Fig. 6

Various variables along a flow line anchored at 1 AU, for the dense MHD disk wind solution and three typical classes of stars: class 0 (M⋆ = 0.1 M⊙, Ṁacc = 5 × 10-6 M⊙ yr-1; dotted blue curves), class I (M⋆ = 0.5 M⊙, Ṁacc = 10-6 M⊙ yr-1; solid red curves) and active class II (M⋆ = 0.5 M⊙, Ṁacc = 10-7 M⊙ yr-1; dashed green curves). a) The gas temperature T; b) the number density of hydrogen nuclei nH; c) the visual extinction AV to the star, in magnitudes; d) the poloidal components of the bulk flow speed v (smooth top curves) and calculated drift speed vin (lower 3 curves); Note that the Class II and Class I have the same M⋆, hence the same bulk flow speed for r0 = 1 AU; e) the X-ray H2 ionization rate per molecule ; f) the effective radiation field in Draine units χexp − 3AV (attenuation factor appropriate for carbon photoionisation); g) the fractional abundance of ions; h) the fractional abundance of H2 (upper limit in the Class II model, see Sect. 3.1.3); i) the fractional abundance of CO (upper limits in the Class I/II models, see Sect. 3.1.4).
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