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1.
以柴油为研究对象,搭建了小尺度油罐火实验台,采用理论分析与实验研究相结合的方法,开展了有风条件下不同液位深度和罐顶开口宽度的小尺度油罐火火焰倾角的实验研究。结果表明,火焰倾角随风速的增加先迅速增加,然后趋于平稳。在相同的罐顶开口宽度和风速条件下,火焰倾角随着液位深度的增加呈现出减小的趋势。这是因为火焰微元在油罐开口处的速度随着液位深度的增加而增加,风速对火焰倾角的影响显著减小。当风速和液位深度一定时,质量损失速率随罐顶开口宽度的增大而增大,火焰倾角随着罐顶开口宽度的增大逐渐减小。  相似文献   

2.
海上石油泄漏常规的处理方法是原位燃烧,加速其燃烧并使其燃尽是降低其对生态环境影响的重要措施之一。以正庚烷为燃料,在油池内插入竖直铝板,研究不同高度铝板对池火燃烧行为的影响。结果表明,插板对池火燃烧速率以及火焰高度具有明显的增强作用,随着板的高度的增加,增强作用先增大后减小,当H_p/D(板高与油池直径之比)为3.5时,增强作用最大。火焰高度、板的温度、热通量以及燃烧速率的变化趋势一致,它们的临界点均在H_p/D=3.5附近。插板后燃烧速率增大主要是因为插板自身的热传导导致了燃料的核态沸腾,使燃料接受的热反馈增大,从而加快了燃料的蒸发,增大了燃烧速率。  相似文献   

3.
池火特性参数计算及其热辐射危害评价   总被引:17,自引:4,他引:13  
可燃性油品池火的火焰及其产生的热辐射 ,可能导致周围人员伤亡或设备设施损坏。笔者介绍了油品池火的质量燃烧速率、火焰长度、火焰倾角及火焰后拖量等特性参数的计算方法 ,提出了池火热辐射强度的预测模型 ,给出了热辐射伤害 /破坏准则 ,并进行了模拟计算和评价。  相似文献   

4.
Spill fires are common during oil product storage and transportation after a loss of containment. Since the burning fuel is moving and the fuel depth is quite shallow, the burning rate in a spill fire is different from that of a pool fire with a static burning zone. Unlike pool fires, which have been studied for decades and have well-established correlations for burning rate, research on spill fires is inadequate. In this paper, continuously released n-heptane spill fire experiments were conducted on open water surfaces with varying fuel discharge rates. The pool diameters were measured, and the spill fire burning rates were estimated based on a dynamic balance between fuel supply and combustion. The burning rates in n-heptane pool fires from the literature were reviewed and compared with the estimated burning rates in spill fires of the same dimension. The spill fire burning rate was found to be close to that in a pool fire during the initial burning phase but lower than that in a bulk burning pool fire and that in a “fuel-level-controlled” pool fire. The distinction between the burning rates of spill fires and pool fires is explained by the heat balance analysis of the fuel layer. A model for the spill fire burning rate was proposed accordingly. The results calculated with the presented model are closer to the measured data than those calculated with pool fire models.  相似文献   

5.
为了分析不同通风条件对柴油池火燃烧特性及引燃特性的影响,进行205 mm带水垫层柴油池火的引燃实验,通过对池火燃料的质量损失速率、火焰高度、温度及热辐射等的监测,分析通风环境中柴油池火的热传递规律。结果表明:当风速为0.5 m/s时,火灾进入旺盛阶段的时间提前,火焰平均温度最高;当风速为1 m/s时,风速的增加导致油池火的质量损失速率增加,位于主火源下风向的待引燃火源获得的热辐射通量增大,火灾旺盛阶段火焰的平均温度降低,火焰高度降低,下风向相邻油盘引燃的时间提前;1 m/s情况下,205 mm带水垫层柴油池火的安全间距需增加到1D以上;通风环境对池火发展及蔓延的影响是显著的,应适当加大下风向可燃物的安全间距,合理选择通风排烟风速,优化火灾应急救援策略。  相似文献   

6.
为研究低压条件下油品燃烧特性,以乙醇油池火为研究对象,搭建高原油池火实验平台,研究不同油盘直径下乙醇油池火燃烧规律,分析燃烧速率、火焰高度和火焰脉动等参数随时间的变化规律。研究结果表明:低压条件下的乙醇油池火,燃烧速率小于同等尺度常压条件下的油池火燃烧速率;乙醇油池火的燃烧速率随油盘直径增加变化不明显;火焰高度随油池直径增加呈现显著上升趋势,并拟合推导出适用于低压乙醇池火的火焰高度公式;火焰脉动频率随油池直径增大而减小,并给出火焰脉动与油池直径的经验公式。研究结果可丰富低压乙醇燃烧的油池火实验数据,为低压乙醇油池火的风险评估提供参考。  相似文献   

