• Journal of the Korean Vacuum Society
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• v.4 no.3
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• pp.238-246
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• 1995

대기, 고진공, 초고진공 등 다양한 압력 조건에서 STS 합금 표면의 오염상태를 AES 측정을 통해 살펴보았다. 모든 환경에서 노출 초기에 많은 오염이 이루어지며, 시간이 증가함에 따라 오염 속도는 감소하지만 지속적인 오염이 이루어지는 것을 볼 수 있었다. 오염층의 구조는 표면 위에 산소, 그 위에 Co,그리고 그 위에 탄소가 놓여 있는 층별 구조 형태로 나타났다.

• Geophysics and Geophysical Exploration
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• v.8 no.4
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• pp.237-242
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• 2005

A seismic refraction study in estimation of depth to the bedrock demonstrates that 1) the average velocity in the medium is about 250 m/s in the surface layer (< 4 m), 2,500 m/s in the weathered formation, and greater than 3,000 m/s in the bedrock, 2) the depth to the deepest reflector assumed to be the bedrock is about 17 m; however, according to the cores collected in a borehole in study area, the bedrock (granite) occurred at depth 25 m, 3) according to the density and velocity logging, at depth 17 m, a measurable velocity and density increase are observed, and 4) the velocity of the weathered formation is relatively high and therefore, the acquisition offsets ($70{\sim}80m$) are turned out not to be long enough to record the refracted signal from the bedrock at depth 25 m as first arrivals.

• Korean Journal of Materials Research
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• v.9 no.2
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• pp.211-216
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• 1999

Corrosion behavior of austenitic stainless steels of SUS 316L and SUS304L in molten salt of LiCl and $LiCl/Li_2O$ has been investigated in the temperature range of $650~850^{\circ}C$. Corrosion products of SUS316L and 304L in hot molten salt consisted of two layers-an outer layer of Li(CrFe)$O_2$and an inner layer of$Cr_2O_3$. The corrosion layer was uniform in molten salt of LiCl, but the intergranular corrosion occurred in addition to the uniform corrosion in mixed molten salt of LiCl/$Li_2O$. The corrosion rate increased slowly with the increase of temperature up to $750^{\circ}C$, but above $750^{\circ}C$ rapid increase in corrosion rate observed. SUS316L stainless steel showed slower corrosion rate than SUS 304L, exhibiting higher corrosion resistance in the molten salt.

• Journal of the Korean earth science society
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• v.28 no.7
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• pp.903-913
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• 2007

In this study, the researchers compared the S-wave velocity structures obtained by two kinds of dispersion curves: phase and group dispersions from a tidal flat located in the SW coast of the Korean peninsula. The ${\tau}-p$ stacking method was used for the phase velocity and two different methods (multiple filtering technique: MFT and continuous wavelet transform: CWT) for the phase velocity. It was difficult to separate higher modes from the fundamental mode phase velocities using the ${\tau}-p$ method, whereas the separation of different modes of group velocity were easily achieved by both MFT and CWT. Of the two methods, CWT was found to be more efficient than MFT. The spatial resolutions for the inversion results of the fundamental mode for both phase and group velocities were good for only a very shallow depth of ${\sim}1.5m$. On the other hand, the spatial resolutions were good up to ${\sim}4m$ when both the fundamental and the 1st higher mode poop velocities obtained by CWT were used for S-wave inversion. This implies that the 1st higher mode Rayleigh waves contain more information on the S-wave velocity in deeper subsurface. The researchers applied the CWT method to obtain the fundamental and the 1st higher mode poop velocities of the S-wave velocity structure of a tidal flat located in SW coast of the Korean peninsula. Thea the S-wave velocity structures were compared with the borehole description of the study area.

