Three Dimensional Computation of Magnetohydrodynamic Equilibrium of Toroidal Pla
Three Dimensional Computation of Magnetohydrodynamic Equilibrium of Toroidal Pla
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In our eReader you can find the full English version of the book. Read Three Dimensional Computation of Magnetohydrodynamic Equilibrium of Toroidal Pla Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Three Dimensional Computation of Magnetohydrodynamic Equilibrium of Toroidal Pla
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, -4 e = min (10, 0. 1 £p/c, ) where min(a, b) denotes the minimum between a and b. The choice of the scale factor c^ is due to the fact that the biggest error in Laplace's equation occurs in the potential ii, , which must be multiplied by the factor c, .
The various convergence factors which occur in the formulation of the problem were determined by trial and error to produce a convergent scheme. For the relaxation factor to in the successive overrelaxation method we used 1. 9 for the vacuum r...egion, and 1. 8 for the plasma region. For the relaxation factor X in the steepest descent method we used values ranging from 0. 02 to 0. 06.
5. 2. Description of the Mesh Size and Computing Time .
For our production runs we have used a mesh with 30 points in the and 9 directions and 12 points in the radial direction, six of which lie in the vacuum region and the other six in the plasma region. The program was -48- designed by trying to minimize the core space needed. For the mesh size just described, the amount of core needed is 110 K which is one-third of the total core available in the CDC 6600 computer.
What to read after Three Dimensional Computation of Magnetohydrodynamic Equilibrium of Toroidal Pla?
You can find similar books in the "Read Also" column, or choose other free books by Octavio L Betancourt to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
, -4 e = min (10, 0. 1 £p/c, ) where min(a, b) denotes the minimum between a and b. The choice of the scale factor c^ is due to the fact that the biggest error in Laplace's equation occurs in the potential ii, , which must be multiplied by the factor c, .
The various convergence factors which occur in the formulation of the problem were determined by trial and error to produce a convergent scheme. For the relaxation factor to in the successive overrelaxation method we used 1. 9 for the vacuum r...egion, and 1. 8 for the plasma region. For the relaxation factor X in the steepest descent method we used values ranging from 0. 02 to 0. 06.
5. 2. Description of the Mesh Size and Computing Time .
For our production runs we have used a mesh with 30 points in the and 9 directions and 12 points in the radial direction, six of which lie in the vacuum region and the other six in the plasma region. The program was -48- designed by trying to minimize the core space needed. For the mesh size just described, the amount of core needed is 110 K which is one-third of the total core available in the CDC 6600 computer.
What to read after Three Dimensional Computation of Magnetohydrodynamic Equilibrium of Toroidal Pla?
You can find similar books in the "Read Also" column, or choose other free books by Octavio L Betancourt to read onlineMoreLess
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