logging in or signing up talk2 Goldie Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 53 Category: Entertainment License: All Rights Reserved Like it (0) Dislike it (0) Added: November 14, 2007 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Structure & Evolution of Protoplanetary Disks:Merging 3D Radiation Transfer & Hydrodynamics: Structure & Evolution of Protoplanetary Disks: Merging 3D Radiation Transfer & Hydrodynamics Kenneth Wood St AndrewsSlide2: Data: Imaging polarimetry Photometric monitoring Scattered light images Spectral energy distributions (SEDs) Theory: Dynamical models of star formation: Collapsing clouds, jets, accretion disks, debris disks, & planet formation RT Models: 3D Monte Carlo techniquesFriends & Collaborators: Friends & Collaborators RT Models & Dust Theory: Barbara Whitney, Jon Bjorkman, Mike Wolff Dynamical Models: Ken Rice, Ian Bonnell, Phil Armitage, Matthew Bate, Scott Kenyon, Adam Frank Observations: Charlie Lada, Ed Churchwell, Anneila Sargent, Glenn Schneider, Angela Cotera, Debbie Padgett, Keivan StassunMonte Carlo Capabilities: Monte Carlo Capabilities 3D geometry & illumination Incorporate MHD density & velocity grids Scattered light images (optical & infrared) Radiative equilibrium dust temperatures SEDs & thermal imaging (mid-IR, sub-mm)Star Formation Theory: Star Formation Theory Class 0 Class I Class IIStar Formation: Observations: Star Formation: Observations l(mm) Bourke 2001 Padgett et al. 1999 Krist et al. 2000 BHR71 TW Hydrae IRAS 04302+2247 “0” “I” “II”Near-IR HST Images: Near-IR HST ImagesDisks, Disks, Disks…: Disks, Disks, Disks…T Tauri Accretion Disks: Images: T Tauri Accretion Disks: Images Disk density: hydrostatic flared disk: h / r = cs(r) / W(r) Shakara & Sunyaev (1973), Lynden-Bell & Pringle (1974) Direct starlight 10,000 brighter than scattered light from disk Best detected when star occulted by edge-on flaring disk Whitney & Hartmann 1992T Tauri Accretion Disks: SEDs: T Tauri Accretion Disks: SEDs Pole-on: Large IR excess Edge-on: Double peaked SED: scattered light + thermal Wood et al. 2002Star Formation in Taurus: Star Formation in Taurus © Steve Kohle & Till Credner, AlltheSky.comL1551 Region: L1551 Region Whitney, Gomez, & Kenyon (Mt Hopkins, 48”) Red = [S II] White = Visual L1551 IRS5 HL Tau XZ Tau HH 30 HH 30 IRS 1’ = 8400AUHH 30 IRS Accretion Disk: HH 30 IRS Accretion Disk Burrows et al. 1996 HST WFPC2: Green: F555W (V Band) Red: F617N (Ha, S[II]) Scattered light models: Assume ISM dust opacity Image morphology: disk geometry, inclination Width of dust lane: optical depth, disk mass Bacciotti et al. 1999HH 30 IRS: Disk Geometry: HH 30 IRS: Disk Geometry HST WFPC2 Model Hydrostatic flared disk, i = 84 Dust + gas suspended above midplane Consistent with T(r), S(r) for irradiated disks (D’Alessio et al. 1999)Multiwavelength Models: Multiwavelength Models ISM Dust: Opacity decreases by 10 from V to K Dust lane width decreases into IR Very compact nebulosity at K Wood et al. 1998 V (0.55mm) I (0.85mm) K (2.25mm)Slide16: Cotera et al. 2001 V (0.55mm) I (0.85mm) K (2.25mm) NICMOS: Wide dust lane at K Circumstellar dust is GRAYER than ISM dust Grain Growth in diskHH 30 IRS: SED Models: HH 30 IRS: SED Models Model: Geometry from HST images; Heating: starlight + accretion Model HST images and SED: Determine dust size distribution Find: Grayer opacity Optical opacity < ISM Larger disk mass (t ~ kM) Md ~ 2 * 10-3 M8 Wood et al. 2002HH 30 IRS: Grain Growth: HH 30 IRS: Grain Growth ISM HH 30 IRS Dust Size Distribution: Power law + exponential decay Grain Sizes in excess of 50mm Grayer opacity, Sub-mm slope ~ 1/l Beckwith & Sargent (1991): sub-mm continuum SEDs: k ~ 1/lHH 30 IRS: Image Variability: HH 30 IRS: Image VariabilityMagnetic Accretion in HH 30 IRS: Magnetic Accretion in HH 30 IRS Stellar B-field not aligned with rotation axis Truncates disk, accretion along field lines Hot Spots on star at magnetic poles