• 제목/요약/키워드: bottom trawl nets

검색결과 14건 처리시간 0.023초

그물어구의 유수저항과 모형수칙 4. 트롤그물의 유수저항 (Flow Resistance and Modeling Rule of Fishing Nets 4. Flow Resistance of Trawl Nets)

  • 김대안
    • 한국수산과학회지
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    • 제30권5호
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    • pp.691-699
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    • 1997
  • 본 연구에서는 트롤그물의 유수저항 특성 및 그 저항을 그물의 구조, 규격 등으로 정도 높게 표현해내는 방법을 얻어내는 것을 목약으로 하여, 벽 면적이 $S(m^2)$되는 트롤그물이 유속 $\nu\;(m/sec)$에서 받는 유수저항 R(kg)을 $R=kSv^2$으로 표시하고, 지금까지 행해진 저항실험 결과들을 수집하여 윗 식의 형태로 정리하였으며, 저항계수 $k(kg{\cdot}sec^2/m^4)$를 전보 에서 구한 저항식에 의해 해석하였다. 그 결과, k는 그물 입구의 단면 을 $S_m\;(m^2)$, 흐름에 수직인 평면에 대한 그물의 총 투영면적을 $S_n\;(m^2)$, 그물감의 대표치수를 $\lambda$($={\pi}d^2/2lsin2\varphi;\;d$ : 그물실의 지름, 2l : 그물코의 크기, $2\varphi$ 그물코의 전개각)라 할때, 저층 트롤과 중층 트롤에서 각각 $$k=4.5(\frac{S_n}{S_m})^{1.2}v^{-0.2}$$ in case of bottom trawl nets and as $$k=5.1\lambda^{-0.1}(\frac{S_n}{S_m})^{1.2}v^{-0.2}$$$$k=5.1\lambda^{-0.1}(\frac{S_n}{S_m})^{1.2}v^{-0.2}$$ 으로 표시할 수 있었고, 이들에서 $S_n/S_m$의 값은 각각의 그물과 벽 면적이 같은 원추형 자루그물로부터 구해도 된다는 것을 알 수 있었으며, 설계 방식이 일반화 되어 있는 그물들의 경우는 유수저항 R(kg)을 저층 트롤과 중층 트롤에서 각각 $$R=1.5\;S\;v^{1.8}$$$$R=0.7\;S\;v^{1.8}$$으로 표시해도 좋다는 것을 알 수 있었다.

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Fluttering Characteristics of the Ropes and Nets as an Active Stimulating Device inside the Cod End of a Trawl Net

  • Kim, Yong-Hae
    • Fisheries and Aquatic Sciences
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    • 제16권2호
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    • pp.101-108
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    • 2013
  • An active stimulating device (ASD) consisting of a net panel or ropes fluttering in the turbulence inside the cod end was effective in driving fish near the cod end to reduce juvenile by-catch. The fluttering characteristics of the rope and net panel were examined by video observations and analyzed for fluttering amplitude and period in a water channel and in field experiments with a bottom trawl. The amplitude ratio of the fluttering ropes or nets in the tank test increased with the fluttering index as the diameter of the twine, mesh size, flexibility, and flow velocity changed, whereas the period decreased with the above factors. In bottom trawl experiments, the range of mean depth difference in the fluttering net panel was 12-17% of the length of the fluttering net, and the period of depth difference or three-dimensional (3D) tilt was revealed, with shorter ones ranging from 2 to 6 s. The amplitude as depth difference and period from field measurements were similar to those of nets in tank experiments and also to the period of 3D flow velocity inside the cod end. These results could be used to design an ASD that could be used for to the cod end of actual towed fishing gear to reduce juvenile by-catch.

쌍끌이 기선저인망의 유수저항 특성 및 모형 실험시의 축척비 영향 (Flow resistance of bottom pair trawl nets and scale effect in their model experiments)

