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Illumination

Total decomposition Reflected light

Light reflected Light specular diffuse

ambient absorbed transmitted object object

Light = reflected + transmitted + absorbed Reflected light = ambient + diffuse + specular

I = Ia + Id + Is

1 Illumination - Examples

ambient ambient + diffuse ambient + diffuse + specular (and a checkerboard)

2 Ambient Reflection

• Uniform background light

•Ia = ka IA

- IA: ambient light

- ka: material’s ambient reflection coefficient • Models general level of brightness in the scene • Accounts for light effects that are difficult to compute (secondary diffuse reflections, etc) • Constant for all surfaces of a particular object and the directions it is viewed at

3 Diffuse Reflection

Dot product: • Models dullness, roughness of a surface N·L = (NxLx + NyLy + NzLz) • Equal light in all directions • For example, chalk is a diffuse reflector

Light Lambertian cosine law: ϕ Id = kd IL cos = kd IL N·L

N ϕ L IL: intensity of lightsource P N: surface vector object L: light vector (unit length) ϕ: angle of light incidence

kd: diffuse reflection coefficient ()Light – P ()Light – P ()Light – P Light– P x x y y z z L ==------,,------(material constant) Light– P L' L' L'

()2 ()2 ()2 L' = Lightx – Px ++Lighty – Py Lightz – Pz Note: Id = 0 for N·L < 0 4 Specular Reflection - Fundamentals • Models reflections on shiny surfaces (polished metal, chrome, plastics, etc.) • Ideal specular reflector (perfect ) reflects light only along reflection vector R • Non-ideal reflectors reflect light in a lobe centered about R - cos(α) models this lobe effect - the width of the lobe is modeled by Phong exponent ns, it scales cos(α)

Light Phong specular reflection model:

ns α ns Eye Is = ks IL cos = ks IL (E·R) N R α ϕ ϕ L E IL: intensity of lightsource P L: light vector lobe object R: reflection vector = 2 N (N·L) - L E: eye vector = (Eye-P) / |Eye-P| R R R α: angle between E and R ns: Phong exponent ∞ ns = ns large (100) ns small (8) ks: specular reflection coefficient (perfect mirror) (shiny surface) (dull surface) 5 Specular and Diffuse Reflection - Varying the Coefficients

diffuse coefficient kd

Phong exponent ns

6 Specular Reflection - Using the Half Vector

• Sometimes the half vector H is used instead of R in specular lighting calculation • Both alternatives have similar effects

Phong specular reflection model:

ns β ns Light Is = ks IL cos = ks IL (H·N) β Eye H N R IL: intensity of lightsource α ϕ L E L: light vector H: half vector = (L + E) / |L + E| R: reflection vector object E: eye vector

7 Total Reflected Light

• Total reflected light (for a white object):

ns I = ka IA + kd IL N·L + ks IL (H·N) • Multiple lightsources: ∑ ns I = ka IA + (kd Ii N·Li + ks Ii (Hi·N) )

• Usually, I is a vector of (R=red, G=green, B=blue)

• Object has a color vector Cobj = (Robj, Gobj, Bobj)

• Object reflects I, modulated by Cobj • Color C reflected by object: ∑ ∑ ns C = Cobj (ka IA + (kd Ii N·Li)) + (ks Ii (Hi·N) )

• In many applications, the specular color is not modulated by object color - has the color of the lightsource • Note: (R, G, B) cannot be larger than 1.0 (later scaled to [0, 255] for display) - either set a maximum for each individual term or clamp final to 1.0 8