This is the second part of ray tracing, and we are starting to add cool features. For next week I'm going to ask you to do as many of the following as you can:
As I mentioned in class (and as I describe in detail in the notes at bottom), to implement this requires "sewing together" ray/shape intersections that are more complex than just a single "in/out" root pair.
Shadows:
Implementing shadows is really are not that hard to do with ray tracing. The trick is, when you're at a single surface point and looping over light sources, fire a ray from the surface point into the direction of each light source. If the ray toward a light source hits any objects, then don't illuminate that surface point by that light source (ie: in your Phong shader, don't add in any Diffuse or Specular contributions for that light source).
There is one little trick though. You don't want the shadow ray to accidentally hit the object itself, due to numerical inaccuracy. So to play it safe, you want to start the ray just a little ways along the direction to the light source. Formally, here is how you form the shadow ray to a point light source:
w' = normalize(L  S)where ε is an appropriately small number such as 0.001.
v' = S + ε w'
If your light source is just a directional light at infinity, rather than an actual point in the scene, then it's even easier, since then you can just set w' = L
Reflecting a ray off a surface:
To do reflections you will want to be able to bounce a ray (v + t w) off a surface to create a reflecting ray (v' + t w'). As we discussed in class, given surface normal vector n you can compute w' by:
w' = w  2 (w • n) n
and then the reflecting ray's origin can be given by moving just a little off of the surface point S:
v' = S + ε w'
Refracting a ray into a surface:
Refraction is implemented by Snell's Law:
n_{1} sin(θ_{1}) = n_{2} sin(θ_{2})
where n_{1} and n_{2} are the respective indices of refraction of the medium that the ray comes from and the medium that the ray passes into.
To compute the direction of the exit ray w_{2}, take the dot product of entering ray direction w_{1} with the surface normal n. This will let you decompose w_{1} into two components c_{1} and s_{1} which are, respectively, perpendicular to and parallel to the surface.
The vector c_{1} = (w_{1} • n) n is the component of w_{1} perpendicular to the surface. This component has length cos(θ_{1}).
The vector s_{1} = w_{1}  c_{1}. is the component of w_{1} parallel to the surface. This component has length sin(θ_{1}).
You can then just adjust the lengths of these two component vectors to cos(θ_{2}) and sin(θ_{2}), respectively. When you sum the lengthadjusted component vectors, you will have w_{2}.
As we discussed in class, the index of refraction in air is essentially 1.0, and the index of refraction in most optically clear solids and fluids such as water or glass is around 1.5.
Ray tracing to polyhedra:
As we said in class, to implement ray tracing to polyhedra:
For example, the six linear inequalities for a unit cube are:
a b c d x ≥ 1 → x1 ≤ 0 → 1 0 0 1 x ≤ +1 → +x1 ≤ 0 → +1 0 0 1 y ≥ 1 → y1 ≤ 0 → 0 1 0 1 y ≤ +1 → +y1 ≤ 0 → 0 +1 0 1 z ≥ 1 → z1 ≤ 0 → 0 0 1 1 z ≤ +1 → +z1 ≤ 0 → 0 0 +1 1
If the planar face is facing toward v (ie: if v is on the positivevalued outside of the face), then t is at a point where the ray enters the polyhedron.
Conversely, if the planar face is facing away from v (ie: if v is on the negativevalued inside of the face), then t is at a point where the ray exits the polyhedron.
Using preexisitng polyhedral models:
Although we didn't cover this in class, you may already have a convex polyhedron described as vertices and faces (eg: a pyramid or rectangular prism or icosohedron), and wish to convert this shape into an intersection of half spaces so you can ray trace to it. You would do this by taking each of your shape's polygonal faces in turn, and computing the half space for that face. You can figure out the linear inequality (a,b,c,d) that goes through the face of any polygon, by considering any three of the polygon's vertices P,Q,R. Remember that we have been following the convention that the points P,Q,R go around counterclockwise, as seen from the outside (ie: from the positivevalued halfspace) of the shape. The method is as follows:

Transforming polyhedral shapes:
To transform, by some matrix M, a polyhedral shape to which we are ray tracing, we need to transform each of the polyhedron's component halfspaces (a b c d).
To do this, you are going to use exactly the same technique that you used for transforming surface normals. But I'm going to go over the math here again anyway, just to make sure it's clear.
In the discussion that follows, I'm going use transpose notation (x y z 1)^{T} when referring to the homogeneous decription of a point in space, to make it clear that I am describing the point as a column vector.
