Table 2
Knot identification and properties.
ID | (∆α;∆δ) | δ | Size | V | ∆V | FP | tdyn | n | Mass |
---|---|---|---|---|---|---|---|---|---|
(″;″) | (″) | (″) | (km s−1) | (km s−1) | (K km s−1) | (yr) | (10−3 M⊙) | ||
North | |||||||||
N0a | (+0.1; +0.2) | 0.2 | 0.5 | +54.6 | 12(3) | 35(9) | 12 | 0 | 0.08 |
N0b | (+0.3; +2.0) | 2.0 | 0.9 | +39.8 | 18.3(0.4) | 430(9) | 154 | 3 | 0.3 |
N0 | (+0.6;+3.1) | 3.2 | 1.4 | +44.5 | 14.1(0.3) | 289(7) | 218 | 4 | 1.9 |
N1 | (+1.2; +4.7) | 4.9 | 1.8 | +54.6 | 18.7(0.7) | 351(13) | 291 | 5 | 3.6 |
N2 | (+2.3; +9.0) | 9.3 | 1.7 | +57.2 | 9.8(0.4) | 270(10) | 532 | 10 | 2.8 |
N3 | (+3.0; +10.4) | 10.8 | 3.0 | +58.2 | 8.5(0.4) | 261(12) | 609 | 11 | 7.8 |
N4 | (+4.6; +13.9) | 14.6 | 2.6 | +58.2 | 9.6(0.4) | 197(7) | 823 | 15 | 4.5 |
N5 | (+5.4; +16.9) | 17.8 | 2.0 | +60.2 | 12.5(0.9) | 189(14) | 975 | 18 | 2.5 |
N6 | (+6.6; +19.4) | 20.5 | 2.9 | +59.2 | 13.3(0.3) | 281(6) | 1139 | 21 | 7.6 |
N7 | (+8.3; +22.9) | 24.4 | 1.9 | +63.2 | 10.2(0.3) | 175(5) | 1283 | 23 | 2.1 |
NB | (+6.3; +34.3) | 34.9 | 4.0 | +83.3 | 13(2) | 70(9) | 1440 | 26 | 1.3 |
South | |||||||||
S0a | (−0.2; −0.8) | −0.8 | 0.9 | −62.5 | 23.6(0.5) | 389(9) | 60 | 1 | 0.7 |
S0b | (−0.8; −2.1) | −2.2 | 1.1 | −85.2 | 19(1) | 216(16) | 115 | 2 | 0.6 |
S1 | (−1.8; −5.4) | −5.7 | 1.3 | −113.5 | 20(2) | 147(11) | 218 | 4 | 0.5 |
S2 | (−3.3; −7.6) | −8.3 | 1.7 | −124.1 | 16.0(0.8) | 135(7) | 286 | 5 | 0.8 |
S3 | (−3.6; −9.3) | −9.9 | 1.8 | −124.1 | 14.7(0.7) | 144(7) | 341 | 6 | 0.9 |
S4 | (−4.9; −11.6) | −12.6 | 2.3 | −125.4 | 8.4(0.3) | 114(4) | 429 | 8 | 1.3 |
S5 | (−6.8; −15.9) | −17.3 | 2.0 | −126.1 | 8.4(0.3) | 124(5) | 585 | 11 | 1.1 |
S6 | (−8.8; −19.9) | −21.8 | 1.4 | −126.1 | 13.2(0.3) | 114(6) | 737 | 13 | 0.5 |
HH377 | (−9.5; −22.7) | −24.6 | 2.2 | −67.0 | 10.9(0.2) | 261(5) | 904 | 16 | 6.0 |
Notes. Coordinates, distance to Cep E-A along the jet main axis, size (beam deconvolved), radial velocity, line width, flux at the peak, dynamical age, period number, and mass of the knots in the jet. The dynamical ages for NB and HH377 were directly computed from the proper motions measured by Noriega-Crespo et al. (2014) after correcting for the difference of inclination angle induced by the jet precession.
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