Changes between Version 1 and Version 2 of PlanetaryAtmospheres


Ignore:
Timestamp:
09/18/13 11:25:00 (11 years ago)
Author:
Jonathan
Comment:

Legend:

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  • PlanetaryAtmospheres

    v1 v2  
    1212 * Non rotating
    1313
     14
    1415Dobbs Dixon '08
    1516Domain
    1617 * Radius goes from 7.95e9 cm to 8.65e9 cm (1.06 -1.2 R_j)
    17  * Single Temperature
     18 * Single Temperature (assumes Planck opacity is >> )
    1819 * They use [[latex($\lambda = \frac{2+R}{6+3R+R^2}$)]] instead of [[latex($\frac{1}{R}\left ( \coth{R}-\frac{1}{R} \right )$)]]
    1920[[Image(Limiter.png, width=400)]]
     21 * [[latex($\gamma=7/5$)]]
     22 * [[latex($\chi=2.3$)]]
     23 * Roseland opacities found using Pollack et al 1985 for low T with Alexander & Ferguson for high T
     24 * Initial Density and Temperature profiles taken from 1D model (B1 of Bodenheimer 2001) (.63 M,,J,, for 4.5 Gyr with a 1200 degree outer boundary)
     25 * Outer boundary set to T= max(1200 K * [cos(phi)*cos(theta)]^(1/4), 100 K)
    2026
     27* Non rotating model - no coriolis or centrifugal forces... - no winds
     28* Rotating model - 3 days
     29
     30
     31
     32Dobbs Dixon'10
     33
     34* Added viscosity
     35* Added stellar heating using optical depth and high energy planck opacity
     36
     37
     38Current differences between Ian's code and AstroBEAR
     39* AstroBEAR folds in gas/radiation energy coupling into implicit solve...  Hypre has both kappa,,R,, and kappa,,P,, terms - with sub-cycling for changes in source function.
     40* AstroBEAR also assumes 'kappa' is constant over implicit update...  assumes [[latex($\frac{\partial \kappa}{\partial T} = 0$)]]... 
     41* No Kappa_A terms (stellar heating) in AstroBEAR
     42* Need to develop communication patterns for calculating optical depth from star to get heating term correct.  Could use initial spherical profile to estimate optical depth as a function of position?  Not sure how this is done in Ian's code
     43* Viscosity may need to be incorporated later...  Shule is developing this.
     44
     45* Second AMR implicit solve may need to be added later (ie Howell and Greenough 2002)
    2146
    2247== Run 1 ==