• 수산해양기술연구
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• 제28권2호
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• pp.132-143
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• 1992

This paper presents a method in order to calculate the vortex distribution, the streak-line and the time-line around the flat and the cambered otter board in two dimensional flow using the discrete vortex method, and to calculate C sub(L) and C sub(D) of the otter boards varied with the passage of time by the numerical simulation using the Blasu's formula. The results obtained are summarized as follows: 1. Flow pattern around the otter boards calculated by the discrete vortex method was resembled closely that of the visualized photograph. 2. C sub(L) and C sub(D) calculated by the numerical simulation was very similar to the model test. 3. The circulation direction around the otter boards and the action direction of the shearing force can be recognized from the time-line around the otter boards. 4. Flow speed in the back side of the otter boards was faster than that in the front side, and the difference of the flow speed in both side of the cambered otter boards was about 1.3 times greater than that of the flat otter boards. 5. The clockwise vortex was generated in the trailing edge, and the counter-clockwise vortex was generated the leading edge of the otter boards. And they were shown the shape of Karman's vortex varied with the passage of time.

• 수산해양기술연구
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• 제43권1호
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• pp.49-61
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• 2007

Otter boards in the trawl are the one of essential equipments for the net mouth to be spread to the horizontal direction. Its performance should be considered in the light of the spreading force to the drag and the stability of towing in the water. Up to the present, studies of the otter boards have focused mainly on the drag and lift force, but not on the stability of otter boards movement in 3 dimensional space. In this study, the otter board is regarded as a rigid body, which has six degrees of freedom motion in three dimensional coordinate system. The forces acting on the otter boards are the underwater weight, the resistance of drag and spread forces and the tension on the warps and otter pendants. The equations of forces were derived and substituted into the governing equations of 6 degrees of freedom motion, then the second order of differential equations to the otter boards were established. For the stable numerical integration of this system, Backward Euler one of implicit methods was used. From the results of the numerical calculation, graphic simulation was carried out. The simulations were conducted for 3 types of otter boards having same area with different aspect ratio(${\lambda}=0.5,\;1.0,\;1.5$). The tested gear was mid-water trawl and the towing speed was 4k't. The length of warp was 350m and all conditions were same to each otter board. The results of this study are like this; First, the otter boards of ${\lambda}=1.0$ showed the longest spread distance, and the ${\lambda}=0.5$ showed the shorted spread distance. Second, the otter boards of ${\lambda}=1.0$ and 1.5 showed the upright at the towing speed of 4k't, but the one of ${\lambda}=0.5$ heeled outside. Third, the yawing angles of three otter boards were similar after 100 seconds with the small oscillation. Fourth, it was revealed that the net height and width are affected by the characteristics of otter boards such as the lift coefficient.

• 수산해양기술연구
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• 제22권4호
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• pp.49-55
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• 1986

The authors carried out an experiment to determine the horizontal opening of the mid water trawl gear, which is the same as was used in the foreward experiment concerned to the attitude and opening efficiency of otter board. The trawl net .used in the experiment was designed to have a square sectional four-seamed body with two three-sepenlted wings. Each wing tip was rigged with a net pendant of 70 m long and the fore ends of the pendants were directly jointed to the otter pendant without inserting hand rope, and a front weight of 200 kg weigh was rigged with in front of the lowest wing tip. To determine the opening between otter boards ani between wing tips, two 50 KHz fish finders were set sideways on the otter board and on the port middle wing tip so as to detect the distance froa the finders to the starboard otter board and to the wing tip respectively, and the informations were transmitted to the indicators onboard the ship through water-tight cables. The results obtained can be summarized as follows: 1. The openings between otter borads were 43-45 m in case of the warp 100 m, 53-55 m in the war;> 150 m and 54-59 m in the warp 200 m. It was increased in linear according to the increase of towin; speed in the range of 1. 1-1. 8 mlscc. 2. The determined values of the openings between otter boards were greater than the estimated values. which were calculated by the opening between warps at the gallows of the ship and the length of tt~ warp, assuming that the warps from the top rollers to the otter boards were straight. The rates of the determined values to the estimated values were 1. 23-11. 0 in case of the warp 100 m, 1. 23-1. 12 in the warp 150 m and 1. 23-1. 15 in the warp 200 m respectively. The rates were almost the same at the slow towing speed of 1. 3 mlscc or so, then the higher the speed, the less the rate, and the longer the warp, the greater the rate. 3. The rates of the openings between otter boards to the total length of net pendant and the net (excluded cod end) showed 43-43% in case of the warp 150-200 m. It was a little smaller than th~ standard. which is 50%. in the common bottom trawl. 4. The determined openings between wing tips were 18-19 m in case of the warp 100m, 21-22 m in the warp 150 rn, They showed that the higher the speed, the greater the openings even though its range was no more than 1 m or so. 5. The rates of openings between otter boards to th~ openings betwee:l wing tips were almost invariably 38%. 6. The rates of openigs b2tween otter boards to the lenth of h~ad rope were 60-65% in cas': of th~ warp lOa-150m. It were much larg2r than th~ standard. which is 50%. in the common botto:n trawl.

