Numerical simulation of heat transfer cooling down by water in microgap structure

Jiancheng Shen, Z. Wen, Jinsong Zhang
{"title":"Numerical simulation of heat transfer cooling down by water in microgap structure","authors":"Jiancheng Shen, Z. Wen, Jinsong Zhang","doi":"10.1109/ICEPT.2015.7236776","DOIUrl":null,"url":null,"abstract":"With the increase of power density in chip, the electronic products have to face the challenge of heat dissipation technology. For the heat transfer of microgap, the fluid flows through the pathway which has a large ratio between the width and depth in the cross-section and a small ratio between the length and width in the top view. The rectangular microgap was built before modeling and Fluent software was applied to simulate and analyze the temperature field. The input heat flux was 8.3 × 104 w/m2, the water flow rate was 0.32 m/s, and the inlet water temperature was 300 K. Some conclusions had been drawn as following. The temperature distribution was symmetrical to the Z axis. The temperature gradient took a radial pattern from the model center to edges. The isotherm in microgap had a “U” shape, which indicated that the water flowing in center had a better capability for heat transfer. The isotherms presented the regular onion shape of wall temperature while the microgap depth varied from 0.05 mm to 0.7 mm. Each isotherm onion diagram had a tip at the right and a bottom at the left to correspond with the water flowing path from inlet to outlet. The center of wall had been cooled down more efficiently and the low temperature region was distributed along the water flowing path. When the depth increases to be 0.9 mm and 1.1 mm, the isotherm curves were so flat that the onion shape had been disappeared. This could be contributed to the large microgap depth reduce the water flow rate. The wall temperature curve had an ascending fluctuation with the increasing of microgap depth.","PeriodicalId":415934,"journal":{"name":"2015 16th International Conference on Electronic Packaging Technology (ICEPT)","volume":"30 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2015-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2015 16th International Conference on Electronic Packaging Technology (ICEPT)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ICEPT.2015.7236776","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

With the increase of power density in chip, the electronic products have to face the challenge of heat dissipation technology. For the heat transfer of microgap, the fluid flows through the pathway which has a large ratio between the width and depth in the cross-section and a small ratio between the length and width in the top view. The rectangular microgap was built before modeling and Fluent software was applied to simulate and analyze the temperature field. The input heat flux was 8.3 × 104 w/m2, the water flow rate was 0.32 m/s, and the inlet water temperature was 300 K. Some conclusions had been drawn as following. The temperature distribution was symmetrical to the Z axis. The temperature gradient took a radial pattern from the model center to edges. The isotherm in microgap had a “U” shape, which indicated that the water flowing in center had a better capability for heat transfer. The isotherms presented the regular onion shape of wall temperature while the microgap depth varied from 0.05 mm to 0.7 mm. Each isotherm onion diagram had a tip at the right and a bottom at the left to correspond with the water flowing path from inlet to outlet. The center of wall had been cooled down more efficiently and the low temperature region was distributed along the water flowing path. When the depth increases to be 0.9 mm and 1.1 mm, the isotherm curves were so flat that the onion shape had been disappeared. This could be contributed to the large microgap depth reduce the water flow rate. The wall temperature curve had an ascending fluctuation with the increasing of microgap depth.
微间隙结构中水冷却传热的数值模拟
随着芯片功率密度的不断提高,电子产品面临着散热技术的挑战。对于微间隙的换热,流体流过截面上宽深比大、顶视图上长宽比小的通道。建模前先建立矩形微间隙,利用Fluent软件对温度场进行仿真分析。输入热流密度为8.3 × 104 w/m2,水流速率为0.32 m/s,进水温度为300 K。得出的一些结论如下。温度分布沿Z轴对称。温度梯度从模型中心到边缘呈放射状分布。微间隙内的等温线呈“U”型,说明在中心流动的水具有较好的换热能力。当微隙深度在0.05 ~ 0.7 mm范围内变化时,等温线呈规则的洋葱状壁温。每个等温线洋葱图右边有一个尖,左边有一个底,以对应水从入口到出口的流动路径。壁面中心冷却效率更高,低温区沿水流路径分布。当深度增加到0.9 mm和1.1 mm时,等温线曲线变得平坦,洋葱形消失了。这可能与较大的微隙深度降低水流速率有关。壁面温度曲线随微隙深度的增加呈上升趋势。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信