• 한국초전도ㆍ저온공학회논문지
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• 제12권4호
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• pp.13-16
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• 2010

The Lorentz force distribution of a high $T_c$ superconducting tape with increasing transport currents in magnetic field ($H_a$) was visualized. The external magnetic field was applied normally to the coated conductor tape surface after zero-field cooling, and the transport current ($I_a$) was increased stepwise from 0 to 90 % of the values of the critical current ($I_c$ ($H_a$)) at applied filed, Ha. The field distribution (H(x)) near the sample surface across the tape width (2w) was measured using the scanning Hall probe method. Applying an inversion to the measured field distribution, we obtained the underlying current distribution (J(x)), from which the magnetic induction, B(x) was calculated with Biot-Savart law. Then Lorentz force per unit length was calculated using F(x)=J(x)${\times}$B(x), which appears to be very inhomogeneous along the tape width due to the complicated distributions of J(x) and B(x).

• 한국초전도ㆍ저온공학회논문지
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• 제25권3호
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• pp.38-42
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• 2023

The evaluation of no-insulation (NI) high-temperature superconducting (HTS) typically uses the lumped equivalent circuit (LEC) model. Constant parameters in the NI HTS LEC model accurately predict voltage and central magnetic field at currents below the critical current. However, it is difficult to find constant circuit parameters that simultaneously satisfy the measured voltage and magnetic field under overcurrent conditions. Recent research highlights changes in contact resistance during transient conditions, which may impact power loss estimation in NI HTS coils. Therefore, we confirm the influence of contact resistance changes on loss calculation in the transient state for NI HTS coil. To achieve this, we introduce a measurement data analysis method based on the LEC model and compare it with the LEC model using constant circuit parameters.

• 한국수정란이식학회지
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• 제19권2호
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• pp.101-112
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• 2004

본 연구는 포유류인 $Cl^-$통로의 존재 여부를 확인하기 위하여 수행되었다. $Cl^-$통로는 비흥분성 세포에서 용적변화와 pH 조절, 이온운반계 등에 중요한 역할을 수행하므로 활발한 세포분화가 이루어지는 난자의 생존과 기능에 필수적 $Cl^-$통로 존재 여부를 확인하고자 하였다. 단일통로 전류를 기록하는 patch clamp 기법을 이용하였다. 세포외(pipette) 용액을 140 mM NaCl로 하고 세포내(bath) 용액을 70 mM, 140 mM, 280 mM NaCl로 바꾸어 주었을 때, 역전압($E_{rev}$) 은 $Cl^-$평형전압을 반영하는 -9.8${\pm}$0.5mV, 0mV, 11.5${\pm}$0.2mV로 변화하였다(n=4). 이런 결과는 이론치와 약간의 편차를 보이고 있으므로 이를 보정하기 위항 Goldman-Hodgkin-Katz(GHK) 식을 이용한 결과 $Cl^-$에 대한 $Na^+$의 투과성 ($P_{Na}$/$P_{Cl}$/)은 0.25로 추측할 수 있었다. Inside out patch mode에서 Pipette 용액과 bath 용액에 imperment인 NMDG-Cl로 구성하였을 경우 단일 통로가 기록되었다.(n=22). 막전압이 증가함에 따라 전도도(conductance)가 같이 증가하였으며 전류-전압 관계는 outward rectification을 보였다. 이런 특성을 나타내는 단일통로로 전류는 선택적 $Cl^-$통로 차단제인 IAA-94(indanyloxyacetic acid 94)에 의해 농도 의존적으로 차단되었으며 가역적으로 회복되었다. IAA의 $IC_{50}$은 32.6$\mu\textrm{M}$이었다. DIDS(4,4'-diisothiocyan ostillben-2-2'disulfonic acid)에 의해서는 전류크기가 감소 되는 빠른 억제기전을 나타내는 차단효과를 보였으며 시간경과에 따라 seblevel로 감소되는 subconductance block 이 나타났다. 이상의 결과는 햄스터 난자에서 chloride 통로가 존재하여, 물질이동과 pH 조절기능을 나타내는 외향성 전류-전압관계를 보이는 $Cl^-$ 통로의 성상으로 미루어 볼 때 난자의 pH 조절과 용적조절과 같은 생리적 환경 조성에 관여할 것으로 추정된다.

