Table 1 Comparison of localized solution with approximate solution for \(\mu _0=1\),and \(\bar{\tau } (=\tau \omega _0)=0.1\).
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 | − 3.1 | − 2.2648\(\times 10^{-13}\) | − 5.0807\(\times 10^{-13}\) | 2.816\(\times 10^{-13}\) |
− 2.5 | − 2.6 | − 3.132\(\times 10^{-11}\) | − 8.2781\(\times 10^{-11}\) | 5.146\(\times 10^{-11}\) |
− 2.0 | − 2.1 | − 4.3314\(\times 10^{-09}\) | − 1.1595\(\times 10^{-08}\) | 7.2638\(\times 10^{-09}\) |
− 1.5 | − 1.6 | − 5.9901\(\times 10^{-07}\) | − 1.6053\(\times 10^{-06}\) | 1.0063\(\times 10^{-06}\) |
\(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) |
\(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) |
\(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) |
\(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) |
\(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) | \(\cdots \) |
1.5 | 1.4 | − 4.3028\(\times 10^{-06}\) | − 1.6056\(\times 10^{-06}\) | 2.6972\(\times 10^{-06}\) |
2.0 | 1.9 | − 3.1114\(\times 10^{-08}\) | − 1.1623\(\times 10^{-08}\) | 1.9491\(\times 10^{-08}\) |
2.5 | 2.4 | − 2.2498\(\times 10^{-10}\) | − 8.5107\(\times 10^{-11}\) | 1.3988\(\times 10^{-11}\) |
3.0 | 2.9 | − 1.6268\(\times 10^{-12}\) | − 7.0592\(\times 10^{-13}\) | 9.2093\(\times 10^{-13}\) |
