• 한국표면공학회:학술대회논문집
• /
• 한국표면공학회 2001년도 추계학술발표회 초록집
• /
• pp.29-30
• /
• 2001

This paper presents some results of plasma nitriding on hard chromium deposit. The substrates were C45 steel and $30~50{\;}\mu\textrm{m}$ of chromium deposit by electroplating was formed. Plasma nitriding was carried out in a plasma nitriding system with $95NH_3{\;}+{\;}SCH_4$ atmosphere at the pressure about 600 Pa and different temperature from $450^{\circ}C{\;}to{\;}720^{\circ}C$ for various time. Optical microscopy and X-ray diffraction were used to evaluate the characteristics of surface nitride layer formed by nitrogen diffusion from plasma atmosphere inward iCr coating and interface carbide layer formed by carbon diffusion from substrate outward Cr coating. The microhardness was measured using microhareness tester at the load of 100 gf. Corrosion resistance was evaluated using the potentiodynamic measurement in 3.5% NaG solution. A saturated calomel electrode (SiCE) was used as the reference electrode. Fig.1 shows the typical microstructures of top surface and cross-section for nitrided and unnitrided samples. Aaer plasma nitriding a sandwich structure was formed consisting of surface nitride layer, center chromium layer and interface carbide layer. The thickness of nitride and carbide layers was increased with the increase of processing temperature and time. Hardness reached about 1000Hv after nitriding while 900Hv for unnitrided hard chromium deposit. X-ray diffraction indicated that surface nitrided layer was a mixture of $Cr_2N$ and CrN at low temperature and erN at high temperature (Fig.2). Anodic polarization curves showed that plasma nitriding can greatly improve the corrosion resistance of chromium e1ectrodeposit. After plasma nitriding, the corrosion potential moved to noble direction and passive current density was lower by 1 to 4 orders of magnitude compared with chromium deposit(Fig.3).

• Bulletin of the Korean Chemical Society
• /
• 제26권4호
• /
• pp.634-640
• /
• 2005

The reaction of cis-[Cr([14]-decane)(OH$_2)_2]^+$ ([14]-decane = rac-5,5,7,12,12,14-hexamethyl-1,4,8,11-teraazacyclotetradecane) with auxiliary ligands {$L_a$ = citrate(cit)} leads to a new dimeric complex cis-[{Cr([14]-decane)($\mu$-cit)}$_2](ClO_4)_2$. This binuclear complex has been structurally characterized by a combination of elemental analysis, conductivity, IR and Vis spectroscopy, mass spectrometry, and X-ray crystallography. Analysis of the crystal structure of cis-[{Cr([14]-decane)($\mu$-cit)})($_2]^+$ reveals that each chromium has a distorted octahedral coordination environment and citrato ligands are monodentate to the two chromium atoms via the carboxyl groups. For dimeric complex the bridging geometry is as follows: Cr$\ldots$Cr = 7.361 $\AA$; Cr-O(average) = 1.958 (8) $\AA$; Cr-N range = 2.108 (9)-2.147(9) $\AA$; N(1)-Cr-N(3) (equatorial position) = 98.0(4)$^{\circ}$; N(2)-Cr-N(4) (axial position) = 166.4(4)$^{\circ}$; O(1)-Cr-N(2) = 98.1(4)$^{\circ}$; O(3)-Cr-N(4) = 96.6(3)$^{\circ}$; O(1)-Cr-O(3) = 90.4$^{\circ}$. The FAB mass spectrum of the dimeric complex displays peak due to the molecular ions cis-[{Cr([14]-decane)($\mu$-cit)})($_2]^+$ at m/z 1053.

• 한국결정성장학회지
• /
• 제23권3호
• /
• pp.135-141
• /
• 2013

본 연구에서는 $CrSi_2$ 열전화합물을 제조하기 위하여 순금속 $Cr_{33}Si_{67}$ 혼합분말을 기계적 합금화 처리하였다. 초미세 $CrSi_2$계 열전화합물을 얻기 위하여 최적 볼밀조건 및 열처리 조건을 X선 회절분석과 시차주사 열량분석을 이용하여 조사하였다. 순금속 $Cr_{33}Si_{67}$ 혼합분말을 70시간까지 볼밀 처리 후 $650^{\circ}C$까지 열처리함으로써 평균 결정립 크기가 70 nm 인 초미세 $CrSi_2$ 열전화합물을 얻을 수 있었다. MA 분말시료의 벌크화를 위하여 소결온도 $600{\sim}1000^{\circ}C$, 압력 60 MPa에서 SPS 소결을 실시하였다. SPS 과정에서 MA 분말의 수축은 소결 개시 후 $600^{\circ}C$ 전후에서 크나 전반적으로 급격하게 발생하지 않으며 $1000^{\circ}C$까지 비교적 단조롭게 수축함을 알 수 있었다. 여기서 수축이 $600^{\circ}C$ 부근에서 큰 이유는 열분석 결과에서도 보여주듯이 $CrSi_2$ 화합물의 생성과 관련이 있는 것으로 판단된다. SPS 성형체의 전기전도도 및 제벡계수는 $900^{\circ}C$까지 측정을 실시하였으며, 그 결과로부터 제벡계수는 $400^{\circ}C$에서 $125{\mu}V/K$ 및 파워팩터는 $350^{\circ}C$에서 $4.3{\times}10^{-4}W/mK^2$의 최대값을 각각 나타내었다.

