Wang Zhili, Sun Yanjun, Jian Yongjun
School of Mathematical Science, Inner Mongolia University, Hohhot 010021, China.
School of Statistics and Mathematics, Inner Mongolia University of Finance and Economics, Hohhot 010070, China.
Micromachines (Basel). 2023 Nov 2;14(11):2054. doi: 10.3390/mi14112054.
The features of stationary random processes and the small parameter expansion approach are used in this work to examine the impact of random roughness on the electromagnetic flow in cylindrical micropipes. Utilizing the perturbation method, the analytical solution until second order velocity is achieved. The analytical expression of the roughness function , which is defined as the deviation of the flow rate ratio with roughness to the case having no roughness in a smooth micropipe, is obtained by integrating the spectral density. The roughness function can be taken as the functions of the Hartmann number and the dimensionless wave number . Two special corrugated walls of micropipes, i.e., sinusoidal and triangular corrugations, are analyzed in this work. The results reveal that the magnitude of the roughness function rises as the wave number increases for the same Ha. The magnitude of the roughness function decreases as the increases for a prescribed wave number. In the case of sinusoidal corrugation, as the wave number increases, the Hartmann number decreases, and the value of increases. We consider the ranging from 0 to 15 and the ranging from 0 to 5, with ranging from -2.5 to 27.5. When the reaches 15, and the is 0, reaches the maximum value of 27.5. At this point, the impact of the roughness on the flow rate reaches its maximum. Similarly, in the case of triangular corrugation, when the reaches 15 and the is 0, reaches the maximum value of 18.7. In addition, the sinusoidal corrugation has a stronger influence on the flow rate under the same values of and compared with triangular corrugation.
本文运用平稳随机过程的特征和小参数展开法,研究随机粗糙度对圆柱形微管内电磁流的影响。利用微扰法,得到了直至二阶速度的解析解。粗糙度函数定义为有粗糙度时的流量比与光滑微管中无粗糙度时的流量比的偏差,通过对谱密度积分得到其解析表达式。粗糙度函数可表示为哈特曼数和无量纲波数的函数。本文分析了微管的两种特殊波纹壁,即正弦波纹和三角波纹。结果表明,对于相同的哈特曼数,粗糙度函数的幅值随波数增加而增大。对于给定的波数,粗糙度函数的幅值随哈特曼数增加而减小。在正弦波纹的情况下,随着波数增加,哈特曼数减小,而粗糙度函数的值增大。我们考虑哈特曼数范围从0到15,无量纲波数范围从0到5,粗糙度函数范围从 -2.5到27.5。当哈特曼数达到15且无量纲波数为0时,粗糙度函数达到最大值27.5。此时,粗糙度对流量的影响达到最大。同样,在三角波纹的情况下,当哈特曼数达到15且无量纲波数为0时,粗糙度函数达到最大值18.7。此外,在相同的哈特曼数和无量纲波数下,正弦波纹对流量的影响比三角波纹更强。