About: About blog posts
Browse by time:
- July 2022 (1)
- May 2022 (1)
- April 2022 (3)
- March 2022 (2)
- February 2022 (3)
- January 2022 (2)
- December 2021 (4)
- November 2021 (2)
- September 2021 (6)
- August 2021 (1)
- July 2021 (7)
- June 2021 (2)
- May 2021 (5)
- April 2021 (3)
- March 2021 (7)
- February 2021 (5)
- January 2021 (4)
- December 2020 (7)
- November 2020 (12)
- October 2020 (13)
- September 2020 (11)
- August 2020 (14)
- July 2020 (17)
- June 2020 (18)
- May 2020 (12)
- April 2020 (14)
- March 2020 (15)
- February 2020 (13)
- January 2020 (7)
- December 2019 (6)
- November 2019 (11)
- October 2019 (15)
- September 2019 (14)
- August 2019 (4)
- July 2019 (10)
- June 2019 (5)
- May 2019 (8)
- April 2019 (5)
- March 2019 (13)
- February 2019 (5)
- January 2019 (10)
- December 2018 (5)
- November 2018 (9)
- October 2018 (13)
- September 2018 (12)
- August 2018 (6)
- July 2018 (5)
- June 2018 (9)
- May 2018 (5)
- April 2018 (9)
- March 2018 (14)
- February 2018 (16)
- January 2018 (7)
- December 2017 (5)
- November 2017 (8)
- October 2017 (11)
- September 2017 (10)
- August 2017 (9)
- June 2017 (16)
- May 2017 (14)
- April 2017 (6)
- March 2017 (6)
- February 2017 (4)
- January 2017 (11)
- December 2016 (5)
- November 2016 (13)
- October 2016 (7)
- September 2016 (11)
- August 2016 (6)
- July 2016 (19)
- June 2016 (12)
- May 2016 (11)
- April 2016 (11)
- March 2016 (13)
- February 2016 (17)
- January 2016 (10)
- December 2015 (5)
- November 2015 (15)
- October 2015 (19)
- September 2015 (18)
- August 2015 (23)
- July 2015 (32)
- June 2015 (17)
- May 2015 (23)
- April 2015 (28)
- March 2015 (23)
- February 2015 (19)
- January 2015 (17)
- December 2014 (26)
- November 2014 (42)
- October 2014 (33)
- September 2014 (30)
- August 2014 (16)
- July 2014 (27)
- June 2014 (37)
- May 2014 (19)
- April 2014 (14)
- March 2014 (35)
- February 2014 (30)
- January 2014 (28)
- December 2013 (25)
- November 2013 (30)
- October 2013 (41)
- September 2013 (48)
- August 2013 (36)
- July 2013 (44)
- June 2013 (39)
- May 2013 (29)
- April 2013 (36)
- March 2013 (35)
- February 2013 (31)
- January 2013 (48)
- December 2012 (20)
- November 2012 (29)
- October 2012 (48)
- September 2012 (30)
- August 2012 (16)
- July 2012 (32)
- June 2012 (27)
- May 2012 (26)
- April 2012 (25)
- March 2012 (30)
- February 2012 (35)
- January 2012 (25)
- December 2011 (23)
- November 2011 (41)
- October 2011 (31)
- September 2011 (29)
- August 2011 (23)
- July 2011 (24)
- June 2011 (18)
- May 2011 (3)
Browse by author:
- rss Bo Peng (1)
- rss Yisheng (26)
- rss aanand6 (20)
- rss adebrech (151)
- rss afrank (30)
- rss aliao (6)
- rss alipnicky (2)
- rss amyzou (54)
- rss aquillen (1)
- rss blin (18)
- rss bliu (270)
- rss bpeng6 (7)
- rss brockjw (7)
- rss bshroyer (6)
- rss ceh5286 (2)
- rss dnp19 (7)
- rss ehansen (290)
- rss elambrid (12)
- rss erica (280)
- rss esavitch (43)
- rss fschmidt (35)
- rss gguidarelli (4)
- rss idilernia (35)
- rss johannjc (245)
- rss lchamandy (104)
- rss likuntian (5)
- rss lsabin (2)
- rss madams (61)
- rss martinhe (76)
- rss mblank (30)
- rss mccann (3)
- rss mehr (16)
- rss noyesma (6)
- rss rmarkwic (20)
- rss shuleli (146)
- rss smurugan (24)
- rss yirak (4)
- rss ytlee (1)
- rss zchen (165)
Browse by category:
- rss Accretion (1)
- rss Bonner-Ebert (1)
- rss Bvn (1)
- rss CollidingFlows (27)
- rss Disks (1)
