Mhaisekar Ashutosh, Kazmierczak Michael J, Banerjee Rupak
Department of Mechanical, Industrial and Nuclear Engineering, University of Cincinnati, OH 45221-0072, USA.
J Synchrotron Radiat. 2005 May;12(Pt 3):318-28. doi: 10.1107/S0909049505003250. Epub 2005 Apr 14.
The differential momentum and thermal energy equations for fluid flow and convective heat-transfer around the sample biocrystal, with coupled internal heat conduction, are solved using advanced computational fluid dynamics techniques. Average \bar{h} as well as local h(theta) values of the convective heat-transfer coefficients are obtained from the fundamental equations. The results of these numerical solutions show the three-dimensional fluid flow field around the sample in conjunction with the detailed internal temperature distribution inside the crystal. The external temperature rise and maximum internal temperature increase are reported for various cases. The effect of the important system parameters, such as gas velocity and properties, crystal size and thermal conductivity and incident beam conditions (intensity and beam size), are all illustrated with comparative examples. For the reference case, an external temperature rise of 7 K and internal temperature increase of 0.5 K are calculated for a 200 microm-diameter cryocooled spherical biocrystal subjected to a 13 keV X-ray beam of 4 x 10(14) photons s(-1) mm(-2) flux density striking half the sample. For all the cases investigated, numerical analysis shows that the controlling thermal resistance is the rate of convective heat-transfer and not internal conduction. Thermal diffusion results in efficient thermal spreading of the deposited energy and this results in almost uniform internal crystal temperatures (DeltaT(internal) approximately 0.5 K), in spite of the non-uniform h(theta) with no more than 1.3 K internal temperature difference for the worst case of localized and focused beam heating. Rather, the major temperature variation occurs between the outer surface of the crystal/loop system and the gas stream, T(s) - T(gas), which itself is only about DeltaT(external) approximately 5-10 K, and depends on the thermal loading imposed by the X-ray beam, the rate of convection and the size of the loop/crystal system.
利用先进的计算流体动力学技术求解了围绕样品生物晶体的流体流动和对流换热的微分动量方程及热能方程,并考虑了内部热传导的耦合。对流换热系数的平均(\bar{h})值以及局部(h(\theta))值可从基本方程中获得。这些数值解的结果显示了样品周围的三维流体流场以及晶体内部详细的温度分布。报告了各种情况下的外部温度升高和内部最大温度升高情况。通过对比示例说明了重要系统参数的影响,如气体速度和性质、晶体尺寸和热导率以及入射束条件(强度和束尺寸)。对于参考情况,计算得出,对于直径为200微米的低温冷却球形生物晶体,在受到通量密度为(4×10^{14})光子(·)秒(^{-1}·)毫米(^{-2})的13keV X射线束照射样品一半面积时,外部温度升高7K,内部温度升高0.5K。对于所有研究的情况,数值分析表明,控制热阻的是对流换热速率而非内部传导。热扩散导致沉积能量的有效热扩散,这使得晶体内部温度几乎均匀((\Delta T_{内部})约为0.5K),尽管(h(\theta))不均匀,在局部和聚焦束加热的最坏情况下,内部温度差不超过1.3K。相反,主要的温度变化发生在晶体/回路系统的外表面与气流之间,即(T_s - T_{气体}),其本身仅约为(\Delta T_{外部})约5 - 10K,并且取决于X射线束施加的热负荷、对流速率以及回路/晶体系统的尺寸。