• 제목/요약/키워드: Thermal Boundary Resistance

검색결과 75건 처리시간 0.027초

그래핀의 합성과 열전도 및 표면 특성 개선 활용 (Synthesis of graphene and its application to thermal and surface modification)

  • 김용유;장희진;최병상
    • 한국전자통신학회논문지
    • /
    • 제8권4호
    • /
    • pp.549-554
    • /
    • 2013
  • CVD를 이용하여 Cu 시편에 그래핀의 합성을 보이고, Cu 시편의 grain 크기와 방향성에 따른 그래핀의 성장거동을 보이고자 한다. 동일한 온도 및 압력 하에서도 사용하는 분위기 가스의 종류에 따라서 Cu의 확산에 영향을 주게 되고, 그래핀 합성 시 사용되는 $H_2$$CH_4$ 가스 분위기 하에서 Cu grain의 성장에도 영향을 미치는 것을 알 수 있었으며, 결과적으로 Cu grain의 성장이 그래핀의 합성과 성장에 직접적인 관련이 있음을 보이고자 하였다. 부식 저항성은 상온에서 동전위 분극실험를 통하여 분석하였으며, 부식속도 비교에서 그래핀 코팅된 Cu 시편의 경우가 그래핀의 화학적 안정성에 기인하여 순수 Cu 시편의 경우보다 동일한 부식 환경에서 약 10배 정도 안정적인 것으로 관찰이 되었다. 또한, grain boundary를 포함, 결함이 없는 그래핀의 균일한 성장의 가능성을 보이고, 이의 합성을 통한 공학적인 활용이 그 최종적인 목적이 될 것이다.

환경하중에 의한 연속철근콘크리트(CRCP) 종방향 철근의 구속정도 (Degree of Restraint(DOR) of Longitudinal Steel at Continuously Reinforced Concrete Pavement(CRCP) Against Environmental Loadings)

  • 남정희;안상혁
    • 한국도로학회논문집
    • /
    • 제16권6호
    • /
    • pp.95-104
    • /
    • 2014
  • PURPOSES : The purpose of this study is to evaluate the degree of restraint (DOR) of longitudinal steel at continuously reinforced concrete pavement (CRCP) against environmental loadings. METHODS : To measure the longitudinal steel strain, 3-electrical resistance and self-temperature compensation gauges were installed to CRCP test section (thickness = 250mm, steel ratio = 0.7%) and continuously measured 10 min. intervals during 259 days. In order to properly analyze the steel strains first, temperature compensation process has been conducted. Secondly, measured steel strains were divided into 12 phases with different events such as before paving, during concrete hardening, and after first cracking, etc. RESULTS : Thermal strain rate (TSR) concept is defined as the linear strain variations with temperature changes and restraints rate of longitudinal steel against environmental loadings (especially thermal loading) with different cases is defined as degree of restraint(DOR). New concept of DOR could be indirect indicator of crack width behaviors of CRCP. CONCLUSIONS : Before paving, DOR of longitudinal steel is almost same at the coefficient of thermal expansion of steel ($12.44m/m/^{\circ}C$) because of no restraint boundary condition. After concrete pouring, DOR is gradually changed into -1 due to concrete stiffness developing with hydration. After first cracking at crack induced area, values of DOR are around -3~-5. The negative DOR stands for the crack width behavior instead of steel strain behavior. During winter season, DOR reached to -5.77 as the highest, but spring this values gradually reduced as -1.7 as the lowest. Based on this observation, we can presume crack width decreased over time within the time frame of this study. This finding is not consistent with the current theory on crack width variations over time, so further study is necessary to identify the causes of crack width reducing. One of the reasons could be related to concrete stress re-distribution and stress relaxation.

