• 제목/요약/키워드: F-V curve

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MR영상의 뇌관류 정보 Mapping을 위한 영상후처리 시스템개발 (Development of Image Post-processing System for the Cerebral Perfusion Information Mapping of MR Image)

  • 이상민;강경훈;장두봉;김광열;김영일;신태민
    • 한국정보통신학회논문지
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    • 제4권1호
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    • pp.131-138
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    • 2000
  • This paper works on development of an algorithm for mapping of cerebral perfusion parameters using the gamma-variate curve fitting. The signal intensity variate curve according to time measured in each pixel of perfusion MRI is nonlinear, and various hemodynamic parameters are not computed accurately. Levenberg-Marquardt algorithm(LMA), nonlinear optimum algorithm with high convergent speed and stability, is used to compute them. That is, the signal intensity variate curve is fitted by the gamma-variate function. Various hemodynamic parameters - Cerebral Blood Volume(C.B.V), Mean Transit Time(M.T.T), Cerebral Blood Flow(C.B.F), Time-to-Peak(T.T.P), Bolus Arrival Time(B.A.T), Maximum Slope(M.S) - are computed using LMA.

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LiF(Mg,Cu,Na,Si)형광체의 열자극엑소전자방출 (Thermally Stimulated Exoelectron Emission from LiF(Mg,Cu,Na,Si) Phosphor)

  • 도시홍;정중현;청목정의;서천조웅;옥천양일;기부광효
    • 센서학회지
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    • 제3권2호
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    • pp.11-15
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    • 1994
  • LiF(Mg,Cu,Na,Si)형광체의 ${\gamma}$ 선과 ${\beta}$ 선에 대한 TSEE 특성을 조사하였다. 이 형광체의 TSEE glow 곡선은 $20^{\circ}C$에서 $400^{\circ}C$사이에서 5개의 피크를 나타내었으며 주피크는 $240^{\circ}C$였다. $^{60}Co$ ${\gamma}$ 선에 대한 형광체의 감도는 약 450 counts/mR 이었다. ${\beta}$ 선에 대한 TSEE 에너지의존성은 ${\beta}$ 입자의 평균에너지 0.02MeV에서 0.8MeV 사이에서 ${\pm}10%$이었다. 그리고 이 형광체의 ${\beta}$ 선에 대한 TSEE 효율은 $(2{\sim}15){\times}10^{-3}$ 이었다.

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헴트 소자의 해석적 직류 모델 (An Analytical DC Model for HEMT's)

  • 김영민
    • 대한전자공학회논문지
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    • 제26권6호
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    • pp.38-47
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    • 1989
  • 헴트(HEMT) 소자의 순수 해석적 DC모델이 2차원 전하제어 시뮬레이션 결과[4]에 기초하여 제작되었다. 이 모델에서는 2-DEG 채널의 전자 운송 역학에 확산 효과를 추가하였다. 이 확산효과는 기존 1차원 DC모델에서 사용하는 전자 이동도 및 문턱전압을 증가시키는 효과를 가졌음을 보였다. 또한 2-DEG 농도분포함수를 piecewise 선형화하여 HEMT 소자의 subthreshold 특성의 해석적 모델을 추가하였고, 따라서 2-DEG의 채널 두께 및 게이트 용량을 게이트 전압의 함수로 나타내었다. I-V curve의 전류포화영역에서의 기울기를 모델하는데는 gate 밑의 전자포화채널 지역에서의 전자채널두께와 채널길이 변조현상을 함께 고려하였다. Troffimenkoff형의 전장의존 전자이동도를 사용하여 I-V곡선의 포화현상을 모델하였다. 또한 기존 1차원 모델에서 감안되지 않은 2차원 효과가 실제 전류특성곡선에서 매우 중요한 역할을 하며, 이 효과가 효과적으로 1개의 보정상수f로 보상됨을 보였고, 물리적으로 이 상수가 채널 GCA 지역과 채널포화지역 사이에 형성되는 채널천이지역의 전자농도와 관계됨을 보였다.

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LiF:Mg,Cu,Na,Si TL 소자의 선량계적 특성 (Dosimetric Properties of LiF:Mg,Cu,Na,Si TL pellets)

