• 한국농공학회지
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• 제34권2호
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• pp.73-84
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• 1992

The TIDE, finite element model for the simulation of tidal flow in shallow sea was tested for its applicability at the Saemangeum area. Several pre and post processors were developed to facilitate handling of the complicated and large amount of input and output data for the model developed. Also an operation scheme to run the model and the processors were established. As a result of calibration test using the observed data collected at 9 points within the region, linearlized friction coefficients were adjusted to be ranged 0.0027~0.0072, and water depths below the mean sea level at every nodes were changed to be increased generally by 1 meter. Comparisons of tidal velocities between the observed and the simulated for the 5 stations were made and obtained the result that the average relative error between simulated and observed tidal velocities was 11% for the maximum velocities and 22% for the minimum, and the absolute errors were less than 0.2m/sec. Also it was found that the average R.M.S. error between the velocities of observed and simulated was 0.119 m/sec and the average correlation coefficient was 0.70 showing close agreement. Another comparison test was done to show the result that R.M.S. error between the simulated and the observed tidal elevations at the 4 stations was 0.476m in average and the correlation coefficients were ranged 0.96~0.99. Though the simulated tidal circulation pattern in the region was well agreed with the observed, the simulated tidal velocities and elevations for specific points showed some errors with the observed. It was thought that the errors mainly due to the characteristics of TIDE Model which was developed to solve only with the linearized scheme. Finally it was concluded that, to improve the simulation results by the model, a new attempt to develop a fully nonlinear model as well as further calibration and the more reasonable generation of finite element grid would be needed.

• 대한조선학회논문집
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• 제49권5호
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• pp.440-446
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• 2012

A twisted cylinder has been newly designed by rotating the elliptic cross section along the spanwise direction in order to reduce the drag and vorticies in wake region. The flow around the twisted cylinder at a subcritical Reynolds number (Re) of 3000 is investigated to analyze the effect of twisted spiral pattern on the drag reduction and vortex suppression using large eddy simulation (LES). The instantaneous wake structures of the twisted cylinder are compared with those of a circular and a wavy cylinder at the same Re. The shear layer of the twisted cylinder covering the recirculation region is more elongated than that of the circular and the wavy cylinder. Successively, vortex shedding of the twisted cylinder is considerably suppressed, compared with those of the circular and the wavy cylinder. Consequently, the mean drag coefficient and the fluctuating lift of the twisted cylinder are less than those of the circular and the wavy cylinder.

• 한국지하수토양환경학회지:지하수토양환경
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• 제11권5호
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• pp.1-8
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• 2006

본 연구에서는 매립장에서 하부 지반으로 누출된 침출수의 이동에 흡착 불균질성이 미치는 영향을 평가하고자 하였다. 이를 위하여 차수막이 설치되어 있지 않은 매립장을 대상으로 일련의 Monte-Carlo 시뮬레이션을 수행하고 그 결과를 검토하였다. 균질한 지층에서 강불균질 지층에 이르는 다양한 불균질도를 가진 랜덤 분배계수 장에 대하여 포화 유동 모델과 오염물 이동 모델을 연결시켜 침출수의 이동을 계산하였다. 100회에 걸쳐 수행된 Monte-Carlo 시뮬레이션의 결과치로부터 얻은 평균, 표준편차, 변이계수와 같은 점기반 통계치들을 이용하여 화학적 불균질도의 영향을 평가하였다. 통계치 결과에 따르면 매립지반의 분배계수 분포가 지반 내 침출수 농도를 결정하는데 매우 중요한 인자로 나타났다. 균질 흡착의 경우와 비교할 때 불균질 분배계수 장에서는 실현 간 침출수 농도 분포의 변동성이 나타났다. 분배계수 장의 분산 및 오염원과 감시정 간의 이동 시간이 커질수록 농도의 변동성이 증가하였다. 이러한 결과는 화학적 변동성이 큰 지반 내에서의 침출수 이동을 예측할 때 단일 분배계수 값을 사용하면 상당한 오차를 유발할 수 있음을 나타낸다.