화력발전소용 슈퍼 듀플렉스 스테인리스 강(STS 329J4L) 조관 튜브 및 핀-튜브재의 부식거동 (Corrosion Behavior of Super Duplex Stainless Steel (STS 329J4L) Tubes and Fin-Tubes Used in Thermal Power Plant Applications)

  • 박진성;김용현;홍승갑;김성진
    • Corrosion Science and Technology
    • /
    • 제22권6호
    • /
    • pp.435-446
    • /
    • 2023
  • Corrosion behaviors of laser-welded super duplex stainless steel (SDSS) tubes after exposure to an actual power plant environment for one year and those of fin-tube welded SDSS were evaluated. Results showed that corrosion damage on the back side of the SDSS tube in the direction of hot air was higher than that on the front side regardless of weldment location. However, corrosion damage showed no difference between weldment and base metal due to recovery of phase fraction in the weldment through post weld heat treatment (PWHT). Nevertheless, the SDSS tube showed severe corrosion damage along grain boundary due to surface phase transformation (δ → γ) and Cr2N precipitation caused by PWHT with a high N2 atmosphere. Corrosion resistance of the SDSS tube was recovered when degraded surface was removed. Corrosion sensitivity of a fin-tube increased significantly due to pre-existing crevice, unbalanced phase fraction, and σ phase precipitation adjacent to the fusion line. Although corrosion resistance was improved by recovered phase fraction and sufficient dissolution of σ phase during PWHT, corrosion reaction was concentrated at the pre-existing crevice. These results suggest that welding conditions for fin-tube steel should be optimized to improve corrosion resistance by removing pre-existing crevice in the weldment.

마그네시아 부분안정화 지르코니아 소결체의 특성에 미치는 열처리 효과 (Effects of Aging on Properties of MgO-Partially Stabilized Zirconia)

  • 정형진;오영제;이홍림
    • 한국세라믹학회지
    • /
    • 제24권3호
    • /
    • pp.243-250
    • /
    • 1987
  • 9mol% 의 MgO로 $1650^{\circ}C$에서 4시간 고상반응과 동시에 소결시킨 부분안정화 지르코니아 소결체(9MZ-PSZ)를 소성후 냉각중 $1200^{\circ}C$~$1400^{\circ}C$의 온도범위에서 열처리하여 이의 열분해 반응, 열충격기등 및 기전력 특성에 대하여 조사하였다. 열충격시럼 전과 후의 강도, 열팽창률, X-선 회절분석에 의한 단사정사 함률과 상전이, 밀도 및 갈바닉 전위를 측정하였으며 SEm에 의한 미세구조를 관찰하였다. 입체부근의 미소화학분석은 $1350^{\circ}C$ 열처리 시편에 한하여 EDX 로 정량하였다. 9MZ-PSZ 시편의 열처리에 의하여 입방정상의 $ZrO^{2}$는 상기 온도범위에서는 준안정-정방정상의 $ZrO^{2}$와 MgO로 열분해되는데, 이때 생성된 준안정 정방정상은 열충격 시험후의 잔류강도를 응력유기상전이 효과에 의해 증가시킨다. 또한 MgO는 입계에 연속적으로 존재하는데 이런하 MgO의 연속상을 통한 열전도롤 인하여 PSZ의 열충격 저항이 크게 향상된다. 이때 PSZ의 열분해 속도와 단사정상 함량은 열처리 온도가 $1400^{\circ}C$에서 $1200^{\circ}C$로 감소됨에 따라 증가한다. 갈바닉전의 측정결과 이상의 열처리에 의하여도 양호한 기전력 특성을 갖는 지르코니아 고체전해질을 제조할 수 있다.

  • PDF

유전함수를 이용한 ZnO-Bi2O3-Mn3O4 바리스터의 a.c. 특성 분석 (Analysis of a.c. Characteristics in ZnO-Bi2O3-Mn3O4 Varistor Using Dielectric Functions)

