Table 5: Model quantities temporally averaged at the outer boundary for Planck mean models. The numbers printed in subscript in the $T_{{\rm tot}}$ column indicates the upper limit in the time-interval used in the calculation of the average quantities of the corresponding model (cf. Sect. 4.2.1). The values shown in bold face for the PC models indicate that the value differ from the corresponding value given by HJLA98 (by $\ge$ $10\%$ ). For the PC models an "H'' in the last column indicates that the same model parameters were used in a model in HJLA98. See the caption of Table 4 for further details.
Model $\ensuremath{\langle\dot{M}\rangle}$ $\ensuremath{\langle u_{\infty}\rangle}$ $\ensuremath{\langle f_{{\rm cond}}\rangle}$ $\ensuremath{\langle\ensuremath{\rho_{{\rm d}}/\rho}\rangle}$ $\ensuremath{\langle\tau_{{\rm d}}\rangle}$ $\ensuremath{\langle v_{{\rm D}}\rangle}$ $T_{{\rm tot}}$ Type

$\ensuremath{[10^{-6}\,{M}_{\odot}/\mbox{yr}]}$ $[\ensuremath{\,\mbox{km}\,\mbox{s}^{-1}} ]$ $[\%]$ [10^-4] [10^-2] $[\ensuremath{\,\mbox{km}\,\mbox{s}^{-1}} ]$ [P]

( $\ensuremath{\sigma_{{\rm s}}}$ ) ( $\ensuremath{\sigma_{{\rm s}}}$ ) ( $\ensuremath{\sigma_{{\rm s}}}$ ) ( $\ensuremath{\sigma_{{\rm s}}}$ ) ( $\ensuremath{\sigma_{{\rm s}}}$ )

POSITION COUPLED MODELS (illustrated with the symbol " $\Box$ '')

P07FU6C14 ${\bf0.60}$ (0.069) 1.7 (0.10) ${\bf 55}$ (0.44) ${\bf 12}$ (0.10) 55 (9.9) 350 i H $_{\boxplus}$

P07FU4C18 0.21 (0.015) 6.4 (0.10) 13 (0.099) 5.6 (0.04) 6.5 (0.3) 330 i H $_{\boxplus}$

P10FU4C14 0.71 (0.12) 2.2 (0.18) ${\bf 23}$ (0.22) 5.2 (0.05) 23 (1.8) 480 i H $_{\boxplus}$

P10FU2C18 0.18 (0.019) 8.6 (0.14) 4.6 (0.18) 2.1 (0.08) 1.6 (0.1) ₁₄₀430 i H $_{\boxplus}$

P10FU4C18 ${\bf 1.1}$ (0.49) 14 (0.77) ${\bf 16}$ (2.6) 7.2 (1.2) 7.3 (2.4) ₁₅₀410 i H

P10FU6C16 2.7 (1.4) 13 (1.1) 27 (4.0) 9.2 (1.3) 22 (11) ₁₈₀390 i

P10FU6C18 ${\bf 2.0}$ (0.61) 16 (0.48) 21 (1.8) 9.3 (0.83) 15 (4.9) ₁₂₀390 i H

P13FU6C14 ${\bf 4.7}$ (2.3) ${\bf 10}$ (0.76) 26 (2.7) 6.0 (0.61) 34 (16) ₁₁₀520 i H

P13FU4C16 2.3 (0.39) 12 (0.30) 15 (1.1) 5.2 (0.39) 8.6 (1.7) ₁₄₀440 i

P13FU6C16 3.9 (0.51) 14 (0.23) 21 (9.6) 7.3 (0.33) 19 (2.0) ₈₀390 i

DRIFT MODELS (illustrated with the symbol " $\ensuremath{\textcolor{mygray}{\blacksquare}}$ '')

P07FU6C14 -- --

P07FU4C18 -- --

P10FU4C14 -- --

P10FU2C18 -- t

P10FU4C18 0.82 (0.12) 11 (0.24) 12 (5.3) 5.4 (2.9) 3.3 (0.5) 4.5 93 i $\ensuremath {\triangledown }$

P10FU6C16 1.1 (1.0) 8.5 (1.1) 19 (18) 7.9 (13) 8.7 (5.6) 7.2 110 i $\ensuremath {\triangledown }$

P10FU6C18 2.2 (2.8) 22 (2.3) 27 (34) 39 (210) 25 (10) 16 65 2q

P13FU6C14 1.9 (2.0) 7.5 (1.5) 24 (24) 8.4 (30) 17 (16) 10 130 i $\ensuremath {\triangledown }$

