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THE INSTABILITY OF A DEVELOPING THERMAL FRONT IN A POROUS MEDIUM. III SUBHARMONIC INSTABILITIES

机译:多孔介质中不断发展的热前沿的不稳定性。 III亚病态不稳定

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In this paper we study the instability of the developing thermal boundary layer that is induced by suddenly raising the temperature of the lower horizontal boundary of a uniformly cold semi-infinite region of saturated porous medium. The basic state consists of no flow, but the evolving temperature field may be described by a similarity solution involving the complementary error function. In very recent papers, Selim and Rees (2007a) (Part I) have sought to determine when this evolving thermal boundary layer becomes unstable and then Selim and Rees (2007b) (Part II) followed the subsequent evolution of horizontally periodic disturbances well into the nonlinear regime. In this paper we investigate the secondary instability of the nonlinear cells by introducing subharmonic disturbances into the evolving flow. We consider three different types of subharmonic disturbance, namely, the 2:1, 3:2, and 4:3 types. Cellular disturbances are seeded into the evolving basic state, the primary mode having an amplitude that is greater than that of the subharmonic. In general, we find that the subharmonic decays at first, while the primary mode grows, but at a time that is dependent on the relative initial amplitudes, the subharmonic experiences an extremely rapid growth and quickly establishes itself as the dominant flow pattern. A fairly detailed account of the 2:1 case is given, including an indication of how the time of transition between the primary and the subharmonic varies with wave number and initial amplitudes. The other two types of subharmonic disturbance yield a richer variety of behaviors; therefore, we present some typical cases to indicate some of the ways in which the primary mode may be destabilized.
机译:在本文中,我们研究了由于突然升高饱和多孔介质的均匀冷半无限区域的下水平边界温度而引起的热边界层发展的不稳定性。基本状态不包含任何流量,但是不断变化的温度场可以用涉及互补误差函数的相似性描述。在最近的论文中,Selim和Rees(2007a)(第I部分)试图确定这种不断发展的热边界层何时变得不稳定,然后Selim和Rees(2007b)(第II部分)跟随了水平周期扰动的后续演变,并将其很好地引入了热力学边界层。非线性状态。在本文中,我们通过将亚谐波扰动引入到演化流中来研究非线性单元的二次不稳定性。我们考虑三种不同类型的次谐波扰动,即2:1、3:2和4:3类型。细胞干扰被植入到不断发展的基本状态中,主要模式的振幅大于次谐波的振幅。总的来说,我们发现次谐波在开始时会衰减,而初级模态会增长,但是在依赖于相对初始振幅的时间,次谐波经历了非常快速的增长,并迅速将其自身确立为主导流动模式。给出了2:1情况的相当详细的说明,包括一次谐波和次谐波之间的过渡时间如何随波数和初始振幅变化的指示。其他两种类型的次谐波扰动产生更丰富的行为。因此,我们介绍一些典型情况,以表明可能破坏主模式的一些方式。

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