• 한국산림과학회지
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• 제77권3호
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• pp.269-275
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• 1988

황발산지(荒發山地)에서 야계수로(野溪水路)의 월류발생원인(越流發生原因)을 구명(究明)하기 위하여 1987년(年) 7월(月)3일(日)부터 7월(月)23일(日)까지 삼성천(三聖川)의 상류지역(上流地域)인 서울대학교(大學校) 부속(附屬) 관악수목원(冠岳樹木園)의 야계수로(野溪水路)를 대상(對象)으로 예상최대홍수류량(豫想最大洪水流量) 및 수로최대유출량(水路最大流出量)을 조사(調査)한 결과(結果)는 다음과 같다. 1. 측정지점(測定地點)에서의 유역면적(流域面積)은 477ha로 설계유역면적(設計流域面積) 410ha의 116%였다. 2. 관측분석(觀測分析)된 최대강우강도(最大降雨强度)는 설계최대강우강도(設計最大降雨强度) 100mm/hr와 거의 같은 99.5mm/hr였다. 3. 실측(實測)한 유출계수(流出係數)는 0.672로 설계유출계수(設計流出係數) 0.35의 약 2배로 나타났다. 4. 예상최대홍수류량(豫想最大洪水流量)은 설계예상최대홍수류량(設計豫想最大洪水流量) $39.9m^3/sec$의 222%인$88.59m^3/sec$였다. 5. 수로횡단면적(水路橫斷面積)을 조사(調査)한 결과(結果), 설계수로횡단면적(設計水路橫斷面積) $25.43m^2$의 68%인 $17.25m^2$을 얻었다. 6. 경심(徑深)은 0.94m로 설계경심(設計徑深) 1.28m 보다 작은 값을 나타내었다. 7. 평균계상(平均溪床)물매는 설계(設計)물매(1.00%)와 거의 같은 0.998%였다. 8. 수로최대평균유속(水路最大平均流速)은 2.87m/sec로 설계수로최대평균유속(設計水路最大平均流速) 3.68m/sec의 78%였다. 9. 수로최대유출용량(水路最大流出容量)을 산출(算出)한 바, 설계수로최대유출용량(設計水路最大流出容量) $93.58m^3/sec$의 53%인 $49.51m^3/sec$였다.

• 한국농공학회지
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• 제20권1호
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• pp.4592-4598
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• 1978

