Table 2 Comparison of localized solution with approximate solution for \(\mu _0=1\),and \(\bar{\tau }=0.01\).
From: Electron-acoustic solitary potential in nonextensive streaming plasma
\(\bar{\xi }\) | \(\bar{\zeta }\)=\(\bar{\xi }-\mu _0\bar{\tau }\) | Localized solution | MDLDM Solution | Absolute Error |
|---|---|---|---|---|
− 3.0 | − 3.01 | − 5.5001\(\times 10^{-13}\) | − 5.971\(\times 10^{-13}\) | 4.7095\(\times 10^{-14}\) |
− 2.5 | − 2.51 | − 7.6063\(\times 10^{-11}\) | − 8.3828\(\times 10^{-11}\) | 7.7646\(\times 10^{-12}\) |
− 2.0 | − 2.01 | − 1.0519\(\times 10^{-08}\) | − 1.1608\(\times 10^{-08}\) | 1.0885\(\times 10^{-09}\) |
− 1.5 | − 1.51 | − 1.4547\(\times 10^{-06}\) | − 1.6054\(\times 10^{-06}\) | 1.5071\(\times 10^{-07}\) |
\(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) |
\(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) |
\(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) |
\(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) |
\(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) |
1.5 | 1.49 | − 1.7718\(\times 10^{-06}\) | − 1.6055\(\times 10^{-06}\) | 1.6633\(\times 10^{-07}\) |
2.0 | 1.99 | − 1.2812\(\times 10^{-08}\) | − 1.161\(\times 10^{-08}\) | 1.2014\(\times 10^{-09}\) |
2.5 | 2.49 | − 9.2641\(\times 10^{-11}\) | − 8.406\(\times 10^{-11}\) | 8.5812\(\times 10^{-12}\) |
3.0 | 2.99 | − 6.6989\(\times 10^{-13}\) | − 6.1689\(\times 10^{-13}\) | 5.2999\(\times 10^{-14}\) |