7.
李永和  刘启金 《火灾科学》2013,22(4):226-231
通过改变风速、液位深度的大小,研究边界条件变化对酒精池火火焰长度的影响。研究结果表明:在无量纲液位深度小于一定值时,酒精池火的火焰长度会随着风速的增加而增大,当无量纲液位深度较大时,油盘外部酒精池火的火焰长度基本为0。风速相同而液位深度不同时,酒精池火的火焰长度会随着液位深度的增大首先增大,而后逐渐减小。这主要是因为,液位深度较大时,燃料表面的供氧量降低导致燃烧效率降低,最终导致火焰长度的减小。  相似文献   

8.
党晓贝  何亚平  汪箭 《火灾科学》2018,27(4):213-221
采用实验和FDS数值模拟相结合的方法,探讨了边沿高度对油池火燃烧特性的影响。在实验部分,研究了燃烧速率和表观火焰高度随边沿高度的变化趋势,并分别分析了各个阶段的热反馈机制。在实验获得不同尺度、边沿高度正庚烷油池火燃烧速率的前提下,建立相应尺度的不同边沿高度油池火的Fire Dynamics Simulator(FDS)计算模型以针对火焰高度进行了数值模拟研究,分析了实际火焰高度、火焰下探高度随边沿高度的变化趋势,并提出了相关的无量纲拟合式。  相似文献   

9.
The spread of burning fuel spilled from oil product containers during offshore storage and transportation may cause large damage and trigger further accidents. Some analytical models already exist to predict the spread and burning behavior of liquid fuel spill fires, however, few experimental studies have been conducted to verify the model results. In this paper, continuous n-heptane spill fire experiments were conducted in a rectangular trench covered with water. The burning area, fuel spread rate, and thermal flux with different discharge flow rates and ignition delay times were investigated by both experimental and modeling means. The spill fire burning area, with 5 typical phases during burning, has a quasi-steady value which is directly proportional to the discharge rate but irrelevant to the ignition delay times. The steady burning rate, as the ratio of discharge rate over burning area, was estimated. A spread model was modified to simulate the spread of continuous liquid fuel spill fires in a one-dimensional channel, based on the balance between gravity and viscous forces. A cuboid solid flame model was used to compute the thermal flux from spill fires. The burning fuel spread and the heat flux calculated by the models agree with the experimental results.  相似文献   

10.
Liquefied petroleum gas (LPG) has potential pool fire risks due to its flammability. The configuration of pool fires plays a significant role when applying the solid flame model or point source model to assess the risks from heat radiation. However, no existing correlations can precisely predict the configuration of large LPG (100% propane) pool fires. To enhance the fundamental understanding on how pool diameter and wind velocity can influence the configuration of large LPG pool fires, an experimentally validated Computational Fluid Dynamics (CFD) model is employed to simulate fires using different burning rate models. Fire temperature profiles, flame heights, and flame tilts predicted by the CFD model were compared with empirical models and experimental data. Accordingly, new correlations for flame height and flame tilt as functions of pool diameter D and wind velocity uw have been developed. The comparisons demonstrate that the new correlations have the best overall accuracy in the prediction of flame height and tilt for large LPG pool fires under different conditions (10 m ≤ D ≤ 20 m, 0 ≤ uw ≤ 3 m·s−1).  相似文献   

11.
文中用CFD技术对甲苯池火灾进行数值模拟,首先对甲苯火焰进行数值计算,得到在稳定的横向风条件下,甲苯燃烧的峰温、产物组分、瞬时速度等火焰特征参数以及其空间分布情况:火焰温度的最高点在对称面y=0上,最高温度为1778K,火焰倾斜角度为26°(与竖直方向夹角),火焰高为22.5m。然后应用CFD软件F luent对池火灾进行热辐射模拟,模拟结果表明:对于锰钢材料、内径为20m甲苯储罐,稳态有风池火灾情况下,相邻两储罐之间安全距离在上风向为59m,下风向为72m。由于描述燃烧过程和湍流情况的数学物理模型还不太完善、对大气状况的简化等原因,结果偏保守,文中对此进行了分析讨论。此项研究为CFD技术研究碳氢化合物火灾的一个尝试。  相似文献   

12.
提出了一种可精确控制燃料床填充比的方法。以刨花为燃料,开展了可燃物填充比对火蔓延影响的系统性实验研究。分析了火焰长度、火焰倾斜角、火蔓延速率、质量损失速率和热流密度随填充比的变化规律。研究发现,随填充比增大,火焰长度逐渐减小,火焰倾斜角逐渐增加,导致火焰热辐射降低、火蔓延速率减小。当填充比小于0.06时,燃料消耗率接近于1;当填充比在0.06~0.08内变化,燃料消耗率突然降低,说明此区间存在一个临界填充比,使得燃料床由热薄型向热厚型转变。  相似文献   

13.
为了评价油品储运过程中的流淌火灾风险,提出1种基于FERC模型的油品流淌火灾定量风险评估方法。以某汽油管道为例,分析大孔泄漏、中孔泄漏、小孔泄漏3种模式下流淌火各参数的动态变化过程,计算管道周边不同位置处的个人风险值。研究结果表明:流淌火燃烧面积的最大值随泄漏速率的增加而增大,对于给定的算例条件,大孔泄漏情景下的最大燃烧半径较小孔泄漏增大了18.4倍;相较小孔泄漏,大孔泄漏下安全距离增大了6.7倍;在距离泄漏点100 m的位置,小孔泄漏、中孔泄漏和大孔泄漏条件下的辐射热流密度值分别为0.13,1.34,8.02 kW/m2;距离泄漏点34 m处时,大孔泄漏已经占总个人风险的99%;在开展风险评价时,应着重分析大孔泄漏的情景。  相似文献   