  • 홍연우;신효순;여동훈;김진호
    • 한국전기전자재료학회논문지
    • /
    • 제23권12호
    • /
    • pp.936-941
    • /
    • 2010
  • In this study, we have investigated the effects of Mn dopant on the bulk trap levels and grain boundary characteristics of $Bi_2O_3$-based ZnO (ZB) varistor using admittance spectroscopy and dielectric functions (such as $Z^*,\;Y^*,\;M^*,\;\varepsilon^*$, and $tan\delta$). Admittance spectra and dielectric functions show two bulk traps of $Zn_i^{..}$ (0.20 eV) and $V^{\bullet}_o$ (0.29~0.33 eV) in ZnO-$Bi_2O_3-Mn_3O_4$ (ZBM). The barrier of grain boundaries in ZBM could be electrochemically single type. However, its thermal stability was slightly disturbed by ambient oxygen because the apparent activation energy of grain boundaries was changed from 0.79 eV at lower temperature to 1.08 eV at higher temperature. The grain boundary capacitance $C_{gb}$ was decreased slightly with temperature as 1.3~1.8 nF but resistance $R_{gb}$ decreased exponentially. The relaxation time distribution can result from the heterogeneity of the barriers constituting the varistor. It is revealed that Mn dopant in ZB reduced the heterogeneity of the barrier in grain boundaries and stabilized the barrier against the ambient temperature.

줄 가열 변화에 따른 박막 트랜지스터 내 포논 열 흐름에 대한 수치적 연구 (Effect of Joule Heating Variation on Phonon Heat Flow in Thin Film Transistor)

  • 진재식;이준식
    • 대한기계학회논문집B
    • /
    • 제33권10호
    • /
    • pp.820-826
    • /
    • 2009
  • The anisotropic phonon conductions with varying Joule heating rate of the silicon film in Silicon-on-Insulator devices are examined using the electron-phonon interaction model. It is found that the phonon heat transfer rate at each boundary of Si-layer has a strong dependence on the heating power rate. And the phonon flow decreases when the temperature gradient has a sharp change within extremely short length scales such as phonon mean free path. Thus the heat generated in the hot spot region is removed primarily by heat conduction through Si-layer at the higher Joule heating level and the phonon nonlocality is mainly attributed to lower group velocity phonons as remarkably dissimilar to the case of electrons in laser heated plasmas. To validate these observations the modified phonon nonlocal model considering complete phonon dispersion relations is introduced as a correct form of the conventional theory. We also reveal that the relation between the phonon heat deposition time from the hot spot region and the relaxation time in Si-layer can be used to estimate the intrinsic thermal resistance in the parallel heat flow direction as Joule heating level varies.

중온형 고체산화물 연료전지를 위한 YSZ 전해질에서의 고성능 공기극 연구 (Study on high performance cathode on YSZ electrolyte for intermediate-temperature solid oxide fuel cells(IT-SOFC))

  • 이창보;배중면
    • 한국신재생에너지학회:학술대회논문집
    • /
    • 한국신재생에너지학회 2006년도 추계학술대회
    • /
    • pp.368-371
    • /
    • 2006
  • [ $La_{0.8}Sr_{0.2}Co_{1-x}Mn_xO_3$ ] cathode as a high performance cathode on YSZ electrolyte was studied by analyzing impedance spectra. It was shown that cathode property of $La_{0.8}Sr_{0.2}Co_{1-x}Mn_xO_3$ is bet ter than that of$La_{0.8}Sr_{0.2}CoO_3$. At $700^{\circ}C$ in air environment, $La_{0.8}Sr_{0.2}Co_{0.4}Mn_{0.6}O_3$ cathode on CGO- layered YSZ electrolyte showed very low area specific resistance of $0.14{\Omega}cm^2$, which is low enough for intermediate-temperature sol id oxide fuel cells. This is because material properties of ionic conductivity and thermal expansion compatibility with electrolyte were optimized. Judging from activation energy and oxygen part i al pressure dependance of cathode property, it was noted that oxygen surface exchange kinetics is dominantly influential on cathode property in higher temperature region than $700^{\circ}C$ and oxygen self-diffusion in cathode material is more influential in lower temperature region.

  • PDF

고온 수전해 전해질 막의 제막조건에 따른 미세구조 분석 (Microstructure Analysis with Preparation Condition of Electrolyte Membrane for High Temperature Electrolysis)

  • 최호상;손효석;황갑진;배기광
    • 한국수소및신에너지학회논문집
    • /
    • 제17권2호
    • /
    • pp.141-148
    • /
    • 2006
  • This study was carried out to analyze the microstructure characteristics of electrolyte membrane through XRD, SEM and AC impedance measurement for using in high temperature steam electrolysis(HTE). It was investigated that thermal stability and electric characteristics by sintering condition using dry and wet process, and confirmed growth of particle and density change by sintering temperature. The sintering temperature and behavior had an effect on the relative density of the ceramic and the average grain size. The more amount of dispersant in organic compound increase, the more the density increased. But the binder was shown opposite phenomenon. It was analyzed that electrolyte resistance and electrical characteristics using AC impedance. The electrical properties of YSZ grain boundary changed with the sintering temperature.