UV excess, photometric modulation Ghosh & Lamb1979 Shu et al. 1994Magnetic Accretion in HH 30 IRS: Magnetic Accretion in HH 30 IRS Wood & Whitney 1998Magnetic Accretion in HH 30 IRS: Magnetic Accretion in HH 30 IRS T*=3500K; Ts=10000K; DA ~ 6% Asymmetric brightening; DV ~ 1.5m Photometric centroid shift: d ~ 0.5’’ Wood & Whitney 1998 Stapelfeldt et al. 1999HH 30 IRS: Photometry: HH 30 IRS: Photometry DV ~ 1.5mag, DT ~ days: Typical of CTTs, accretion hot spots Variability all due to scattered light Wood et al. 2000GM Aur: Disk/Planet Interaction?: GM Aur: Disk/Planet Interaction? NICMOS coronagraph Scattered light modeling: Mdisk ~ 0.04 M8; Rdisk ~ 300 AU; i ~ 50 Schneider et al. 2002GM Aur: Disk/Planet Interaction?: GM Aur: Disk/Planet Interaction? No near-IR excess SED model requires 4AU gap: planet? Lin & Papaloizou; Seyer & Clarke; Nelson, etcGM Aur: Disk/Planet Interaction?: GM Aur: Disk/Planet Interaction? 3D SPH calculation from Ken Rice Planet at 2.5 AU clears disk out to 4AU Rice et al. 2002GM Aur: Disk/Planet Interaction?: GM Aur: Disk/Planet Interaction? 3D SPH calculation from Ken Rice Planet at 2.5 AU clears disk out to 4AU Rice et al. 2002GM Aur: Disk/Planet Interaction?: GM Aur: Disk/Planet Interaction? 3D SPH density grid into Monte Carlo code SIRTF SED can discriminate planet mass Centroid shifting ~ 0.1mas: Keck, SIM? Rice et al. 2002Disk Evolution: Disk Evolution Lada et al. 2000 Trapezium Cluster IR-EXCESS = DISKS Cluster age ~ 1.5Myr Disk Frequency: 80%Disk Lifetimes: Disk Lifetimes Haisch et al. 2000 CLUSTER SURVEYS: Disk frequency declines with cluster age Disk Lifetime: ~ 6MyrDisk Evolution: Disk Evolution Disk structure does not change Disk mass decreases homologously Mass = mass of dust contributing to SED What Md can near-IR surveys detect? Observables: SEDs, colors Current evidence for disk mass evolution?SED Evolution: SED Evolution d = 500pc; 10-8 M8 < Md < 10-1 M8 SIRTF 5s, 500secs Wood et al. 2002Color Evolution: Color Evolution Wood et al. 2001Observing Disk Evolution: Observing Disk Evolution JHKL surveys: disk frequency & lifetime JHKL surveys: detect Md > 10-7M8 Far-IR & (sub)mm: disk mass evolution Mid-IR (10mm & 25mm): disk mass evolution Taurus-Auriga Sources: Taurus-Auriga Sources Gap in K-N distribution: transition from disks to no disks Kenyon & Hartmann 1995 * = I + = II ( = IIIDisk Masses in Taurus-Auriga: Disk Masses in Taurus-Auriga Evolution models: disk clearing rapid for Md < 10-6 M8 Wood et al. 2002 1 = 10-1 M8 2 = 10-2 M8 3 = 10-3 M8 etcSpace Infrared Telescope: Space Infrared Telescope SIRTF: launch in January 2003 Lot’s of data: 6 Legacy programs Infrared spectra for 3mm < l < 160mm Study disks: environments and ages Website with grid of models Feedback in Star Formation: Feedback in Star Formation HH 30 IRS, GM Aur: Signatures of magnetic accretion & SPH models Bigger Goal: Combine RT and hydro simulations Temperature, radiation pressure & ionization structureDisk Temperature Structure: Disk Temperature Structure Stellar photons absorbed at ~ 4 h(r) above midplane Iterate with dynamics Self-consistent disk structureSummary & Future Research: Summary & Future Research Disk Structure & Variability: HH 30, GM Aur Model data with analytic density structures Now testing hydro simulations SIRTF: characterize large numbers of disks Goal: merge radiation transfer & hydro Monte Carlo Photoionization: Monte Carlo Photoionization Calculate 3D ionization structure Study percolation of ionizing photons in fractal ISMStromgren Volume in a Dickey-Lockman Disk: Stromgren Volume in a Dickey-Lockman Disk 2 Kpc n(H0) Ionization fraction f ~ 10-3 Q(H0) = 2 1050 s-1: Escape fraction = 22% Ionization of HVCs, Magellanic Stream, IGM…Slide43: 3D Stromgren Volumes n(H0) (before) Ionization fraction n(H0) (after) Clumpy density; 2 sources with Q(H0) = 2 1050 s-1 3D ionization structure, shadow regions You do not have the permission to view this presentation. In order to view it, please contact the author of the presentation.
