热分层环境下红外光束感烟探测器探测报警时间研究
 
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            VI 
摘  要 
大空间建筑往往存在着危险等级高、火灾水平蔓延速度快的特点,一旦发生
火灾极易造成群死群伤和大面积火灾。由于大空间建筑通常具有一定的高度,受
太阳辐射、室内热源及建筑底部空调系统的影响,室内环境往往在垂直方向上存
在着较大的温度梯度,温度分层现象显著。火灾时烟气羽流受浮力作用上升的现
象受温度分层影响而减弱,严重时环境产生的热障效应将导致烟气无法上升,从
而延缓了探测烟气的时间。为了实现对大空间建筑火灾的快速探测,尽可能减少
人员和财产损失,对热分层环境下烟气羽流上升特性及探测报警时间的相关研究
就显得尤为重要。 
论文针对大空间 15m×15m×30m 的物理模型,就火源释热率在 100~
1000kW、基准环境温度为 13~28℃、温度梯度分别为 0℃/m、0.5℃/m、1.0℃/m
的120 个工况进行了烟气上升运动模拟计算,分析了火源释热率,基准环境温度
及温度梯度对烟气羽流上升的影响。结果表明,烟气羽流上升时间与火源释热率
呈负相关,与基准环境温度及温度梯度呈正相关。三个影响因素中火源释热率对
上升时间的影响最大,温度梯度次之,基准环境温度最小。分析温度分层对烟气
羽流影响的结果表明,火源释热率为 500kW 及以上的烟气羽流均能抵达屋顶,而
火源释热率为 200kW 及以下的烟气羽流因受热障效应影响较大,当环境梯度为
1.0℃/m 时不能到达屋顶。 
论文通过对模拟计算结果的分析,就火源释热率为 300kW和400kW的各工况,
对不同热分层环境和不同基准环境温度下红外光束感烟探测器的探测报警时间进
行了分析。探测报警时间由羽流上升时间 tz和烟气浓度增大至探测器报警阈值的
时间 t’两部分组成。分析结果表明当火源释热率较大时,tz占探测时间的比重较大,
此时分层环境对探测时间的影响非常微小;当火源释热率较小时,t’占探测时间的
比重较大,此时温度梯度较大的分层环境能够显著减少探测时间。此外论文根据
模拟结果还分析确定了红外光束感烟探测器在大空间建筑中的最佳布设方式:在
垂直方向上,当大空间建筑高度低于 9m 时,可单层设置;当高度为 10~14m 时,
可双层设置;当高度为 15~30m 时,可三层设置。在水平方向上,可根据安装间距
不得大于该高度处烟气羽流直径的原则来确定。 
通过对热分层环境下烟气羽流最大上升高度公式的修正及轴心温度计算公式
的推导,应用伯努利方程与数值模拟结果,通过分析羽流上升时间分段发展的特
点,建立了稳定线性热分层环境下轴对称烟气羽流上升时间分两段的求解数学模
VII 
型tz=f(z),计算结果表明所建模型能够很好地反映热分层环境下烟气羽流的上升特
性。计算基准环境温度为 13℃,环境梯度为 0.5℃/m 和1.0℃/m 的12 个工况结果
表明,4m 至分段转折点高度区间内,羽流上升所需时间的模型计算值和模拟值的
标准差均在 0.6s 以内,标准差平均值为 0.42s;在 4m 至屋顶或羽流最大上升高度
的区间内,模型计算值和模拟值的标准差也大部分在 1s 以内,标准差平均值为
0.66s。最后,文章提出了烟气浓度上升至报警阈值所需时间 t’的计算方案及理论求
解思路。 
本文对烟气羽流上升特性及红外光束感烟探测器探测报警时间的相关研究可
为消防性能化设计及相关规范和标准的制定提供一定参考。 
关键词:烟气羽流 大空间建筑 热分层环境 红外光束感烟探测器 上
升时间 探测报警时间  
VIII 
ABSTRACT 
There are always high level of fire risk category and high rate of fire spread in large 
space  buildings,  which  may  result  in  heavy  casualties  in  case  of  fire.  Large  space 
buildings usually have  certain height above  the  floor. So affected by solar radiation, 
indoor heat source and HVAC system, big vertical temperature gradient will form in the 
indoor environment of large space buildings. The rising of smoke plumes is driven by 
buoyancy  force  due  to  the  difference  in  temperature  between  smoke  plumes  and 
ambient enviroment. Therefore, in thermally stratified environments, the difference in 
temperature  will  decrease  with  height,  which  will  delay  or  even  block  up  the  rising 
process  of  smoke  plumes.  Once  the  so  called  heat  barrier  effect  is  produced,  the 
detection time of smoke plumes will increase. In order to fulfill the rapid detection to 
large space building fires and largely avoid casualties and property losses, it is quite 
necessary to do related research on rising characteristic of smoke plumes and detection 
time in thermally stratified environments.   
