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Combined consequence of ambient and diffused reflection
At this time the resulting intensity I will be the total sum of the intensities in case 8.3.2 and 8.3.3 we find that:
I = Ia Ka + Id Kd cos θ = Ia Ka + Id Kd ( N¯ .L¯)
Obtain Ka = Kd ; here Q both constant properties of material to that light is incident, for both sources there constant are similar.
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Derive the common transformation for parallel projection into a specified view plane, here the direction of projection d=aI+bJ+cK is along the normal N=n1I+n2J+n3K along with the r
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