From: Fast rapidly convergent penetrable scattering computations
\({\varvec{N}}^{\mathcal B}_{\varvec{u}}\) | \({\varvec{N}}^{\mathcal B}_{\varvec{t}}\) | \({\varvec{N}}^{\mathcal I}_{\varvec{u}}\) | \({\varvec{N}}^{\mathcal I}_{\varvec{t}}\) | \({\varvec{\varepsilon }}_{\varvec{2}}\) | \({\varvec{\varepsilon }}_{\varvec{\infty }}\) | \({\varvec{\kappa }}_{\varvec{e}}\) | Time (S) |
---|---|---|---|---|---|---|---|
\(33\) | \(9\) | \(33\) | \(33\) | \(2.79\times 10^{-2}\) | \(7.16\times 10^{-3}\) | \(4\) | \(1.53\) |
\(65\) | \(17\) | \(65\) | \(65\) | \(2.20\times 10^{-3}\) | \(2.64\times 10^{-3}\) | \(8\) | \(6.8\) |
\(129\) | \(33\) | \(129\) | \(129\) | \(4.60\times 10^{-4}\) | \(5.93\times 10^{-4}\) | \(16\) | \(25.7\) |
\(257\) | \(65\) | \(257\) | \(257\) | \(1.02\times 10^{-4}\) | \(1.23\times 10^{-4}\) | \(32\) | \(102.6\) |