论文标题
通过浮动气泡和声波加热群内培养基
Heating of the intracluster medium by buoyant bubbles and sound waves
论文作者
论文摘要
由中央超级黑洞(SMBHS)提供动力的活性银河核(AGN)在修饰簇内培养基(ICM)的热特性方面起着重要作用。在这项工作中,我们实施了两个AGN加热模型:(i)通过分层ICM(泡腾模型)上升的浮腔,以及(ii)通过粘性和导电性耗散声波(声波模型)。我们的目的是确定这些加热模型是否与ICM可观察物相一致,以及一个比另一个比另一个优先选择。我们假设ICM的初始熵曲线可从暗物质晕电势中纯粹的引力中心。然后,我们结合加热,辐射冷却和热传导,以研究簇年龄段ICM的演变。我们的结果是:(i)两个加热过程都可以通过对相关参数进行一些调整来产生ICM的可比热轮廓。 (ii)在将注入的能量传递到中央区域以外的情况下,热传导即使在Spitzer值的10 \%的水平上也至关重要,并且温度/熵剖面是不切实际的。 (iii)两种型号的所需注入的AGN功率尺度为$ m _ {\ rm vir}^{1.5} $。 (iv)所需的AGN光度与观察到的无线电射流功率相当,从而增强了AGN是簇中主要的加热源的想法。 (v)最后,我们估计,作为$ 0.02R_ {500} $的AGN机械发光度可用的总AGN发光度的比例小于0.05 \%。
Active galactic nuclei (AGN) powered by the central Super-Massive Black Holes (SMBHs) play a major role in modifying the thermal properties of the intracluster medium (ICM). In this work, we implement two AGN heating models: (i) by buoyant cavities rising through stratified ICM (effervescent model) and, (ii) by viscous and conductive dissipation of sound waves (acoustic model). Our aim is to determine whether these heating models are consistent with ICM observables and if one is preferred over the other. We assume an initial entropy profile of ICM that is expected from the purely gravitational infall of the gas in the potential of the dark matter halo. We then incorporate heating, radiative cooling, and thermal conduction to study the evolution of ICM over the age of the clusters. Our results are: (i) Both the heating processes can produce comparable thermal profiles of the ICM with some tuning of relevant parameters. (ii) Thermal conduction is crucially important, even at the level of 10\% of the Spitzer values, in transferring the injected energy beyond the central regions, and without which the temperature/entropy profiles are unrealistically high. (iii) The required injected AGN power scales with cluster mass as $M_{\rm vir}^{1.5}$ for both models. (iv) The required AGN luminosity is comparable with the observed radio jet power, reinforcing the idea that AGNs are the dominant heating source in clusters. (v) Finally, we estimate that the fraction of the total AGN luminosity available as the AGN mechanical luminosity at $0.02r_{500}$ is less than 0.05\%.