• 한국산학기술학회논문지
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• 제18권11호
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• pp.23-30
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• 2017

20T 이상의 높은 자장을 발생시키는 초전도마그넷은 다중 마그넷형태로 제작된다. 주로 저온초전도선재와 고온초전도선재를 혼합하여 제작되며 근래에는 고온초전도선재만을 이용하는 연구도활발하게 진행되고 있다. 고온초전도선재는 외부자계의 방향에 따라 임계상태가 달라지고 임계전류가 달라지는 자계이방성 성질을 가지고 있다. 따라서 고자장용 다중마그넷의 임계전류를 계산할 때에는 적절한 해석기법을 사용해야 한다. 기존에 사용되어왔던 고자장용 다중마그넷의 임계전류 계산방법은 대부분 수직 및 수평각도만을 고려한 부하선 기법이 사용되어왔다. 이 계산방법은 외부자계의 최대수직자장에 의해서 임계전류가 제한되기 때문에 수평자장의 영향이 잘 고려되지 않는 단점이 있다. 본 논문에서는 마그넷의 임계전류를 정밀하게 계산하기위하여 수직 및 수평각도뿐만 아니라 $0{\sim}90^{\circ}$ 사이 모든 각도의 $I_C-B({\Theta})$ 데이터를 고려하였다. 본 논문에서 제시한 해석기법을 사용하여 두 가지 고자장용 다중마그넷 모델을 해석하고 임계전류를 계산하였다. 마그넷에 인가되는 자계분포를 해석하기 위해 전자계수치해석 프로그램을 사용하였으며 진화론적 최적화 알고리즘을 사용하여 중심 자장이 최대로 되는 임계전류를 계산하였다.

• The Korean Journal of Physiology and Pharmacology
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• 제21권2호
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• pp.225-232
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• 2017

We demonstrated the effect of nortriptyline, a tricyclic antidepressant drug and serotonin reuptake inhibitor, on voltage-dependent $K^+$ (Kv) channels in freshly isolated rabbit coronary arterial smooth muscle cells using a whole-cell patch clamp technique. Nortriptyline inhibited Kv currents in a concentration-dependent manner, with an apparent $IC_{50}$ value of $2.86{\pm}0.52{\mu}M$ and a Hill coefficient of $0.77{\pm}0.1$. Although application of nortriptyline did not change the activation curve, nortriptyline shifted the inactivation current toward a more negative potential. Application of train pulses (1 or 2 Hz) did not change the nortriptyline-induced Kv channel inhibition, suggesting that the effects of nortiprtyline were not use-dependent. Preincubation with the Kv1.5 and Kv2.1/2.2 inhibitors, DPO-1 and guangxitoxin did not affect nortriptyline inhibition of Kv channels. From these results, we concluded that nortriptyline inhibited Kv channels in a concentration-dependent and state-independent manner independently of serotonin reuptake.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2001년도 춘계학술대회논문집D
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• pp.325-330
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• 2001

One of the principal components of the KSTAR (Korea Superconducting Tokamak Advanced Research) tokamak structure is the vacuum vessel, which acts as the high vacuum boundary for the plasma and also provides the structural support for internal components. Hyundai Heavy Industries Inc. has performed the engineering design of the vacuum vessel. Here the overall configuration of the KSTAR vacuum vessel was briefly described and then the design methodology and the analysis results were presented. The vacuum vessel consists of double walls, several ports, leaf spring style supports. Double walls are separated by reinforcing ribs and filled with baking/shielding water. The overall external dimensions of the main body are 3.39 m high, 1.11 m inner radius, 2.99 m outer radius, and made of SA240-316LN. The vacuum vessel was designed to be capable of achieving the base pressure of $1\times10^{-8}$ Torr, and also to be structurally capable of sustaining the vacuum pressure, the electromagnetic and thermal loads during plasma disruption and bakeout, respectively. The vacuum vessel will be baked out maximum $150^{\circ}C$ by hot pressurized water through the channels formed between double walls and the reinforcing ribs. A 3-D temperature distribution and the resulting thermal loads in the vessel were calculated during bakeout. It was found that the vacuum vessel and its supports were structurally rigid based on the thermal stress analysis. The maximum electromagnetic loads on the vacuum vessel induced by eddy and halo currents resulting from the engineering plasma radial and vertical disruption scenarios have been estimated. The stress analyses have been performed based on these electromagnetic loads and the resulting stresses at he critical locations of the vacuum vessel were within the allowable stresses.

• 한국초전도ㆍ저온공학회논문지
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• 제5권3호
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• pp.6-10
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• 2003

Silver nano-powder was added to Ma $B_2$ to make (Ag)$_{(x)wt.%}$(Mg $B_2$)$_{(l00-x)wt.%}$ (A $g_{x}$-Mg $B_2$) (10 $\leq$ x $\leq$ 50) composite superconductors to investigate the effect of the Ag nano-powder on the vortex pinning. Pellets made out of the mixed powder were put inside stainless steel tubes, which were sintered at 85$0^{\circ}C$ in Ar atmosphere. No impurity phase was identified for as-rolled samples. However, both the Mg $B_2$ and the A $g_{x}$-Mg $B_2$ composite pellets, when sintered, contain small amount of Mg $B_4$ and MgAg impurity phases. From the magnetization study, it was found that the flux pinning was improved in the high magnetic field region (> 3 T) only when 10w/o Ag was added to Mg $B_2$. The "two step" structures in ZFC M(T) curve gradually increased as the amount of Ag added increased. Pinning centers can be created by adding a suitable amount of Ag nano-powder which is not too large to increase the decoupling between the Mg $B_2$ grains.crease the decoupling between the Mg $B_2$ grains.

