• 제목/요약/키워드: Discharge time lag

검색결과 71건 처리시간 0.024초

한국주요빙계의 소유역에 대한 순간단위권 유도에 관한 연구 (I) (Studies on the Derivation of the Instantaneous Unit Hydrograph for Small Watersheds of Main River Systems in Korea)

  • 이순혁
    • 한국농공학회지
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    • 제19권1호
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    • pp.4296-4311
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    • 1977
  • This study was conducted to derive an Instantaneous Unit Hydrograph for the accurate and reliable unitgraph which can be used to the estimation and control of flood for the development of agricultural water resources and rational design of hydraulic structures. Eight small watersheds were selected as studying basins from Han, Geum, Nakdong, Yeongsan and Inchon River systems which may be considered as a main river systems in Korea. The area of small watersheds are within the range of 85 to 470$\textrm{km}^2$. It is to derive an accurate Instantaneous Unit Hydrograph under the condition of having a short duration of heavy rain and uniform rainfall intensity with the basic and reliable data of rainfall records, pluviographs, records of river stages and of the main river systems mentioned above. Investigation was carried out for the relations between measurable unitgraph and watershed characteristics such as watershed area, A, river length L, and centroid distance of the watershed area, Lca. Especially, this study laid emphasis on the derivation and application of Instantaneous Unit Hydrograph (IUH) by applying Nash's conceptual model and by using an electronic computer. I U H by Nash's conceptual model and I U H by flood routing which can be applied to the ungaged small watersheds were derived and compared with each other to the observed unitgraph. 1 U H for each small watersheds can be solved by using an electronic computer. The results summarized for these studies are as follows; 1. Distribution of uniform rainfall intensity appears in the analysis for the temporal rainfall pattern of selected heavy rainfall event. 2. Mean value of recession constants, Kl, is 0.931 in all watersheds observed. 3. Time to peak discharge, Tp, occurs at the position of 0.02 Tb, base length of hlrdrograph with an indication of lower value than that in larger watersheds. 4. Peak discharge, Qp, in relation to the watershed area, A, and effective rainfall, R, is found to be {{{{ { Q}_{ p} = { 0.895} over { { A}^{0.145 } } }}}} AR having high significance of correlation coefficient, 0.927, between peak discharge, Qp, and effective rainfall, R. Design chart for the peak discharge (refer to Fig. 15) with watershed area and effective rainfall was established by the author. 5. The mean slopes of main streams within the range of 1.46 meters per kilometer to 13.6 meter per kilometer. These indicate higher slopes in the small watersheds than those in larger watersheds. Lengths of main streams are within the range of 9.4 kilometer to 41.75 kilometer, which can be regarded as a short distance. It is remarkable thing that the time of flood concentration was more rapid in the small watersheds than that in the other larger watersheds. 6. Length of main stream, L, in relation to the watershed area, A, is found to be L=2.044A0.48 having a high significance of correlation coefficient, 0.968. 