• 제목/요약/키워드: 3 phase

검색결과 21,012건 처리시간 0.05초

Pb(Mg1/3Nb2/3)O3-based 강유전체의 상전이 및 완화특성 (Phase Transition and Relaxor Behaviors in the Lead Magnesium Niobate-based Ferroelectrics)

  • 김연중;이주호
    • 한국진공학회지
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    • 제17권2호
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    • pp.148-155
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    • 2008
  • PMN계 강유전체의 MPB 조성과 공존영역의 확산성을 이해하기 위해 유전 및 초전 특성을 분석하였다. PMN-PT계는 완만한 상전이를 보였으며, 이는 하나의 상유전과 2개의 강유전상이 공존함을 의미한다. 즉, 0.7PMN-0.3PT 조성 부근에서 능면정계와 정방정계의 공존 영역인 조성변태 상경계를 확인하였으며, 이들 조성은 연속적으로 능면정계$\rightarrow$정방정계$\rightarrow$입방정계로 상전이를 하였다. PT>0.325인 조성들은 측정된 진동수 범위에서 진동수 의존성을 보이지 않는 단일상의 강유전 특성을 보였으며, PMN>0.7인 조성들은 큰 진동수 의존성과 확산상전이의 전형적인 완화형 강유전 특성을 보였다. PMN-PT계의 조성변태 상경계 조성들은 우수한 유전 및 초전특성을 나타내었다.

Structural, Magnetic, and Optical Studies on Normal to Inverse Spinel Phase Transition in FexCo3-xO4 Thin Films

  • Kim, Kwang-Joo;Kim, Hee-Kyung;Park, Young-Ran;Ahn, Geun-Young;Kim, Chul-Sung;Park, Jae-Yun
    • 한국자기학회지
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    • 제15권2호
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    • pp.96-99
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    • 2005
  • Phase transition from normal- to inverse-spinel structure has been observed for $Fe_xCo_{3-x}O_4$ thin films as the Fe composition (x) increases from 0 to 2. The samples were fabricated as thin films by sol-gel method on Si(100) substrates. X-ray diffraction measurements revealed a coexistence of two phases, normal and inverse spinel, for $0.76{\le}x{\le}0.93$. The normal-spinel phase is dominant for $x{\le}0.55$ while the inverse-spinel phase for $x{\ge}l.22$. The cubic lattice constant of the inverse-spinel phase is larger than that of the normal-spinel phase. For both phases the lattice constant increases with increasing x. X-ray photoelectron spectroscopy measurements revealed that both $Fe^{2+}$ and $Fe^{3+}$ ions exist with similar strength in the x=0.93 sample. Conversion electron $M\ddot{o}ssbauer$ spectra measured on the same sample showed that $Fe^{2+}$ ions prefer the octahedral $Co^{3+}$ sites, indicating the formation of the inverse-spinel phase. Analysis on the measured optical absorption spectra for the samples by spectroscopic ellipsometry indicates the dominance of the normal spinel phase for low x in which $Fe^{3+}$ ions tend to substitute the octahedral sites.

3상 복합재의 등가열전도계수 예측에 대한 연구 (Analytical Study on Effective Thermal Conductivity of Three-Phase Composites)

  • 이재곤;김진곤
    • 한국산학기술학회논문지
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    • 제12권7호
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    • pp.2931-2938
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    • 2011
  • 2상 복합재에 적용되어오던 수정된 Eshelby 모델(MEM)을 두 종류의 구형 입자를 포함하는 3상 복합재로 확장하여 복합재의 등가열전도계수를 간단히 양함수 형태로 표시한다. 이의 유효성 검증을 위해 이 결과를 미소등가물모델(DEMM)로 구한 결과와 비교하고, 또 참고문헌의 2상 및 3상 복합재의 실험결과와 비교한다. 2상 복합재의 경우 MEM이 충전재의 체적비 0.5 미만에서는 DEMM보다 잘 예측한다. 3상 복합재의 경우 모재 대비 큰 열전도계수비를 갖는 충전재의 체적비가 적은 경우 MEM이 잘 예측하나, 체적비가 증가할수록 DEMM이 잘 예측한다. 이 체적비가 두 모델의 예측결과에 결정적 영향을 주는 인자임이 변수들의 영향 연구를 통해 밝혀졌으며, Molina 등이 제안한 3상 복합재에 대해 MEM과 DEMM은 동등한 예측 수준을 보였다.