• Progress in Superconductivity
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• 제13권2호
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• pp.111-116
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• 2011

Since superconducting wires have no resistance, electromagnets based on the superconducting wires produce no resistive heating with DC current as long as the current does not exceed the critical current of the wire. However, unlike resistive wires, superconducting wires exhibit AC heat loss. Embedding fine superconducting filaments inside copper matrix can reduce this AC loss to an acceptable level and opens the way to AC-capable superconducting coils. Here, we introduce an easy and accurate method to measure AC heat loss from sample superconducting coils by measuring changes in the rate of gas helium outflow from the liquid helium dewar in which the sample coil is placed. This method provides accurate information on total heat loss of a superconducting coil without any size limit, as long as the coil can fit inside the liquid helium dewar. With this method, we have evaluated AC heat loss of two superconducting solenoids, a 180-turn solid NbTi wire with 0.127 mm diameter (NbTi coil) and a 100-turn filamented wire with 1.4 mm diameter where 7 NbTi filaments were embedded in a copper matrix with copper to NbTi ratio of 6.7:1 (NbTi-Cu coil). Both coils were wound on 15 mm-diameter G-10 epoxy tubes. The AC heat losses of the NbTi and NbTi-Cu coils were evaluated as $53{\pm}4.7\;{\mu}W/A^2Hzcm^3$ and $0.67{\pm}0.16\;{\mu}W/A^2Hzcm^3$, respectively.

• 한국진공학회지
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• 제20권4호
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• pp.307-312
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• 2011

정상 세포로부터 암과 같은 종양세포를 제거하는 방법으로 라디오주파수의 전자파를 이용하여 세포가 사멸되는 임계온도보다 높은 온도로 국소 가열하는 발열 치료법이 임상에서 시술되고 있다. 그러나 이 기술은 임상에서 활발히 사용되기에는 여러 가지 제약 요인이 존재한다. 본 연구에서는 교류파 대신에 미소 직류전원을 사용하여 국소부위에 열을 발생하는 안전성이 증가된 방법의 실효성을 이론적으로 입증하고자 한다. 종양세포의 형태에 따라 적당한 모양의 전극을 종양조직에 삽입하고 종양조직의 형태와 유사한 열분포를 갖도록 제어하는 기술을 개발한다. 열원은 조직 내에 삽입된 전극과 매질에 형성되는 전기장에 의한 저항열이다. 종양 조직 내에 삽입된 전극에 10 V, 20 V, 30 V를 각각 인가하고 시간에 따른 열분포를 전산모의 하였다. 결과적으로, 20 V를 전극에 인가하면 1~2 분 이내에 버섯모양의 등온도 분포를 갖으며 세포를 고사시키는 온도 이상의 치료영역이 형성됨을 보였다. 4개의 전극에 대칭적인 전위를 인가하고 $50^{\circ}C$ 이상의 온도 분포를 암 조직의 모양과 유사하게 분포하도록 조절하여 효과적인 치료를 수행 할 수 있는 가능성을 제시하고자 한다.

• 한국전기전자재료학회논문지
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• 제17권12호
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• pp.1356-1361
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• 2004

High temperature superconducting coated conductor has a structure of ///. The buffer layer consists of multi-layer, this study reports the deposition method and optimal deposition conditions of YSZ(Yttria-stabilized zirconia) layer which plays a important part in preventing the elements of substrate from diffusing into the superconducting layer. YSZ layer was deposited by DC reactive sputtering technique using water vapor for oxidizing deposited elements on substrate. To investigate optimal thickness of YSZ film, four YSZ/CeO$_2$/Ni samples with different YSZ thickness(130 nm, 260 nm, 390 nm, and 650 nm) were prepared. The SEM image showed that the surface of YSZ layer was getting to be rougher as YSZ layer was getting thicker and the growth mode of YSZ layer was columnar grain growth. After CeO$_2$ layer was deposited with the same thickness of 18.3 nm on each four samples, YBCO layer was deposited by PLD method with the thickness of 300 nm. The critical currents of four samples were 0, 6 A, 7.5 A, and 5 A respectively. This shows that as YSZ layer is getting thicker, YSZ layer plays a good role as a diffusion barrier but the surface of YSZ layer is getting rougher.