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A Method for Determining the Flammable Limits of Gases in a Spherical Vessel

机译:确定球形容器中气体易燃极限的方法

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The current method for determining the flammable limits for a gas in a closed spherical vessel is based on a specification of the maximum pressure increase during the combustion, usually from 5 to 10% of the initial ambient pressure. This approach is completely arbitrary and is not fundamentally based. For most hydrocarbons this pressure boundary and hence the flammable limits are easy to determine experimentally since an abrupt pressure drop occurs at the flammable limits as the fuel concentration in air is adjusted. However, for some species, particularly hydrogen mixed with air, the drop in maximum combustion pressure is not very abrupt and the fuel concentration can range several percentage points depending on the arbitrary criterion used for the flammable limits.rnThis article will discuss a new approach for determining the flammable limits for a gas in a spherical vessel. The approach is based on the maximum second derivative of pressure rise. The second derivative is indicative of an acceleration of the combustion process and is, hence, fundamentally based. Furthermore, we have identified a new approach to determine the downward propagating flammable limits based on the combustion time, that is, the time that the gas actually burns in the vessel.rnFxperimental data for methane and hydrogen show that the second derivative flammable limit criterion produces slightly conservative values for combustion in air. Visual inspection of the combustion during the tests showed that no visual combustion was observed at the second derivative criterion. For methane, the second derivative criterion resulted in arnflammable range in air from 4.6 to 15.8% methane. For hydrogen these limits are 3.6-75.2%.rnWe believe that this method will provide a much more fundamentally based method to determine both the upper and lower flammable limits of upward flame propagation and also provide a means to determine the downward propagation limits in a spherical combustion vessel.
机译:确定密闭球形容器中气体可燃极限的当前方法是基于燃烧过程中最大压力增加的规范,通常是初始环境压力的5%到10%。这种方法是完全任意的,不是从根本上建立的。对于大多数碳氢化合物,该压力边界和易燃极限很容易通过实验确定,因为在调节空气中的燃料浓度时,在易燃极限处会发生突然的压降。但是,对于某些物种,特别是氢气与空气混合,最大燃烧压力的下降不是很突然,并且燃料浓度可能会根据可燃性限值所使用的任意标准而变化几个百分点。确定球形容器中气体的可燃极限。该方法基于压力上升的最大二阶导数。二阶导数表示燃烧过程的加速,因此是基础。此外,我们发现了一种基于燃烧时间(即气体在容器中实际燃烧的时间)确定向下传播的可燃极限的新方法。甲烷和氢气的实验数据表明,二阶导数可燃极限准则产生了空气中的燃烧值稍微保守一些。在测试过程中目视检查燃烧表明,在二阶导数标准下未观察到目视燃烧。对于甲烷,二阶导数标准导致空气中易燃范围为4.6%至15.8%的甲烷。对于氢气,这些限制为3.6-75.2%。rn我们相信,该方法将提供一种更基本的方法来确定向上火焰传播的可燃极限的上限和下限,并且还提供一种确定球状体向下传播极限的方法燃烧容器。

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