• 文献检索
  • 文档翻译
  • 深度研究
  • 学术资讯
  • Suppr Zotero 插件Zotero 插件
  • 邀请有礼
  • 套餐&价格
  • 历史记录
应用&插件
Suppr Zotero 插件Zotero 插件浏览器插件Mac 客户端Windows 客户端微信小程序
定价
高级版会员购买积分包购买API积分包
服务
文献检索文档翻译深度研究API 文档MCP 服务
关于我们
关于 Suppr公司介绍联系我们用户协议隐私条款
关注我们

Suppr 超能文献

核心技术专利:CN118964589B侵权必究
粤ICP备2023148730 号-1Suppr @ 2026

文献检索

告别复杂PubMed语法,用中文像聊天一样搜索,搜遍4000万医学文献。AI智能推荐,让科研检索更轻松。

立即免费搜索

文件翻译

保留排版,准确专业,支持PDF/Word/PPT等文件格式,支持 12+语言互译。

免费翻译文档

深度研究

AI帮你快速写综述,25分钟生成高质量综述,智能提取关键信息,辅助科研写作。

立即免费体验

微通道中绝热气体流动平均摩擦系数计算的数据缩减方法比较

A Comparison of Data Reduction Methods for Average Friction Factor Calculation of Adiabatic Gas Flows in Microchannels.

作者信息

Rehman Danish, Morini Gian Luca, Hong Chungpyo

机构信息

Microfluidics Laboratory, Department of Industrial Engineering (DIN), University of Bologna, Via Zamboni, 33, 40126 Bologna BO, Italy.

Microscale Heat Transfer Laboratory, Department of Mechanical Engineering, Kagoshima University, Kagoshima Prefecture 890-8580, Japan.

出版信息

Micromachines (Basel). 2019 Feb 28;10(2):171. doi: 10.3390/mi10030171.

DOI:10.3390/mi10030171
PMID:30823482
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6471641/
Abstract

In this paper, a combined numerical and experimental approach for the estimation of the average friction factor along adiabatic microchannels with compressible gas flows is presented. Pressure-drop experiments are performed for a rectangular microchannel with a hydraulic diameter of 295 μ m by varying Reynolds number up to 17,000. In parallel, the calculation of friction factor has been repeated numerically and results are compared with the experimental work. The validated numerical model was also used to gain an insight of flow physics by varying the aspect ratio and hydraulic diameter of rectangular microchannels with respect to the channel tested experimentally. This was done with an aim of verifying the role of minor loss coefficients for the estimation of the average friction factor. To have laminar, transitional, and turbulent regimes captured, numerical analysis has been performed by varying Reynolds number from 200 to 20,000. Comparison of numerically and experimentally calculated gas flow characteristics has shown that adiabatic wall treatment (Fanno flow) results in better agreement of average friction factor values with conventional theory than the isothermal treatment of gas along the microchannel. The use of a constant value for minor loss coefficients available in the literature is not recommended for microflows as they change from one assembly to the other and their accurate estimation for compressible flows requires a coupling of numerical analysis with experimental data reduction. Results presented in this work demonstrate how an adiabatic wall treatment along the length of the channel coupled with the assumption of an isentropic flow from manifold to microchannel inlet results in a self-sustained experimental data reduction method for the accurate estimation of friction factor values even in presence of significant compressibility effects. Results also demonstrate that both the assumption of perfect expansion and consequently wrong estimation of average temperature between inlet and outlet of a microchannel can be responsible for an apparent increase in experimental average friction factor in choked flow regime.

摘要

本文提出了一种结合数值和实验的方法,用于估算沿绝热微通道的可压缩气流的平均摩擦系数。对水力直径为295μm的矩形微通道进行了压降实验,雷诺数变化范围高达17000。同时,对摩擦系数进行了数值计算,并将结果与实验工作进行了比较。经验证的数值模型还用于通过改变矩形微通道的纵横比和水力直径(相对于实验测试的通道)来深入了解流动物理。这样做的目的是验证次要损失系数在估算平均摩擦系数中的作用。为了捕捉层流、过渡流和湍流状态,通过将雷诺数从200变化到20000进行了数值分析。数值计算和实验计算的气流特性比较表明,与沿微通道对气体进行等温处理相比,绝热壁处理(范诺流)能使平均摩擦系数值与传统理论更好地吻合。对于微流动,不建议使用文献中可用的次要损失系数的恒定值,因为它们在不同组件之间会发生变化,并且对于可压缩流的准确估算需要将数值分析与实验数据处理相结合。本文给出的结果表明,沿通道长度进行绝热壁处理,再加上从歧管到微通道入口的等熵流假设,会产生一种自维持的实验数据处理方法,即使在存在显著压缩效应的情况下,也能准确估算摩擦系数值。结果还表明,微通道进出口之间完美膨胀的假设以及由此导致的平均温度错误估算,可能是导致阻塞流状态下实验平均摩擦系数明显增加的原因。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/35d691e1f501/micromachines-10-00171-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/b6a8bdd5d8c4/micromachines-10-00171-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/38adb365a0f7/micromachines-10-00171-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/a5ec4bc8202c/micromachines-10-00171-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/74429239bfe4/micromachines-10-00171-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/b1e44754f7a4/micromachines-10-00171-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/009e174650f5/micromachines-10-00171-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/273ac9caf3e0/micromachines-10-00171-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/bfdd43bce4db/micromachines-10-00171-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/8fc3fcc7d3d7/micromachines-10-00171-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/64737e1cc44a/micromachines-10-00171-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/cd261b504596/micromachines-10-00171-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/611b77e1ae6b/micromachines-10-00171-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/35d691e1f501/micromachines-10-00171-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/b6a8bdd5d8c4/micromachines-10-00171-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/38adb365a0f7/micromachines-10-00171-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/a5ec4bc8202c/micromachines-10-00171-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/74429239bfe4/micromachines-10-00171-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/b1e44754f7a4/micromachines-10-00171-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/009e174650f5/micromachines-10-00171-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/273ac9caf3e0/micromachines-10-00171-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/bfdd43bce4db/micromachines-10-00171-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/8fc3fcc7d3d7/micromachines-10-00171-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/64737e1cc44a/micromachines-10-00171-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/cd261b504596/micromachines-10-00171-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/611b77e1ae6b/micromachines-10-00171-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4b4d/6471641/35d691e1f501/micromachines-10-00171-g013.jpg