talk2 Goldie Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 53 Category: Entertainment License: All Rights Reserved Like it (0) Dislike it (0) Added: November 14, 2007 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Structure & Evolution of Protoplanetary Disks:Merging 3D Radiation Transfer & Hydrodynamics: Structure & Evolution of Protoplanetary Disks: Merging 3D Radiation Transfer & Hydrodynamics Kenneth Wood St AndrewsSlide2: Data: Imaging polarimetry Photometric monitoring Scattered light images Spectral energy distributions (SEDs) Theory: Dynamical models of star formation: Collapsing clouds, jets, accretion disks, debris disks, & planet formation RT Models: 3D Monte Carlo techniquesFriends & Collaborators: Friends & Collaborators RT Models & Dust Theory: Barbara Whitney, Jon Bjorkman, Mike Wolff Dynamical Models: Ken Rice, Ian Bonnell, Phil Armitage, Matthew Bate, Scott Kenyon, Adam Frank Observations: Charlie Lada, Ed Churchwell, Anneila Sargent, Glenn Schneider, Angela Cotera, Debbie Padgett, Keivan StassunMonte Carlo Capabilities: Monte Carlo Capabilities 3D geometry & illumination Incorporate MHD density & velocity grids Scattered light images (optical & infrared) Radiative equilibrium dust temperatures SEDs & thermal imaging (mid-IR, sub-mm)Star Formation Theory: Star Formation Theory Class 0 Class I Class IIStar Formation: Observations: Star Formation: Observations l(mm) Bourke 2001 Padgett et al. 1999 Krist et al. 2000 BHR71 TW Hydrae IRAS 04302+2247 “0” “I” “II”Near-IR HST Images: Near-IR HST ImagesDisks, Disks, Disks…: Disks, Disks, Disks…T Tauri Accretion Disks: Images: T Tauri Accretion Disks: Images Disk density: hydrostatic flared disk: h / r = cs(r) / W(r) Shakara & Sunyaev (1973), Lynden-Bell & Pringle (1974) Direct starlight 10,000 brighter than scattered light from disk Best detected when star occulted by edge-on flaring disk Whitney & Hartmann 1992T Tauri Accretion Disks: SEDs: T Tauri Accretion Disks: SEDs Pole-on: Large IR excess Edge-on: Double peaked SED: scattered light + thermal Wood et al. 2002Star Formation in Taurus: Star Formation in Taurus © Steve Kohle & Till Credner, AlltheSky.comL1551 Region: L1551 Region Whitney, Gomez, & Kenyon (Mt Hopkins, 48”) Red = [S II] White = Visual L1551 IRS5 HL Tau XZ Tau HH 30 HH 30 IRS 1’ = 8400AUHH 30 IRS Accretion Disk: HH 30 IRS Accretion Disk Burrows et al. 1996 HST WFPC2: Green: F555W (V Band) Red: F617N (Ha, S[II]) Scattered light models: Assume ISM dust opacity Image morphology: disk geometry, inclination Width of dust lane: optical depth, disk mass Bacciotti et al. 1999HH 30 IRS: Disk Geometry: HH 30 IRS: Disk Geometry HST WFPC2 Model Hydrostatic flared disk, i = 84 Dust + gas suspended above midplane Consistent with T(r), S(r) for irradiated disks (D’Alessio et al. 1999)Multiwavelength Models: Multiwavelength Models ISM Dust: Opacity decreases by 10 from V to K Dust lane width decreases into IR Very compact nebulosity at K Wood et al. 1998 V (0.55mm) I (0.85mm) K (2.25mm)Slide16: Cotera et al. 2001 V (0.55mm) I (0.85mm) K (2.25mm) NICMOS: Wide dust lane at K Circumstellar dust is GRAYER than ISM dust Grain Growth in diskHH 30 IRS: SED Models: HH 30 IRS: SED Models Model: Geometry from HST images; Heating: starlight + accretion Model HST images and SED: Determine dust size distribution Find: Grayer opacity Optical opacity < ISM Larger disk mass (t ~ kM) Md ~ 2 * 10-3 M8 Wood et al. 2002HH 30 IRS: Grain Growth: HH 30 IRS: Grain Growth ISM HH 30 IRS Dust Size Distribution: Power law + exponential decay Grain Sizes in excess of 50mm Grayer opacity, Sub-mm slope ~ 1/l Beckwith & Sargent (1991): sub-mm continuum SEDs: k ~ 1/lHH 30 IRS: Image Variability: HH 30 IRS: Image VariabilityMagnetic Accretion in HH 30 IRS: Magnetic Accretion in HH 30 IRS Stellar B-field not aligned with rotation axis Truncates disk, accretion along