the diffusometer.
dd d d
(1) In principle it is important to keep R/L=R /L and r/R=r /R ,
(2) Since it is not practical to change geometrical dimensions of the involved parts, it is a practically
better solution to adjust geometry for representative solar zenith angle. The earth's equivalent
dd
solar zenith angle of 53º, can be regarded as a working angle. Therefore, R /L which is slightly
dd
larger than R/L, or r /R which is slightly larger than r/R suits the best for the present requirement.
Since the latter possibility is difficult to fulfil du to a relatively large difference in radii between
dd
the sensor and the outer glass dome, the best solution can be obtained by adjusting R /L ,
d
by making L smaller than the designated length which is calculated based a perfect symmetry
requirem ent.
C 4.6 Conclusion
Most diffusometers adopted by the BSRN stations are capable of keeping the errors induced by the
shadow effect within 2 to 3 W m . The best recommended diffusometer is to use Eppley B/W pyranometer
-2
8-48, with the shading disc radius of 28.0 mm and the arm's length of 641 mm.
C 4.7 References
Major, G., 1994: Circumsolar correction for pyrheliometers and diffusometers. WMO/TD-No.635, 42
pp.
Major, G., Nagy, Z., and Putsay, M., 2000: The effect of diffusometer shading geometry. Report for
the BSRN Meeting, May 1-5, 2000, Melbourne, 8 pp.
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