• E2M - 전기 전자와 첨단 소재
• /
• 제9권9호
• /
• pp.900-905
• /
• 1996

We have investigated dielectric properties of low fired ceramics BiNbO$_{4}$ containing 0.05[wt%] V$_{2}$O$_{5}$ and x[wt%l Cr$_{2}$O$_{3}$ (x=0, 0.2, 0.4, 0.8, 1.2). By substituting Cr for Bi, dielectric constant .epsilon.$_{r}$ and quality factor Q.f increased and temperature coefficient of resonant frecquency .tau.$_{f}$ changed to positive value. In the composition of BiNbO$_{4}$+0.05 [Wt%] V$_{2}$O$_{5}$+0.8[wt%]Cr$_{2}$O$_{3}$ sintered at 960[.deg. C], we could obtain microwave dielectric properties of .epsilon.$_{r}$=49, Q.f.simeq.3000[GHz](at 4.8[GHz]), .tau.$_{f}$.simeq.0[ppm/.deg. C]. As the above ceramics can be sintered near 960[.deg. C], it is applicable to multilayer microwave device with Ag conductor.tor.tor.tor.

• 천문학회보
• /
• 제43권1호
• /
• pp.35.1-35.1
• /
• 2018

Shock waves have been observed in the outskirts of galaxy clusters. They are commonly interpreted as being driven by mergers of sub-clumps, so are called "merger shocks". We here report a study of the properties of merger shocks in merging galaxy clusters with cosmological hydrodynamic simulations. As a representative case, we describe the case where sub-clusters with mass ratio ~ 2 go through an almost head-on, binary-like merger. Because of the turbulent nature of hierarchical clustering, shock surfaces are not uniform, but composed of parts with different Mach numbers. As merger shocks expand from the core to the outskirts, the average Mach number, < $M_s$ >, increases. The shocks propagating along the merger axis could be observed as X-ray shocks and/or radio relics. The kinetic energy through the shocks peaks at ~ 1 Gyr after shock launching, or at ~ 1 - 2 Mpc from the core. The most energetic shocks are found to have the kinetic-energy weighted Mach number, < $M_s$ > $_{\phi}{\simeq}2-3$, and the CR-energy weighted Mach number, < $M_s$ > $_{CR}{\simeq}3-4$. We then discuss the observational implications of our results.

• 대한금속재료학회지
• /
• 제48권7호
• /
• pp.589-597
• /
• 2010

In the present study, the effect of variation in alloying elements on the carbide formation behavior during casting and homogenization treatment of M2 high speed steels was investigated. M2 high speed steels of various compositions were produced by vacuum induction melting. Contents of C, Cr, W, Mo, and V were varied from the basic composition of 0.8C, 0.3Si, 0.2Mn, 4.0Cr, 6.0W, 5.0Mo, and 2.0V in weight percent. Homogenization treatment at $1150^{\circ}C$ for 1.5 hr followed by furnace cooling was performed on the ingots. Area fraction and chemical compositions of eutectic carbide in as-cast and homogenized ingots were analyzed. Area fraction of eutectic carbide appeared to be higher in the ingots with higher contents of alloying elements the area fraction of eutectic carbide also appeared to be higher on the surface regions than in the center regions of ingots. As a result of the homogenization treatment, $M_2C$ carbide, which was the primary eutectic carbide in the as-cast ingots, decomposed into thermodynamically stable carbides, MC and $M_6C$. The latter carbide was found to be the main one after homogenization. Fine carbides uniformly distributed in the matrix was found to be MC type carbide and coarsened by homogenization.

• 대한화학회지
• /
• 제56권4호
• /
• pp.448-458
• /
• 2012

In order to develop alloy resistance in aggressive sulphat ion, the corrosion behavior of metallic glasses $Ni_{92{\cdot}3}Si_{4.5}B_{32}$, $Ni_{82,3}Cr_7Fe_3Si_{4.5}B_{3.2}$ and $Ni_{75.5}Cr_{13}Fe_{4.2}Si_{4.5}B_{2.8}$ (at %) at different concentrations of $H_2SO_4$ solutions was examined by electrochemical methods and Scanning Electron Microscope (SEM) and X-ray Photoelectron Microscopy (XPS) analyses. The corrosion kinetics and passivation behavior was studied. A direct proportion was observed between the corrosion rate and acid concentration in the case of $Ni_{92{\cdot}3}Si_{4.5}B_{32}$ and $Ni_{75.5}Cr_{13}Fe_{4.2}Si_{4.5}B_{2.8}$ alloys. Critical concentration was observed in the case of $Ni_{82,3}Cr_7Fe_3Si_{4.5}B_{3.2}$ alloy. The influence of the alloying element is reflected in the increasing resistance of the protective film. XPS analysis confirms that the protection film on the $Ni_{92{\cdot}3}Si_{4.5}B_{32}$ alloy was NiS which is less protective than that formed on Cr containing alloys. The corrosion rate of $Ni_{82,3}Cr_7Fe_3Si_{4.5}B_{3.2}$ and $Ni_{75.5}Cr_{13}Fe_{4.2}Si_{4.5}B_{2.8}$. alloys containing 7% and 13% Cr are $7.90-26.1{\times}10^{-3}$ mm/y which is lower about 43-54 times of the alloy $Ni_{92{\cdot}3}Si_{4.5}B_{32}$ (free of Cr). The high resistance of $Ni_{75.5}Cr_{13}Fe_{4.2}Si_{4.5}B_{2.8}$ alloy at the very aggressive media may due to thicker passive film of $Cr_2O_3$ which hydrated to hydrated chromium oxyhydroxide.

