MARC

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035 |a (TOE)ost6148514 
035 |a (TOE)6148514 
040 |a TOE  |c TOE 
049 |a GDWR 
072 7 |a 99  |2 edbsc 
086 0 |a E 1.99: conf-830581-1 
086 0 |a E 1.99:la-ur-83-1362 
086 0 |a E 1.99: conf-830581-1 
088 |a conf-830581-1 
088 |a la-ur-83-1362 
245 0 0 |a Multigrid semi-implicit hydrodynamics revisited  |h [electronic resource] 
260 |a Los Alamos, N.M. :  |b Los Alamos National Laboratory ;  |a Oak Ridge, Tenn. :  |b distributed by the Office of Scientific and Technical Information, U.S. Department of Energy,  |c 1983. 
300 |a Pages: 22 :  |b digital, PDF file. 
336 |a text  |b txt  |2 rdacontent. 
337 |a computer  |b c  |2 rdamedia. 
338 |a online resource  |b cr  |2 rdacarrier. 
500 |a Published through SciTech Connect. 
500 |a 01/01/1983. 
500 |a "la-ur-83-1362" 
500 |a " conf-830581-1" 
500 |a "DE83012675" 
500 |a Conference on large scale scientific computation, Madison, WI, USA, 16 May 1983. 
500 |a Dendy, J.E. 
520 3 |a The multigrid method has for several years been very successful for simple equations like Laplace's equation on a rectangle. For more complicated situations, however, success has been more elusive. Indeeed, there are only a few applications in which the multigrid method is now being successfully used in complicated production codes. The one with which we are most familiar is the application by Alcouffe to TTDAMG. We are more familiar with this second application in which, for a set of test problems, TTDAMG ran seven to twenty times less expensively (on a CRAY-1 computer) than its best competitor. This impressive performance, in a field where a factor of two improvement is considered significant, encourages one to attempt the application of the multigrid method in other complicated situations. The application discussed in this paper was actually attempted several years ago. In that paper the multigrid method was applied to the pressure iteration in three Eulerian and Lagrangian codes. The application to the Eulerian codes, both incompressible and compressible, was successful, but the application to the Lagrangian code was less so. The reason given for this lack of success was that the differencing for the pressure equation in the Lagrangian code, SALE, was bad. In this paper, we examine again the application of multigrad to the pressure equation in SALE with the goal of succeeding this time without cheating. 
536 |b W-7405-ENG-36. 
650 7 |a Hydrodynamics.  |2 local. 
650 7 |a Iterative Methods.  |2 local. 
650 7 |a Computer Calculations.  |2 local. 
650 7 |a Lagrangian Function.  |2 local. 
650 7 |a Laplace Equation.  |2 local. 
650 7 |a Matrices.  |2 local. 
650 7 |a Differential Equations.  |2 local. 
650 7 |a Equations.  |2 local. 
650 7 |a Fluid Mechanics.  |2 local. 
650 7 |a Functions.  |2 local. 
650 7 |a Mechanics.  |2 local. 
650 7 |a Partial Differential Equations.  |2 local. 
650 7 |a General And Miscellaneous//Mathematics, Computing, And Information Science.  |2 edbsc. 
710 2 |a Los Alamos National Laboratory.  |4 res. 
710 1 |a United States.  |b Department of Energy.  |b Office of Scientific and Technical Information.  |4 dst. 
856 4 0 |u http://www.osti.gov/scitech/biblio/6148514  |z Online Access 
907 |a .b60005397  |b 03-06-23  |c 05-30-10 
998 |a web  |b 09-09-16  |c f  |d m   |e p  |f eng  |g    |h 0  |i 3 
956 |a Information bridge 
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952 f f |p Can circulate  |a University of Colorado Boulder  |b Online  |c Online  |d Online  |e E 1.99: conf-830581-1  |h Superintendent of Documents classification  |i web  |n 1