Materials and methods Directory UMM :Data Elmu:jurnal:A:Agricultural & Forest Meterology:Vol104Issue3Sept2000:
216 J. Ross, M. Mõttus Agricultural and Forest Meteorology 104 2000 215–231
of sunflecks, umbra and penumbra is closely related to the progress of new comprehensive computer mod-
els of canopy photosynthesis and evapotranspiration, which require detailed 3D characteristics of different
radiation types for input. As the interrelationship be- tween PAR and photosynthesis is nonlinear, the mean
values of radiation do not yield correct results. In our opinion, for further calculation of canopy photosyn-
thesis, leaves in plant canopies should be divided into three groups according to the type of direct sunlight
they receive: sunflecks, umbra and penumbra; and photosynthesis should be calculated separately for
each group. Therefore, it is necessary to know the area of sunflecks, its vertical distribution and tempo-
ral dynamics in order that different data for umbra, penumbra and sunflecks could be used in modern
radiation transfer models.
Ross et al. 1998 proposed a statistical treatment of PAR variability and its application to willow cop-
pice. In this treatment, statistical distribution of PAR global irradiance, obtained with a LI-COR quantum
sensor, was approximated by a normal distribution in sunfleck and umbra areas, and the fractional area of
penumbra was approximated by the Beta-distribution and considered to be function of pathlength τ and
solar elevation h.
This paper is a continuation of the previous work by Ross and Mõttus 2000 on a statistical treatment of
umbra length and is focused on the statistical treatment of sunfleck length inside a willow coppice. Experi-
mental data were obtained with a new instrument — the sunfleck sensor constructed by Sulev; the method-
ology of statistical data processing is analogous to that used in our previous paper Ross and Mõttus, 2000.
Sunfleck’s different statistical characteristics, such as sunfleck length distribution, sunfleck fractional
area, number of sunflecks, mean sunfleck length, etc. in different canopy layers will be studied as the func-
tions of the pathlength of the direct solar radiation
1
τ =Lsin h, where Lz = R
z
U
z
u
L
z dz is the down- ward cumulative leaf area index and u
L
z is the leaf area density.
1
In our previous paper Ross and Mõttus, 2000, we used the term ‘optical pathlength’ for this quantity. However, to avoid
any confusion that might arise from this general term, we use a more comprehensive term, ‘pathlength of the direct solar radiation
beam’, in this paper.