  • 김대진
    • 수산해양기술연구
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    • 제51권2호
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    • pp.203-211
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    • 2015
  • The purpose of this study is to identify the flow resistance of the bottom pair trawl nets. The bottom pair trawl nets being used in fishing vessel (100G/T, 550ps) was selected as a full-scale net, and 1/10, 1/25 and 1/50 of the model nets were made. Converted into the full-scale net by Tauti's modeling rule and Kim's modeling rule, when resistance coefficient k of each net was calculated by substituting into above equation for flow resistance R and wall area of nets S values of each net ${\upsilon}$. Because resistant coefficient k decreases exponentially according as flow velocity ${\upsilon}$ increases to make $k=c{\upsilon}^{-m}$, c and m values of each net were compared. As a result, as the model was smaller, c and m values was smaller in the two rule into standard of 1/10 model value, decrease degree of 1/25 model was almost same in the two rule, decrease degree of 1/50 model was very big in Tauti's modeling rule. Therefore, in the result of experiment, because average of c and m values for similarly 1/10 and 1/25 model were given $c=4.9(kgf{\cdot}s^2/m^4)$ and m=0.45, R (kgf) of bottom pair trawl net could show $R=4.9S{\upsilon}^{1.55}$ using these values. As in the order of cod-end, wing and bag part for 1/25 and 1/50 model net were removed in turn, measured flow resistance of each, converted into the full-scale, total resistance of the net and the resistance of each part net were calculated. The resistance ratio of each part for total net was not same in 1/25 and 1/50 model each other, but average of two nets was perfectly same area ratio of each part as the wing, bag and cod-end part was 43%, 45% and 12%. However, the resistance of each part divided area of the part, calculated the resistance of per unit area, wing and bag part were not big difference each other, while the resistance of cod-end part was very large.

그물어구의 유수저항과 모형수칙 5. 저층 트롤그물의 예망저항 (Flow Resistance and Modeling Rule of Fishing Nets 5. Total Resistance of Bottom Trawl Nets Subjected Simultaneously to the Water Flow and the Bottom Friction)

  • 김대안
    • 한국수산과학회지
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    • 제30권5호
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    • pp.700-707
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    • 1997
  • 본 연구에서는 유수저항과 해저 마찰력을 동시에 받는 저층 트롤그물의 예망저항을 정도 높게 표현해낼 목적으로, 전보에서 구한 유수저항만을 받을 때의 저항식에 해저 마찰력의 영향을 추가하고, 지금까지 행해진 실험 결과들을 수집하여 분석하였다. 그 결과, 벽 면적이 $S(m^2)$ 되는 저층 트롤그물이 예망속도 $\nu(m/sec)$에서 받는 예망저항 R(kg)은 그물 입구의 단면적을 $S_m\;(m^2)$, 흐름에 수직인 평면에 대한 그물의 총 투영면적을 $S_n\;(m^2)$, 자루그물 앞끝의 완성 둘레를 B(m)라 할 때 $$R=4.5(\frac{S_n}{S_m})^{1.2}S\;v^{-1.8}+20(Bv)^{1.1}$$으로 주어졌다. 그러나, 실용적으로는 윗 식보다 $R=kS\nu^2$의 형태로 표시하는 것이 더욱 편리하다고 볼 수 있기 때문에, 실험 결과들을 이 식에 적용하여 저항계수 $k(kg{\cdot}sec^2/m^4)$를 여러 가지 측면에서 검토해 본 결과, k는 근사적으로딜만의 함수로 표시할 수 있다는 것을 알 수 있었으며, 그물의 완성 전장을 L (m)이라 할 때 $S{\propto}BL$이어서 $S/BL=\alpha$라 둘 수 있기 때문에 R(kg)은 근사적으로 $$R=18{\alpha}B^{0.5}L\;v^{1.5}$$으로 표시해도 좋다는 것을 알 수 있었다. 또한, $\alpha$의 값은 그물마다 달라 $0.40\~0.55$의 범위이긴 하나 전체 평균치 0.48에서 크게 벗어나지 않았기 때문에, 저층 트롤그물들을 총괄해서 표시할 때는 $\alpha=0.48$을 적용함으로써 R (kg)을 $$R=9\;B^{0.5}\;L\;v^{1.5}$$ 으로 대신해도 좋다는 것을 알 수 있었다.

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Comparison of Tilt Variation in the Otter Board and Codend of Bottom Trawl Gear during Fishing Operations

  • Kim, Yong-Hae
    • Fisheries and Aquatic Sciences
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    • 제17권1호
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    • pp.145-153
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    • 2014
  • The motion of the otter board on a trawl can affect the motion of trawl nets, and the motion of the codend can affect fish selectivity. Preliminary measurements of the tilt of bottom trawl gear were carried out to compare the tilts of the otter board and codend. The tilt of the otter board was measured by Vector and tilt at 1.5 m anterior to the end of the codend, and the middle upper panel was measured with a micro-DST-tilt logger. Tilt data such as yaw, pitch, and roll were analyzed by the fast Fourier transformation method and global wavelet and event analyses for the period or amplitude. The mean period ${\pm}$ standard deviation of the tilt in the otter board, $(5-6){\pm}2s$, was similar to the period of the codend, $(4-6){\pm}(2-3)s$, whereas the amplitude of the codend was greater than that of the otter board. The yaw and pitch periods were not significantly different between the otter board and codend, but roll was different. Furthermore, the tilt period frequencies of the otter board and codend were not significantly different. Accordingly, the tilt motion of the codend was mostly related to the tilt of the otter board.

