| ファイル名 File name |
出力される量 Quantity |
| parameters/variable0.rho.log | 密度 Density |
| parameters/variable0.lambda.log | ラメ定数\(\lambda\) Lame constant \(\lambda\) |
| parameters/variable0.mu.log | ラメ定数\(\mu\) Lame constant \(\mu\) |
| parameters/variable0.alpha_k.log, \(k=0,1,2\) | PML領域における吸収の強さ\(\alpha^k\) The strength, \(\alpha^k\), of absorption in the PML volume |
| parameters/variable0.c0_k.log, \(k=0,1,2\) | 差分方程式の係数\(c_0^k\) The coefficient \(c_0^k\) of difference equations |
| parameters/variable9.c1_k.log, \(k=0,1,2\) | 差分方程式の係数\(c_1^k\) The coefficient \(c_1^k\) of difference equations |
| parameters/variable10.c2_ic.log, \(ic=0,2,3,5,6,8\) | 差分方程式の係数\(c_2^{ijpl}\)であり、\((i,j,p,l)\)とicは
弾性定数の成分番号ic
の通り関係づけられる The coefficient \(c_2^{ijpl}\) of difference equations; \((i,j,p,l)\) and ic are related following an integer index ic that represents the component of an elastic constant |
| parameters/variable11.c2_ic.log, \(ic=1,4,7\) | 差分方程式の係数\(c_2^{ijpl}\)であり、\((i,j,p,l)\)とicは
弾性定数の成分番号ic
の通り関係づけられる The coefficient \(c_2^{ijpl}\) of difference equations; \((i,j,p,l)\) and ic are related following an integer index ic that represents the component of an elastic constant |
| parameters/variablep.f_q_r.log | 等価体積力を位置の関数と時間の関数の積の重ね合わせで
\[\begin{equation}
f_i(\posx,t)=\sum_{is}F_i^{(is)}(\posx)s^{(is)}(t)
\label{eq.f}
\end{equation}\]
と表したときの\(F_i^{(is)}\)であり、
ファイル名との対応は\(p=12+3is+i\), \(q=is+1\), \(r=i+1\)である The value of \(F_i^{(is)}\) when the equivalent body force is expressed as a summation of products of position and time functions as Eq. (\ref{eq.f}); the indices \(i\) and \(is\) correspond to the file name as \(p=12+3is+i\), \(q=is+1\), and \(r=i+1\) |
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