The purpose of this research is to find out mathemetically an economical intake water depth in the design of head works through the derivation of some formulas. For the performance of the purpose the following formulas were found out for the design intake water depth in each flow type of intake sluice, such as overflow type and orifice type. (1) The conditional equations of !he economical intake water depth in .case that weir body is placed on permeable soil layer ; (a) in the overflow type of intake sluice, {{{{ { zp}_{1 } { Lh}_{1 }+ { 1} over {2 } { Cp}_{3 }L(0.67 SQRT { q} -0.61) { ( { d}_{0 }+ { h}_{1 }+ { h}_{0 } )}^{- { 1} over {2 } }- { { { 3Q}_{1 } { p}_{5 } { h}_{1 } }^{- { 5} over {2 } } } over { { 2m}_{1 }(1-s) SQRT { 2gs} }+[ LEFT { b+ { 4C TIMES { 0.61}^{2 } } over {3(r-1) }+z( { d}_{0 }+ { h}_{0 } ) RIGHT } { p}_{1 }L+(1+ SQRT { 1+ { z}^{2 } } ) { p}_{2 }L+ { dcp}_{3 }L+ { nkp}_{5 }+( { 2z}_{0 }+m )(1-s) { L}_{d } { p}_{7 } ] =0}}}} (b) in the orifice type of intake sluice, {{{{ { zp}_{1 } { Lh}_{1 }+ { 1} over {2 } C { p}_{3 }L(0.67 SQRT { q} -0.61)}}}} {{{{ { ({d }_{0 }+ { h}_{1 }+ { h}_{0 } )}^{ - { 1} over {2 } }- { { 3Q}_{1 } { p}_{ 6} { { h}_{1 } }^{- { 5} over {2 } } } over { { 2m}_{ 2}m' SQRT { 2gs} }+[ LEFT { b+ { 4C TIMES { 0.61}^{2 } } over {3(r-1) }+z( { d}_{0 }+ { h}_{0 } ) RIGHT } { p}_{1 }L }}}} {{{{+(1+ SQRT { 1+ { z}^{2 } } ) { p}_{2 } L+dC { p}_{4 }L+(2 { z}_{0 }+m )(1-s) { L}_{d } { p}_{7 }]=0 }}}} where, z=outer slope of weir body (value of cotangent), h1=intake water depth (m), L=total length of weir (m), C=Bligh's creep ratio, q=flood discharge overflowing weir crest per unit length of weir (m3/sec/m), d0=average height to intake sill elevation in weir (m), h0=freeboard of weir (m), Q1=design irrigation requirements (m3/sec), m1=coefficient of head loss (0.9∼0.95) s=(h1-h2)/h1, h2=flow water depth outside intake sluice gate (m), b=width of weir crest (m), r=specific weight of weir materials, d=depth of cutting along seepage length under the weir (m), n=number of side contraction, k=coefficient of side contraction loss (0.02∼0.04), m2=coefficient of discharge (0.7∼0.9) m'=h0/h1, h0=open height of gate (m), p1 and p4=unit price of weir body and of excavation of weir site, respectively (won/㎥), p2 and p3=unit price of construction form and of revetment for protection of downstream riverbed, respectively (won/㎡), p5 and p6=average cost per unit width of intake sluice including cost of intake canal having the same one as width of the sluice in case of overflow type and orifice type respectively (won/m), zo : inner slope of section area in intake canal from its beginning point to its changing point to ordinary flow section, m: coefficient concerning the mean width of intak canal site,a : freeboard of intake canal. (2) The conditional equations of the economical intake water depth in case that weir body is built on the foundation of rock bed ; (a) in the overflow type of intake sluice, {{{{ { zp}_{1 } { Lh}_{1 }- { { { 3Q}_{1 } { p}_{5 } { h}_{1 } }^{- {5 } over {2 } } } over { { 2m}_{1 }(1-s) SQRT { 2gs} }+[ LEFT { b+z( { d}_{0 }+ { h}_{0 } )RIGHT } { p}_{1 }L+(1+ SQRT { 1+ { z}^{2 } } ) { p}_{2 }L+ { nkp}_{5 }}}}} {{{{+( { 2z}_{0 }+m )(1-s) { L}_{d } { p}_{7 } ]=0 }}}} (b) in the orifice type of intake sluice, {{{{ { zp}_{1 } { Lh}_{1 }- { { { 3Q}_{1 } { p}_{6 } { h}_{1 } }^{- {5 } over {2 } } } over { { 2m}_{2 }m' SQRT { 2gs} }+[ LEFT { b+z( { d}_{0 }+ { h}_{0 } )RIGHT } { p}_{1 }L+(1+ SQRT { 1+ { z}^{2 } } ) { p}_{2 }L}}}} {{{{+( { 2z}_{0 }+m )(1-s) { L}_{d } { p}_{7 } ]=0}}}} The construction cost of weir cut-off and revetment on outside slope of leeve, and the damages suffered from inundation in upstream area were not included in the process of deriving the above conditional equations, but it is true that magnitude of intake water depth influences somewhat on the cost and damages. Therefore, in applying the above equations the fact that should not be over looked is that the design value of intake water depth to be adopted should not be more largely determined than the value of h1 satisfying the above formulas.