7. Watershed lag, Lg, in hrs in relation to the watershed area, A, and length of main stream, L, was derived as Lg=3.228 A0.904 L-1.293 with a high significance. On the other hand, It was found that watershed lag, Lg, could also be expressed as {{{{Lg=0.247 { ( { LLca} over { SQRT { S} } )}^{ 0.604} }}}} in connection with the product of main stream length and the centroid length of the basin of the watershed area, LLca which could be expressed as a measure of the shape and the size of the watershed with the slopes except watershed area, A. But the latter showed a lower correlation than that of the former in the significance test. Therefore, it can be concluded that watershed lag, Lg, is more closely related with the such watersheds characteristics as watershed area and length of main stream in the small watersheds. Empirical formula for the peak discharge per unit area, qp, ㎥/sec/$\textrm{km}^2$, was derived as qp=10-0.389-0.0424Lg with a high significance, r=0.91. This indicates that the peak discharge per unit area of the unitgraph is in inverse proportion to the watershed lag time. 8. The base length of the unitgraph, Tb, in connection with the watershed lag, Lg, was extra.essed as {{{{ { T}_{ b} =1.14+0.564( { Lg} over {24 } )}}}} which has defined with a high significance. 9. For the derivation of IUH by applying linear conceptual model, the storage constant, K, with the length of main stream, L, and slopes, S, was adopted as {{{{K=0.1197( {L } over { SQRT {S } } )}}}} with a highly significant correlation coefficient, 0.90. Gamma function argument, N, derived with such watershed characteristics as watershed area, A, river length, L, centroid distance of the basin of the watershed area, Lca, and slopes, S, was found to be N=49.2 A1.481L-2.202 Lca-1.297 S-0.112 with a high significance having the F value, 4.83, through analysis of variance. 10. According to the linear conceptual model, Formular established in relation to the time distribution, Peak discharge and time to peak discharge for instantaneous Unit Hydrograph when unit effective rainfall of unitgraph and dimension of watershed area are applied as 10mm, and $\textrm{km}^2$ respectively are as follows; Time distribution of IUH {{{{u(0, t)= { 2.78A} over {K GAMMA (N) } { e}^{-t/k } { (t.K)}^{N-1 } }}}} (㎥/sec) Peak discharge of IUH {{{{ {u(0, t) }_{max } = { 2.78A} over {K GAMMA (N) } { e}^{-(N-1) } { (N-1)}^{N-1 } }}}} (㎥/sec) Time to peak discharge of IUH tp=(N-1)K (hrs) 11. Through mathematical analysis in the recession curve of Hydrograph, It was confirmed that empirical formula of Gamma function argument, N, had connection with recession constant, Kl, peak discharge, QP, and time to peak discharge, tp, as {{{{{ K'} over { { t}_{ p} } = { 1} over {N-1 } - { ln { t} over { { t}_{p } } } over {ln { Q} over { { Q}_{p } } } }}}} where {{{{K'= { 1} over { { lnK}_{1 } } }}}} 12. Linking the two, empirical formulars for storage constant, K, and Gamma function argument, N, into closer relations with each other, derivation of unit hydrograph for the ungaged small watersheds can be established by having formulars for the time distribution and peak discharge of IUH as follows. Time distribution of IUH u(0, t)=23.2 A L-1S1/2 F(N, K, t) (㎥/sec) where {{{{F(N, K, t)= { { e}^{-t/k } { (t/K)}^{N-1 } } over { GAMMA (N) } }}}} Peak discharge of IUH) u(0, t)max=23.2 A L-1S1/2 F(N) (㎥/sec) where {{{{F(N)= { { e}^{-(N-1) } { (N-1)}^{N-1 } } over { GAMMA (N) } }}}} 13. The base length of the Time-Area Diagram for the IUH was given by {{{{C=0.778 { ( { LLca} over { SQRT { S} } )}^{0.423 } }}}} with correlation coefficient, 0.85, which has an indication of the relations to the length of main stream, L, centroid distance of the basin of the watershed area, Lca, and slopes, S. 14. Relative errors in the peak discharge of the IUH by using linear conceptual model and IUH by routing showed to be 2.5 and 16.9 percent respectively to the peak of observed unitgraph. Therefore, it confirmed that the accuracy of IUH using linear conceptual model was approaching more closely to the observed unitgraph than that of the flood routing in the small watersheds.