Effects of Nb Content and Thermal History on the Mechanical and Corrosion Characteristics of Stainless Steels

  • Choe, Han-Cheol;Kim, Kwan-Hyu
    • Corrosion Science and Technology
    • /
    • 제2권3호
    • /
    • pp.117-126
    • /
    • 2003
  • Due to excellent corrosion resistance and mechanical properties, austenitic stainless steel is widely used as the material for chemical plants. nuclear power plants, and food processing facilities. But, the zone affected by heat in the range of 400 to $800^{\circ}C$ during welding loses corrosion resistance and tensile strength since Cr-carbide precipitation like $Cr_{23}C_6$ forms at the grain boundary and thereby takes place the intergranular corrosion. In this study, AISI 304 stainless steel with the added Nb of 0.3 to 0.7 wt% was solutionized at $1050^{\circ}C$ and sensitized at $650^{\circ}C$. Specimen was welded by MIG. The phase and the microstructure of the specimens were examined by an optical microscope, a scanning electron microscope, and a x-ray diffractometer. The corrosion characteristics of specimens were tested by electrolytic etching and by double loop electrochemical potentiokinetic reactivation method(EPR) in the mixed solution of 0.5M $H_2SO_4$ + 0.01M KSCN. The melting zone had dendritic structure constituted of austenitic phase and $\delta$-ferrite phase. Cr carbide at the matrix did not appear, as Nb content increased. At the grain boundaries of the heat affected zone, the precipitates decreased and the twins appeared. The hardness increased, as Nb content increased. The hardness was highest in the order of the heat affected zone>melted zone>matrix. According to EPR curve, as the Nb content decreased, the reactivation current density(Ir) and the activation current density(la) were highest in the order of the melted zone

A FLOW AND PRESSURE DISTRIBUTION OF APR+ REACTOR UNDER THE 4-PUMP RUNNING CONDITIONS WITH A BALANCED FLOW RATE

  • Euh, D.J.;Kim, K.H.;Youn, Y.J.;Bae, J.H.;Chu, I.C.;Kim, J.T.;Kang, H.S.;Choi, H.S.;Lee, S.T.;Kwon, T.S.
    • Nuclear Engineering and Technology
    • /
    • 제44권7호
    • /
    • pp.735-744
    • /
    • 2012
  • In order to quantify the flow distribution characteristics of APR+ reactor, a test was performed on a test facility, ACOP ($\underline{A}$PR+ $\underline{C}$ore Flow & $\underline{P}$ressure Test Facility), having a length scale of 1/5 referring to the prototype plant. The major parameters are core inlet flow and outlet pressure distribution and sectional pressure drops along the major flow path inside reactor vessel. To preserve the flow characteristics of prototype plant, the test facility was designed based on a preservation of major flow path geometry. An Euler number is considered as primary dimensionless parameter, which is conserved with a 1/40.9 of Reynolds number scaling ratio. ACOP simplifies each fuel assembly into a hydraulic simulator having the same axial flow resistance and lateral cross flow characteristics. In order to supply boundary condition to estimate thermal margins of the reactor, the distribution of inlet core flow and core exit pressure were measured in each of 257 fuel assembly simulators. In total, 584 points of static pressure and differential pressures were measured with a limited number of differential pressure transmitters by developing a sequential operation system of valves. In the current study, reactor flow characteristics under the balanced four-cold leg flow conditions at each of the cold legs were quantified, which is a part of the test matrix composing the APR+ flow distribution test program. The final identification of the reactor flow distribution was obtained by ensemble averaging 15 independent test data. The details of the design of the test facility, experiment, and data analysis are included in the current paper.