• Journal of Korean Society of Environmental Engineers
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• v.22 no.7
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• pp.1193-1203
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• 2000

In this study, in order to remove Cd(II) from aqueous solutions, strongly acidic cation exchange resin(SK1B) by Diaion Co. was employed as an adsorbent. Experiments were mainly performed in two parts at room temperature($25{\pm}5^{\circ}C$) : batch tests and adsorption kinetics tests. In batch tests adsorption equilibrium time, pH effects, temperature effects, several adsorption isotherms, and finally desorption tests were examined. In differential bed tests, an optimum flow rate and an overall adsorption rate were obtained. In the batch experiment, adsorption capability increased with pH and became constant above pH 6 and adsorption quantity increased with temperature. Batch experimental data found that Freundlich and Sips adsorption isotherms were more favorable than Langmuir adsorption isotherm over the range of concentration (5~15ppm). The desorbent used in the desorption test was hydrochloric acid solution with different concentrations(0.01~2N). The degree of regeneration increased with concentration of desorbent and decreased slightly with the number of regeneration. In the continuous flow process using a differential bed reactor, the optimum flow rate was $564m{\ell}/min$ above which the film diffusion resistance was minimized. The overall adsorption rate for the removal of Cd(II) by cation exchange resin was found as follows ; $r=1.3785C_{fc}^{1.2421}-2.0907{\times}10^{0.0746C_i}\;q_e^{0.0121C_i-0.0301}$

• Journal of the Korean Society of Fisheries and Ocean Technology
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• v.25 no.4
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• pp.209-213
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• 1989

The author suggested control method of partial cavitation with electro-magnetic accelerator and showed that the cavity shape decreased with this suggestion which compared with the theoretical ones. Using the cavity flow method proposed by the author in this paper, it is predicted that cavitation volume of the shape is less than the previous type one. Comparisons were performed in order to verify these facts, using both shape which calculated by the method. It was found that the difference of cavitation performance between the two shape of volume were decreased, because of the new method accelerated of flow more than previous theoretical ones.

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.45 no.7
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• pp.1-8
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• 2008

We fabricated flexible electrophoretic display(EPD) driven by organic thin film transistors(OTFTs) on plastic substrate. We designed the W/L of OTFT to be 15, considering EPD's transient characteristics. The OTFTs employed bottom contact structure and used Al for gate electrode, the cross-linked polyvinylphenol for gate insulator, pentacene for active layer. The plastic substrate was coated by PVP barrier layer in order to remove the islands which were formed after pre-shrinkage process and caused the electrical short between bottom scan and top data metal lines. Pentacene active layer was confined within the gate electrodes so that the off current was controlled and reduced by gate electrodes. Especially, PVA/Acryl double layers were inserted between EPD panel and OTFT-backplane in order to protect OTFT-backplane from the damages created by lamination process of EPD panel on the backplane and also accommodate pixel electrodes through via holes. From the OTFT-backplane the mobility was $0.21cm^2/V.s$, Ion/Ioff current ratio $10^5$. The OTFT-EPD panel worked successfully and demonstrated to display some patterns.

• Proceedings of the International Microelectronics And Packaging Society Conference
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• 2003.11a
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• pp.110-113
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• 2003

여러가지 Sn-Ag-Cu 솔더조성과 솔더링 후의 냉각속도에 따라 솔더링 접합부에서의 계면 미세조직의 다양한 변화를 관찰해 보았다. 현재까지 Sn-Ag-Cu 3원계 공정점에 대한 정확한 연구가 미흡하고, 상용으로 제품화되고 있는 Sn-Ag-Cu 합금계는 3원계 공정조성에서 약간 벗어난 조성들을 선택하고 있다고 할 수 있다. 따라서, 본 연구에서 사용한 Sn-Ag-Cu 합금 조성은 Sn-3.5Ag, Sn-3Ag-0.7Cu, Sn-3Ag-1.5Cu, Sn-3.7Ag-0.9Cu, Sn-6Ag-0.5Cu로 선택하였으며, 각 조성에서 Lap Shear Joint를 제조하였다. 사용한 Solder pad는 Cu pad와 Cu pad 위에 Au/Ni를 plating한 것을 이용하였다. 리플로우 솔더링 조건은 $250^{\circ}C$ 이상의 온도에서 60초 실시하였으며, 리플로우 솔더링 후의 냉각속도를 달리하여 냉각시켰다. 솔더링 후의 냉각속도가 느려질수록 계면 금속간화합물(IMC)의 두께가 더욱 증가하며, 조대화되었다. 또한 솔더 조성의 영향에서 Cu와 Ag의 함량이 높을수록 계면 IMC의 두께가 증가되었으며, 이는 솔더내부에 형성된 IMC 입자들이 조대화되어 계면 IMC층에 결합되어 나타났기 때문이다.