相似文献

1
A Comparison of Data Reduction Methods for Average Friction Factor Calculation of Adiabatic Gas Flows in Microchannels.微通道中绝热气体流动平均摩擦系数计算的数据缩减方法比较
Micromachines (Basel). 2019 Feb 28;10(2):171. doi: 10.3390/mi10030171.
2
Lattice Boltzmann Simulation of the Hydrodynamic Entrance Region of Rectangular Microchannels in the Slip Regime.滑移流态下矩形微通道流体动力学入口区域的格子玻尔兹曼模拟
Micromachines (Basel). 2018 Feb 16;9(2):87. doi: 10.3390/mi9020087.
3
A Hybrid Numerical Methodology Based on CFD and Porous Medium for Thermal Performance Evaluation of Gas to Gas Micro Heat Exchanger.一种基于计算流体动力学(CFD)和多孔介质的混合数值方法用于气-气微热交换器热性能评估
Micromachines (Basel). 2020 Feb 20;11(2):218. doi: 10.3390/mi11020218.
4
Simulations of Flows via CFD in Microchannels for Characterizing Entrance Region and Developing New Correlations for Hydrodynamic Entrance Length.通过计算流体动力学(CFD)对微通道内流动进行模拟,以表征入口区域并建立关于流体动力学入口长度的新关联式。
Micromachines (Basel). 2023 Jul 14;14(7):1418. doi: 10.3390/mi14071418.
5
Contribution of Reynolds stress distribution to the skin friction in compressible turbulent channel flows.雷诺应力分布对可压缩湍流槽道流中壁面摩擦力的贡献。
Phys Rev E Stat Nonlin Soft Matter Phys. 2009 Mar;79(3 Pt 2):035301. doi: 10.1103/PhysRevE.79.035301. Epub 2009 Mar 3.
6
Sustained superhydrophobic friction reduction at high liquid pressures and large flows.在高液体压力和大流量下持续的超疏水减阻。
Langmuir. 2011 Jan 4;27(1):487-93. doi: 10.1021/la103624d. Epub 2010 Dec 1.
7
Investigation of Heat Transfer and Pressure Drop in Microchannel Heat Sink Using AlO and ZrO Nanofluids.使用AlO和ZrO纳米流体对微通道散热器中的传热和压降进行研究。
Nanomaterials (Basel). 2020 Sep 9;10(9):1796. doi: 10.3390/nano10091796.
8
Numerical Study of Gas Flow in Super Nanoporous Materials Using the Direct Simulation Monte-Carlo Method.基于直接模拟蒙特卡洛方法的超纳米多孔材料中气体流动的数值研究。
Micromachines (Basel). 2023 Jan 4;14(1):139. doi: 10.3390/mi14010139.
9
Pressure drop of slug flow in microchannels with increasing void fraction: experiment and modeling.微通道内弹状流压降随含气率增加的变化:实验与模型。
Lab Chip. 2011 Jun 7;11(11):1968-78. doi: 10.1039/c0lc00478b. Epub 2011 Apr 21.
10
Study on Flow Characteristics of Working Medium in Microchannel Simulated by Porous Media Model.基于多孔介质模型模拟微通道内工作介质流动特性的研究
Micromachines (Basel). 2020 Dec 26;12(1):18. doi: 10.3390/mi12010018.

引用本文的文献

1
Numerical and Experimental Study of Microchannel Performance on Flow Maldistribution.微通道流动分配不均性能的数值与实验研究
Micromachines (Basel). 2020 Mar 20;11(3):323. doi: 10.3390/mi11030323.
2
A Hybrid Numerical Methodology Based on CFD and Porous Medium for Thermal Performance Evaluation of Gas to Gas Micro Heat Exchanger.一种基于计算流体动力学(CFD)和多孔介质的混合数值方法用于气-气微热交换器热性能评估
Micromachines (Basel). 2020 Feb 20;11(2):218. doi: 10.3390/mi11020218.
3
Editorial for the Special Issue on Gas Flows in Microsystems.
微系统中气体流动专题的社论。
Micromachines (Basel). 2019 Jul 25;10(8):494. doi: 10.3390/mi10080494.