• 수산해양기술연구
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• 제27권4호
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• pp.286-292
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• 1991

현재 사용되고 있는 전개판의 성능을 보다 향상시키기 위한 방안으로 비행기의 익이론에 기초를 두고, 전개판의 경계층을 흡입하거나 제거하는 방법 중에서 역류역을 제거하는 와발생기의 부착을 전개판에 적용하였다. 성능분석을 위해서 단순만곡형, V-만곡형 그리고 슬롯만곡형 전개판의 3종에 와발생기를 부착하지 않은 경우와 부착한 경우에 대하여 성능 및 유체역학적 특성을 성능실험과 가시화실험을 통하여 비교해 보았다. 실험결과를 요약하면 다음과 같다. \circled1 단순만곡형전개판에 와발생기를 부착한 경우 최대전개력계수는 10~15% 증가, 항력계수는 2%미만증가, 양항비는 5~20% 증가하였다. \circled2 V-만곡형전개판에 와발생기를 부착한 경우 양항비가 10~20% 증가하였다. \circled3 슬롯만곡형에 와발생기를 부착한 경우 영각 20$^{\circ}$ 이내에서 최대전개력계수는 약 20%이상 증가, 항력계수는 5~20% 증가, 양항비는 약간 높게 나타났으나, 영각 25$^{\circ}$이상에서는 이들 계수의 값들이 기준형에 비하여 낮게 나타났다. \circled4 와발생기를 부착한 전개판에서 박리점이 기준형에 비하여 다소 후연에 나타났다. \circled5 와발생기에 따른 전.후면의 유속차는 단순만곡형의 경우 모든 영각에서 약 10% 증가, V-만곡형의 경우 전반적으로 증가하였으나 영각 25$^{\circ}$에서는 비슷하게, 슬롯만곡형의 경우 영각 25$^{\circ}$까지는 증가하는 것으로 나타났다. \circled6 와발생기에 따른 박리역의 크기는 단순만곡형에서 약 5~15% 감소, V-만곡형과 슬롯만곡형은 영각 15$^{\circ}$~20$^{\circ}$에서는 약 10% 감소, 영각 25$^{\circ}$ 이상일 때는 비슷하게 나타났다.

• 수산해양기술연구
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• 제27권4호
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• pp.278-285
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• 1991

현재 사용되고 있는 전개판의 성능을 보다 향상시키기 위한 방안으로 비행기의 익이론에 기초를 두고, 전개판의 경계층을 흡입하거나 제거하는 방법 중에서 역류역을 흡입하는 슬롯(slot)을 전개판에 적용하였다. 성능분석을 위해서 단순만곡형전개판에 슬롯이 없는 기준형과 슬롯의 위치에 따른 5종의 모형전개판에 대하여 성능실험과 가시화실험을 통하여 그 성능과 유체역학적 특성을 비교해 보았다. 실험결과를 요약하면 다음과 같다. \circled1 최대전개력계수는 0.6C, 0.4C, 기준형, 0.8C, 0.2C의 순으로, 슬롯의 위치 0.6C인 전개판이 영각 27$^{\circ}$에서 1.59로 가장 우수하였다. \circled2 항력계수는 슬롯의 위치가 후연으로 갈수록 감소하며, 슬롯을 준 경우가 기준형보다 작게 나타났다. \circled3 양항비는 0.6C, 0.4C, 0.8C, 0.2C, 기준형의 순으로 모두 기준형보다 높게 나타났다. \circled4 0.2C, 0.4C 및 0.6C의 전개판이 기준형과 0.8C의 전개판보다 박리가 후연에서 발생하였다. \circled5 전개판의 전.후면에서 유속차는 영각 15$^{\circ}$~25$^{\circ}$까지는 점차 증가하고, 30$^{\circ}$에서는 감소하는 것으로 나타났다. \circled6 박리역의 크기는 0.6C의 전개판에서 가장 적게 나타났다.

