Table 2. Open in new tab Radiation and...

Quantity

Model-110

Model-130

Model-140

Model-180

Model-380

BH accretion rate

|$\dot{M}_{\rm BH}$| [L_Edd/c²]

∼110

∼130

∼140

∼180

∼380

Mass injection rate

|$\dot{M}_{\rm inj}$| [L_Edd/c²]

350

500

700

2000

Outflow rate at r_out

|$\dot{M}_{\rm outflow}$| [L_Edd/c²]

∼10

∼13

∼16

∼24

∼230

Failed outflow rate at r_out

|$\dot{M}_{\rm failed}$| [L_Edd/c²]

∼4

∼8

∼15

∼100

Quasi steady-state radius

r_qss [r_S]

∼500

∼400

∼600

∼1000

Pure outflow: inner radius

|$R_{\rm pure}^{\rm in}$| [r_S]

∼40

Pure outflow: outer radius

|$R_{\rm pure}^{\rm out}$| [r_S]

∼170

∼110

∼130

∼180

∼480

Failed outflow: outer radius

|$R_{\rm failed}^{\rm out}$| [r_S]

∼170

∼180

∼210

∼820

Photon trapping radius

R_trap [r_S]

∼300

∼330

∼350

∼450

∼1100

X-ray luminosity

L_X [L_Edd]

∼2.0

∼2.1

∼2.3

∼2.4

∼2.7

Mechanical luminosity

L_mech [L_Edd]

∼0.07

∼0.09

∼0.11

∼0.16

∼0.61

Isotropic X-ray luminosity

|$L_{\rm X}^{\rm ISO} (\theta )$| [L_Edd]

2.0–4.0

2.3–4.4

2.4–4.8

2.3–4.6

2.1–11

Isotropic mechanical luminosity

|$L_{\rm mech}^{\rm ISO}(\theta )$| [L_Edd]

0.04–0.18

0.02–0.35

0.03–0.60

0.04–1.4

1.0–8.0

Luminosity ratio

|$L_{\rm mech}/L_{\rm X}^{\rm ISO}(\theta )$|

0.02–0.04

0.02–0.05

0.04–0.07

0.06–0.29

Table 2.

Open in new tab

Radiation and outflow properties.*

Quantity		Model-110	Model-130	Model-140	Model-180	Model-380
BH accretion rate	\|$\dot{M}_{\rm BH}$\| [L_Edd/c²]	∼110	∼130	∼140	∼180	∼380
Mass injection rate	\|$\dot{M}_{\rm inj}$\| [L_Edd/c²]	350	500	700	700	2000
Outflow rate at r_out	\|$\dot{M}_{\rm outflow}$\| [L_Edd/c²]	∼10	∼13	∼16	∼24	∼230
Failed outflow rate at r_out	\|$\dot{M}_{\rm failed}$\| [L_Edd/c²]	0	∼4	∼8	∼15	∼100
Quasi steady-state radius	r_qss [r_S]	∼500	∼400	∼400	∼600	∼1000
Pure outflow: inner radius	\|$R_{\rm pure}^{\rm in}$\| [r_S]	∼40	∼40	∼40	∼40	∼40
Pure outflow: outer radius	\|$R_{\rm pure}^{\rm out}$\| [r_S]	∼170	∼110	∼130	∼180	∼480
Failed outflow: outer radius	\|$R_{\rm failed}^{\rm out}$\| [r_S]	∼170	∼180	∼210	∼210	∼820
Photon trapping radius	R_trap [r_S]	∼300	∼330	∼350	∼450	∼1100
X-ray luminosity	L_X [L_Edd]	∼2.0	∼2.1	∼2.3	∼2.4	∼2.7
Mechanical luminosity	L_mech [L_Edd]	∼0.07	∼0.09	∼0.11	∼0.16	∼0.61
Isotropic X-ray luminosity	\|$L_{\rm X}^{\rm ISO} (\theta )$\| [L_Edd]	2.0–4.0	2.3–4.4	2.4–4.8	2.3–4.6	2.1–11
Isotropic mechanical luminosity	\|$L_{\rm mech}^{\rm ISO}(\theta )$\| [L_Edd]	0.04–0.18	0.02–0.35	0.03–0.60	0.04–1.4	1.0–8.0
Luminosity ratio	\|$L_{\rm mech}/L_{\rm X}^{\rm ISO}(\theta )$\|	0.02–0.04	0.02–0.04	0.02–0.05	0.04–0.07	0.06–0.29

Quantity		Model-110	Model-130	Model-140	Model-180	Model-380
BH accretion rate	\|$\dot{M}_{\rm BH}$\| [L_Edd/c²]	∼110	∼130	∼140	∼180	∼380
Mass injection rate	\|$\dot{M}_{\rm inj}$\| [L_Edd/c²]	350	500	700	700	2000
Outflow rate at r_out	\|$\dot{M}_{\rm outflow}$\| [L_Edd/c²]	∼10	∼13	∼16	∼24	∼230
Failed outflow rate at r_out	\|$\dot{M}_{\rm failed}$\| [L_Edd/c²]	0	∼4	∼8	∼15	∼100
Quasi steady-state radius	r_qss [r_S]	∼500	∼400	∼400	∼600	∼1000
Pure outflow: inner radius	\|$R_{\rm pure}^{\rm in}$\| [r_S]	∼40	∼40	∼40	∼40	∼40
Pure outflow: outer radius	\|$R_{\rm pure}^{\rm out}$\| [r_S]	∼170	∼110	∼130	∼180	∼480
Failed outflow: outer radius	\|$R_{\rm failed}^{\rm out}$\| [r_S]	∼170	∼180	∼210	∼210	∼820
Photon trapping radius	R_trap [r_S]	∼300	∼330	∼350	∼450	∼1100
X-ray luminosity	L_X [L_Edd]	∼2.0	∼2.1	∼2.3	∼2.4	∼2.7
Mechanical luminosity	L_mech [L_Edd]	∼0.07	∼0.09	∼0.11	∼0.16	∼0.61
Isotropic X-ray luminosity	\|$L_{\rm X}^{\rm ISO} (\theta )$\| [L_Edd]	2.0–4.0	2.3–4.4	2.4–4.8	2.3–4.6	2.1–11
Isotropic mechanical luminosity	\|$L_{\rm mech}^{\rm ISO}(\theta )$\| [L_Edd]	0.04–0.18	0.02–0.35	0.03–0.60	0.04–1.4	1.0–8.0
Luminosity ratio	\|$L_{\rm mech}/L_{\rm X}^{\rm ISO}(\theta )$\|	0.02–0.04	0.02–0.04	0.02–0.05	0.04–0.07	0.06–0.29

Note again that the results of Model-180 are taken from K21. In the calculations of isotropic luminosities (see the last three rows), we take an angular range of 0° < θ < θ_surf.

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