A building model that measures 15 by 15 by 30 is built to simulate and analyze the 
infulence from fire heat release rate, reference temperature and temperature gradient on 
the  rising  process  of  smoke  plumes  when  fire  heat  release  rate  is  100~1000kW, 
reference temperature  is  13~28℃  and  temperature  gradient  is  0~1℃/m  .  The  120 
numerical simulation  and analyzed results demonstrate  that  the rising time of smoke 
plumes  has  a  positive  correlation  with  fire  heat  release  rate  and  has  a  negative 
correlation  with  reference temperature  and  temperature  gradient.  Besides,  fire  heat 
release rate  affects  the  rising  time  most,  the  temperature  gradient  does  less,  and  the 
reference temperature  does  the  least.  The  analysis  results  of  the  influence  from 
thermally stratified environment on smoke plumes show that when fire heat release rate 
is greater than or equal to 500kW, smoke plumes can easily reach the ceiling. But when 
fire heat release rate is less than or equal to 200kW, smoke plumes are notably affected 
by heat barrier effect and can’t reach the ceiling when temperature gradient is 1℃/m. 
According  to  the  simulation  and  calculation  results,  the  cases  whose  fire  heat 
release rate is 300kW or 400kW are chosen to analyze the the detection time of infrared 
beam smoke detector. The detection time consists of the rising time tz and the time t’ 
IX 
during which the smoke concentration rises up to alarm threshold. The analysis results 
indicate that when fire heat release rate is large, tz is in a larger proportion of detection 
time. In that case thermally stratified environments have little effect on detection time. 
But when fire heat release rate is small, t’ is in a larger proportion of detection time. In 
this instance, the detection time can be remarkably reduced by the  great temperature 
gradient. In addition, according to the analysis on the detection time of infrared beam 
smoke  detector  under  different  fire  heat  release  rates  and  thermally  stratified 
environments, the optimal form and location of infrared beam smoke detector in large 
space buildings is determined. When building height is below 9 meters, the detectors 
can be set within a single level. When building height is 10~14 meters, the detectors can 
be set at two levels. When building height is 15~30 meters, the detectors can be set at 
three levels. The spacing between beams is based on the narrowest potential width of 
the plume at the level of detection. 
Meanwhile,  through  modifying  the  calculating  formula  of  maximum  rise  of  fire 
smoke  plumes  and  formula  derivation  of  centreline  plume  temperature,  a  piecewise 
mathematical model tz=f(z)  is  presented  to  calculate  the rising time of  axisymmetric 
plume fronts in stably linearly thermally stratified environments by applying Bernoulli 
equation  and  numerical  simulation.  The  rising  characteristic  of  smoke  plumes  in  in 
thermally stratified environments can be well represented by the mathematical model. 
