User manual
Table Of Contents
- N
- Introduction
- Introduction
- Getting Started
- S
- SunScan Tutorial
- M
- Menus and Screens
- More Psion and file handling notes
- M
- Measurement options
- L
- LAI theory
- Technical Reference section
- Maintenance and repair
- Troubleshooting
- Psion Workabout
- Problems running the SunData application.
- While running SunData
- SunData reports “SunScan probe not connected”.
- SunData recognises the SunScan probe, but fails to take readings.
- On running SunData, all the system settings are scrambled.
- “Out of memory” reported on drive A:.
- “Insufficient power to write data” reported.
- When transferring files to a PC, data is transferred, but there are repeated checksum or device IO errors.
- SunScan or BFS give inconsistent light readings.
- Technical Support
- Specifications
- PAR Performance
- Appendices
- Index

SunScan User Manual v 1.05 LAI theory •
••
• 57
The next section derives the transmission of light from a uniform overcast sky
through a uniform infinite canopy of black leaves of constant LAI with an ellipsoidal
leaf angle distribution.
Let the sky have uniform brightness of 1 per steradian over the hemisphere.
The radiance of a strip around the sky at angle θ is given by:
R
...
2
π
sin( )
θ
d
θ
and the irradiance on a horizontal surface due to that strip is given by
I
0
....
2
π
sin( )
θ
cos( )
θ
d
θ
The total irradiance due to the hemisphere is obtained by integrating over the
complete sky area:
=d
0
π
2
θ
...
2
π
sin( )
θ
cos( )
θ
1
π
For each strip of sky, the transmitted radiation is given by
I
.
I
0
exp( )
.
KL
where K is the extinction coefficient from Campbell,
so the total transmitted radiation is
I d
0
π
2
θ
....
2
π
sin( )
θ
cos( )
θ
exp( )
.
K( ),x
θ
L
and the transmission fraction τ is given by I/I
0
τ
diff
(),xL
.
1
π
d
0
π
2
θ
....
2
π
sin( )
θ
cos( )
θ
exp( )
.
K( ),x
θ
L
This integral was evaluated numerically over the range x = 0 to 1000 and L = 0 to
10, and is graphed below for three different values of
x.