3D Dust Modeling of Circumplanetary Disks

3D Dust Modeling of Circumplanetary Disks

3D dust modeling of circumplanetary disks Mark van der Keijl July 11, 2019 Second examiner: Supervisors: MSc Kateryna Frantseva Prof. Dr. Inga Kamp Dr. Christian Rab MSc Nick Oberg 1/21 Motivation I Giant planets in solar system have moons I These moons are regular satellites I Possibly formed in circumplanetary disks (CPD) I Candidates have only recently been observed (Credit: The Graduate University for Advanced Studies/NAOJ) 2/21 Formation I Planets form in protoplanetary disks via agglomeration I Gaps form due to planet-disk interactions I Planet forms circumplanetary disk in gap due to non-vanishing gas accretion Observation of AS 209 (Credit: Zhang et al., 2018) 3/21 Scientific goal I Study impact of star on temperature and radiation field of circumplanetary disk I Important for chemistry and thus observations I Also study impact of circumplanetary disk/planet on protoplanetary disk I Investigate the limits of the modelling program for this new set-up 4/21 Monte Carlo I Solves continuum radiative transfer process by following photons individually I Calculates the temperature of the system via the photon packets I Relies on randomness which leads to noise I Mimics 3D propagation of photons (Credit: Pinte, 2015) 5/21 MCMax3D I Simulates RT process using Monte Carlo method Vertical cut (xz-plane) of a `zone' I Flexible in building up structure via `zones' I Generates a `static' model in 3D I Grid points are volume elements with which the photon packet interact 6/21 Model set-up (Dust density of system) Quantity Inner disk Outer disk CPD Inner radius 0:4 au 22 au 3 × 10−3 au I T Tauri star with L∗ = 1:01 L Outer radius 18 au 500 au 1 au −5 −4 −10 Dust mass 2 × 10 M 1 × 10 M 10 M I Default planet luminosity of Optical depth 4:7 × 104 2:3 × 102 9:1 × 102 −2 Position (0,0,0) au (0,0,0) au (20,0,0) au Lp = 1:01 × 10 L Vertical cut (xz-plane) Midplane cut (xy-plane) 7/21 2 Main models 1. Full system (i.e., inner disk, outer disk and CPD) 2. Inner disk removed and CPD + planet placed at 10 au distance from the star −2 Tested for two planetary luminosities: Lp = 1:01 × 10 L −3 and Lp = 1:01 × 10 L 8/21 −2 Dust temperature full system for Lp = 1:01 × 10 L I 3D model shows temperature asymmetry in midplane I Interested in `Solar' and `Dark' side of circumplanetary disk Vertical cut (xz-plane) Midplane cut (xy-plane) 9/21 −2 Dust temperature in midplane (Lp = 1:01 × 10 L ) I Planet heats up surrounding inner and outer disk 10/21 −3 Dust temperature in midplane (Lp = 1:01 × 10 L ) 11/21 −2 Impact of CPD/planet on protoplanetary disk for Lp = 1:01 × 10 L I Stellar photons heat up midplane of outer disk via gap Inner disk Outer disk Inner disk (NO CPD/planet) Outer disk (NO CPD/planet) 102 T [K] 101 100 101 102 x [au] 12/21 −2 Inner disk removed and CPD/planet closer to star for Lp = 1:01 × 10 L Vertical cut (xz-plane) Midplane cut (xy-plane) 13/21 Monte Carlo Noise reduction for temperature and radiation field Midplane cut (xy-plane) I Averaging procedure for temperature I Sextants in order to maintain difference between Solar and Dark side I Radiation field will be averaged over complete semi circles 14/21 SOLARDARKrPhotonsPlanetStar Temperature CPD full system −2 −3 Lp = 1:01 × 10 L Lp = 1:01 × 10 L I Average temperature of Dark and Solar side as function of distance to planet I 1σ error bars is Monte Carlo noise I Large errors are due to lack of photons I Interested in outer edge to see maximal possible difference I Star does not heat the circumplanetary disk 15/21 Temperature CPD reduced system −2 −3 Lp = 1:01 × 10 L Lp = 1:01 × 10 L I Inner disk removed and planet/CPD placed at 10 au I Solar side is clearly heated by star at the outer edge 16/21 −2 Radiation field only for Lp = 1:01 × 10 L Full system Reduced system I Far-UV (0:1 µm < λ < 0:2 µm) I Radiation field (χ) is normalized to Draine field I Monte Carlo noise is very strong here I Due to lack of radiation field photons I Still a trend emerges 17/21 Comparing the differences I Ratio of temperature at outer edge indicates asymmetry I Correlation between χSolar and TSolar 18/21 Concluding remarks and future prospects I The inner disk can make stellar radiation extinct, interesting to test for lower density I MCMax3D could be improved by better control over selecting number of photon packets per source I To properly study a circumplanetary disk model, more photon packets are required to account for its small size 19/21 Planet-disk interaction (Credit: W. Kley and R.P. Nelson, 2012 ) p l = rvφ,gas = GM∗r 20/21 Dust grain opacity law I Far-UV (0:1 µm < λ < 0:2 µm) has very high dust opacity I Meaning it interacts easier with medium and thus propagates less far (Credit: Weingartner and B. T. Draine, 2001) 21/21.

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