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n
dA
= p r
p
p p
Figure 1.7. Geometric construction of point p r when the light plane is pointing away
from the surface.
As previously discussed, we were searching for the most important sample of
the integral on a segment between points p r and p c representing component-wise
local maximums (see Figure 1.8).
With those conditions set, we used a computational software package to nu-
merically find a point on line p c p r that approximates the most important point
as much as possible. We worked on a data set of several hundred area lights ran-
domly generated as disk or rectangle light shapes. For every light shape we found
a point on the plane that best resembles the full integral. Then, we computed the
end points of our line between p c and p r (as if it would be calculated at runtime).
Then, we numerically checked the points along the line, computing the lighting
equation and comparing against a reference, using the least squares method to
find point p d , which would most accurately represent the integral.
p'
p c
n
dA
p r
p
p p
Figure 1.8. Geometric construction of line p c p r .
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