1次元拡散方程式 - 北海道大学
(6) となる. ここで時間差分スキーム(2)の(1)式を用いた. 摩擦方程式で考察したとき と同様にK = (2ˇ ∆x)2 ∆t とおいて安定性を議論する. 1. = 1; = 0(オイラースキーム)の場合 2012 0202-ogihara.tex 2013/06/05(荻原弘尭)
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