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Table 2

Parameters of pulsed conical high-density jet simulations with the resulting opening angles and full widths (Fig. 3).

Fixed parameters
Mean jet velocity v0 = 120 km s–1
Jet density variation
Core density profile
Jet temperature Tj = 100K
Ambient core temperature Ta = 100K
Radiative cooling function Λ(100 K ≤ T < 104 K) from Dalgarno & McCray (1972)
Λ(T ≥ 104 K) from Schure et al. (2009)
Simulation domain (R, z) = (7.0 × 1016 cm, 1.9 × 1017 cm) = (4679 au, 12700 au)
Number of cells nR × nz = 56 × 152 for the full grid at AMR level 1
Maximum resolution 7.8 × 1013 cm = 5.2 au at AMR level 5
Snapshot age 700 yr
Parameter Reference model Modified Modified α800(b) W800 (b) W12700 (d)
H_REF parameter(α) Model name (°) (1016 cm) (1016 cm)
Core base density pα0 1.6 × 10–18gcm–3 1.6 × 10–20gcm–3 H_DENSA 112 3.5 13.8
Jet semi opening angle θj H_THETA 95 2.6 10.5
Jet base initial density(e) pj0 1.8 × 10–17gcm–3 1.8 × 10–15gcm–3 H_DENSJ 86 2.2 8.4
Semi-amplitude ΔV 60kms 1 90kms 1 H_VARAMP 91 2.4 8.0
Jet variability period P 115 yr 300 yr H_PER 90 2.4 7.4
Jet variability profile h(t) H_SAWT 86 2.2 7.2
Jet radius Rj 7.5 × 1014 cm 3.0 × 1014cm H_RAD 84 2.2 6.9

Notes. (α)In each modified model, only one parameter at a time is changed with respect to the reference model. (b)Shell full opening angle at z = 800 au. We obtain α800 = 88° for the reference model. (c)Full shell width at z = 800 au. We obtain W800 = 2.3 × 1016cm for the reference model. (d)Full shell width at z = 12700 au (top of the grid). We obtain W12700 = 7.6 × 1016cm for the reference model. (e)High jet density case, yielding a one-sided mass-flux M/yr for the reference values of θj and Rj.

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