• 한국재료학회지
• /
• 제14권1호
• /
• pp.52-58
• /
• 2004

The surface property and formation behavior of a boride layer formed on Ni-Cr-Mo steel in a plasma paste boronizing treatment were investigated. The plasma paste boronizing treatment was carried out at 973～1273 K for 1-7 hrs under the gas ratio of Ar:H$_2$ (2:1). The thickness of the boride layer increased with increasing temperature and time in the boronizing treatment. The cross-section of the boride layer was a tooth structure and the hardness was Hv 2000～2500. XRD analysis revealed that the compound was identified as FeB, $Fe_2$B, and mixed phase of FeB/$Fe_2$B in the boride layer formed at 973～1073 K, 1173K, and 1273K, respectively. The Ni-Cr-Mo alloy boronized at 1173-1273 K showed the best excellent wear resistance against the sand. As a results of corrosion test in 1 M $H_2$$SO_4$ solution, $Fe_2$B formed on the matrix alloy exhibited higher corrosion resistance than FeB.

• 한국전기전자재료학회:학술대회논문집
• /
• 한국전기전자재료학회 2004년도 하계학술대회 논문집 Vol.5 No.2
• /
• pp.898-901
• /
• 2004

[ $ZnCr_2O_4$ ]를 모물질로 하고 MgO, $TiO_2$를 몰비로 2:1, 4:1, 6:1, 및 8:1이 되게 정량적으로 조합한 후, 조사하였다. $ZnCr_2O_4$-MgO와 $ZnCr_2O_4-TiO_2$를 X-선 분석한 결과 Spinel 결정구조를 형성하였으며, 또한 SEM과 EDX 분석결과 각각 $Li_2CrO_4$와 $Li_3VO_4$의 형성으로 인하여 저항 특성이 나타나는 것을 알 수 있었다. $ZnCr_2O_4-MgO$, $ZnCr_2O_4-TiO_2$에서 MgO의 양이 증가할수록 저항값은 약간 감소하는 반면, $TiO_2$의 양이 증가할수록 저항값이 급격히 증가하는 특성을 나타내었고, 감습 특성에서도 M??보다 TiO2가 더 높게 나타내었다. 습에 따른 복원 특성의 경우 $700^{\circ}C$에서 소결한 ($ZnCr_2O_4:MgO=4:1$)과 ($ZnCr_2O_4:TiO_2=6:1$) 조성의 센서가 가장 양호하였다.

• 공업화학
• /
• 제17권5호
• /
• pp.451-457
• /
• 2006

$CrCl_{3}$를 $NH_{3}$와 반응시켜 약 $850^{\circ}C$에서 표면적이 높은 단일 상 CrN 촉매를 합성하였다. 열질량분석을 통해 고체상 화학변이가 발생하는 온도를 파악하였고 물질의 상을 XRD로 분석하였다. 합성물질의 표면적, 결정크기 등을 분석하였고 합성변수의 영향을 확인하였다. 합성된 질화물의 표면적은 $12{\sim}47m^2/g$이었다. 공간속도는 표면적 증가에 약하게나마 영향을 미쳤는데 반응중간생성물의 빠른 제거가 표면적을 높이는데 기여하는 것으로 파악되었다. 승온환원반응 분석 결과 CrN은 비활성화(passivation)시 거의 산화되지 않아 수소분위기에서의 환원이 거의 일어나지 않았으며 약 $700^{\circ}C$와 $950^{\circ}C$ 부근에서 결정격자 중의 질소가 $N_{2}$로 분해되었다. 공기분위기에서 10 K/min의 속도로 가열하면 $300^{\circ}C$ 이후의 온도에서 산화가 진행되어 $800^{\circ}C$ 부근에서 $Cr_{2}O_{3}$ 상이 형성되기 시작하였으며 $900^{\circ}C$에서도 완전히 산화되지 않았다. 부탄과 피리딘을 이용한 활성실험 결과 CrN 촉매는 탈수소반응에 선택적으로 높은 활성을 가졌으며 수첨탈질이나 수소분해반응 활성은 거의 없었다. 부탄의 탈수소반응에서 부피반응속도는 상용 촉매인 $Pt-Sn/Al_{2}O_{3}$보다 우수하였다.