저층 트롤어구의 유수저항 특성 및 모형 실험시의 축척비 영향 (Flow resistance of bottom trawl nets and scale effect in their model experiments)

  • 김대진;김대안;김태호;신형호;장덕종;차봉진
    • 수산해양기술연구
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    • 제47권4호
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    • pp.281-289
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    • 2011
  • 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.

Distribution Characteristics of Bottom Litter in Chinhae Bay, Korea

  • Kim Jong-Hwa;Kim Sam-Kon;Kim Jong-Kyu
    • Fisheries and Aquatic Sciences
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    • 제4권3호
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    • pp.150-158
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    • 2001
  • A study on the amount, distribution and item of bottom litter on the sea-bed was conducted by the bottom trawl net at 5 sections in Chinhae Bay over a year. The number and weight of litter found per unit of swept area (1 hectare) in each section were estimated as the range of 8.76-80.63 pieces, 3.51-108.39kg, respectively. The seasonal variation of high (Aug., '97) and low season (Feb., '98) in quantity was small, and it was about 2 times as the range of 24.58- 52.61 pieces/ha between them. But the weight variation between high (Apr., '98) and low season (Aug., '97) was very large, about 30 times as the range of 4.06-119.64kg/ha. The largest and second composition on the weight of bottom litter in Chinhae Bay are $76\%$ in other-litter with compound and bulky materials, and $93\%$ in fishing gear, respectively. The relationship between quantity and weight of bottom litter was not occurred due to the variety of specific gravity. Of the fishing gear, fishing nets was portioned to be 2.571kg/ha in weight and $84.9\%$ in composition. So these results prove that fishing nets were discarded as the most part of fishing gear during fishing activity in the bay. The largest composition of the soiled state classified into 3 styles in overall bottom litter was $69\%$ in very soiled state, and the second one of $28\%$ in the soiled state. On the other hand, new state is very small and portioned in $3.0\%$ of all. Chinhae Bay was estimated to be about 10 times in quantity and about 36 times in weight of Tokyo Bay. Therefore, these suggest that Chinhae Bay is a very serious polluted estuary caused by the bottom litter such as heavy and bulky wastes, fishing gear.

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우리나라 서해 근해 해저 쓰레기 분포 및 조성 (The distribution and composition of seabed litter in the exclusive economic zone of the West Sea of South Korea)

  • 김정년;강명희;조현수
    • 수산해양기술연구
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    • 제53권4호
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    • pp.437-445
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    • 2017
  • Distribution and composition of the seabed litters in the exclusive economic zone of the West Sea of South Korea including 18 sea-blocks were investigated using a bottom trawl gear of the R/V Tamgtu 20 (National Institute of Fisheries Science) from 24th April 2011 to 4th May 2012. Each trawl shot was conducted for an hour in each sea-block and the total trawl shots was 18. As a result, 325.6 kg of seabed litter in total has been collected. The quantity of the seabed litter was highest at No. 202 of the sea-block, close to the Heuksan-Do. The highest occupied sea material was plastic (83.1% of entire seabed litters), the second highest material was metal combined with plastic (10.6%), and glass (2.9%), metals (2.3%), vinyl (0.6%), cloth (0.4%) and wood (0.2%) in order. The origin of seabed litters was from fishing gear (89.0% of all seabed litters). Therefore, it could be assumed that most seabed litters were derived from the fishing activity for example fishing nets and ropes.

동해구 트롤 어구어법의 개량 (Improvement of the Fishing Gear and Fishing Method of the East-Sea Trawl Fishery)

