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KMID : 1171820030180030027
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Journal of Environmental and Sanitary Engineering
2003 Volume.18 No. 3 p.27 ~ p.34
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A Study on the Reduction of Entry Loss by Inner Structure in Square Hood in Industrial Ventilation System
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Bae Hyun-Joo
Yang Won-Ho
Kim Jong-Oh
Son Bu-Soon
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Abstract
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An objective of local exhaust hood design is to design the hood to operate as efficiently as possible. The greatest loss normally occurs at the entrance to the duct, due to the vena contracta in the throat of the duct. This can be accomplished by minimizing the loss that results from the vena contracta. There have been little studied to be cost-effective approach as installing simple instrument inside the throat of the hood. The aims of this paper were to minimize entry loss using inner square, and to measure the effect of inner square when installed inside hood throat. The results of this study were as follows; First, the magnitude of vena contracta could be considered as the difference between direct measured velocity and calculated velocity, which is from Bernoulli theory. In circle hood, calculated velocity and direct measured velocity were 10.7m/sec and 10.3m/sec, respectively. And the calculated velocity and direct measured velocity in square hood were 7.7m/sec and 6.5m/sec, respectively. Second, effect of inner square by width was carried out. The widths of inner square were L/1(18m), L/2(9cm), L3(6cm) and L6(3cm). In case inner square was installed with 3cm width, the entry of coefficient was 0.93, comparing with 0.85 of entry of coefficient of general hood. Third, effect of inner square by distance from hood inside surface to inner square was carried out. The distances were L3(6cm), L6(3cm), L9(2cm) and L18(1cm). In case the distance was 3cm, the best efficiency was shown (Ce-0.93). Fourth, effect of inner square by location from hood entry to duct inside was carried out. The locations of inner square were entry(0cm), L6(3cm), L3(6cm), L2(9cm) and L/1(12cm). In case the location was 0cm, 3cm and 6cm, the entry of coefficients were 0.93, 0.92 and 0.90, respectively.
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