Fig. 10

Schematic representation of the 4 scenarii discussed for the origin of the wide-angle rovibrational H2 emission in DG Tau. The layer of emitting H2 at 2000 K is drawn in solid red. Wide-angle wind streamlines are shown as dashed (black if atomic, red if molecular) lines. The velocity of the emitting gas perpendicular and parallel to the cavity wall (V⊥ and V∥), and the shock speed Vs and preshock density nH when applicable, are also listed as a function of the expansion proper motion of the cavity Vexp, the velocity of the H2 1–0 S(1) emitting layer in the frame of the shock wave, Vn(H2), and the initial velocity of the ambient gas (Va) or molecular wind (Vw).
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