P13FU4C16 2.5 (0.69) 13 (0.43) 23 (24) 11 (18) 8.7 (1.5) 4.9 130 2q

P13FU6C16 4.1 (4.0) 14 (1.1) 19 (21) 11 (39) 16 (4.1) 4.0 130 i

**Table 5:** Model quantities temporally averaged at the outer boundary for Planck mean models. The numbers printed in subscript in the $T_{{\rm tot}}$ column indicates the upper limit in the time-interval used in the calculation of the average quantities of the corresponding model (cf. Sect. 4.2.1). The values shown in bold face for the PC models indicate that the value differ from the corresponding value given by HJLA98 (by $\ge$ $10\%$ ). For the PC models an "H'' in the last column indicates that the same model parameters were used in a model in HJLA98. See the caption of Table 4 for further details.
Model	$\ensuremath{\langle\dot{M}\rangle}$		$\ensuremath{\langle u_{\infty}\rangle}$		$\ensuremath{\langle f_{{\rm cond}}\rangle}$		$\ensuremath{\langle\ensuremath{\rho_{{\rm d}}/\rho}\rangle}$		$\ensuremath{\langle\tau_{{\rm d}}\rangle}$	$\ensuremath{\langle v_{{\rm D}}\rangle}$	$T_{{\rm tot}}$	Type
$\ensuremath{[10^{-6}\,{M}_{\odot}/\mbox{yr}]}$		$[\ensuremath{\,\mbox{km}\,\mbox{s}^{-1}} ]$		$[\%]$		[10^-4]		[10^-2]	$[\ensuremath{\,\mbox{km}\,\mbox{s}^{-1}} ]$	[P]
		( $\ensuremath{\sigma_{{\rm s}}}$ )			( $\ensuremath{\sigma_{{\rm s}}}$ )			( $\ensuremath{\sigma_{{\rm s}}}$ )			( $\ensuremath{\sigma_{{\rm s}}}$ )			( $\ensuremath{\sigma_{{\rm s}}}$ )
POSITION COUPLED MODELS	(illustrated with the symbol " $\Box$ '')
P07FU6C14	${\bf0.60}$	(0.069)		1.7	(0.10)		${\bf 55}$	(0.44)		${\bf 12}$	(0.10)		55	(9.9)		350	i	H $_{\boxplus}$
P07FU4C18	0.21	(0.015)		6.4	(0.10)		13	(0.099)		5.6	(0.04)		6.5	(0.3)		330	i	H $_{\boxplus}$
P10FU4C14	0.71	(0.12)		2.2	(0.18)		${\bf 23}$	(0.22)		5.2	(0.05)		23	(1.8)		480	i	H $_{\boxplus}$
P10FU2C18	0.18	(0.019)		8.6	(0.14)		4.6	(0.18)		2.1	(0.08)		1.6	(0.1)		₁₄₀430	i	H $_{\boxplus}$
P10FU4C18	${\bf 1.1}$	(0.49)		14	(0.77)		${\bf 16}$	(2.6)		7.2	(1.2)		7.3	(2.4)		₁₅₀410	i	H
P10FU6C16	2.7	(1.4)		13	(1.1)		27	(4.0)		9.2	(1.3)		22	(11)		₁₈₀390	i
P10FU6C18	${\bf 2.0}$	(0.61)		16	(0.48)		21	(1.8)		9.3	(0.83)		15	(4.9)		₁₂₀390	i	H
P13FU6C14	${\bf 4.7}$	(2.3)		${\bf 10}$	(0.76)		26	(2.7)		6.0	(0.61)		34	(16)		₁₁₀520	i	H
P13FU4C16	2.3	(0.39)		12	(0.30)		15	(1.1)		5.2	(0.39)		8.6	(1.7)		₁₄₀440	i
P13FU6C16	3.9	(0.51)		14	(0.23)		21	(9.6)		7.3	(0.33)		19	(2.0)		₈₀390	i
DRIFT MODELS	(illustrated with the symbol " $\ensuremath{\textcolor{mygray}{\blacksquare}}$ '')
P07FU6C14	--															--
P07FU4C18	--															--
P10FU4C14	--															--
P10FU2C18	--															t
P10FU4C18	0.82	(0.12)		11	(0.24)		12	(5.3)		5.4	(2.9)		3.3	(0.5)	4.5	93	i	$\ensuremath {\triangledown }$
P10FU6C16	1.1	(1.0)		8.5	(1.1)		19	(18)		7.9	(13)		8.7	(5.6)	7.2	110	i	$\ensuremath {\triangledown }$
P10FU6C18	2.2	(2.8)		22	(2.3)		27	(34)		39	(210)		25	(10)	16	65	2q
P13FU6C14	1.9	(2.0)		7.5	(1.5)		24	(24)		8.4	(30)		17	(16)	10	130	i	$\ensuremath {\triangledown }$
P13FU4C16	2.5	(0.69)		13	(0.43)		23	(24)		11	(18)		8.7	(1.5)	4.9	130	2q
P13FU6C16	4.1	(4.0)		14	(1.1)		19	(21)		11	(39)		16	(4.1)	4.0	130	i

Source LaTeX | All tables | In the text