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首页> 外文期刊>Journal of Agricultural Engineering Research >Condensation and radiation transmittance of greenhouse cladding materials, Part 2: results for a complete condensation cycle
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Condensation and radiation transmittance of greenhouse cladding materials, Part 2: results for a complete condensation cycle

机译:温室覆盖材料的凝结和辐射透射率,第2部分:完整凝结循环的结果

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摘要

The radiation transmittances of a standard glass plate and an ordinary polyethylene (PE) film were measured during a complete condensation cycle (dry phase; condensation without run-off; condensation with run-off evaporation phase). The measurements were performed in a specially developed laboratory measuring unit, using perpendicularly polarized monochromatic radiation in the range of photosynthetically active radiation (PAR). Transmittances were determined for three angles of incidence: 0, 30, and 60°. In the dry phase, at normal incidence, the transmittance of the ordinary PE film (about 90% was almost similar to the one of the standard glass plate (about 89%). For increasing incidence angles, the transmittance of both dry cladding materials decreased. As soon as condensate was formed, a quick decrease of the transmittance was found for the PE film for the three angles of incidence (23% at normal incidence). This transmittance decrease adopted an equilibrium value after approximately 1 h. On the glass plate, however, the quick drop of the transmittance was only observed for higher incidence angles. At normal incidence, the effect of condensate on the transmittance of the glass plate was found to be negligible. In most cases, the occurrence of run-off caused a slight change of the transmittance of both cladding materials with respect to the phase of condensation without run-off. As soon as the evaporation of the condensate started, the transmittance returned gradually to its original value for the dry state. In general, it can be stated that the effects of condensation on the radiation transmittance were greater on the PE film than on the glass plate.
机译:在完整的冷凝周期(干燥阶段;无径流冷凝;有径流蒸发相冷凝)期间,测量标准玻璃板和普通聚乙烯(PE)膜的辐射透射率。测量是在专门开发的实验室测量单元中进行的,使用光合有效辐射(PAR)范围内的垂直偏振单色辐射。确定了三个入射角的透射率:0、30和60°。在干相中,在法向入射时,普通PE膜的透射率(约90%几乎与标准玻璃板的透射率(约89%)相似),随着入射角的增加,两种干包层材料的透射率均降低。 。一旦形成冷凝水,就发现PE膜在三个入射角(法向入射时为23%)的透射率迅速降低,这种透射率的降低在大约1 h后采用平衡值。但是,只有在较大的入射角下,透射率才出现快速下降,在法向入射时,冷凝物对玻璃板透射率的影响可以忽略不计,在大多数情况下,径流的发生会引起两种包层材料的透射率相对于凝结相略有变化而没有流失,一旦冷凝物开始蒸发,透射率便逐渐恢复到其原始值干燥状态的值。通常,可以说凝结对辐射透过率的影响在PE膜上比在玻璃板上要大。

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