• Title/Summary/Keyword: 소결 온도

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Kinetic Study Of $La_2$O_3-A1_2O_3-SiO_2$ glass infiltration into Spinel Preforms (스피넬 전성형체의 $La_2$O_3-A1_2O_3-SiO_2$계 유리 침투 kinetic)

  • 이득용;장주웅;김병수;김대준;송요승
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.12 no.1
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    • pp.31-35
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    • 2002
  • Abstract Spinel powder having a particle size of 0.9$\mu$m was calcined for 30 min at $1300^{\circ}C$, followed by ball milling for 4h, to obtain the spinel particle size of 3.29$\mu$m. The die-pressed spinel was presintered at $1100^{\circ}C$ for 2h and then lanthanum aluminosilicate glass was infiltrated at $1080^{\circ}C$ for 0~2 h to investigate the penetration kinetics in glass-spinel composite. The infiltration distance is parabolic in time due to capillarity. The strength and the fracture toughness of glassspinel composites were 317 MPa and 3.56 MPa $m^{1/2}$ respectively and dual microstructure of column (needle) and polygonal shapes as a result of recrystallization was observed due to the high calcination temperature.

Preparation and Oxygen Permeability of $PrBa_{0.9}Sr_{0.1}Co_2O_{5+{\delta}}$ Ceramic Membrane ($PrBa_{0.9}Sr_{0.1}Co_2O_{5+{\delta}}$ 세라믹 분리막의 제조 및 산소투과 특성)

  • Pyo, Dae-Woong;Kim, Jong-Pyo;Son, Su-Hwan;Park, Jung-Hoon
    • Membrane Journal
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    • v.21 no.4
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    • pp.321-328
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    • 2011
  • $PrBa_{0.9}Sr_{0.1}Co_2O_{5+{\delta}}$ oxide was synthesized by soild state reaction method. Dense ceramic membrane was prepared using as-prepared powder by pressing and sintering at $1250^{\circ}C$. XRD result of membrane showed double perovskite structure. Leakage and oxygen permeation test were conducted on the membrane sealed by pyrex ring as a sealing material. Oxygen permeation was measured in the temperature range from 850 to $950^{\circ}C$. The oxygen flux of $PrBa_{0.9}Sr_{0.1}Co_2O_{5+{\delta}}$ membrane was increased with the temperature from 0.15 to $0.32mL/cm^2{\cdot}min$.

Property of MgO with Different Sintering Temperatures under High Pressures (고압 환경에서 소결 온도에 따른 MgO 물성의 변화)

  • Song, Jeongho;Noh, Yunyoung;Song, Ohsung
    • Journal of the Korean Ceramic Society
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    • v.49 no.6
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    • pp.608-613
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    • 2012
  • We investigated the property changes of MgO powders sintered at temperatures ranging from $700^{\circ}C$ to $1900^{\circ}C$ for 5minutes at a pressure of 2.7 GPa for a high-pressure high-temperature(HPHT) diamond synthesis process. The physical properties of the sintered MgO powders were characterized by optical microscopy, field emission scanning electron microscopy (FE-SEM), Vickers hardness tests, and by the apparent density, and X-ray diffractometry. An optical micro-analysis showed that white MgO powders became black after sintering due to carbon contamination from the graphite heat source. FE-SEM revealed the growth in the grain size of the MgO powders from $0.3{\mu}m$ to $50{\mu}m$ after sintering at $1700^{\circ}C$. The hardness and apparent density increased to $1800^{\circ}C$ while the samples were dedensified at $1900^{\circ}C$ due to the growth of isolated pores. According to the XRD analysis, no phase transformation occurred in the MgO powders. These results suggest that HPHT-sintered MgO powders can show an accelerated sintering process characterized by grain neck growth, pore connections, isolated pore growth and dedensification in 5 minutes, while these processes with the conventional sintering process take at least 5 hours.

