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arXiv 1009.4374astro-ph.GA
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原行星盘的辐射热化学模型。III。内边缘对光谱能量分布的影响

Radiation thermo-chemical models of protoplanetary discs. III. Impact of inner rims on Spectral Energy Distributions

Wing-Fai Thi, Peter Woitke, Inga Kamp

摘要:

我们使用热化学流体静力学程序ProDiMo研究了HerbigAe恒星内部盘缘的流体静力学密度结构。我们比较光谱能量分布(SED)和图像从我们的流体静力学光盘模型,从规定的密度结构光盘。ProDiMo中的2D连续辐射转移包括各向同性散射。尘埃温度由辐射平衡条件确定。在热解耦的情况下,气体温度由各种加热和冷却过程之间的平衡决定。气体和尘埃通过光电子、辐射和颗粒表面的气体调节进行热相互作用。因此,气体比热耦合情况下的温度高得多,在热耦合情况下,气体和尘埃的温度相等,在上圆盘层达到几千K,使内缘更高。在内部半径(“软边缘”)处的物理激发的密度下降导致圆形的内部边缘,其在近红外图像中呈现环状。较低的重力拉力和超过~1 AU的热气体的组合导致圆盘大气达到0.1的高度与半径比z/r,而该比率仅在热耦合情况下为0.2。这种膨胀的盘状大气拦截了大量的恒星辐射,这些辐射转化为来自约500 K温度下较热颗粒的3- 30微米波长区域的增强连续辐射。我们还考虑了光盘的质量和粒度分布的影响,自洽的SED反馈到气体的温度,化学和流体静力平衡计算这些量。

英文摘要:

We study the hydrostatic density structure of the inner disc rim around HerbigAe stars using the thermo-chemical hydrostatic code ProDiMo. We compare the Spectral Energy Distributions (SEDs) and images from our hydrostatic disc models to that from prescribed density structure discs. The 2D continuum radiative transfer in ProDiMo includes isotropic scattering. The dust temperature is set by the condition of radiative equilibrium. In the thermal-decoupled case the gas temperature is governed by the balance between various heating and cooling processes. The gas and dust interact thermally via photoelectrons, radiatively, and via gas accommodation on grain surfaces. As a result, the gas is much hotter than in the thermo-coupled case, where the gas and dust temperatures are equal, reaching a few thousands K in the upper disc layers and making the inner rim higher. A physically motivated density drop at the inner radius ("soft-edge") results in rounded inner rims, which appear ring-like in near-infrared images. The combination of lower gravity pull and hot gas beyond ~1 AU results in a disc atmosphere that reaches a height over radius ratio z/r of 0.1 while this ratio is 0.2 only in the thermo-coupled case. This puffed-up disc atmosphere intercepts larger amount of stellar radiation, which translates into enhanced continuum emission in the 3- 30 micron wavelength region from hotter grains at ~500 K. We also consider the effect of disc mass and grain size distribution on the SEDs self-consistently feeding those quantities back into the gas temperature, chemistry, and hydrostatic equilibrium computation.

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