When reference temperature is 13℃ and temperature gradient is 0.5℃/m and 1.0℃/m 
respectively,  the  simulation  results  show  that  the  standard  deviations  between 
theoretical results and simulated results of 12 fire cases are below 0.6 second in the 
segment of 4~ zsep and are mostly below 1 second in the segment of 4~29(or 4~
m
z
). The 
average of standard deviations are 0.42 second and 0.66 second respectively in above 
two segments. At last, a scheme to calculate the during time when smoke concentration 
rises up to alarm threshold is introduced.   
In  the  paper,  the  related  research  of  rising  characteristic  of  smoke  plumes  and 
detection  time  of  infrared  beam  smoke  detector  is  useful  to  performance-based  fire 
design and will offer reference to making out correlative criterions and standards. 
Key words: Smoke plume, Large space buildings, Thermally stratified 
environments, Infrared beam smoke detector, Rising time, 
Detection time. 
X 
目  录 
中文摘要 
ABSTRACT 
第一章 绪论 .......................................................... 1 
§1.1 研究背景及意义 ............................................ 1 
§1.2 烟羽流特性及探测器探测时间研究现状 ........................ 2 
§1.2.1 热分层环境下烟羽流特性研究现状 ...................... 2 
§1.2.2 烟羽流上升时间及探测时间研究现状 .................... 3 
§1.2.3 火灾 CFD 模拟技术发展现状 ............................ 4 
§1.3 课题研究基本思路及其主要研究内容 ........................... 6 
§1.3.1 课题研究的基本思路 .................................. 6 
§1.3.2 主要研究内容 ........................................ 6 
第二章 火灾探测器选用与布局的分析 .................................... 8 
§2.1 火灾发展过程与人员安全疏散分析 ............................ 8 
§2.1.1 建筑火灾发展过程 .................................... 8 
§2.1.2 火源及其释热率 ...................................... 9 
§2.1.3 人员安全疏散分析 ................................... 11 
§2.2 火灾探测器的选用及布局的思考 ............................. 12 
§2.2.1 常用的火灾探测器及选用原则 ......................... 12 
§2.2.2 红外光束感烟探测器安装位置设置存在的问题 ........... 15 
§2.2.3 设置红外光束感烟探测器安装位置的思考 ............... 17 
§2.3 本章小结 ................................................. 18 
第三章 红外光束感烟探测器探测时间数值模拟研究 ....................... 19 
§3.1 模拟案例设定 ............................................. 19 
§3.1.1 FDS 软件介绍 ........................................ 19 
§3.1.2 羽流形态及其分类 ................................... 20 
§3.1.3 模型建立与测点布置 ................................. 21 
§3.1.4 火源设置及网格划分 ................................. 22 
§3.1.5 火灾场景设置 ....................................... 24 
§3.2 烟羽流环境模拟结果分析 ................................... 25 
§3.2.1 分层环境作用下烟羽流温度场及速度场分析 ............. 25 
§3.2.2 羽流上升影响因素分析 ............................... 30 
XI 
§3.2.3 探测报警时间分析 ................................... 40
§3.2.4 探测器最佳布置方案 ................................. 44
§3.3 本章小结 ................................................. 46
第四章 红外光束感烟探测器探测报警时间理论分析 .......................47
§4.1 均匀环境下烟气羽流上升时间理论分析 ....................... 48
§4.2 稳定线性热分层环境下烟气羽流上升时间分段求解模型 ......... 50
§4.2.1 烟气羽流最大上升高度和中性浮力点高度 ............... 50
§4.2.2 环境温度及烟气羽流轴心温度 ......................... 51
§4.2.3 上升时间分段求解模型建立 ........................... 53
§4.3 烟气浓度增大至报警阈值所需时间的分析 ..................... 62
§4.4 本章小结 ................................................. 64
第五章 结论及展望 ...................................................65
§5.1 结论 ..................................................... 65
§5.2 展望 ..................................................... 66
参考文献 ............................................................67
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                作者:高德中
                分类:高等教育资料
                价格:15积分
                        属性:76 页
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        时间:2025-01-09
    
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