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Page 1: quintin.bizquintin.biz/ArticlePDFs/1995 Ahmed Sherlock Rayer NNFM.pdf · finite—difference formulations which conserve mass, momentum and energy only in the limit as the simulation
Page 2: quintin.bizquintin.biz/ArticlePDFs/1995 Ahmed Sherlock Rayer NNFM.pdf · finite—difference formulations which conserve mass, momentum and energy only in the limit as the simulation
Page 3: quintin.bizquintin.biz/ArticlePDFs/1995 Ahmed Sherlock Rayer NNFM.pdf · finite—difference formulations which conserve mass, momentum and energy only in the limit as the simulation
Page 4: quintin.bizquintin.biz/ArticlePDFs/1995 Ahmed Sherlock Rayer NNFM.pdf · finite—difference formulations which conserve mass, momentum and energy only in the limit as the simulation
Page 5: quintin.bizquintin.biz/ArticlePDFs/1995 Ahmed Sherlock Rayer NNFM.pdf · finite—difference formulations which conserve mass, momentum and energy only in the limit as the simulation
Page 6: quintin.bizquintin.biz/ArticlePDFs/1995 Ahmed Sherlock Rayer NNFM.pdf · finite—difference formulations which conserve mass, momentum and energy only in the limit as the simulation
Page 7: quintin.bizquintin.biz/ArticlePDFs/1995 Ahmed Sherlock Rayer NNFM.pdf · finite—difference formulations which conserve mass, momentum and energy only in the limit as the simulation
Page 8: quintin.bizquintin.biz/ArticlePDFs/1995 Ahmed Sherlock Rayer NNFM.pdf · finite—difference formulations which conserve mass, momentum and energy only in the limit as the simulation

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