• 한국토양환경학회지
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• 제1권2호
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• pp.73-81
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• 1996

실험실 내에서 부피비로 약 50%내외의 수분함량을 가진 3개의 서로 다른 깊이의 토양에서 염소와 중수의 확산계수는 4.8$\times$ $10${-7}$ 부터 7.2$\times$ $10${-7}$ $\textrm{cm}^2$/sec와 5.5 $\times$ $10${-5}$ 부터 1.6$\times$ $10${-4}$ $\textrm{cm}^2$//sec였다. 한편, 물과 물질의 이동성에 대한 연구는 중간사로 구성된 토양층 위에 위치하는 점토로부터 미사질 양토에 속하는 약 70cm깊이의 토양에서 실시되었고, 87일간의 실험기간동안 리터당 15.2$m\ell$의 염소와 0.6bq의 중수로 처리된 물을 일정한 유량(2cm/일)으로 관개하였다. 토양의 깊이와 시간에 따른 염소와 중수의 변동위치는 suction probe에 채취된 토양수를 가지고 측정하였는데 실험지 안에서 서로 다른 깊이 또는 동일 위치에서 염소와 중수가 발견되었다. 이러한 실험의 결과로부터 추정컨대 토양수의 유속과 표면확산 계수가 염소와 중수의 분포에 직접적인 영향을 미쳤고 24개의 suction probe에서의 결과는 실질적 물질과 토양의 상호작용의 효과를 나타내는 순수치의 25% 내외에서 평가치를 추정할 수 있었다.

• 한국농공학회지
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• 제17권1호
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• pp.3642-3654
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• 1975

