• 제목/요약/키워드: flux data

검색결과 1,544건 처리시간 0.03초

주간에 두 타워로부터 관측된 에디 공분산 자료의 확률 오차의 추정 (Estimation of the Random Error of Eddy Covariance Data from Two Towers during Daytime)

  • 임희정;이영희;조창범;김규랑;김백조
    • 대기
    • /
    • 제26권3호
    • /
    • pp.483-492
    • /
    • 2016
  • We have examined the random error of eddy covariance (EC) measurements on the basis of two-tower approach during daytime. Two EC towers were placed on the grassland with different vegetation density near Gumi-weir. We calculated the random error using three different methods. The first method (M1) is two-tower method suggested by Hollinger and Richardson (2005) where random error is based on differences between simultaneous flux measurements from two towers in very similar environmental conditions. The second one (M2) is suggested by Kessomkiat et al. (2013), which is extended procedure to estimate random error of EC data for two towers in more heterogeneous environmental conditions. They removed systematic flux difference due to the energy balance deficit and evaporative fraction difference between two sites before determining the random error of fluxes using M1 method. Here, we introduce the third method (M3) where we additionally removed systematic flux difference due to available energy difference between two sites. Compared to M1 and M2 methods, application of M3 method results in more symmetric random error distribution. The magnitude of estimated random error is smallest when using M3 method because application of M3 method results in the least systematic flux difference between two sites among three methods. An empirical formula of random error is developed as a function of flux magnitude, wind speed and measurement height for use in single tower sites near Nakdong River. This study suggests that correcting available energy difference between two sites is also required for calculating the random error of EC data from two towers at heterogeneous site where vegetation density is low.

플럭스 타워 관측 자료 및 통합수문모형을 이용한 순복사량 산정: 설마천, 청미천 유역을 대상으로 (Net Radiation Estimation Using Flux Tower Data and Integrated Hydrological Model: For the Seolmacheon and Chungmichen Watersheds)

  • 김다은;백종진;정성원;최민하
    • 한국수자원학회논문집
    • /
    • 제46권3호
    • /
    • pp.301-314
    • /
    • 2013
  • 기후변화로 야기될 수 있는 태양복사에너지의 공간적인 불균형은 수자원을 포함한 전반적인 생태 시스템에서의 에너지 불균형을 초래한다. 따라서 정확한 에너지의 흐름을 이해하기 위하여 정량적인 관측을 목적으로 하는 플럭스 타워가 세계 곳곳에 설치되어 운영되고 있다. 국내의 주역에서도 플럭스 타워를 통안 관측이 실시되고 있는 데, 본 연구에서는 이 중 설마천과 청미천 유역의 플럭스 타워의 자료를 대상으로 수문기상 및 생태학적으로 중요한 역할을 하는 에너지원인 하향 단파 및 장파 복사량과 순복사량을 기존의 연구에서 제안된 물리식을 기반으로 계산하고, 산정된 순복사량과 관측 자료를 비교 검증하였다. 이를 통하여 관측이 미흡한 수문기상인자에 대해 기존의 물리적인 방법의 사용 가능성 및 관측 자료의 활용 가능성을 확인하였다.

UHF 센서 탑재 UAV를 이용한 지표층 열 플럭스 산출 (Estimation of Surface Layer Heat Flux Using the UHF Sensor Installed on UAV)

  • 김민성;권병혁;윤홍주
    • 한국전자통신학회논문지
    • /
    • 제13권1호
    • /
    • pp.265-276
    • /
    • 2018
  • 지상에 고정된 기기로 감시하기 어려운 대기 하층의 관측 사각 지역에서 유용한 관측 및 자료 분석 기술을 개발하였다. 상층 기상 관측에 사용되는 UHF 라디오존데를 UAV에 탑재하여 기온과 상대습도의 연직 자료를 원격 수집하여 10 m 기상 타워에서 측정한 자료와 비교하였다. 검증된 연직 분포로부터 외삽된 지표 기온과 총체 전달 방법을 이용하여 대기 안정도 변화에 따른 현열 플럭스를 추정하였다. 지상에서 3차원 초음파 풍속계로 측정한 현열 플럭스와 비교한 결과는 원격탐사로 산출되는 현열 플럭스에 허용되는 오차 범위 30%보다 작은 23% 이내의 오차를 보였다. UAV 관측 현열 플럭스로부터 추정한 대기경계층 고도는 대기 오염 확산 모델에 유용한 자료를 실시간, 경제적으로 제공할 수 있다.

