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We’re moving the UMBC GAIM blog over to a university server. All the old posts have been copied over, so you can just switch on over to get anything new. The new site is gaim.umbc.edu
Posted in Uncategorized
There’s a nice article in today’s Baltimore Sun business section on Zynga East and the Baltimore area’s inroads in social game development. Plus, I’m quoted about social games vs. PC and console games.
Posted in Uncategorized
The White House announced the National STEM Video Game Challenge yesterday. This is a mobile game development contest, with a $50,000 grand prize and $25,000 prize for the best undergraduate or graduate student developed game, and a $25,000 prize for the best game reaching an underserved population.
Games should emphasize some specific (but fairly broad) Science, Technology, Engineering and Math skills. Submissions are due January 5th.
Posted in Game Competitions
Almost every graphics game developer I’ve met knows Schlick’s approximation for Fresnel reflectance. This approximation has all the features to be well used in games. It looks visually equivalent to the real Fresnel computation for unpolarized light, while being way easier to compute. However, very few developers have actually looked at Christophe Schlick’s original 1994 Computer Graphics Forum paper, “An Inexpensive BRDF Model for Physicallybased Rendering“. That is a shame, because this paper has some really good ideas for coming up with other approximations for shader computation.
The basic idea is to come up with a rational function (ratio of two polynomials) as an approximation. There’s a long history of this in and out of graphics, but it usually has some inherent problems. Consider “Fast Phong Shading“, published by Bishop and Weimer in SIGGRAPH 1986. This method attempts to avoid the vector renormalization inherent in Phong normal interpolation by using a quadratic Taylor series. Unfortunately, Taylor expansion is inherently centered around a point, in this case the center of the triangle. The approximation will have some error by the time you get to the edge of the triangle, and two triangles sharing that edge won’t necessarily have the same amount of error in their normalization. For big triangles, this can result in a visible shading discontinuity along trangle edges. Not good.
Schlick’s idea is to express what’s important about any function as kernel conditions, then apply those as constraints. For his Fresnel approximation
These constraints are that F should be 1 when dot(N,V)=0, F_{0} when dot(N,V)=1, and the first several derivatives of F should also be 0 when dot(N,V)=1. In the paper, he also has similar approximations for the geometric attenuation and distribution terms of a CookTorrance shading model, but the method is a good one to know in general for reducing shader computation:
Multivariate functions are OK, though will potentially introduce many additional coefficients. This kind of approximation is usually best applied near the visual output end of a shader. Applied to computation too early on, and the small errors may be magnified by the intervening shader code. None the less, it can be a great way to reduce a computationally expensive shader.
Posted in Graphics Tricks
Throwing elections with an electronic voting machine is too easy these days. Does your voting machine run Pac Man? This one does, without even breaking the “tamperproof” seals!
Posted in Uncategorized
Quaternions are an extremely handy representation for rotations. Unfortunately, they fall into a slightly dusty corner of math, so often seem just a little scary. It’s good to understand what they mean, at least for rotations, when it makes sense to them, and when it makes more sense to use rotation matrices. Euler angles occasionally make sense as an interface for specifying rotation, but please convert them to something else as soon as possible!
Quaternions are a combination of a 3D vector and a scalar. Rotation by an angle θ
around a unit vector v
is represented by the quaternion
q = vec4(sin(θ/2)*v, cos(θ/2))
The quaternion, q
, will be unit length (the sum of the squares of all for components is one). You can easily look at a quaternion and tell the axis it rotates around by looking at the vector part, which won’t be unit length anymore since it is scaled by sin(θ/2)
, but still points in the right direction. You can tell the angle by either looking at the scalar part, or the length of the scaled vector part. The inverse rotation will have the axis pointing in the opposite direction, which you can think of as either a rotation around the opposite axis, or the result of flipping the sign of θ
.
One great thing about quaternions is how well they interpolate between two rotations. If you just linearly interpolate and renormalize, you get a nice interpolation of rotation axes along a great circle, plus a smooth rotation of twists around those axes. For t
in [0,1],
normalize( q1*(1t) + q2*t )
In comparison, directly interpolating between rotation matrices gives you weird squishy nonrotations in the middle, and interpolating Euler angles tends to take you on odd paths, especially near the singularities.
You can do even better with the spherical linear interpolation or slerp, as straight linear interpolation goes faster in the middle than at the ends. There’s nothing quaternionspecific about slerp. Given two Ndimensional unitlength vectors, it’ll interpolate between them along an Ndimensional sphere. slerp between unitlength vectors q1
and q2
is given by
φ=acos(dot(q1,q2)) slerp(q1,q2,t) = q1*sin(φ*(1t))/sin(φ) + q2*sin(φ*t)/sin(t)
That looks quite a bit like the linear interpolation, but with different mixing factors for q1
and q2
. If the linear interpolate and renormalize isn’t good enough, but slerp’s trig functions are too slow, there are several approximations that land somewhere in between. My favorite is the one that does normal linear interpolation but replaces t
with a polynomial to adjust the interpolation speed.