The purpose of this thesis is to derive a unit hydrograph which may be applied to the ungaged watershed area from the relations between directly measurable unitgraph properties such as peak discharge(qp), time to peak discharge (Tp), and lag time (Lg) and watershed characteristics such as river length(L) from the given station to the upstream limits of the watershed area in km, river length from station to centroid of gravity of the watershed area in km (Lca), and main stream slope in meter per km (S). Other procedure based on routing a time-area diagram through catchment storage named Instantaneous Unit Hydrograph(IUH). Dimensionless unitgraph also analysed in brief. The basic data (1969 to 1973) used in these studies are 9 recording level gages and rating curves, 41 rain gages and pluviographs, and 40 observed unitgraphs through the 9 sub watersheds in Nak Oong River basin. The results summarized in these studies are as follows; 1. Time in hour from start of rise to peak rate (Tp) generally occured at the position of 0.3Tb (time base of hydrograph) with some indication of higher values for larger watershed. The base flow is comparelatively higher than the other small watershed area. 2. Te losses from rainfall were divided into initial loss and continuing loss. Initial loss may be defined as that portion of storm rainfall which is intercepted by vegetation, held in deppression storage or infiltrated at a high rate early in the storm and continuing loss is defined as the loss which continues at a constant rate throughout the duration of the storm after the initial loss has been satisfied. Tis continuing loss approximates the nearly constant rate of infiltration (${\Phi}$-index method). The loss rate from this analysis was estimated 50 Per cent to the rainfall excess approximately during the surface runoff occured. 3. Stream slope seems approximate, as is usual, to consider the mainstreamonly, not giving any specific consideration to tributary. It is desirable to develop a single measure of slope that is representative of the who1e stream. The mean slope of channel increment in 1 meter per 200 meters and 1 meter per 1400 meters were defined at Gazang and Jindong respectively. It is considered that the slopes are low slightly in the light of other river studies. Flood concentration rate might slightly be low in the Nak Dong river basin. 4. It found that the watershed lag (Lg, hrs) could be expressed by Lg=0.253 (L.Lca)0.4171 The product L.Lca is a measure of the size and shape of the watershed. For the logarithms, the correlation coefficient for Lg was 0.97 which defined that Lg is closely related with the watershed characteristics, L and Lca. 5. Expression for basin might be expected to take form containing theslope as {{{{ { L}_{g }=0.545 {( { L. { L}_{ca } } over { SQRT {s} } ) }^{0.346 } }}}} For the logarithms, the correlation coefficient for Lg was 0.97 which defined that Lg is closely related with the basin characteristics too. It should be needed to take care of analysis which relating to the mean slopes 6. Peak discharge per unit area of unitgraph for standard duration tr, ㎥/sec/$\textrm{km}^2$, was given by qp=10-0.52-0.0184Lg with a indication of lower values for watershed contrary to the higher lag time. For the logarithms, the correlation coefficient qp was 0.998 which defined high sign ificance. The peak discharge of the unitgraph for an area could therefore be expected to take the from Qp=qp. A(㎥/sec). 7. Using the unitgraph parameter Lg, the base length of the unitgraph, in days, was adopted as {{{{ {T}_{b } =0.73+2.073( { { L}_{g } } over {24 } )}}}} with high significant correlation coefficient, 0.92. The constant of the above equation are fixed by the procedure used to separate base flow from direct runoff. 8. The width W75 of the unitgraph at discharge equal to 75 per cent of the peak discharge, in hours and the width W50 at discharge equal to 50 Per cent of the peak discharge in hours, can be estimated from {{{{ { W}_{75 }= { 1.61} over { { q}_{b } ^{1.05 } } }}}} and {{{{ { W}_{50 }= { 2.5} over { { q}_{b } ^{1.05 } } }}}} respectively. This provides supplementary guide for sketching the unitgraph. 9. Above equations define the three factors necessary to construct the unitgraph for duration tr. For the duration tR, the lag is LgR=Lg+0.2(tR-tr) and this modified lag, LgRis used in qp and Tb It the tr happens to be equal to or close to tR, further assume qpR=qp. 10. Triangular hydrograph is a dimensionless unitgraph prepared from the 40 unitgraphs. The equation is shown as {{{{ { q}_{p } = { K.A.Q} over { { T}_{p } } }}}} or {{{{ { q}_{p } = { 0.21A.Q} over { { T}_{p } } }}}} The constant 0.21 is defined to Nak Dong River basin. 11. The base length of the time-area diagram for the IUH routing is {{{{C=0.9 {( { L. { L}_{ca } } over { SQRT { s} } ) }^{1/3 } }}}}. Correlation coefficient for C was 0.983 which defined a high significance. The base length of the T-AD was set to equal the time from the midpoint of rain fall excess to the point of contraflexure. The constant K, derived in this studies is K=8.32+0.0213 {{{{ { L} over { SQRT { s} } }}}} with correlation coefficient, 0.964. 12. In the light of the results analysed in these studies, average errors in the peak discharge of the Synthetic unitgraph, Triangular unitgraph, and IUH were estimated as 2.2, 7.7 and 6.4 per cent respectively to the peak of observed average unitgraph. Each ordinate of the Synthetic unitgraph was approached closely to the observed one.

• 대한토목학회논문집
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• 제29권4B호
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• pp.357-363
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• 2009

일반적으로 사용되는 관수로의 평균유속을 구하려면 Darcy-Weisbach의 마찰손실수두공식을 사용하면 되나, 그러나 이 식의 마찰손실계수 f는 Reynolds수와 상대조도(${\varepsilon}$/d)의 함수이므로 사용하기에 매우 불편하며 따라서 보다 편리한 식이 요구된다. 이에 본 연구에서 Chiu 유속공식의 신뢰성과 정확성을 증명하기 위하여 관수로에서 비삽입식 유속측정 장치인 레이저 유속계(Laser Doppler Velocimeter: LDV) 및 초음파 유량계(Ultrasonic Flowmeter: U/F), 삽입식 유속측정장치인 피토관 (Pitot Tube)을 이용하여 실측한 유속측정 자료와 Chiu의 공식을 이용한 유속분포가 매우 잘 일치함을 증명하였다. 유량의 증감에 관계없이 실험실 수로에서의 최대유속과 평균유속간의 이론적인 선형관계를 증명함으로써 관수로내 유속의 평형상태, 즉 엔트로피 파라미터 M값에 대응하는 평형상태에 도달하려 하고 이 평형상태를 지속적으로 유지하려고 하는 경향이 있음을 증명하였다. 또한, 한 단면을 대표하는 엔트로피 파라미터 M값이 결정되면 최대유속이 발생하는 지점에서의 유속 측정만으로 단면 전체의 평균유속을 쉽게 구할 수 있고 이로부터 간단히 유량을 산정할 수 있음을 증명하였으며, 이는 추후 관수로 설계 및 운영관리 시 가장 중요한 평균유량을 측정할 수 있는 이론적인 도구로 사용될 수 있음을 의미하는 것이다.