  • 권병국;이주희;이춘우;김형석;김용식;안영일;김정문
    • 수산해양기술연구
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    • 제37권2호
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    • pp.106-116
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    • 2001
  • 동해구 트롤 어구어법을 개발하기 위하여 생력화 조업시스템을 개발하고, 생산성을 높이는 선택형 개량어구를 개발하는데 연구목표를 두었다. 생력화 조업시스템으로 폭 2.0m 1.8m인 네트드럼을 제작하고, 현용 와이어드럼에 와이어리더를 설비하여 생력화를 도모하였고, 선미에 겔로스를 설비하였다. 그 결과, 투양망시에 인력에 의한 그물을 들어올리거나 적재하는 일이 조업시스템으로 대체되어 선원들의 노동력은 기존의 것에 비하여 80% 정도 낮게 개선되었다. 또한, 중\ulcorner저층 겸용어구 A형과 저층용어구 B형을 개발하고, 단일 슬롯 V-만곡형 전개판을 설계\ulcorner제작하고, 네트레코더를 설치하여 1999년 9월말부터 2000년 5월까지 시험조업한 결과를 요약하면 다음과 같다. 1. A형의 망고는 중층예망시 약 30-35 m이나 저층예망에서는 19-20 m이며, 망폭은 29-31 m 정도로 추정되었으며, 저층예망시 전개판의 수중위치는 해저에서 10 m 정도 위쪽에 위치하고 있는 것이 확인되었다. 2. A형의 저층예망시의 기관 부하는 어구의 유체저항이 커서 재래식에서 보다 10rpm 정도가 더 요구되었다. 3. A형의 어획성능은 4시간 정도 예망하였을 때 분홍새우의 어획량이 재래식 어구에 비하여 약 3배정도가 더 많았고, 선택성이 매우 강한 특성을 보였다. 4. A형 어구에 의하여 어획된 분홍새우는 상품성이 우수하여 타선의 것보다 상자당 3,000-7,000원 정도 고가로 위판되었으며, 동급의 기존 트롤선에 비하여 생산성이 약 30%정도 향상된 것으로 나타났다. 5. A형 어구에 의한 조업에서는 펄을 뜨는 일은 전혀 없으며, 재래식 그물에서 대량으로 올라오는 불가사리나 기타 쓰레기 등이 거의 입망되지 않으므로, 어획물의 처리과정이 용이하여 선원의 노동력도 크게 절감할 수 있었다. 6. 천장망 길이가 약 23 m인 B형은 망고가 약 10 m, 망폭이 약 33m로 각각 추정되었으며, 예망시의 기관 부하도 예망속도 2.5노트까지는 큰 무리 없이 조업이 가능하였다. 7. B형의 어획성능은 새우의 어획량이 재래식 어구를 사용하는 어선에 비하여 5배 이상으로 나타났고, 청어는 약 2배정도 많은 것으로 확인되었으며, 기타 어류의 어획도 약 2배가 많았으나, 고등류, 문어류, 그리고 게류의 어획은 거의 없어서 선택성이 큰 것으로 나타났다. 8. B형의 생산량과 생산액은 재래식에 비하여 약 1.1배와 1.7배로 크게 나타나서 어업의 생산성이 크게 개선되었다. 동해구트롤어업의 합리적인 운용을 위하여 청어, 가자미, 게, 오징어 등의 어종을 효율적으로 어획할 수 있도록 어구의 기능을 확대하여야 할 것이고, 조업에 막대한 지장을 주고 있는 해파리의 탈출을 위한 그리드(grid)의 적용이 필요하다. 나아가 이 개량어구의 보급이 확산되면 분홍새우의 남획은 피할 수 없을 것이므로 합리적인 어획을 위한 자원관리방안이 확립되어야 할 것으로 보아진다.

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실선 시험에 의한 저층 트롤 어구에 관한 연구-II -어구의 수중 형태에 관하여- (A study on the bottom trawl gear by the trial of a stern trawler-II -On the net shape of a bottom trawl gear-)

  • 조봉곤;고광수
    • 수산해양기술연구
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    • 제36권4호
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    • pp.281-286
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    • 2000
  • 저층트롤 실물 어구를 이용한 해상 실험을 통하여 예망 중인 어구의 망구 형태에 관련되는 전개판의 간격 및 망고 등을 예망 속도별, 끌줄의 길이별로 측정하고, 이론적인 수치 해석 결과와 비교하여 실물어구의 수중 현황을 해석함으로서 어구의 효율적인 운용과 어획효과의 증대를 위한 기초자료를 제공하고자 한다. 수중 현황을 해석한 결과를 요약하면 다음과 같다. 1. 전개판의 전개간격은 예망 속도와 끌줄길이의 증가에 따라 직선적으로 증가하며 끌줄 길이에 의한 증가율이 예망 속도에 의한 증가율보다 현저히 크게 나타났으며, 그 간격의 변화는 57.0∼82.8m로서 후릿줄과 그물목줄 및 그물길이 전체의 43∼62%를 차지하였다. 2. 망구의 높이는 예망 속도와 끌줄길이의 증가에 따라 직선적으로 감소하며, 예망 속도에 의한 감소율이 끌줄 길이에 의한 감소율보다 현저히 크게 나타났는데 그 높이의 변화는 3.1∼4.0m로 나타났다. 3. 양 날개끝의 간격이 커지면 망고는 낮아지나 끌줄 길이가 증가할수록 날개 끝 간격의 증가에 대한 망구 높이 감소율의 비는 점차 작아졌다. 4. 망고에 대한 양 날개 끝 간격의 비는 예망속도와 끌줄 길이의 증가에 따라 점차 커졌는데, 그 비는 4.17∼7.81로 나타났다.

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