국립기상과학원 플럭스 관측 자료 기반의 JULES 지면 모델 모의 성능 분석 (Evaluation of JULES Land Surface Model Based on In-Situ Data of NIMS Flux Sites)

  • 김혜리;홍제우;임윤진;홍진규;신승숙;김윤재
    • 대기
    • /
    • 제29권4호
    • /
    • pp.355-365
    • /
    • 2019
  • Based on in-situ monitoring data produced by National Institute of Meteorological Sciences, we evaluated the performance of Joint UK Land Environment Simulator (JULES) on the surface energy balance for rice-paddy and cropland in Korea with the operational ancillary data used for Unified Model (UM) Local Data Assimilation and Prediction System (LDAPS) (CTL) and the high-resolution ancillary data from external sources (EXP). For these experiments, we employed the one-year (March 2015~February 2016) observations of eddy-covariance fluxes and soil moisture contents from a double-cropping rice-paddy in BoSeong and a cropland in AnDong. On the rice-paddy site the model performed better in the CTL experiment except for the sensible heat flux, and the latent heat flux was underestimated in both of experiments which can be inferred that the model represents flood-irrigated surface poorly. On the cropland site the model performance of the EXP experiment was worse than that of CTL experiment related to unrealistic surface type fractions. The pattern of the modeled soil moisture was similar to the observation but more variable in time. Our results shed a light on that 1) the improvement of land scheme for the flood-irrigated rice-paddy and 2) the construction of appropriate high-resolution ancillary data should be considered in the future research.

북극해 지역의 위성 기반 복사 에너지 산출물의 비교 분석 (Comparative Analysis of Radiative Flux Based on Satellite over Arctic)

  • 서민지;이은경;이경상;최성원;진동현;성노훈;한현경;김현철;한경수
    • 대한원격탐사학회지
    • /
    • 제34권6_2호
    • /
    • pp.1193-1202
    • /
    • 2018
  • 북극의 장기간 기후 변화 관측을 위해서는 에너지 수지를 정량적으로 파악하는 것이 중요하다. 에너지 수지를 정량적으로 파악하기 위해서 고품질의 장기간 복사 에너지 변수들이 필요하지만 대부분 위성 기반 복사 에너지 변수 자료들은 제공되는 기간이 짧아 자료들을 연계하여 사용해야한다. 자료를 연계해서 사용하기 위해서는 사용되는 자료의 차이를 정확하게 파악하고 일치시키는 것이 중요하다. 따라서 본 연구에서는 위성 기반 복사 에너지 자료인 Global Energy and Water Exchanges Project(GEWEX) 와 Clouds and the Earth's Radiant Energy System(CERES)를 비교 분석하여 자료 연계를 위한 기초자료를 제공하고자 한다. 두 자료를 비교 분석한 결과 CERES자료를 기준으로 했을 때, GEWEX 자료가 과소 추정되었다. 또한 두 자료는 약 $3{\sim}25W/m^2$의 차이가 발생하였으며, 고위도 지역이거나 해빙지역일수록 두 자료의 차이가 더 증가하였다. 또한 두 자료의 월별 평균을 비교하였을 때는 하향 장파 복사 에너지를 제외한 나머지 변수들은 봄과 여름철에 $9.26{\sim}26.71W/m^2$의 높은 차이를 보였다. 본 연구 결과는 북극지역에서 CERES와 GEWEX 자료를 합성하거나 선택할 때 좋은 기준 자료로 사용 가능하다.

Statistical Analysis on the trapping boundary of outer radiation belt during geosynchronous electron flux dropout : THEMIS observation

  • 황정아;이대영;김경찬;최은진;신대규;김진희;조정희
    • 천문학회보
    • /
    • 제37권1호
    • /
    • pp.90.2-90.2
    • /
    • 2012
  • Geosynchronous electron flux dropouts are most likely due to fast drift loss of the particles to the magnetopause (or equivalently, the "magnetopause shadowing effect"). A possible effect related to the drift loss is the radial diffusion of PSD due to gradient of PSD set by the drift loss effect at an outer L region. This possibly implies that the drift loss can affect the flux levels even inside the trapping boundary. We recently investigated the details of such diffusion process by solving the diffusion equation with a set of initial and boundary conditions set by the drift loss. Motivated by the simulation work, we have examined observationally the energy spectrum and pitch angle distribution near trapping boundary during the geosynchronous flux dropouts. For this work, we have first identified a list of geosynchronous flux dropout events for 2007-2010 from GOES satellite electron measurements and solar wind pressures observed by ACE satellite. We have then used the electron data from the Time History of Events and Macroscale Interactions during Substorms (THEMIS) spacecraft measurements to investigate the particle fluxes. The five THEMIS spacecraft sufficiently cover the inner magnetospheric regions near the equatorial plane and thus provide us with data of much higher spatial resolution. In this paper, we report the results of our investigations on the energy spectrum and pitch angle distribution near trapping boundary during the geosynchronous flux dropout events and discuss implications on the effects of the drift loss on the flux levels at inner L regions.

