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首页> 外文期刊>Environment control in biology >Concept of the Un-cooled Air in a Greenhouse Cooled by Fogging in Summer: An Aid to Estimate the Cooling Efficiency of a Fogging System
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Concept of the Un-cooled Air in a Greenhouse Cooled by Fogging in Summer: An Aid to Estimate the Cooling Efficiency of a Fogging System

机译:夏季通过雾气冷却的温室中未冷却空气的概念:估算雾气系统冷却效率的辅助手段

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The current definition of the evaporative cooling efficiency (η_c) can be applied only for a greenhouse with a wet pad-fan system, in which no sensible or latent heat is added to the air during the cooling process. However, η_c of the wet pad-fan system cannot be applied for a greenhouse with a fogging system, in which sensible and latent heat are added to the air during the cooling process. The purpose of this study is to define η_c correctly for a greenhouse with a fogging system and to describe the fogging process. For this purpose, the concept of un-cooled air was developed, which is the greenhouse air gaining sensible and latent heat from the cover, the floor and the plant surfaces. The dry bulb temperature of un-cooled air (T_u) was defined based on the sensible heat added to the air. Sensible heat strongly depends on the convective heat transfer coefficients in the greenhouse (i.e., between the air and the cover, the floor, the plant surfaces). Therefore, different relations expressing each coefficient were examined. η_c was defined using T_u and the measured values of the dry and wet bulb temperatures in the greenhouse with fog. Values of T_u and η_c were estimated in a greenhouse located in the Tokyo area, Japan, and cooled by intermittent fogging on a hot summer day. The results show that value of 71, was found to be not very sensitive to the selection of convective coefficients, with maximum relative error of 4% observed using different expressions for the convective coefficients from the literature. The assumption that the fogging process takes place in the greenhouse air at a constant wet bulb temperature is practically acceptable.
机译:当前对蒸发冷却效率(η_c)的定义仅适用于带有湿垫风扇系统的温室,在该温室中,在冷却过程中未向空气中添加显热或潜热。但是,湿式垫扇系统的η_c不适用于带有雾化系统的温室,在该系统中,在冷却过程中将显热和潜热添加到空气中。本研究的目的是为带有雾化系统的温室正确定义η_c,并描述雾化过程。为此,开发了非冷却空气的概念,即从覆盖物,地板和植物表面获取显热和潜热的温室空气。基于添加到空气中的显热定义未冷却空气的干球温度(T_u)。显热很大程度上取决于温室中的对流传热系数(即,空气与覆盖层,地板,植物表面之间)。因此,研究了表达每个系数的不同关系。 η_c是使用T_u和带雾温室中干球温度和湿球温度的测量值定义的。 T_u和η_c的值是在位于日本东京地区的温室中估算的,并在炎热的夏季通过间歇性雾化冷却。结果表明,发现值71对对流系数的选择不是很敏感,使用文献中对流系数的不同表达式观察到的最大相对误差为4%。雾化过程是在恒定湿球温度下在温室空气中进行的假设在实践中是可以接受的。

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