field lines Hot Spots on star at magnetic poles UV excess, photometric modulation Ghosh & Lamb1979 Shu et al. 1994Magnetic Accretion in HH 30 IRS: Magnetic Accretion in HH 30 IRS Wood & Whitney 1998Magnetic Accretion in HH 30 IRS: Magnetic Accretion in HH 30 IRS T*=3500K; Ts=10000K; DA ~ 6% Asymmetric brightening; DV ~ 1.5m Photometric centroid shift: d ~ 0.5’’ Wood & Whitney 1998 Stapelfeldt et al. 1999HH 30 IRS: Photometry: HH 30 IRS: Photometry DV ~ 1.5mag, DT ~ days: Typical of CTTs, accretion hot spots Variability all due to scattered light Wood et al. 2000GM Aur: Disk/Planet Interaction?: GM Aur: Disk/Planet Interaction? NICMOS coronagraph Scattered light modeling: Mdisk ~ 0.04 M8; Rdisk ~ 300 AU; i ~ 50 Schneider et al. 2002GM Aur: Disk/Planet Interaction?: GM Aur: Disk/Planet Interaction? No near-IR excess SED model requires 4AU gap: planet? Lin & Papaloizou; Seyer & Clarke; Nelson, etcGM Aur: Disk/Planet Interaction?: GM Aur: Disk/Planet Interaction? 3D SPH calculation from Ken Rice Planet at 2.5 AU clears disk out to 4AU Rice et al. 2002GM Aur: Disk/Planet Interaction?: GM Aur: Disk/Planet Interaction? 3D SPH calculation from Ken Rice Planet at 2.5 AU clears disk out to 4AU Rice et al. 2002GM Aur: Disk/Planet Interaction?: GM Aur: Disk/Planet Interaction? 3D SPH density grid into Monte Carlo code SIRTF SED can discriminate planet mass Centroid shifting ~ 0.1mas: Keck, SIM? Rice et al. 2002Disk Evolution: Disk Evolution Lada et al. 2000 Trapezium Cluster IR-EXCESS = DISKS Cluster age ~ 1.5Myr Disk Frequency: 80%Disk Lifetimes: Disk Lifetimes Haisch et al. 2000 CLUSTER SURVEYS: Disk frequency declines with cluster age Disk Lifetime: ~ 6MyrDisk Evolution: Disk Evolution Disk structure does not change Disk mass decreases homologously Mass = mass of dust contributing to SED What Md can near-IR surveys detect? Observables: SEDs, colors Current evidence for disk mass evolution?SED Evolution: SED Evolution d = 500pc; 10-8 M8 < Md < 10-1 M8 SIRTF 5s, 500secs Wood et al. 2002Color Evolution: Color Evolution Wood et al. 2001Observing Disk Evolution: Observing Disk Evolution JHKL surveys: disk frequency & lifetime JHKL surveys: detect Md > 10-7M8 Far-IR & (sub)mm: disk mass evolution Mid-IR (10mm & 25mm): disk mass evolution Taurus-Auriga Sources: Taurus-Auriga Sources Gap in K-N distribution: transition from disks to no disks Kenyon & Hartmann 1995 * = I + = II ( = IIIDisk Masses in Taurus-Auriga: Disk Masses in Taurus-Auriga Evolution models: disk clearing rapid for Md < 10-6 M8 Wood et al. 2002 1 = 10-1 M8 2 = 10-2 M8 3 = 10-3 M8 etcSpace Infrared Telescope: Space Infrared Telescope SIRTF: launch in January 2003 Lot’s of data: 6 Legacy programs Infrared spectra for 3mm < l < 160mm Study disks: environments and ages Website with grid of models Feedback in Star Formation: Feedback in Star Formation HH 30 IRS, GM Aur: Signatures of magnetic accretion & SPH models Bigger Goal: Combine RT and hydro simulations Temperature, radiation pressure & ionization structureDisk Temperature Structure: Disk Temperature Structure Stellar photons absorbed at ~ 4 h(r) above midplane Iterate with dynamics Self-consistent disk structureSummary & Future Research: Summary & Future Research Disk Structure & Variability: HH 30, GM Aur Model data with analytic density structures Now testing hydro simulations SIRTF: characterize large numbers of disks Goal: merge radiation transfer & hydro Monte Carlo Photoionization: Monte Carlo Photoionization Calculate 3D ionization structure Study percolation of ionizing photons in fractal ISMStromgren Volume in a Dickey-Lockman Disk: Stromgren Volume in a Dickey-Lockman Disk 2 Kpc n(H0) Ionization fraction f ~ 10-3 Q(H0) = 2 1050 s-1: Escape fraction = 22% Ionization of HVCs, Magellanic Stream, IGM…Slide43: 3D Stromgren Volumes n(H0) (before) Ionization fraction n(H0) (after) Clumpy density; 2 sources with Q(H0) = 2 1050 s-1 3D ionization structure, shadow regions