Table 2.

HH 900 proper motions.

ObjectδxδyvTavRbvelocitycαaged
(mas)(mas)(km s−1)(km s−1)(km s−1)(degrees)(yr)
HH 900 A43 (1)−24 (0.4)60 (1)60 (1)3523 (115)
HH 900 B31 (1)−2 (2)37 (2)37 (2)5364 (307)
HH 900 C55 (0.1)−11 (1)68 (1)68 (2)2803 (87)
HH 900 D74 (1)−31 (4)97 (3)97 (3)859 (34)
HH 900 E76 (2)−25 (1)97 (3)97 (3)682 (25)
HH 900 F−60 (1)42 (2)89 (2)−16 (4)90 (5)−10 (0.3)691 (24)
HH 900 G−77 (1)39 (1)104 (2)−7 (10)105 (10)−4 (0.1)746 (24)
HH 900 H−40 (3)14 (1)51 (3)51 (3)5379 (365)
HH 900 I−42 (1)28 (1)61 (2)61 (2)4664 (174)
PCYC 838−3 (1)2 (1)4 (1)4 (1)11 201 (3126)
PCYC 8425 (3)−11.8 (0.4)15 (2)15 (2)1393 (140)
ObjectδxδyvTavRbvelocitycαaged
(mas)(mas)(km s−1)(km s−1)(km s−1)(degrees)(yr)
HH 900 A43 (1)−24 (0.4)60 (1)60 (1)3523 (115)
HH 900 B31 (1)−2 (2)37 (2)37 (2)5364 (307)
HH 900 C55 (0.1)−11 (1)68 (1)68 (2)2803 (87)
HH 900 D74 (1)−31 (4)97 (3)97 (3)859 (34)
HH 900 E76 (2)−25 (1)97 (3)97 (3)682 (25)
HH 900 F−60 (1)42 (2)89 (2)−16 (4)90 (5)−10 (0.3)691 (24)
HH 900 G−77 (1)39 (1)104 (2)−7 (10)105 (10)−4 (0.1)746 (24)
HH 900 H−40 (3)14 (1)51 (3)51 (3)5379 (365)
HH 900 I−42 (1)28 (1)61 (2)61 (2)4664 (174)
PCYC 838−3 (1)2 (1)4 (1)4 (1)11 201 (3126)
PCYC 8425 (3)−11.8 (0.4)15 (2)15 (2)1393 (140)

Notes. Proper motions measured for the YSOs and the knots marked in Fig. 8.

Uncertainties are listed in parentheses alongside the best-fitting value.

aThe transverse velocity, assuming a distance of 2.3 kpc.

bThe radial velocity measured from spectra.

cThe total velocity, assuming the average inclination when a radial velocity is not measured directly.

dTime for the object to reach its current location at the measured velocity, assuming ballistic motion.

Table 2.

HH 900 proper motions.

ObjectδxδyvTavRbvelocitycαaged
(mas)(mas)(km s−1)(km s−1)(km s−1)(degrees)(yr)
HH 900 A43 (1)−24 (0.4)60 (1)60 (1)3523 (115)
HH 900 B31 (1)−2 (2)37 (2)37 (2)5364 (307)
HH 900 C55 (0.1)−11 (1)68 (1)68 (2)2803 (87)
HH 900 D74 (1)−31 (4)97 (3)97 (3)859 (34)
HH 900 E76 (2)−25 (1)97 (3)97 (3)682 (25)
HH 900 F−60 (1)42 (2)89 (2)−16 (4)90 (5)−10 (0.3)691 (24)
HH 900 G−77 (1)39 (1)104 (2)−7 (10)105 (10)−4 (0.1)746 (24)
HH 900 H−40 (3)14 (1)51 (3)51 (3)5379 (365)
HH 900 I−42 (1)28 (1)61 (2)61 (2)4664 (174)
PCYC 838−3 (1)2 (1)4 (1)4 (1)11 201 (3126)
PCYC 8425 (3)−11.8 (0.4)15 (2)15 (2)1393 (140)
ObjectδxδyvTavRbvelocitycαaged
(mas)(mas)(km s−1)(km s−1)(km s−1)(degrees)(yr)
HH 900 A43 (1)−24 (0.4)60 (1)60 (1)3523 (115)
HH 900 B31 (1)−2 (2)37 (2)37 (2)5364 (307)
HH 900 C55 (0.1)−11 (1)68 (1)68 (2)2803 (87)
HH 900 D74 (1)−31 (4)97 (3)97 (3)859 (34)
HH 900 E76 (2)−25 (1)97 (3)97 (3)682 (25)
HH 900 F−60 (1)42 (2)89 (2)−16 (4)90 (5)−10 (0.3)691 (24)
HH 900 G−77 (1)39 (1)104 (2)−7 (10)105 (10)−4 (0.1)746 (24)
HH 900 H−40 (3)14 (1)51 (3)51 (3)5379 (365)
HH 900 I−42 (1)28 (1)61 (2)61 (2)4664 (174)
PCYC 838−3 (1)2 (1)4 (1)4 (1)11 201 (3126)
PCYC 8425 (3)−11.8 (0.4)15 (2)15 (2)1393 (140)

Notes. Proper motions measured for the YSOs and the knots marked in Fig. 8.

Uncertainties are listed in parentheses alongside the best-fitting value.

aThe transverse velocity, assuming a distance of 2.3 kpc.

bThe radial velocity measured from spectra.

cThe total velocity, assuming the average inclination when a radial velocity is not measured directly.

dTime for the object to reach its current location at the measured velocity, assuming ballistic motion.

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