  • PDF

Critical Heat Flux in Uniformly Heated Vertical Annulus Under a Wide Range of Pressures 0.57 to 15.0 MPa

  • Chun, Se-Young;Chung, Heung-June;Hong, Sung-Deok;Yang, Sun-Kyu;Chung, Moon-Ki
    • Nuclear Engineering and Technology
    • /
    • 제32권2호
    • /
    • pp.128-141
    • /
    • 2000
  • The critical heat flux (CHF)experiments have been carried out in a wide range of pressures for an internally heated vertical annulus. The experimental conditions covered ranges of pressures from 0.57 to 15.01 MPa, mass fluxes of 0 kg/$m^2$s and from 200 to 650 kg/$m^2$s, and inlet subcoolings from 85 to 413 kJ/kg. The characteristics of the present data and the effect of pressure on CHF are discussed. Most of the CHFs were identified to dryout of the liquid film in the annular or annular-mist flow. For the mass flux of 200 kg/$m^2$s, there were the indications that the CHF occurred at the transition from annular to annular-mist How in the pressure range of 3~10 MPa. For the mass fluxes of 550 and 650 kg/$m^2$s, the CHFs had a maximum value at a pressure of 2~3 MPa, and the pressure at the maximum CHF values had a trend moving toward the pressure at the peak value of pool boiling CHF as the mass flux decreased. The CHF data under a zero mass flux condition indicate that both the effects of pressure and inlet subcooling on the CHF were smaller, compared with those on the CHF with net water upward flow.

  • PDF

잔디밭에서 지온에 대한 이산화탄소 플럭스의 민감도(Q10) 분석 (Sensitivity Analysis (Q10) of Carbon Dioxide Flux with Soil Temperature in the Grassplot)

  • 강동환;소윤환;권병혁;김박사
    • 한국환경과학회지
    • /
    • 제28권9호
    • /
    • pp.785-795
    • /
    • 2019
  • In order to analyze the sensitivity of carbon dioxide flux by soil temperature in the grassplot, carbon dioxide flux and soil temperature were observed 24 times from March, 2010 to March, 2011 at nine sites in the grassplot. The average of $CO_2$ in the grassplot is $2.2{\sim}36.7^{\circ}C$, the highest in August, the lowest in January, and the average of carbon dioxide flux is $12{\sim}1479mgCO_2{\cdot}m^{-2}{\cdot}hr^{-1}$, and the carbon dioxide emission from the grassplot to the atmosphere was 10 times higher in summer than in winter. The temperature response coefficient estimated by the exponential function of carbon dioxide flux according to soil temperature was ranged from 0.1065 to 0.1274, and the increase tendency of $CO_2$ flux with soil temperature was linear at $0{\sim}20^{\circ}C$ and exponential at $20{\sim}40^{\circ}C$. The $Q_{10}$ values for each of nine observation sites on the grassplot was in the range of 2.901 ~ 3.575, and the $Q_{10}$ value using the total data observed in the lawn was estimated to be 3.374. In the homogeneous grassplot area, the average of $Q_{10}$ values by observation point and the $Q_{10}$ value by the total data were estimated similarly.

Ellipting Blending Model을 사용하여 자연대류 해석 시 난류 열유속 처리법 비교 (COMPARISON OF THE TREATMENTS OF TURBULENT HEAT FLUX FOR NATURAL CONVECTION WITH THE ELLIPTIC BLENDING SECOND MOMENT CLOSURE)

  • 최석기;김성오
    • 한국전산유체공학회:학술대회논문집
    • /
    • 한국전산유체공학회 2007년도 춘계 학술대회논문집
    • /
    • pp.171-176
    • /
    • 2007
  • A comparative study on the treatment of the turbulent heat flux with the elliptic mlending second moment closure for a natural convection is performed. Four cases of different treating the turbulent heat flux are considered. Those are the generalized gradient diffusion hypothesis (GGDH) the algebraic flux model (AFM) and the differential heat flux model (DFM). These models are implemented in the computer code specially designed for evaluation of turbulent models. Calculations are performed for a turbulent natural convection in the 1:5 rectangular cavity and the calculated results are compared with the experimental data. The results show that three models produce nearly the same accuracy of solutions.

  • PDF

상용 스테인리스 스틸 튜브 봉합기법(COSSET)으로 제작 된 MgB$_2$flux jump 현상 (Flux Jump of $MgB_2$ fabricated by commercial stainless steel tube enveloping technique)

  • Lee, H.B.;Kim, B.J.;Kim, Y.C.;Jeong, D.Y.
    • Progress in Superconductivity
    • /
    • 제4권1호
    • /
    • pp.27-31
    • /
    • 2002
  • MgB$_2$samples have been prepared by a stoichiometry mixture of Mg and B inside stainless steel tubes(Commercial Stainless Steel Tube Enveloping Technique). XRD data show that there are no second phases like MgO. The transition temperature of specimens is 37.5 K with a sharp transition width of ΔTc within 1K. From magnetic hysteresis measurement, flux jump was shown up to 15K, which was higher than that of samples by other methods. We have concluded that the flux jump is mainly affected by impurities and second phases.

  • PDF