  • 남영미;김장렬;장시영
    • Journal of Radiation Protection and Research
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    • 제26권1호
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    • pp.7-12
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    • 2001
  • 최근 개발된 방사선량 측정용 LiF:Mg,Cu,Na,Si TL 소자의 글로우 곡선, 방출스펙트럼, 광자에 대한 선량의존성, 에너지의존성 및 페이팅 등과 같은 물리적 및 선량계적 특성들을 연구하였다. LiF:Mg,Cu,Na,Si TL 소자는 LiF:Mg,Cu,Na,Si TL 분말에 압력을 가한 후 소결하는 방법으로 제조되었다. 방사선에 대한 특성을 알아보기 위하여 광자선 조사는 한국원자력연구소의 X선 발생 장치 및 $^{137}Cs$ ${\gamma}$선 원격조사장치를 이용하였으며, 사용된 광자선 에너지 범위는 20-662keV, 선량 범위는 $10^{-6}-10^{-2}\;Gy$이었다. 글로우 곡선은 수동형의 TLD 판독장치 (System 310, Teledyne)로 질소를 흘리면서 선형적인 가열률로 측정하였으며, TL 강도는 글로우 곡선을 전체 적분한 면적으로 평가하였다. $5^{\circ}C\;s^{-1}$의 선형적인 가열률로 측정한 글로우 곡선은 5개의 피크들로 분리되었으며, $234^{\circ}C$에 나타나는 주피크의 활성화에너지는 2.34 eV, 진동수인자는 $1.00{\times}10^{23}$이고, 방출스펙트럼은 410nm를 중심으로한 단일한 분포로 나타났다. 선량의존성은 100Gy 이상까지 선형성을 나타내었으며, $^{137}Cs$에 대한 저에너지 광자의 상대적인 에너지 반응값은 20% 범위 이내였다. 또한 실온에서 1년간 보관하였을 때, 시간경과에 따른 TL 감도의 감소가 거의 없는 좋은 페이딩 특성을 보였다.

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스퍼터링법을 이용한 OLED용 Al 음전극 제작 (Preparation of Al Cathode for OLED by Sputtering Method)

  • 금민종;김경환
    • 한국전기전자재료학회논문지
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    • 제18권8호
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    • pp.729-733
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    • 2005
  • Al electrode for OLED was deposited by FTS (Facing Targets Sputtering) system which can deposit thin films with low substrate damage. The Al thin films were deposited on the cell (LiF/EML/HTL/Bottom electrode) as a function of working gas such as Ar or Ar+kr mixed gas. Also Al thin films were prepared with working gas pressure (1, 6 mTorr). The film thickness and I-V curve of Al/cell were measured and evaluated. In the results, when Al thin films were deposited using pure Ar gas, the turn-on voltage of Al/cell was about 11 V. And using the Ar:Kr($75\%:25\%$) mixed gas, the turn-on voltage of Al/cell decreased to about 7 V.

스퍼터링법을 이용한 OLED용 Al 전극의 제작 (Preparing of the AI electrode for OLED by Sputtering Methode)

  • 김경환;금민종
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2005년도 춘계학술대회 논문집 디스플레이 광소자 분야
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    • pp.72-75
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    • 2005
  • In this study Al electrode for OLED was deposited by FTS(Facing Targets Sputtering) system which can deposit thin films with low substrate damage. The Al thin films were deposited on the cell(LiF/EML/HTL/Bottom electrode) as a function of working gas such as Ar, Kr or mixed gas. Also Al thin films were prepared with working gas pressure (1, 6 mTorr ). The film thickness and I-V curve of Al/cell were evaluated by $\alpha$-step and semiconductor parameter (HP4156A) measurement. In the results, when Al thin film were deposited using pure Ar gas, the turn-on voltage of Al/cell was about 11[V]. And the turn-on voltage of Al/cell can be decrease to about 7[V].

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펄스 전류 하에서 AZ31 마그네슘 합금의 플라즈마전해산화 피막의 형성 거동 (PEO Film Formation Behavior of AZ31 Mg Alloy under Pulse Current)

  • 문성모
    • 한국표면공학회지
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    • 제55권5호
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    • pp.292-298
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    • 2022
  • In this study, PEO (plasma electrolytic oxidation) film formation behavior of AZ31 Mg alloy under application of 300 Hz pulse current was studied by the analyses of V-t curve, arc generation behavior, PEO film thickness and morphology of PEO films with treatment time in 0.05 M NaOH + 0.05 M Na2SiO3 + 0.1 M NaF solution. PEO films was observed to grow after 10 s of application of pulse current together with generation of micro-arcs. PEO film grew linearly with treatment time at a growth rate of about 5.58 ㎛/min at 200 mA/cm2 of pulse current but increasing rate of film formation voltage became lowered largely with increasing treatment time after passing about 250 V, suggesting that resistivity of PEO films during micro-arc generation decreases with increasing film formation voltage at more than 250 V.