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Study on Discharge Characteristics Using $V_t$ Close-Curve Analysis in ac PDPs

  • Cho, Byung-Gwon;Tae, Heung-Sik
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2007년도 7th International Meeting on Information Display 제7권2호
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    • pp.1185-1188
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    • 2007
  • The address discharge characteristics by the various scan-low and common-bias voltages are investigated based on measured address discharge time lags and $V_t$ close-curve analysis. The scan-low voltages are changed under the same voltage difference between the X and Y electrodes during an address period. As the voltage difference between the scan and address electrodes is increased during an address period, the address discharge time lag is shortened but the background luminance is increased. It is found that the improved address discharge characteristics is caused by the effect of the higher external applied voltage during an address period than the accumulated wall charges during a reset period and the high background luminance can be prevented by applying an address-bias voltage during a rising-ramp period and low reset voltage.

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보 개방에 의한 하도의 지형변화 과정 수치모의 분석(세종보를 중심으로) (Numerical analysis of morphological changes by opening gates of Sejong Weir)

  • 장창래;박태효;강태운;옥기영
    • 한국수자원학회논문집
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    • 제54권8호
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    • pp.629-641
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    • 2021
  • 본 연구에서는 2차원 수치모형(Nays2DH)을 적용하여 금강에 건설된 세종보를 중심으로 보 개방 후에 홍수량 변화에 의한 하도의 지형변화 과정을 분석하였다. 이를 위해 부등류, 부정류(단일사상), 연속홍수사상을 수문특성을 반영한 흐름조건으로 수치모의를 수행하였다. 부등류 수치모의 조건은 유황에 따른 정상유량으로 상류단 경계조건을 가정하였다. 부정류와 연속홍수사상의 경우에는 실제 홍수사상들로부터 정규 수문곡선 (normalized hydrograph)을 산정 한 후, 시나리오에 따른 첨두유량으로 정규 수문곡선을 재구성하여 상류단 유량으로 가정하였다. 본 연구에서는 지형학적 변화를 정량적으로 평가하기 위해 하상기복지수(BRI)를 산정하여 시간에 따른 하상변동을 분석하였으며, 연구지역의 항공사진과 수치모의 결과를 정성적으로 비교하였다. 부등류 수치모의 결과, 각 유황별 유량이 증가하면 하폭 대 수심의 비는 감소하고, 사주의 이동속도는 증가하였다. 하상기복지수는 초기에는 증가하지만, 시간이 증가함에 따라 변화량이 작아졌다. 또한 유량이 증가하면 하상기 복지수가 증가했다. 부정류 수치모의 결과 사주의 이동속도는 유량의 변화에 따라 감소했다. 또한 첨두홍수에 대한 지형적 반응에서 시간지체(time lag)가 발생했다. 즉, 부정류에서는 하상고의 변화는 수리학적 조건에 대하여 위상지연(Phase lag) 이 나타났다. 연속홍수사상 발생에 의한 부정류 수치모의 결과에서는 각각 첨두홍수 발생에 따른 사주의 이동속도는 홍수발생이 반복됨에도 불구하고 급격하게 감소했다. 또한 부정류 수치모의 결과와 마찬가지로 위상지연이 나타났으며 사주의 이동속도는 지수적으로 감소하는 특성을 보였다. 하상기복지수는 시간경과에 따라 증가하였으나, 첨두홍수가 연속으로 발생하였음에도 불구하고 하상기복지수의 증가율은 완만하였다. 본 연구를 통해 하천의 수문특성을 반영한 지형변화 과정을 수치모의를 수행하여 분석하였으며, 이를 통해 흐름특성에 따른 하상변동의 정량적인 예측모의를 현장에 적용할 수 있는 방법을 제시할 수 있을 것으로 판단된다.

Underwater Discharge Phenomena in Inhomogeneous Electric Fields Caused by Impulse Voltages

  • Lee, Bok-Hee;Kim, Dong-Seong;Choi, Jong-Hyuk
    • Journal of Electrical Engineering and Technology
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    • 제5권2호
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    • pp.329-336
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    • 2010
  • The paper describes the electrical and optical properties of underwater discharges in highly inhomogeneous electric fields caused by 1.2/50 ${\mu}s$ impulse voltages as functions of the polarity and amplitude of the applied voltage, and various water conductivities. The electric fields are formed by a point-to-plane electrode system. The formation of air bubbles is associated with a thermal process of the water located at the tip of the needle electrode, and streamer coronas can be initiated in the air bubbles and propagated through the test gap with stepped leaders. The fastest streamer channel experiences the final jump across the test gap. The negative streamer channels not only have more branches but are also more widely spread out than the positive streamer channels. The propagation velocity of the positive streamer is much faster than that of the negative one and, in fact, both these velocities are independent of the water conductivity; in addition the time-lag to breakdown is insensitive to water conductivity. The higher the water conductivity the larger the pre-breakdown energy, therefore, the ionic currents do not contribute to the initiation and propagation of the underwater discharges in the test conditions considered.

선행강우를 고려한 제주하천 유출특성 분석 (Rainfall-Runoff Characteristics in a Jeju Stream considering Antecedent Precipitation)

  • 양성기;김동수;정우열
    • 한국환경과학회지
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    • 제23권4호
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    • pp.553-560
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    • 2014
  • The rainfall-runoff characteristics in Jeju Island significantly differ from those in inland, due to highly permeable geologic features driven by volcanic island. Streams are usually sustained in the dry conditions and thereby the rainfall-runoff characteristics changes in terms of initiating stream discharge and its types, depending highly on the antecedent precipitation. Among various the rainfall-runoff characteristics, lag time mainly used for flood warning system in river and direct runoff ratio for determining water budget to estimate groundwater recharge quantity are practically crucial. They are expected to vary accordingly with the given antecedent precipitation. This study assessed the lag time in the measured hydrograph and direct runoff ratio, which are especially in the upstream watershed having the outlet as $2^{nd}$ Dongsan bridge of Han stream, Jeju, based upon several typhoon events such as Khanun, Bolaven, Tembin, Sanba as well as a specific heavy rainfall event in August 23, 2012. As results, considering that the lag time changed a bit over the rainfall events, the averaged lag time without antecedent precipitation was around 1.5 hour, but it became increased with antecedent precipitation. Though the direct run-off ratio showed similar percentages (i.e., 23%)without antecedent precipitation, it was substantially increased up to around 45% when antecedent precipitation existed. In addition, the direct run-off ration without antecedent precipitation was also very high (43.8%), especially when there was extremely heavy rainfall event in the more than five hundreds return period such as typhoon Sanba.

