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 = I_a K_a + I_d K_d cos θ = I_a K_a + I_d K_d ( N¯ .L¯)

Obtain K_a = K_d ; here Q both constant properties of material to that light is incident, for both sources there constant are similar.

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