DMD를 이용한 위상천이 모아레 3차원 형상 측정 (Application of DMD for Phase Shifting in Moire Topology)

  • 정경석;정용상
    • 한국산학기술학회논문지
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    • 제12권6호
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    • pp.2457-2462
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    • 2011
  • 생산방식의 변화에 따라 3차원 형상을 신속하고 정확하게 측정하는 것이 중요해졌다. 가장 훌륭한 비접촉 3차원 측정방법인 모아레 방법 중 잡음신호를 효과적으로 제거할 수 있는 위상천이 방법을 구현함에 있어 DMD를 이용하여 격자를 생성하고 이송하는 효과를 발생하도록 하였다. 컴퓨터에서 격자를 이송하고 위상천이를 발생하므로 기계적 이송으로 인한 잡음신호의 발생 가능성을 배제할 수 있으며 광학렌즈와의 적절한 조합을 통해 쉽게 분해능을 변화하며 3차원 정보 획득이 가능하다. 근본적인 $2\pi$ 모호성문제를 극복하기 위하여 2차원 위상정력을 실시하였다. 이 방법을 적용하여 3차원 형상의 측정을 수행하였다.

산화물계의 액상소결에서 입자 형상이 입자성장 거동에 미치는 영향 (The effect of grain shape on grain growth behavior of oxide system during liquid phase sintering)

  • 조동희;박상엽
    • 한국결정성장학회지
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    • 제11권3호
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    • pp.127-131
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    • 2001
  • 산화물계의 액상소결시 액상량을 변수로 하여 입자형성이 입자성장 거동에 미치는 영향을 고찰하였다. 산화물계 모델로 구형입자의 경우는 MgO$CaMgSiO_{4}$계를 선택하였으며, 각진입자의 경우는 $Al_{2}O_{3}$/ $CaAl_{2}Si_{2}O_{8}$계를 선택하였다. 구형입자인 MgO의 경우 액상량 증가에 따라 입자크기가 감소하였으나,각진입자인 $Al_{2}O_{3}$ 입자의 경우는 계면지배과정에 의해 성장하는 반면, 거친 고상/액상계면을 지닐 것으로 예상되는 구형 MgO입자의 경우는 확산지배과정에 의해 성장하였다.

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Changes in the thyroid hormone profiles in children with nephrotic syndrome

  • Jung, Sun Hee;Lee, Jeong Eun;Chung, Woo Yeong
    • Clinical and Experimental Pediatrics
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    • 제62권3호
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    • pp.85-89
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    • 2019
  • Purpose: We compared thyroid hormone profiles in children with nephrotic syndrome (NS) during the nephrotic phase and after remission. Methods: This study included 31 pediatric NS patients. The thyroid hormone profiles included serum levels of triiodothyronine (T3), thyroxine (T4), thyroid-stimulating hormone (TSH), and free T4. Results: Of the 31 patients, 16 (51.6%) showed abnormal thyroid hormone profiles: 6 had overt hypothyroidism, 8 had subclinical hypothyroidism, and 2 had low T3 syndrome. The mean serum T3, T4, and free T4 levels in the nephrotic phase and after remission were $82.37{\pm}23.64$ and $117.88{\pm}29.49ng/dL$, $5.47{\pm}1.14$ and $7.91{\pm}1.56{\mu}g/dL$, and $1.02{\pm}0.26$ and $1.38{\pm}0.23ng/dL$, respectively; the levels were significantly lower in the NS nephrotic phase (P=0.0007, P<0.0001, and P=0.0002). The mean serum TSH levels during the nephrotic phase and after remission were $8.05{\pm}3.53$ and $4.08{\pm}2.05{\mu}IU/mL$, respectively; they were significantly higher in the nephrotic phase (P=0.0005). The urinary protein/creatinine ratio during the nephrotic phase was significantly correlated with serum T3, T4, and free T4 levels (r=-0.5995, P=0.0032; r=-0.5797, P=0.0047; r=-0.5513, P=0.0078) as well as with TSH levels (r=0.5022, P=0.0172). A significant correlation was found between serum albumin and serum T3 levels during the nephrotic phase (r=0.5385, P=0.0018) but not between serum albumin and T4, TSH, or free T4 levels. These significant correlations all disappeared after remission. Conclusion: Abnormal thyroid hormone profile findings were observed in 51.6% of pediatric patients with NS. Thyroid hormone levels normalized after remission, regardless of levothyroxine therapy.