14.
在全尺寸热释放速率实验台的基础上,搭建有风条件池火实验平台,开展了不同风速条件下的航空煤油池火燃烧实验,实验所用正方形油盘的边长分别为0.2m、0.3m和0.4m,风速范围为0 m.s-1至4.99 m.s-1。实验结果表明,风速为0 m.s-1时航空煤油池火的燃烧速率随油盘尺寸增大而单调递增,实验值与理论值的差距随风速增大而减小。实验所得.m″windy/.ms″till与v/D呈线性关系,与前人结论一致,但实验所得参数与前人值不同。同尺寸油盘池火的热释放速率峰值来临时间随风速增大有减小的趋势;不同尺寸油池火的燃烧速率随风速增加而单调递增。对不同尺寸油池火的热释放速率峰值随风速的变化规律作了讨论。  相似文献   

15.
针对液体燃油储运过程中泄漏引发的火灾爆炸事故,设计并搭建流淌槽坡度可调式液体燃油流淌火燃烧试验平台,开展连续泄漏正庚烷流淌火试验。选择水平表面(0°)流淌试验作为基准,改变流淌槽的坡度(0.5°,1°和3°),研究分析不同泄漏速率下连续泄漏正庚烷流淌火的燃烧面积、燃烧速率等燃烧特征参数的变化规律。结果表明:1)连续泄漏正庚烷流淌火燃烧特征参数均随泄漏速率增加而明显增加;2)坡度对连续泄漏正庚烷流淌火燃烧特性影响显著,即使流淌槽坡度增加0.5°,其燃烧特性即发生明显改变;3)连续泄漏正庚烷流淌火的平均稳定燃烧速率随流淌槽坡度的增加反而减小。  相似文献   

16.
开展了点火源引燃的上坡火蔓延实验,用刨花丝为燃料,研究不同坡度角对火蔓延速率、火线夹角、火焰长度、火焰倾斜角等的影响规律,并简要分析了火焰对火前未燃燃料的辐射传热。发现平坡条件下会形成圆形火线,而坡度条件下会形成泪滴状的火线。当坡度角高于20°时,上坡火蔓延速率随坡度的增大迅速上升。  相似文献   

17.
以正庚烷为研究对象,开展了不同因素耦合作用下小尺度油罐火燃烧特性的实验研究。结果表明:在不改变其他工况条件下,开口因子直接影响燃料燃烧速率,发现不同开口因子下燃烧速率与全开口下燃烧速率之比始终正比于对应的开口面积之比,且之间存在着相应的关系式。在实验所测两种液位6cm和8cm下,其燃烧速率变化不大,由此可发现,在该实验液位下油罐火液位高度不是影响燃烧速率的主要因素。在不同的风速下,随着风速的增加燃烧速率逐渐增加并趋于一定值,且不同开口因子下风速对燃烧速率的影响程度不同。风速对开口因子大的油罐燃烧速率的影响小于开口因子较小的油罐。  相似文献   

18.
为研究多火源条件下火旋风的相互作用,利用四面边墙夹缝式实验装置对3种不同直径油盘形成的火旋风进行实验研究。由电子天平记录的燃料质量随时间变化曲线,得到准稳态阶段火旋风的质量燃烧速率;利用摄像机记录的火焰连续图像,获得火焰高度;基于实验现象及实验数据对质量燃烧速率、火焰高度和火焰形态的分析,提出多火源火旋风质量燃烧速率和火焰高度的半经验线性关系式。研究表明:大直径油盘形成的火旋风比小直径油盘更容易受到拖拽力和涡量的作用影响。  相似文献   

19.
油品火灾扬沸前兆现象的实验研究   总被引:1,自引:0,他引:1  
本文研究典型油品扬沸前兆期的火行为。应用火焰显示技术观察扬沸前兆期的火焰结构;测量扬沸过程中油、水层的温度——时间历程;在时域、频域上分析扬沸前兆的微爆噪声特性;并在原理上提出诊断,预报油品火灾扬沸发生的新途径。  相似文献   

20.
This study presents a quantitative analysis and interpretation of the variation in oil tank fire flame lengths for different oil tank sizes, top cover widths, and horizontal air flow velocities. The experimental results show that, at first, the flame length rises slowly with an increase in air flow speed. Then, once over a critical speed (0.6 m/s), the flame length decreases significantly with a further increase in air flow speed. Based on the characteristic length, a new dimensionless heat release rate is obtained, allowing the correlation between flame length, air flow speed, and dimensionless heat release rate to be calculated, which can be used to predict the flame length of an oil tank fire under different air flow speeds, lip heights, and cover widths.  相似文献   

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