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Flow resistance of bottom trawl nets and scale effect in their model experiments

저층 트롤어구의 유수저항 특성 및 모형 실험시의 축척비 영향

  • Kim, Dae-Jin (Department of Fisheries Science, Chonnam National University) ;
  • Kim, Dae-An (Division of Marine Technology, Chonnam National University) ;
  • Kim, Tae-Ho (Division of Marine Technology, Chonnam National University) ;
  • Shin, Hyeong-Ho (Division of Marine Technology, Chonnam National University) ;
  • Jang, Duck-Jong (Department of Maritime Police Science, Chonnam National University) ;
  • Cha, Bong-Jin (Fisheries Engineering Division, National Fisheries Research & Development Institute)
  • 김대진 (전남대학교 수산과학과) ;
  • 김대안 (전남대학교 해양기술학부) ;
  • 김태호 (전남대학교 해양기술학부) ;
  • 신형호 (전남대학교 해양기술학부) ;
  • 장덕종 (전남대학교 해양경찰학과) ;
  • 차봉진 (국립수산과학원 시스템공학과)
  • Received : 2011.10.17
  • Accepted : 2011.11.04
  • Published : 2011.11.30

Abstract

The purpose of this study is to identify the flow resistance of the bottom trawl net. The bottom trawl net being used in the training ship of Chonnam National University was selected as a full-scale net, and model nets such as 1/10, 1/25 and 1/50 of the actual net were made. Total resistance of the net part, the height of the net mouth and the flow resistance of components of the net such as wing, bag and cod-end part was measured, converted into full-scale and compared. Additionally, the model rule of Tauti (1934), which has been most frequently used in fishing net modeling experiments, was applied to interpret flow resistance and scale effect of model experiment was investigated. Presumed that the flow resistance R is $R=kS{\upsilon}^2$ against the flow velocity of each net ${\upsilon}$, resistance coefficient k was calculated by substituting R, ${\upsilon}$ and S of the net. From the result, it was found that k decreases exponentially when u increases which makes $k=c{\upsilon}^{-m}$. Whereas m of each net is ranged between 0.13-0.16 and there was not significant difference between nets. c does not show big difference in 1/10 and 1/25 model and the value itself was relatively bigger than in 1/50 model. The height of the net mouth of 1/25 and 1/50 model net h decreases exponentially according as ${\upsilon}$ increases to make $h=d{\upsilon}^{-n}$. Whereas d and n values were almost same in two nets. Additionally, when resistance of cod-end, wing and bag part in 1/25 and 1/50 model nets, both nets showed big resistance in bag part when flow is 1m/s as more than 60%. Wing and cod-end part showed almost same value or wing part had little bit larger value. On the other hand, when reviewing the reasons why both models showed difference in 1/50 model while c value against the resistance coefficient k did not show big difference in 1/10 and 1/25 model, it is inferred that the difference occurred not from material difference but from the difference in net size according to scale. It was judged that they are the scale effects concomitant to the model experiments.

Keywords

References

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