• Wind and Structures
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• 제23권6호
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• pp.559-575
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• 2016

In order to investigate the influence of different blade positions on aerodynamic load and wind loads and load-effects of large scale wind turbine tower under the halt state, we take a certain 3 MW large scale horizontal axis three-blade wind turbine as the example for analysis. First of all, numerical simulation was conducted for wind turbine flow field and aerodynamic characteristics under different halt states (8 calculating conditions in total) based on LES (large eddy simulation) method. The influence of different halt states on the average and fluctuating wind pressure coefficients of turbine tower surface, total lift force and resistance coefficient, circular flow and wake flow characteristics was compared and analysed. Then on this basis, the time-domain analysis of wind loads and load-effects was performed for the wind turbine tower structure under different halt states by making use of the finite element method. The main conclusions of this paper are as follows: The halt positions of wind blade could have a big impact on tower circular flow and aerodynamic distribution, in which Condition 5 is the most unfavourable while Condition 1 is the most beneficial condition. The wind loads and load-effects of disturbed region of tower is obviously affected by different halt positions of wind blades, especially the large fluctuating displacement mean square deviation at both windward and leeward sides, among which the maximum response occurs in $350^{\circ}$ to the tower top under Condition 8; the maximum bending moment of tower bottom occurs in $330^{\circ}$ under Condition 2. The extreme displacement of blade top all exceeds 2.5 m under Condition 5, and the maximum value of windward displacement response for the tip of Blade 3 under Condition 8 could reach 3.35 m. All these results indicate that the influence of halt positions of different blades should be taken into consideration carefully when making wind-resistance design for large scale wind turbine tower.

• 수산해양기술연구
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• 제37권2호
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• pp.78-84
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• 2001

1999년 5월 29일부터 6월 30일까지의 남해안에서의 수심에 따른 수중광의 변화와 조업시간의 경과에 따른 예망 상대유속을 측정하고, 권현망어구에 대한 체장 4~7cm정도 되는 멸치들의 도피 반응행동을 관찰하고 분석한 결과는 다음과 같다. 1) 남해안 통영, 거제 부근 멸치어장에서 수심에 대한 수중광의 변화를 자연대수 곡선식으로 나타내면 광흡수 계수 c는 대표적인 관측점에서 주로 0.24~1.03 범위로 나타나서, 멸치의 어구에 대한 시인도가 어장에 따라 클 것으로 보인다. 2) 권현망어구의 원형그물과 1/2축소그물의 자루그물 입구부분의 상대유속을 기준으로 할때, 수비와 자루의 연결부분의 유속비는 평균 1.46, 자루부분의 유속비는 평균 0.67로 나타나서, 어구의 부위에 따른 상대유속변화가 멸치의 유영운동과 도피운동에 영향을 줄 것으로 보인다. 축소된 권형망어구에 있어서의 멸치의 대망행동을 관찰한 결과 수비와 자루연결부분에서 빠져나가는 1분당 멸치도피수는 평균 455미 정도였으며, 자루의 앞에서 예인방향으로 유영하는 깔대기를 빠져나가는 1분당 멸치도피 수는 평균 308미 정도로 나타나서, 어구 전체적으로는 상당수의 멸치들이 능동적인 도피행동을 나타내는 것으로 추측된다.