• 수산해양기술연구
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• 제22권4호
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• pp.41-48
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• 1986

To investigate the midwater trawl gear available for the Korean near sea trawlers, the authors carried out a field experiment on the attitude and the opening efficiency of the otter board with the Pusan 404 (160GT, 750ps), a training ship of National Fisheries University of Pusan. The experimental trawl gear was designed to be operable by the ship and the otter board was made of single iron plate with 12% camber ratio. The special-prepared potentiometric angle detector was used for determining the attitude, and the 50 KHz fish finder for the opening between the otter boards. The results obtained can be summarized as follows: 1. The angle of attack varied by moving the towing point on the towing plate of the otter board. It showed 33 to 36 degrees when the point was set at the outmost position, 25 to 31 degrees at the middle position and 19 to 30 degrees at the inmost position, with a decreasing tendency according to the increase of towing speed in each cases. 2. The heel of the otter board always occured inwards, increasing slightly according to the increase of towing speed. 3. The tilt of the otter board always occured outwards, increasing slightly according to the move of the towing point inwards, and decreasing slightly according to the increase of towing speed. 4. The opening between otter boards showed the largest value when the towing point was set at the outmost position.

• 한국수산과학회지
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• 제34권3호
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• pp.238-244
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• 2001

중층트롤 어구의 유체저항을 구하거나 전개판의 간격을 구하는 것은 어구설계나 어로작업에 유용하다. 본 논문에서는 끌줄에 관해 신장을 포함하여 간이해석적 (semi-analytic)으로 푼 3차원해석을 이용하여 중층트롤 어구의 끌줄에 적용시키고, 줄의 형상에 대해 기존의 직선이라는 가정은 실제로 이루는 곡선과는 차이가 있기에, 여기서는 줄의 형상을 곡선 형태로 도입하였는데, 날개그물 끝에서 후릿줄, 뜸$\cdot$발줄 및 (자루그물의) 힘줄에 미치는 세 힘의 합력을 역학적으로 고려하여 어구의 유체저항을 구한 방법을 나타낸 것으로서. 이때 전개판 (OB) 뒤쪽의 후릿줄 (hand rope), bridle 및 뜸 (발)줄의 형상을 곡선인 $y_{r}=Ax_{r}^{B}$의 형태 (B=2이면 포물선 (parabola)임)로 가정하였다. 기존의 중층트롤의 실험자료에서 끌줄의 길이가 100m인 경우에 예망속도의 변화에 따른 여러가지 측정값을 이용하여 트롤어구의 유체저항을 구하는 새로운 방법을 제시하였는데, 10매로 구성된 망지의 유체저항 ($R_{n}(kg)$)과 유속 (V)과의 관계는$1.34 범위에서 $R_{n}=1204.6\;V_{(m/s)}^{1.99}$ 관계가 있었다. 여기에서 제안한 방법을 이용하면 트롤어구의 그물만의 유체저항을 직접적으로 구할 수 있다.

• 수산해양기술연구
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• 제34권3호
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• pp.294-301
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• 1998

Towing performance of a midwater trawl system was examined aboard the training ship KAYA(2900ps) at the East Sea using the midwater trawl gear that had been designed and manufactured in accordance with the vessel. In this experiment, the trawl system data, the towing speed, the length and tension of the warp, net mouth height, and the depth of otter boards and net were measured and analyzed. The results are as follows: 1. In case of heaving in the warp with constant towing speed, the tension was suddenly increased and then again was reduced and after returned to the original steady state tension. At this time, net height was reduced a bit by ascension of ground rope, but returned to it’s original value. In the case where the warp was paid out, the tension was suddenly decreased and after increased and then returned to the tension of the original state, and the net height was greatly increased instantly by the sinking of the ground rope and then returned to the steady state 2. In the case of increased towing speed mm constant warp length, the tension was increased, and reducing the net height, the gear depth was decreased. On the other hand, in the case where towing speed was reduced, the tension was reduced and the gear depth and net height was increased. 3. Otter boards show a swing motion in the scope of 5~ 10m continuously. Otter boards responded to the state change of the trawl system at first, and then the motion of the net appeared. 4. The depth of net center was about 20m deeper than that of the otter boards, it shows about 0.4 times the warp length at the 4knots towing speed.