When transforming a halfspace (a b c d) by matrix M, the key thing to observe is that if you transform each point
(x y z 1)^{T} → M(x y z 1)^{T},
then your corresponding transformation (a b c d) → (a' b' c' d') has to ensure that the transformed point still lies on the same side of the transformed plane:
(a' b' c' d') (M(x y z 1)^{T}) = (a b c d) (x y z 1)^{T}.
In other words, if we ask the question "is this point inside the original halfspace?", we need to get the same answer after we transform both the point and the halfspace.
As we have discussed in class, the way to do this is to postmultiply by the matrix inverse, so that:
(a b c d) → ( (a b c d) M^{1} ).
This works because linear transformations are associative:
( (a b c d) M^{1} ) ( M(x y z 1)^{T} ) =
(a b c d) ( M^{1} M ) (x y z 1)^{T} =
(a b c d) (x y z 1)^{T}
Boolean intersections:
Given any convex shapes (such as spheres, cylinders, or boxes), it is very easy to do boolean intersection via raytracing. When you trace a ray to any convex shape, either the ray misses the shape, or else the ray intersects the shape along some interval [t_{in} , t_{out}] along the ray.
Given a collection of convex shapes, if the ray misses any one of them, then the ray misses their intersection. If the ray hits all of them, then the intersection is given by the interval [max(t_{in}) , min(t_{out})], where max(t_{in}) is the maximum over all the t_{in}, and where min(t_{in}) is the minimum over all the t_{out}.
For example, you can create a unit length cylinder by intersecting the infinite cylinder x^{2} + y^{2}  1 = 0 with the cube that goes from 1 to +1 in x, y and z. Then you can apply a matrix to the component shapes in order to transform this cylinder to any other finite length cylinder.
Boolean unions and differences (making nonconvex shapes):
Nonconvex shapes are more difficult to deal with than are convex shapes, because the same ray can enter and leave a shape multiple times, to it is not sufficient just to speak of a single interval [t_{in} , t_{out}]. Instead, we need to describe the places where the ray is inside the shape by a sequence of t values: [ t_{0} t_{1} t_{2} ... t_{n1} ], where the even numbered elements represent places where the ray enters the shape, and the odd numbered elements represent places where the ray exits from the shape. For example, [0.3 1.4 2.7 3.5] represents two successive segments where the ray is inside the shape: a first segment between t=0.3 and t=1.4, followed by a second segment between t=2.7 and t=3.5.
This notation makes it possible to describe nonconvex things
like the result of boolean difference.
For example, suppose shape A
contains a hollow cavity with shape B, and suppose that
a particular ray intersects shape A
at
[t(A)_{in} , t(A)_{out}],
and that the same ray intersects shape B at
[t(B)_{in} , t(B)_{out}].
If t(A)_{in} < t(B)_{in} < t(B)_{out} < t(A)_{in}, then the boolean difference A  B is described along this ray by: [ t(A)_{in} t(B)_{in} t(B)_{out} t(A)_{out} ]. 
In general you can implement boolean difference by replacing:
[ t_{0} t_{2} t_{3} ... t_{n1} ] → [ 0 t_{0} t_{1} t_{2} ... t_{n1} ∞ ]
Notice that if t_{0} was already zero, then the first interval becomes null, and you can just drop the first two elements of the resulting sequence. Similarly, if if t_{n1} was already ∞ then you can just drop the last two elements of the resulting sequence.
In order to implement boolean union, you only need to implement boolean intersection and boolean difference, since de Morgan's law gives us:
A ˇ B = ¬ ( (A ˆ B) ˆ (A ˆ B) )
The hardest part is implementing intersection for nonconvex shapes. To intersect two nonconvex shapes along a ray you need to merge together their two sequences. This is done by progressively moving along the two sequences, looking for values of t where the ray is inside both shapes, and using those values of t to construct a new sequence. Here is a sketch of the algorithm:
Create an empty destination sequence. Starting from the beginning of both sequences, Repeat until at the end of both sequences: Choose the smallest remaining t value, from whichever of the two input sequences you find it. If this was an entering (even numbered) t: If this t value is inside the other shape: then append it to the destination sequence. If this was an exiting (odd numbered) t: If this t value is outside the other shape: then append it to the destination sequence.
HOMEWORK:
Your job for this assignment is to use as many different ray tracing techniques as you feel comfortable implementing, and come up with an interesting collection of reflecting, refracting and shaded shapes, rendered by ray tracing, to produce cool and compelling pictures or animations. Try to use a variety of shapes, and make sure to create something fun!