 
  
  
  
  
 
The FCT code was ported to the nCUBE-1 by David W. Walker [Walker:88b]. Gary Montry of Sandia National Laboratories supplied the original code, and made several helpful suggestions. A videotape of the evolution of the Kelvin-Helmholtz instability was produced by Jeff Goldsmith at the Image Processing Laboratory of the Jet Propulsion Laboratory.
   
Figure 6.3: Overhead, f, as a Function of  , Where n Is 
the Number of Grid Points per Processor.  Results are shown for nCUBE-1 
hypercubes of dimension one to nine. The overhead for the 2-processor case 
(open circles) lies below that for the higher dimensional hypercubes.  This 
is because the processors only communicate in one direction in the 
2-processor case, whereas for hypercubes of dimension greater than one, 
communication is necessary in both the x and y directions.
, Where n Is 
the Number of Grid Points per Processor.  Results are shown for nCUBE-1 
hypercubes of dimension one to nine. The overhead for the 2-processor case 
(open circles) lies below that for the higher dimensional hypercubes.  This 
is because the processors only communicate in one direction in the 
2-processor case, whereas for hypercubes of dimension greater than one, 
communication is necessary in both the x and y directions.