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加齿调控个性化风口流场多尺度湍涡结构的实验研究

崔旭佳 唐湛棋 姜楠 刘俊杰

崔旭佳, 唐湛棋, 姜楠, 等. 加齿调控个性化风口流场多尺度湍涡结构的实验研究[J]. 实验流体力学, 2018, 32(2): 68-73. doi: 10.11729/syltlx20170110
引用本文: 崔旭佳, 唐湛棋, 姜楠, 等. 加齿调控个性化风口流场多尺度湍涡结构的实验研究[J]. 实验流体力学, 2018, 32(2): 68-73. doi: 10.11729/syltlx20170110
Cui Xujia, Tang Zhanqi, Jiang Nan, et al. Experimental investigation of multi-scale turbulent eddy adjustment in personal gasper flow with wedges[J]. Journal of Experiments in Fluid Mechanics, 2018, 32(2): 68-73. doi: 10.11729/syltlx20170110
Citation: Cui Xujia, Tang Zhanqi, Jiang Nan, et al. Experimental investigation of multi-scale turbulent eddy adjustment in personal gasper flow with wedges[J]. Journal of Experiments in Fluid Mechanics, 2018, 32(2): 68-73. doi: 10.11729/syltlx20170110

加齿调控个性化风口流场多尺度湍涡结构的实验研究

doi: 10.11729/syltlx20170110
基金项目: 

国家自然科学基金项目 11332006

国家自然科学基金项目 11732010

国家自然科学基金项目 11572221

国家自然科学基金项目 11502066

详细信息
    作者简介:

    崔旭佳(1992-), 男, 河北保定人, 博士研究生。研究方向:实验流体力学。通信地址:天津大学(北洋园校区)力学大楼412室(300354)。E-mail:jiayu_cui@tju.edu.cn

    通讯作者:

    姜楠, E-mail:nanj@tju.edu.cn

  • 中图分类号:  O358;V223+.2

Experimental investigation of multi-scale turbulent eddy adjustment in personal gasper flow with wedges

  • 摘要: 客机座舱个性化风口是座舱环控系统中重要的送风单元,其主要作用为快速通风、换热,对乘客的热舒适起到改善作用,但现有个性化送风常引起乘客头部的强烈吹风感。本文通过对现有个性化风口进行边缘加齿的优化设计,调控风口流场中不同尺度的湍涡成分,降低吹风感,从而获得使人体更为舒适的气流流场。实验中使用高时间分辨率热线风速仪,精细测量安装不同尺寸加齿喷嘴的风口流场,采用子波分析的方法对流场多尺度湍涡成分进行分析,对比不同尺寸大小的加齿喷嘴对个性化风口流场多尺度湍涡成分的调控效果,得出齿尖间距离为5mm时,个性化风口的送风使人体更舒适。个性化风口圆环射流经过加齿调控,增强了动量、能量和质量交换,降低了含能尺度的湍流强度,从而降低了吹风感,提高了流场的舒适性。
  • 图  1  环境模型舱尺寸示意图

    Figure  1.  Schematic of the size of environment mockup cabin

    图  2  个性化风口尺寸示意图

    Figure  2.  Schematic of the size of the personal gasper

    图  3  4种加齿结构的尺寸示意图

    Figure  3.  Schematic of the size of four wedge structures

    图  4  有无加齿个性化风口射流中心线平均速度剖面

    Figure  4.  Comparison of mean velocity profiles in the axial direction of personal gasper jet flow with and without wedges

    图  5  有无加齿个性化风口射流径向无量纲平均速度剖面

    Figure  5.  Comparison of non-dimensional mean velocity profiles in the radial direction of personal gasper jet flow with and without wedges

    图  6  有无加齿个性化风口射流中心线湍流强度剖面

    Figure  6.  Comparison of turbulence level proliles of personal gasper jet flow on the central line with and without wedges

    图  7  不加齿结构径向(x=13.13D0r=40mm)与加齿结构xy径向(z=13.13D0y=40mm)能量随尺度分布对比

    Figure  7.  Comparsion of turbulent fluctuating kinetic energy evolutions across scales at x=13.13D0, r=40mm in personal gasper jet flow with and without wedges

    图  8  轴向位置为13.13D0, 径向位置为40mm处空间测点的瞬时速度信号的子波系数等值云图

    Figure  8.  The contour of wavelet coefficients across time and scale parameters at x(z)=13.13D0, r(x or y)=40mm in personal gasper jet flow with and without wedges

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出版历程
  • 收稿日期:  2017-08-22
  • 修回日期:  2017-11-17
  • 刊出日期:  2018-04-25

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