New Configuration of a PLDRO with an Interconnected Dual PLL Structure for K-Band Application

  • Jeon, Yuseok;Bang, Sungil
    • Journal of electromagnetic engineering and science
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    • 제17권3호
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    • pp.138-146
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    • 2017
  • A phase-locked dielectric resonator oscillator (PLDRO) is an essential component of millimeter-wave communication, in which phase noise is critical for satisfactory performance. The general structure of a PLDRO typically includes a dual loop of digital phase-locked loop (PLL) and analog PLL. A dual-loop PLDRO structure is generally used. The digital PLL generates an internal voltage controlled crystal oscillator (VCXO) frequency locked to an external reference frequency, and the analog PLL loop generates a DRO frequency locked to an internal VCXO frequency. A dual loop is used to ease the phase-locked frequency by using an internal VCXO. However, some of the output frequencies in each PLL structure worsen the phase noise because of the N divider ratio increase in the digital phase-locked loop integrated circuit. This study examines the design aspects of an interconnected PLL structure. In the proposed structure, the voltage tuning; which uses a varactor diode for the phase tracking of VCXO to match with the external reference) port of the VCXO in the digital PLL is controlled by one output port of the frequency divider in the analog PLL. We compare the proposed scheme with a typical PLDRO in terms of phase noise to show that the proposed structure has no performance degradation.

複合組織鋼의 第2相 硬度變化가 腐蝕疲勞 크랙傳播에 미치는 影響 (The Influence on the Corrosion Fatigue Crack Propagation in Changing of the Second Phase Hardness of Dual Phase Steel)

  • 오세욱;김웅집
    • Journal of Welding and Joining
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    • 제11권2호
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    • pp.42-52
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    • 1993
  • The corrosion fatigue fracture behaviour of dual phase steel was investigated in 3% NaCl solution at 302MPa and 137MPa. Fatigue test was conducted by cantilever type of self-made rotary bending fatigue testing machine. The fatigue strength increased with increasing the hardness of 2nd phase. Corrosion pit originated at the boundary of the 2nd phase. The size and number of corrosion pits were influenced by the 2nd phase hardness, and pits remained constant in size just after they were transited into cracks. The life of crack initiation was effected by stress level. The shape of relation of .DELTA. K and da/dN has smaller scattering in it in 3% NaCl solution than that in air. The higher the 2nd phase hardness is, the greater the corrosion fatigue life becomes. Corrosion fatigue fracture behaviour was primarily effected by mechanical factor in case of high stress(302MPa), but by electro-chemical reaction in a lower stress(137MPa). As stress level got lower and hardness of the 2nd phase got higher, the roughness of fracture surface increased.

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수핵란 세포질의 세포주기 조절에 의한 소 체외수정란의 핵이식 (Nuclear Transplantation of Bovine IVF Embryos by Cell Cycle Control of Recipient Cytoplasm)

  • 정희태;임석기;박춘근;양부근;김정익
    • 한국가축번식학회지
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    • 제20권3호
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    • pp.307-313
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    • 1996
  • This study was conducted to investigate the effect of S-phase synthronized nuclear transfer on the development of nuclear transplant bovine embryos. A blastomere derived from the 16~32 cell stage bovine embryos was transferred into an enucleated metaphase II(MII) oocytes or activated S-phase eggs. From the MII-phase and S-phase nuclear transfer, 6.3%(4/63) and 13.8%(9/65) of nuclear transplant embryos developed to the blastocyst stage, respectively. In the S-phase nuclear transfer, maximal proportion of embryos developed to the blastocyst stage(16.6%) was obtained after the recipient cell was activated 8 h prior to receving a donor nucleus. MII-phase nuclear transplant embryos showed the PCC state of their nuclear at 1.5~2 h after fusion, whereas, S-phase nuclear transplant embryos did not undergo PCC. The result of this study suggests that if blastomeres of unknown cell-cycle-stage are used, S-phase nuclear transplantation through the activation of enucleated oocytes prior to fusion enhances development of nuclear transplant embryos. This result also suggests that the interval time from oocyte activation to cell fusion may affect the development of nuclear transplant embryos.

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Molecular Dynamics Study on the Structural Phase Transition of Crystalline Silver Iodide

  • Jun Sik Lee;Mee Kyung Song;Mu Shik Jhon
    • Bulletin of the Korean Chemical Society
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    • 제12권5호
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    • pp.490-494
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    • 1991
  • The ${\beta} to {\alpha}$ phase transition in silver iodide is studied with the (N, V, E) and (N, P, T) molecular dynamics (MD) method. In experiments, the phase transition temperature is 420 K. Upon heating of ${\beta}$ form, the iodine ions undergo hcp to bcc transformation and silver ions become mobile. MD simulations for the ${\beta}$ and ${\alpha}$ phases are carried out at several temperatures and the radial distribution functions (rdf) are obtained at those temperatures in the (N, V, E) ensemble. But the phase transition is not found in our calculation. Next the phase transition is studied with the (N, P, T) MD and we find some evidences of phase transition. At 3 Kbars and 2 Kbars the phase transition temperatu re is about 300 K. For 3.55 Kbars, the phase transition is higher (420 K) than the low pressure case. The phase transition temperature is somewhat dependent on the pressure in our calculations.