Cosmical Electrodynamics, 2nd Ed. (International Series of by Hannes Alfvén, C-.Y. Falthammar; Hannes Alfven

By Hannes Alfvén, C-.Y. Falthammar; Hannes Alfven

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17] D. Uffelman, W. Bender, L. Ratkc and B. Feuerbacher: Acta Metall. Mater. 43 (1995) p. 173. 40 Sintering Fundamentals [18] T. Mookherji, W. B. McAncelly and E. C. McKannan, in: Proceedings of the Third Space Processing Symposium: Skylab Results, Vol. 11 (NASA Marshall Space Flight Center, AL, 1974) p. 963. [19] A. Keneissl and H. Fischmeister, in: Material Sciences Under Microgravity, Results of Spacelab-1 ESA SP-222 (European Space Agency, France, 1984) p. 63. [20] L. Ratkc, H. Fischmeister and A.

For every k-th solid grains we will define the hypothetical sphere HS k ( RkH , rkH ) , where the radius RkH  Rk  Rmin , and Rmin  min{R } . Thus the nearest neighbors  of k-th solid grain will be those solid grains, which fulfilled the condition (Fig. , N ;   k ) . e.  (t ) , due to time dependent domain position, D ( xc (t ), yc (t ), zc (t )) . e. D ( xc (t ), yc (t ), zc (t ))  DT ( xc (t ), yc (t ), zc (t )  q t ) (8) D ( xc (t ), yc (t ), zc (t ))  DT ( xc (t )  q t , x , yc (t )  q t , y , zc (t )  q t , z ) (9) for Model S1 and Model S2, respectively.

493. -C. Yang, and R. M. German: Metall. Trans. 22A (1991) p. 786. [41] D. F. Heaney, R. M. German and I. S. Ahn: J. Mater. Sci. 30 (1995) 5808. [42] R. M. German, Y. Liu and A. Griffo: Metall. Mater. Trans. A 28 (1997) 215. [43] R. M. German: Sintering Theory and Practice (Wiley-Interscience, New York, 1996). S. Upadhyaya 41 [44] L. Xu, S. Z. Lu and T. H. Courtney: Scripta Materialia 46 [12] (2002) pp. 887-891. [45] T. H. Courtney, Y. Du and S. Z. Lu: Metall Mater Trans A 31 (2000) 2907. [46] Y.

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