Publications index

Paul Heckel, Butler Lampson

Communications of the ACM | July 1977, Vol 20(7): pp. 486-494

Jim Blinn

Siggraph 1977 | July 1977

Andrew Birrell

ACM SIGPLAN Notices | June 1977, Vol 12(6)

Yuri Gurevich

Studia Logica | May 1977, Vol 36: pp. 49-59

Yuri Gurevich

Annals of Mathematical Logic | May 1977, Vol 12: pp. 193-228

Yuri Gurevich

Israel Journal of Mathematics | April 1977, Vol 27: pp. 299-319

Leslie Lamport

IEEE Transactions on Software Engineering SE-3 | March 1977, Vol 2: pp. 125-143

Leslie Lamport

In A Dynamic and Quick Intellect, John Tromp editor (1996)--a Liber Amicorum issued by the CWI in honor of Paul Vitanyi's 25-year jubilee. | January 1977

Jim Blinn

Siggraph 1977 | January 1977

When I was a grad student at Utah I spend a lot of time poking around the engineering library for interesting information. There I happened to stumble upon the archived editions of the Transactions of the Illumination Engineering Society which seemed like it would have useful info. Sure enough in the 1910 volume there was an article by F. H. Gilpin where he actually measured the reflection off of some surfaces and had actual graphs of the reflection amount as a function of various angles. I originally attempted to digitize these graphs to make a sort of table-look-up function that was driven by the physical measurements. At the time there were no such things as scanners or digitizers. The most sophisticated tool I had was a Xerox machine that could make enlargements on paper. I did this and started to measure points on the curves with a ruler and enter the measurements manually. This got a bit boring, so I decided to go back to the library to troll for a more recent result. I ultimately found a whole lot of articles on the subject but most of them were models that were not understandable or real useful for computer graphics. I was particularly amused, though, by one with a title something like “The bidirectional reflectance characteristics of snow” which came out of the University of Minnesota (home of much snow). This led me to the Torrance-Sparrow paper that ultimately made the most sense to me. They modeled specular reflection in terms of the vector H, halfway between the light and eye. If the surface was a perfect mirror and if the surface normal, N, aligned with H then the light and eye were in the right position for perfect mirror reflection. If the surface was rougher, then the specular amount was a function of what percentage was pointed in the direction of H. Again this led to a function of the dot product (N.H). The particular function they derived was in terms of spherical geometry giving a very complicated function involving many trig functions. I spent weeks trying to simplify this formulation filling up dozens of pages with trig identities. One of the hardest things was that the function was a choice between three different functions which applied to different regions of (N,L,E) space and whose boundaries in spherical geometry had to be calculated in order to figure out which sub-function to use. Finally I gave up and went back to their original geometric ideas and rederived the whole thing using dot and cross products. And I realized that the boundaries were simply the regions where two of the three functions were equal. That led to the considerably simpler formulation that I wrote up for Siggraph as a practical solution that you could evaluate relatively quickly in rendering software. When I wrote up the result I was focused on the final result as a function of (N.H) and so I introduced the paper with a simpler model that was reminiscent of Phong’s model. He did (E.R) to a power and I did (N.H) to a power. I realized that these two functions were different, but they were similar. They both had a maximum of 1 when E=R (or equivalently (N=H)) and fell off to smaller values as these vectors moved apart. In the second section of the paper I then proceeded to show my derivation of the more complex Torrance-Sparrow model as a function of (N.H). One thing has always bothered me a bit. The TS model gives the fall-off function in terms of a physically meaningful quantity (statistical distribution of micro-facet directions, a property of the surface) while Phong’s calculation (cosine to a power) was just picked as a convenient way to sculpt the function to a desired shape. But taking a number to an arbitrary power (that is not a power of 2) is actually more computationally expensive than the TS model calculations. So I always wondered why people still speak of “cosine power” as a property of a surface even today. I understand that there is a menu item in programs such as Maya called "Blinn Shading" (as an alte

Butler Lampson

Proc. 5th Ann. III Conf: Implementation and Design of Algorithmic Languages | January 1977