Table 1
Overview of simulations performed.
Run label | Comparison | τ | Radiation transport | (ΔT)max [%] |
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Pa-1e-1-grayRT+FLD | Pascucci et al. | 10-1 | gray RT + FLD | 3 |
Pa-1e-1-freqRT+FLD | freq. RT + FLD | 3 | ||
Pa-1e-1-FLD | FLD | 55 | ||
Pa-1e-1-MC | Monte-Carlo | 1 | ||
|
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Pa-1e+2-grayRT+FLD | Pascucci et al. | 10+ 2 | gray RT + FLD | 54 |
Pa-1e+2-freqRT+FLD | freq. RT + FLD | 16 | ||
Pa-1e+2-FLD | FLD | 42 | ||
Pa-1e+2-MC | Monte-Carlo | 14 | ||
|
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Pi-1e+3-grayRT+FLD | Pinte et al. | 10+ 3 | gray RT + FLD | 48 |
Pi-1e+3-freqRT+FLD | freq. RT + FLD | 48 | ||
Pi-1e+3-FLD | FLD | 282 | ||
Pi-1e+3-MC | Monte-Carlo | 19 | ||
|
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Pi-1e+4-grayRT+FLD | Pinte et al. | 10+ 4 | gray RT + FLD | 46 |
Pi-1e+4-freqRT+FLD | freq. RT + FLD | 46 | ||
Pi-1e+4-FLD | FLD | 284 | ||
Pi-1e+4-MC | Monte-Carlo | – | ||
|
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Pi-1e+6-grayRT+FLD | Pinte et al. | 10+6 | gray RT + FLD | 37 |
Pi-1e+6-freqRT+FLD | freq. RT + FLD | 37 | ||
Pi-1e+6-FLD | FLD | 289 | ||
Pi-1e+6-MC | Monte-Carlo | 42 |
Notes.The columns denote the run label, the reference to the original benchmark test (either Pascucci et al. 2004 or Pinte et al. 2009), the optical depth of the disk’s midplane (either τ550 nm or τ810 nm, respectively), the radiation transport method used in the simulation, and the resulting temperature deviation in percent. The deviations are computed with respect to the Monte-Carlo solution by RADMC. The temperature deviations given for the Monte-Carlo runs are taken from Pascucci et al. (2004), Figs. 4 and 5, or Pinte et al. (2009), Fig. 10, with respect to the deviation to the other radiation transport codes participating in the original benchmark tests. A visualization of the final maximum temperature deviations as a function of optical depth is given in Fig. 8.
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