Table 5.
Adopted parameters for the hot spot and lobe models shown in Figs. 5–7.
| Source | Comp. | R | Pe, 45 | B | γb | γmax | s1 | s2 | log Ee | log EB | β |
|---|---|---|---|---|---|---|---|---|---|---|---|
| [1] | [2] | [3] | [4] | [5] | [6] | [7] | [8] | [9] | [10] | [11] | [12] |
| 0100+2802 | lobe | 70 | 1.1 | 7 | 4e3 | 1e5 | 1 | 2 | 58.1 | 58.9 | 0.2 |
| 0306+185 | lobe | 10 | 2 | 21.7 | 1e3 | 3e5 | 1 | 2.7 | 57.4 | 57.3 | 0.14 |
| B2 1023+25 | hot spot | 3 | 10 | 250 | 1e4 | 1e6 | 1.3 | 2.5 | 57.9 | 57.4 | 0.2 |
Notes. Column [1]: source; Col. [2]: component; Col. [3]: size in kpc; Col. [4]: power injected in relativistic electrons in units of 1045 erg s−1; Col. [5]: magnetic field in μG; Cols. [6] and [7]: break and maximum Lorenz factor of the injected electron distribution; Cols. [8] and [9]: slopes of the injected electron distribution; Col. [10]: logarithm of the total energy in relativistic electrons, in erg; Col. [11]: logarithm of the total energy in the magnetic field, in erg; Col. [12]: bulk velocity of the lobe or the hot spot. The values of the powers and the energetics refer to each hot spot and lobe.
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