• Plant Journal
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• v.12 no.1
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• pp.37-43
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• 2016

The corrosivity evaluations on soil surrounding the buried steel piles under manufacturing plants. It was proven that the soil structure of this sample area is composed of several soil layers, and that each layer show the different corrosivity. The predicted average corrosion rates of some layers are about 0.33mm/y, which is over than the general corrosion rate, 0.01-0.02mm/y.

• Proceedings of the Korean Vacuum Society Conference
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• 1999.07a
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• pp.143-143
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• 1999

Co/Ti 다층 박막을 제조하기 위해 직류원 마그네트론 스퍼터링 시스템을 이용하여 (100)실리콘 단결정 기판위에 Co와 Ti층을 각각 2/2, 5/5, 10/10 nm 정도의 두께로 조절하여 세가지 조성의 Co/Ti 다층 박막을 제조하였다. 이러한 Co/Ti 다층 박막의 후속 열처리는 Ar 가스분위기 하에서 Tube furnace를 이용하여 20$0^{\circ}C$와 30$0^{\circ}C$, 40$0^{\circ}C$의 온도에서 진행하였다. 증착초기에서부터 후속 열처리 공정을 진행하는 동안, Co/Ti 다층 박막에서의 계면반응을 미세 구조 변화 및 전기, 자기적 특성변화와 연관지어 관찰하였다. Co/Ti 다층 박막의 결정 구조와 미세 구조 변화를 관찰하기 위해 각각 X-선 회절기와 투과 전자 현미경을 사용하였고, 다층 박막의 전기적, 자기적 특성 변화를 관찰하기 위해 각각 4점 탐침기, 진동 시료형 자속계를 이용하였다. Co/Ti 다층 박막을 20$0^{\circ}C$의 저온에서 열처리를 한 경우에는 증착 초기의 계면반응에 의해 형성된 비정질 층이 성장하였고, 30$0^{\circ}C$와 40$0^{\circ}C$의 고온에서 열처리를 하는 경우에는 비정질 측의 성장보다는 새로운 화합물 CoTi 결정상이 형성되면서 비정질상은 오히려 감소하였다. 즉, Co/Ti 다층 박막의 계면 반응은 결정질 Co와 Ti을 계면 반응물로 소모시키면서 비정질 층을 성장시키는 비정질화 반응이 활발히 일어났다. 특히, 소모된 계면 반응물로 소모시키면서 비정질 층을 성장시키는 비정질화 반응일 활발히 일어났다. 특히, 계면 반응물로 소모시키면서 비정질 층을 성장시키는 비정질화 반응일 활발히 일어났다. 특히, 소모된 계면 반응물 Co와 Ti 중에서 Ti의 소모속도가 더 빠르게 관찰되었다. 이로부터 Ti 이 증착초기에서 저온 열처리 과정동안 Co/Ti 다층 박막의 계면에서 일어나는 비정질화 반응의 주 확산자로 작용했다는 것을 알 수 있다. 한편, 30$0^{\circ}C$와 40$0^{\circ}C$의 고온에서 열처리한 Co/Ti 다층 박막의 계면 반응은, 비정질 반응에 의한 비정질층의 형성보다는 새로운 화합물 결정질 CoTi상을 형성시키는 결정화 반응이 우세했다. Co/Ti 다층 박막의 전기적 저항은, 열처리에 의한 비정질 층의 생성 및 성장으로 인해 증가하였고 새로운 저저항 CoTi 결정상의 형성으로 인해 감소하는 것을 알 수 있었다. 또한 Co/Ti 다층 박막의 포화 자화값은, 열처리에 의한 계면에서의 비정질화 반응과 CoTi 결정화 반응으로 인해 강자성체인 Co 결정상이 감소됨에 따라 감소하는 경향을 나타냈다.