• 한국수산과학회지
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• 제20권6호
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• pp.484-488
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• 1987

단순만곡형과 슈퍼-V형 모형 전개판의 뒷전 쪽에 각각 flap을 부착하고, 회류수조에서 진행각도와 유속에 따른 항력과 전개력을 측정하여 유체역학적인 전개성능을 분석한 결과는 다음과 같다. 1. flap을 부착한 모형 전개판의 전개력계수 $C_L$은 flap각도 $30^{\circ}$와 $50^{\circ}$일 때 단순만곡형은 최대유효진행각도 $\alpha_{max}=25^{\circ}$ 1.75 정도이었고, 슈퍼-V형은 $\alpha_{max}=20^{\circ}$에서 1.80정도로 flap을 부착하지 않은 경우보다 $20\~30\%$ 정도 $C_L$이 증가하였다. 2. 항력계수 $C_D$는 $\alpha_{max}$ 일 때 flap각도에 관계없이 단순만곡형과 슈퍼-V형 모두가 0.5 정도로 거의 차이가 없었고, flap을 부착하지 않은 경우보다는 약간 $C_D$가 증가하였다. 3. 유체효율 $C_L/C_D$는 flap각도 $30^{\circ}$일 경우가 $50^{\circ}$일 경우보다 약간 높았으나, $\alpha_{max}$일 때는 거의 비슷하였으며, flap를 부착하지 않은 경우보다는 악간 높은 경향을 보였다.

• 수산해양기술연구
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• 제24권2호
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• pp.78-82
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• 1988

한국근해의 중층 트로올선에서 전개판의 수중중량을 경감시켜서 끌줄을 길게 주므로서 전개력을 향상시키기 위하여 스티로폴뜸을 전개판의 천정판에 고정시키고 끌줄 길이와 예망속력을 변화시켰을 때의 전개판의 깊이와 전개간격을 실측한 것을 분석.검토한 결과는 다음과 같다. 1. 전개판 깊이는 끌줄 길이가 100m이고 예망속력이 101~108m/sec인 범위에서 뜸이 있을 경우 41~25m, 뜸이 없을 경우 45~26m이고, 뜸줄 길이가 150m일 경우는 뜸이 있을 경우 68~44m, 뜸이 없을 경우 74~46m로서 뜸이 있을 경우가 없을 경우보다도 9~4% 정도 얕았다. 또 실측치는 어느 경우나 계산치보다도 15% 작았다. 2. 전개판의 전개간격은 끌줄 길이가 100m이고, 예망속력이 1.1~1.8m/sec인 범위에서는 뜸이 있을 경우 34~41m, 뜸이 없을 경우 30~38m이고, 끌줄 길이가 150m일 때는 뜸이 있을 경우 44~50m, 뜸이 없을 경우 37~46로서 있을 경우가 없을 경우보다도 끌줄 길이 100m에서 10%, 150m에서 15%정도 더 컸다. 또, 실측치는 계산치보다 항상 컸으며 계산치에 대한 실측치의 비는 끌줄 길이가 100m일 때 1.17~1.14, 150m일 때 1.17~1.09이었다. 3. 날개 끝 간격은 끌줄 길이 100m인 때 뜸이 있을 경우가 없을 경우보다 1m 정도 크고 유효망구면적으로는 10% 정도 크며, 끌줄 길이가 150m인 때는 그 차이가 2m로서 유효망구면적으로는 20% 정도 크다고 추정된다. 따라서 전개판에 뜸을 달아서 전개판의 수중중량을 일시적으로 가볍게 해 주는 것은 유효망구면적을 크게 하므로 어획성능향상에 상당히 도움이 될 것이 기대된다