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Modeling conjugate heat transfer

机译:建模共轭传热

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Modeling conduction heat transfer in electronic systems has gained some maturity over the past 3 decades. Although new modeling challenges were associated with 3D stacked dies or packages, some modeling approaches were proposed to handle this rather complicated multiple heat source problem. An even newer problem has started to emerge related to this growing tendency towards exploiting the vertical direction. In fact cooling becomes more and more 3D also, in the sense intermediate micro-channels are proposed going between dies and or packages. This brings convection into play aside with convection in an intimate coupling, commonly called conjugate heat transfer. It is no longer possible to treat convection as an “external” phenomenon, to be modeled by a simple external resistance. In this lecture, fundamental aspects about conjugate heat transfer are revised to obtain a realistic model that avoids large errors that could have been encountered had we treated conduction and convection separately. Fundamental concepts are revised, going up to the notion of heat transfer coefficient in order to elaborate a better model of forced convection in its most general form. The new modeling strategy will build upon progress already realized in Compact Thermal Models (CTM) for conduction in complicated electronic systems. Advanced conduction CTM will be generalized to include convection as well. This will allow a better modeling of convection, but more important a homogeneous and coherent modeling of conjugate heat transfer. Cooling of electronic systems is continuously raising new challenges not only for innovative solutions, but also for modeling of new atypical cases. The higher frequency we ask for, the greater number of functionalities we require as well, both tend to increase heat flux densities to unprecedented levels in industrial applications. Densities higher than those of a nuclear reactor were already realized in electronic systems. We are heading towar- - ds densities of rocket nozzle. Complexity related to these high heat fluxes has many origins that will be addressed, in order to motivate subsequent discussions. A summary of recent advances in conduction modeling will be given before generalizing them to convection. Conjugate convection will be studied.
机译:在过去的3年内,电子系统中的传导传热造型在过去的三十年中取得了一些成熟。虽然新的建模挑战与3D堆叠的模具或包装有关,但提出了一些建模方法来处理这种相当复杂的多个热源问题。甚至更新的问题已经开始出现与利用垂直方向的这种日益增长的倾向。实际上,冷却变得越来越多的3D,在感测中间微通道中建议在模具和包装之间进行。这将对流抛入游戏中,在私密耦合中,通常称为共轭传热。不再可能将对流视为“外部”现象,以通过简单的外部电阻进行建模。在本讲座中,修订了关于共轭传热的基本方面,以获得避免在我们对处理传导和对流的情况下遇到的大错误的实际模型。修订基本概念,达到传热系数的概念,以便在其最一般的形式中详细说明更好的强制对流模式。新的建模策略将在Compact Mather-Models(CTM)中实现的进展,以便在复杂的电子系统中传导。高级传导CTM将概括为包括对流。这将允许更好的对流建模,但更重要的是缀合物传热的均匀和相干建模。电子系统的冷却不仅是为了创新的解决方案而持续提高新的挑战,也是为了建模新的非典型案例。我们要求的频率越高,我们所需要的历程数量越多,两者都倾向于将热通量密度增加到工业应用中前所未有的水平。在电子系统中已经实现了高于核反应堆的密度。我们正在前往火箭喷嘴的拖拉机密度。与这些高热量通量相关的复杂性具有许多将要解决的起源,以便激励随后的讨论。在将它们概括到对流之前,将给出最近的传导建模前进的总结。将研究共轭对流。

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