- rss FieldLoop (1)
- rss Magnetic-tower (1)
- rss Meeting-outline (1)
- rss RAID (1)
- rss RT (1)
- rss Resistive_MHD (1)
- rss Test (1)
- rss alfalfa (3)
- rss animation (1)
- rss bamboo (2)
- rss bipolar (1)
- rss bluehive2 (1)
- rss bluestreak (3)
- rss cameraobjects (6)
- rss clover (1)
- rss clump (4)
- rss cooling (1)
- rss data-management (4)
- rss development (1)
- rss disks (3)
- rss documentation (15)
- rss dust (32)
- rss gpu (1)
- rss grass (2)
- rss hydrostatic (1)
- rss mGlobal (1)
- rss magnetic-field (1)
- rss mass (2)
- rss movies (1)
- rss mx (1)
- rss nebula (1)
- rss notification (1)
- rss others-research (1)
- rss outreach (1)
- rss parameter (1)
- rss plugins (1)
- rss query (1)
- rss scaling (1)
- rss script (1)
- rss shape (3)
- rss sinks (1)
- rss stampede (2)
- rss streamlines (2)
- rss study (1)
- rss tasks (7)
- rss testing (6)
- rss ticketchart (1)
- rss tutorial (1)
- rss visit (4)
- rss visualization (3)
- rss vnc (1)
- rss vpn (3)
- rss w00t (1)
- rss wind (4)
- rss wind-capture (1)
Timescale for the inwards migration of the circumnuclear disk's inner rim -- Marvin
The central stellar cluster's wind extracts angular momentum from the circumnuclear disk's inner rim, therefore the inner rim migrates
inwards. In the following I derive the timescale for the inwards migration of the CND's inner rim. Please see our paper draft for more
details.
We assume that angular momentum is extracted from a ring of radius s and radial extension \Delta l, therefore it has the mass M_{\text{D}} = 2 \pi \Sigma s \Delta l. This ring has a total angular momentum of J=j M_{\text{D}} with specific angular momentum j.
After a time dt the wind adds the mass f \dot{M} dt to the ring, where \dot{M} is the wind's outflow rate and f is the
fraction of the wind that interacts with the disk. Thus the ring has the mass M_{D} + f \dot{M} dt and the specific angular momentum
j' = \frac{J}{M_{D} + f \dot{M} dt} = \frac{j}{1+\frac{f \dot{M}}{M_{\text{D}}} dt}.
Furthermore the ring moves to s-ds, and because j = \sqrt{GMs} and j' = \sqrt{GM(s-ds)} we get
dt = \frac{M_{\text{D}}}{f \dot{M}} \left( \sqrt{\frac{s}{s-ds}} - 1\right) = \frac{M_{\text{D}}}{f \dot{M}} \frac{ds}{2 s}
where I used a taylor expansion in the last step.
Using M_{\text{D}} = 2 \pi \Sigma s \Delta l, f=\frac{h}{2s} and integrating this equation gives the time the inner rim needs to
migrate inwards:
\tau = \int dt = \int \frac{M_{\text{D}}}{f \dot{M}} \frac{ds}{2 s} = \frac{2 \pi \Sigma \Delta l}{h \dot{M}} \int s ds = \frac{\pi \Sigma \Delta l}{h \dot{M}} \left( s_0^2 - s_\text{i}^2\right),
where s_0 is the disk's initial inner rim and s_\text{i} the location of the rim after inwards migration.
In our simulations s_\text{i} = 0.5 \text{pc}, for s_0 = 1 \text{pc} we get \tau = 22 \cdot 10^4 \text{yrs}, for s_0 = 2 \text{pc} we get \tau = 112 \cdot 10^4 \text{yrs}. The actual time the inner rim needs to move inwards (as observed in the simulations) is 20 \cdot 10^4 \text{yrs} and 65 \cdot 10^4 \text{yrs}, respectively. For the s_0 = 1 \text{pc} simulation this is pretty close, for the s_0 = 2 \text{pc} simulation the deviation is less than a factor of two, which I find an acceptable deviation considering that the above mentioned derivation is only an order of magnitude estimate.
- Posted: 9 years ago
- Author: Marvin Blank
- Categories: (none)
Comments
No comments.