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CS 4620 Lecture 5

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 1 Image so far

• With eye ray generation and scene intersection

for 0 <= iy < ny for 0 <= ix < nx { ray = camera.getRay(ix, iy); c = scene.trace(ray, 0, +inf); image.set(ix, iy, c); } …

Scene.trace(ray, tMin, tMax) { surface, t = surfs.intersect(ray, tMin, tMax); if (surface != null) return surface.color(); else return black; }

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 2 Shading

• Compute reflected toward • Inputs: – eye direction – light direction (for each of many ) l n – surface v – surface parameters (color, shininess, …)

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 3 Diffuse reflection

• Light is scattered uniformly in all directions – the surface color is the same for all viewing directions • Lambert’s cosine law

l n Q

Top face of cube Top face of In general, light per unit receives a certain 60º rotated cube area is proportional to amount of light intercepts half the light cos θ = l • n

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 4 Light falloff

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 5 Light falloff

1

intensity here: I

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 5 Light falloff

intensity r here: I/r2

1

intensity here: I

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 5 Lambertian shading

• Shading independent of view direction

illumination from source

l n 2 Ld = kd (I/r ) max(0, n l) Q v ·

diffuse coefficient

diffusely reflected light

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 6 Lambertian shading

• Produces matte appearance [Foley et al.] et [Foley

kd

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 7 Diffuse shading

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 8 Image so far

Scene.trace(Ray ray, tMin, tMax) { surface, t = hit(ray, tMin, tMax); if surface is not null { point = ray.evaluate(t); normal = surface.getNormal(point); return surface.shade(ray, point, normal, light); } else return backgroundColor; } … Surface.shade(ray, point, normal, light) { v = –normalize(ray.direction); l = normalize(light.pos – point); // compute shading }

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 9 Shadows

• Surface is only illuminated if nothing blocks the light – i.e. if the surface can “see” the light • With ray tracing it’s easy to check – just intersect a ray with the scene!

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 10 Image so far

Surface.shade(ray, point, normal, light) { shadRay = (point, light.pos – point); if (shadRay not blocked) { v = –normalize(ray.direction); l = normalize(light.pos – point); // compute shading } return black; }

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 11 Shadow rounding errors

• Don’t fall victim to one of the classic blunders:

• What’s going on? – hint: at what t does the shadow ray intersect the surface you’re shading?

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 12 Shadow rounding errors

• Solution: shadow rays start a tiny distance from the surface

• Do this by moving the start point, or by limiting the t range

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 13 Multiple lights

• Important to fill in black shadows • Just loop over lights, add contributions • Ambient shading – black shadows are not really right – one solution: dim light at camera – alternative: add a constant “ambient” color to the shading…

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 14 Image so far

shade(ray, point, normal, lights) { result = ambient; for light in lights { if (shadow ray not blocked) { result += shading contribution; } } return result; }

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 15 Specular shading (Blinn-Phong)

• Intensity depends on view direction – bright near mirror configuration

l n v

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 16 Specular shading (Blinn-Phong)

• Close to mirror ⇔ half vector near normal – Measure “near” by dot product of unit vectors

h = bisector(v, l) v + l = l n h v + l A v 2 p Ls = ks (I/r ) max(0, cos ↵) = k (I/r2) max(0, n h)p s · specularly reflected light specular coefficient Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 17 Phong model—plots

• Increasing p narrows the lobe [Foley et al.] et [Foley

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 18 Specular shading

ks al.] et [Foley

p

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 19 Diffuse +

Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 20 Ambient shading

• Shading that does not depend on anything – add constant color to account for disregarded illumination and fill in black shadows

La = ka Ia

ambient coefficient

reflected ambient light Cornell CS4620 Spring 2017 • Lecture 5 © 2017 Steve Marschner • 21 Putting it together

• Usually include ambient, diffuse, Phong in one model

L = La + Ld + Ls = k I + k (I/r2) max(0, n l)+k (I/r2) max(0, n h)p a a d · s · • The final result is the sum over many lights N

L = La + [(Ld)i +(Ls)i] i=1 X N L = k I + k (I /r2) max(0, n l )+ a a d i i · i i=1 X ⇥ k (I /r2) max(0, n h )p s i i · i

Cornell CS4620 Spring 2017 • Lecture 5 ⇤ © 2017 Steve Marschner • 22