Characteristics of Laser-Guided DC Discharge by Nd: YAG Laser at Low Pressure

  • Lee, Dong-Hoon;Kim, Hee-Je
    • Journal of Electrical Engineering and information Science
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    • 제3권3호
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    • pp.316-321
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    • 1998
  • In recent years, concern has been raised about the technique of controlling electrical breakdown by using laser in many fields. Especially, laser has attracted much attention in the Electro-Discharge Macining(EDM) because of its many merits. Therefore, this research has been performed to obtain fundamental data relevant to discharge processing by using a pulsed Nd:YAG laser. The experiments of laser-guided dc discharge by laser radiation have been carried out at low air pressure ranging from 0.2 to 20 torr. The minimum laser-guided dc discharge voltage V\ulcorner at the given pressures P and distances D between an anode and a cathode was measured. It is found that the minimum laser-guided dc discharge voltage is much lower than the natural discharge voltage V\ulcorner\ulcorner, and the values of V\ulcorner and V\ulcorner as a function of P.D has a similar tendency. The laser output energy Eout decreases with input pulse duration tp increasing, and the more the value of tp increases, the higher that of V\ulcorner is obtained because the number of photons during the discharge time N decreases with t\ulcorner increasing. There is the time lag frequently when the discharge by laser radiation is misguided under the condition of the applied voltage less than V_G.min.

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유역분할에 따른 첨두홍수량 특성에 관한 연구 (A Study of Peak Discharge Variation by Dividing Watershed)

  • 박기범
    • 한국환경과학회지
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    • 제15권4호
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    • pp.365-372
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    • 2006
  • In this study investigated that topographical parametersestimate and calculated travel time, storage coefficient and lag time by watershed dividing 11, 8, 6 and 2. The results showed the more divide watershed, the more increase peak discharges. The results showed that Kraven-Clark-Kraven case is good simulated by compared observed data with calculated data. The sub-basin number are adequate $6{\sim}11$ for wichun and travel times compare observed data with calculated data at the younggok, to take about $18{\sim}20hr$ by simulated results but observed data shorter $8{\sim}10hr$. From this study results showed that it could be make narrow parameter estimate for observed hydrograph simulation, if more observed velocity and hydrograph. Also, as results of this study that is help to estimate parameters (arrival time, storage coefficient and lag time for Clark model.

방전논리게이트 플라즈마 디스플레이 패널의 직류방전 지연특성 (The Delay-Time Characteristics of DC Discharge in the Discharge Logic Gate Plasma Display Panel)

  • 염정덕;곽희로
    • 조명전기설비학회논문지
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    • 제21권1호
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    • pp.28-34
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    • 2007
  • 본 연구에서는 새로 고안된 방전 논리 게이트 PDP의 논리 게이트 입력인 DC 방전특성에 대해 고찰하였다. 새로 고안된 방전 논리 게이트는 방전 경로에 따른 전극사이의 전위차를 제어하여 논리 출력을 유도한다. 실험결과 이 DC 방전들의 안정성을 위해 프라이밍 방전을 인가한 경우가 인가하지 않은 경우에 비해 방전지연시간이 1/3로 단축되며 방전개시전압은 1/2로 감소하였다. 또한 이 프라이밍 방전에서 발생한 공간전하는 방전종료 후 $30[{\mu}s]$ 정도까지 영향을 미친다. 그리고 시간적, 공간적 거리변화에 파라 공간전하가 DC 방전에 미치는 영향을 측정한 결과, 주 방전에서부터 시간적으로 멀어지는 것보다 공간적으로 멀어지는 것이 주 방전의 영향에서 쉽게 벗어날 수 있음을 알았다. 그러므로 각 주사전극 마다 방전 논리 게이트들을 독립적으로 동작시킬 수 있다는 결론을 얻었다.

AC PDP에서 고속 어드레싱을 위한 ADR(Address During Reset) 구동 방식 (The ADR(Address During Reset) Driving Method for High-Speed Addressing in an AC-PDP)

  • 송근영;김근수;이석현
    • 대한전기학회논문지:전기물성ㆍ응용부문C
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    • 제54권6호
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    • pp.269-273
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    • 2005
  • In order to achieve high efficiency and low cost, new high-speed addressing method is suggested. This can be implemented by reducing the address discharge time lag through the priming effect. This paper suggests a new ADR(Address During Reset) driving method which provides priming particles by a separated driving method without adding auxiliary electrode or auxiliary discharge. The experimental results show an approximately 100ns reduction in the formative delay time of address discharge and a reduction in jitter of over 200ns. Also, due to enough time being available for reset, there was a reduction of about 29$\%$ in linht emitted during the reset period considerably.