Table 1: Limits of the outflow speeds providing results in agreement with the observations and corresponding to different values of the ratio $(\alpha_{\!_\perp}/\alpha_{\!_{/\!/})}$ and to different ranges of the polar angle $\eta$ (weak inclinations, weak + medium inclinations and weak + medium+ strong inclinations, respectively). The outflow speed V is in km s^-1.
$\displaystyle\frac{\alpha_{\!_\perp}}{\alpha_{\!_{/\!/}}}$ $0\hbox{$^\circ$ }\le\eta\le20\hbox{$^\circ$ }$ $0\hbox{$^\circ$ }\le\eta\le30\hbox{$^\circ$ }$ $0\hbox{$^\circ$ }\le\eta\le90\hbox{$^\circ$ }$

1.0 $35\le V\le39$ $30\le V\le43$ $29\le V\le49$

1.5 $37\le V\le42$ $34\le V\le44$ $34\le V\le48$

2.0 $36\le V\le42$ $34\le V\le43$ $34\le V\le47$

2.5 $35\le V\le42$ $34\le V\le43$ $34\le V\le47$

3.0 $35\le V\le42$ $33\le V\le43$ $33\le V\le47$

**Table 1:** Limits of the outflow speeds providing results in agreement with the observations and corresponding to different values of the ratio $(\alpha_{\!_\perp}/\alpha_{\!_{/\!/})}$ and to different ranges of the polar angle $\eta$ (weak inclinations, weak + medium inclinations and weak + medium+ strong inclinations, respectively). The outflow speed V is in km s^-1.
$\displaystyle\frac{\alpha_{\!_\perp}}{\alpha_{\!_{/\!/}}}$	$0\hbox{$^\circ$ }\le\eta\le20\hbox{$^\circ$ }$	$0\hbox{$^\circ$ }\le\eta\le30\hbox{$^\circ$ }$	$0\hbox{$^\circ$ }\le\eta\le90\hbox{$^\circ$ }$
1.0	$35\le V\le39$	$30\le V\le43$	$29\le V\le49$
1.5	$37\le V\le42$	$34\le V\le44$	$34\le V\le48$
2.0	$36\le V\le42$	$34\le V\le43$	$34\le V\le47$
2.5	$35\le V\le42$	$34\le V\le43$	$34\le V\le47$
3.0	$35\le V\le42$	$33\le V\le43$	$33\le V\le47$

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