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By Sangwon Chae, Soon-Bin Yim, Youngshin Han (auth.), Jong-Hyun Kim, Kangsun Lee, Satoshi Tanaka, Soo-Hyun Park (eds.)

This booklet is a compilation of analysis accomplishments within the fields of modeling, simulation, and their functions, as offered at AsiaSim 2011 (Asia Simulation convention 2011). The convention, held in Seoul, Korea, November 16–18, used to be prepared by means of ASIASIM (Federation of Asian Simulation Societies), KSS (Korea Society for Simulation), CASS (Chinese organization for procedure Simulation), and JSST (Japan Society for Simulation Technology). AsiaSim 2011 supplied a discussion board for scientists, academicians, and pros from the Asia-Pacific sector and different components of the area to proportion their newest fascinating learn findings in modeling and simulation methodologies, thoughts, and their instruments and purposes in army, communique community, undefined, and basic engineering problems.

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Extra info for Advanced Methods, Techniques, and Applications in Modeling and Simulation: Asia Simulation Conference 2011, Seoul, Korea, November 2011, Proceedings

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Geophys. Res. jp Abstract. The parameter α , which at first was introduced to modify the coordinate of the equilibrium point of Euler’s equations[1], is used to represent the canonical equations of (θ , pθ ) for Lagrange’s top. We then take a perspective approach to the top by doing an analysis of the potential function U (θ , α ) , and settle on a mapping between typical motions of the top and the values of α . This approach makes it clear that there are two different modes of stationary precession and that a sleeping top mode can be reduced from a Lagrange’s top.

In this way, we can always use two newly computed values in the iteration formula. Thus the Gauss-Seidel iteration formula is him, j+1 = (h m +1 i , j +1 ) ( + him, j+−11 + R him−1+,1j + him+1+,1j 2(1 + R ) ) (10) The change between two successive Gauss-Seidel iterations is called the residual c. The residual is then defined by c = him, j+1 + him, j (11) By replacing hmi,j with hm+1i,j after each calculation, the Gauss-Seidel procedure liquidates or relaxes the residuals at every node and thus leads to a solution of each algebraic equation.

Thus, Tqueue becomes: Tqueue = ake 2 N . 2 (3) The time for an event routine execution Texecute is beN, where b is the average execution time of event routines. Therefore, the total time of a sequential simulation is: TS = ake 2 N + beN , 2 (4) and the total time of a parallel simulation can be described as: TP = ake N 2 N ( ) + be + v, 2 P P (5) where P is the number of LPs and v is the time due to synchronization overhead for parallel simulation. The speedup is the ratio of the sequential simulation time to the parallel simulation time.

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