표면파를 이용한 터키 이즈밋 근교 부지의 S파 속도 구조 규명 (Characterization of S-velocity Structure Near Izmit City of Turkey Using Ambient Noise and MASW)

  • 조창수
    • 지구물리와물리탐사
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    • 제11권3호
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    • pp.230-241
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    • 2008
  • 주변 잡음 자료를 이용한 부지 특성 규명 방법으로 삼각형 배열, 육각형 배열, 반원형 배열에 따른 표면파 분산곡선의 도출 특성을 파악하였고, 터키 이즈밋시의 인근 부지에 대한 부지특성을 살펴보기 위하여 주변 잡음 자료로부터 표면파 분산곡선과 H/V비를 도출하였다. 또한 MASW를 수행하여 고주파 분산곡선인 기본 모드와 1차 모드 분산곡선을 도출하였고 역산을 수행하여 S파 속도 구조를 구하였다. 표면파를 이용한 5파 속도 구조 규명에서는 역산시 비유일해의 문제가 발생하므로, MASW자료의 초동을 이용한 굴절법 토모그래피를 동시에 수행하여 얻어진 속도구조 비교를 통해서 유일해를 결정하였다.

수위유량곡선보정방법에 대하여 (A Method of Rating Curve Adjustment)

  • 박정근
    • 한국농공학회지
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    • 제18권2호
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    • pp.4116-4120
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    • 1976
  • With the use of many rivers increased nearly to the capacity, the need for information concerning daily quantities of water and the total annual or seasonal runoff has became increased. A systematic record of the flow of a river is commonly made in terms of the mean daily discharge Since. a single observation of stage is converted into discharge by means of rating curve, it is essential that the stage discharge relations shall be accurately established. All rating curves have the looping effect due chiefly to channel storage and variation in surface slope. Loop rating curves are most characteristic on streams with somewhat flatter gradients and more constricted channels. The great majority of gauge readings are taken by unskilled observers once a day without any indication of whether the stage is rising or falling. Therefore, normal rating curves shall show one discharge for one gauge height, regardless of falling or rising stage. The above reasons call for the correction of the discharge measurements taken on either side of flood waves to the theoretical steady-state condition. The correction of the discharge measurement is to consider channel storage and variation in surface slope. (1) Channel storage As the surface elevation of a river rises, water is temporarily stored in the river channel. There fore, the actual discharge at the control section can be attained by substracting the rate of change of storage from the measured discharge. (2) Variation in surface slope From the Manning equation, the steady state discharge Q in a channel of given roughness and cross-section, is given as {{{{Q PROPTO SQRT { 1} }}}} When the slope is not equal, the actual discharge will be {{{{ { Q}_{r CDOT f } PROPTO SQRT { 1 +- TRIANGLE I} CDOT TRIANGLE I }}}} may be expressed in the form of {{{{ TRIANGLE I= { dh/dt} over {c } }}}} and the celerity is approximately equal to 1.3 times the mean watrr velocity. Therefore, The steady-state discharge can be estimated from the following equation. {{{{Q= { { Q}_{r CDOT f } } over { SQRT { (1 +- { A CDOT dh/dt} over {1.3 { Q}_{r CDOT f }I } )} } }}}} If a sufficient number of observations are available, an alternative procedure can be applied. A rating curve may be drawn as a median line through the uncorrected values. The values of {{{{ { 1} over {cI } }}}} can be yielded from the measured quantities of Qr$.$f and dh/dt by use of Eq. (7) and (8). From the 1/cI v. stage relationship, new vlues of 1/cI are obtained and inserted in Eq. (7) and (8) to yield the steady-state discharge Q. The new values of Q are then plotted against stage as the corrected steadystate curve.

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The Influence of Cimetidine on the Pharmacokinetics of Diltiazem and its Main Metabolite in Rabbits

  • Park, Jun-Shik;Burm, Jin-Pil
    • Archives of Pharmacal Research
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    • 제27권2호
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    • pp.254-258
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    • 2004
  • The purpose of this study was to investigate the pharmacokinetic alteration of diltiazem and its main metabolite, deacetyldiltiazem, after oral administration of diltiazem in rabbits with or with-out cimetidine co-administration. The area under the plasma concentration-time curve (AUC) of diltiazem was significantly elevated in rabbits pretreated with cimetidine, suggesting that the oral clearance, an index of intrinsic clearance, may be decreased by the cimetidine treatment. Consistent with the increased AUC by the treatment, peak plasma concentration ($C_{max}$) for diltiazem was also elevated. Apparent volume of distribution normalized by the bioavailability (($V_{d}$/F) of diltiazem increased sigrificantly in rabbits pretreated with cimetidine increased. Taken together with the fact that the first pass metabolism for diltiazem is the primary determinant for the oral bioavailability, these observations indicate that increases in the oral clearance and (($V_{d}$/F may be a manifestation of the decreased first pass metabolism. Consistent with the hypothesis, the AUC of deacetyldiltiazem was significantly decreased in rabbits with cimetidine treatment. Ratio of deacetyldiltiazem to total diltiazem in the plasma was significantly decreased in rabbits with cimetidine treatment. These observations suggested that the metabolism of diltiazem to deacetyldiltiazem was reduced by cimetidine treatment and that the dosage of diltiazem should be adjusted when the drug is co-administered chronically with cimetidine in a clinical setting.