There are three main things to know for using quaternions. First, to rotate a single point p
by quaternion q
:
pRot = p + 2*cross(q.xyz, q.w*p + cross(q.xyz, p))
The second big operation is converting a quaternion rotation into a 3×3 rotation matrix. That’s
vec3 Q = 2.*q.xyz; qMat = mat3( 1  Q.y*q.y  Q.z*q.z, Q.x*q.y + Q.z*q.w, Q.x*q.z  Q.y*q.w, Q.x*q.y  Q.z*q.w, 1  Q.x*q.x  Q.z*q.z, Q.y*q.z + Q.x*q.w, Q.x*q.z + Q.y*q.w, Q.y*q.z  Q.x*q.w, 1  Q.x*q.x  Q.y*q.y);
The final big one is how to combine two quaternion rotations into a new one. That’s just
q = vec4(q1.w*q2.w  dot(q1.xyz,q2.xyz), q1.w*q2.xyz + q2.w*q2.zyx + cross(q1.xyz,q2.xyz));
So when do we use each? In raw operations, the direct quaternion rotation is 18 multiplies and 12 adds. GPU operations are at least somewhat dependent on the GPU, but assuming up to a fourelement multiplyandadd or dot product is a single operation, it’s probably about 6 GPU instructions. That’s two for the inner cross product, one more to add in q.w*p
, two more for the outer cross product, and one more to multiply by 2 and add to p
.
The matrix construction, assuming the common multiplies are factored out, is 12 multiplies and 12 adds, while the matrix multiply to actually rotate with it would be 9 multiplies and 6 adds, for a total of 21 multiplies and 18 adds (clearly more expensive). In GPU terms, it’s about 7 GPU instructions to create the matrix and 3 to use it (still more expensive). On the other hand, to apply the same rotation to two points is 36 multiplies and 24 adds using the direct rotation, but only 30 multiples and 24 adds with the matrix multiply since you can use the same rotation matrix twice. So, to transform a single point, it’s best to use direct quaternion rotation, but for two or more (or even a point and normal), converting to a 3×3 matrix form is a big win.
Finally, combining two quaternions is 16 multiplies and 8 adds, or about 6 GPU operations. In comparison, combining two rotation matrices takes 27 multiplies and 18 adds or about 9 GPU instructions.
So… If you are doing lots of work with rotations, or need to do any interpolation between transformations at all, quaternions are the tool for you. If you are transforming more than one point by the resulting rotation, you’re better off converting the quaternion to a matrix to use it, but given that quaternions interpolate so much better and are so much cheaper to combine together, it’s still often worth it.
Perhaps in a later post I’ll go through the math behind quaternions, and how to get a quaternion given a rotation matrix, but for now, this is just enough quaternion to be dangerous.
Posted in Graphics Tricks
Today, a look at Fresnelmodulated reflections. Hardly a secret trick, but it makes a surprising difference for somewhat shiny objects. Fresnel reflectance is the property that glancing reflections are stronger than headon reflections. It’s particularly noticeable in surfaces like water or glass, but is even visible on a piece of paper. Oh, and since Fresnel reflectance is named after a person, it should always be capitalized (and since he was French, you don’t pronounce the ‘s’).
The most important directions for Fresnel reflectance are the surface normal, N, the direction you see the surface from, V, the direction the reflected light is coming from L (all unitlength vectors). Since it’s dealing with reflected rays, N should be half way between V and L, so N = normalize(V+L) and dot(N,V) = dot(N,L). I’m ultimately going to be applying it to an environment map, so I’ll stick with the dot(N,V) version.
There are also constants that control the strength of the effect: n_{1} and n_{2}, the indices of refraction of each material, or sometimes rewritten in terms of n, the ratio of the two indices of refraction. Indices of refraction for common materials are pretty easy to find in a Physics text or online: vacuum is 1, air is pretty close to 1, water is about 1.33, glass is about 1.5.
Fresnel reflectance has different terms for incoming light polarized parallel to the surface than for light that’s not parallel to the surface. I’ll add another direction T, for the refracted light, since it makes the equations easier, though you can always rewrite the refracted direction in terms of the reflected one.
The polarization dependence is handy if you’re using a polarizing filter to enhance or diminish the reflections in a photograph, but most graphics assumes unpolarized light, which is an equal mix of both terms. Cook and Torrance came up with the combined form that was used in graphics for many years:
If you don’t have the index of refraction, it’s easier to measure the reflectance at normal incidence (looking headon where it is smallest). From Cook and Torrance’s paper, that’s
But… almost everyone these days uses Schlick’s approximation for Fresnel. There’s actually lots of good stuff on approximating functions in Schlick’s paper, but only the Fresnel approximation seems to have really stuck:
For a little more intuitive control, you can write this in terms of F_{0} at normal incidence and F_{90} at the edge of the object:
Image d above is what it looks like for a high dynamic range environment map. I’ve also included a regular BlinnPhong layer with a light source positioned at the brightest point in the environment texture. F is just the blend factor between the two.
It’s important to use a highdynamic range texture for this, because ordinary 8bit textures can’t distinguish between “the sky is bright”, maxed out at 255 and “the sun is 10,000 times brighter”, also maxed out at 255. Multiply by 0.04, and you get about 10 in both cases. But image was exposed so the sky really is 255, the sun should be around 25,500,000. When multiplied by 0.04, that’s still 10,200,000 (or really bright). If we don’t keep the full dynamic range of the environment map, we get the somewhat disappointing result in image c
Oh, and images a and b are what you get for a couple of choices of constant blend fraction. The glancing reflections around the edges of the model really add an extra dimension of shininess.
Posted in Graphics Tricks