Structural and Microwave Dielectric Properties of the Mg$_{1-x}Sr_xTiO-3$ Ceramics with Sintering Temperature and Sr Mole Ratio (소결온도와 Sr몰비에 따른 Mg$_{1-x}Sr_xTiO-3$ 세라믹스의 구조 및 마이크로파 유전특성)

  • Choi, Eui-Sun;Chung, Jang-Ho;Ryu, Ki-Won;Lee, Young-Hie
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.50 no.5
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    • pp.226-231
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    • 2001
  • The $Mg_{1-x}Sr_xTiO_3\;(x=0.02{\sim}0.08)$ ceramics were fabricated by the conventional mixed oxide method. The sintering temperature and time were $1250^{\circ}C{\sim}1350^{\circ}C$, 2hr., respectively. From the X-ray diffraction patterns, it was found that the perovskite $SrTiO_3$ and ilmenite $MgTiO_3$ structures were coexisted in the $Mg_{1-x}Sr_xTiO_3\;(x=0.02{\sim}0.08)$ ceramics. The dielectric constant( ${\epsilon}_r$) was increased with addition of $SrTiO_3$. The temperature coefficient of resonant frequency( ${\tau}_f$) was gradually varied from negative value to the positive value with increasing the $SrTiO_3$. The temperature coefficient of resonant frequency of the $Mg_{1-x}Sr_xTiO_3(x=0.036)$ ceramics was near zero, where the dielectric constant, quality factor, and ${\tau}_f$ were 20.65, 95120 and +1.3ppm/$^{\circ}C$, respectively.

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Microwave Dielectric Properties of (1-X)$Mg_4Ta_2O_{9-x}TiO_2$(X=0, 0.3, 0.4) Ceramics with Sintering Temperature (소결온도에 따른 (1-x)$Mg_4Ta_2O_{9-x}TiO_2$(X=0, 0.3, 0.4) 세라믹스의 마이크로파 유전특성)

  • 김재식;최의선;이문기;이영희
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.53 no.2
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    • pp.67-72
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    • 2004
  • The microwave dielectric properties and microstructure of the (1-x)$Mg_4Ta_2O_{9-x}TiO_2$(X=0, 0.3, 0.4) ceramic were, investigated. The specimens were prepared by the conventional mixed oxide method with sintering temperature of $1350^{\circ}C$$1425^{\circ}C$. According to the XRD patterns, the (1-x)$Mg_4Ta_2O_{9-x}TiO_2$(X=0, 0.3, 0.4) ceramics have the $Mg_4Ta_2O_{9}$ phase(hexagonal). The dielectric constant($\varepsilon$$_{\gamma}$) and density increased with sintering temperature and mole fraction of x. To improve the quality factor and the temperature coefficient of resonant frequency, TiO$_2$($\varepsilon_{r}$=100, $Q{\times}f_{r}$=40,000GHz, $\tau$$_{f}$=+450 ppm/$^{\circ}C$) was added in $Mg_4Ta_2O_{9}$ ceramics. In the case of the $0.7Mg_4Ta_2O_{9}$-$0.3TiO_2$ and the $0.6Mg_4Ta_2O_{9}$-$0.4TiO_2$ceramics sintered at $1400^{\circ}C$ for 5hr., the microwave dielectric properties were $\varepsilon$$_{\gamma}$=11.72, $Q{\times}f_{r}$=126,419GHz, $\tau_{f}$=-31.82 ppm/$^{\circ}C$ and $\varepsilon_{r}$=12.19, $Q{\times}f_{r}$=109,411GHZ, $\tau$$_{f}$= -17.21 ppm/$^{\circ}C$, respectively.

Structural and Microwave Dielectric Properties of $Mg_{5}B_{4}O_{15}$ (B=Ta, Nb) Ceramics with Sintering Temperature (소결온도에 따른 $Mg_{5}B_{4}O_{15}$ (B=Ta, Nb) 세라믹스의 구조 및 마이크로파 유전 특성)

  • Kim, Jae-Sik;Choi, Eui-Sun;Lee, Moon-Kee;Ryu, Ki-Won;Lee, Young-Hie
    • Proceedings of the KIEE Conference
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    • 2006.07c
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    • pp.1420-1421
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    • 2006
  • In this study, structural and micowave dielectric properties of the $Mg_{5}B_{4}O_{15}$ (B=Ta, Nb) cation-deficient perovskite ceeramics. The specimens are prepared through the solid-state route. According to the XRD pattern, $Mg_{4}Ta_{2}O_9$ and $MgTa_{2}O_6$ phase exist in calcined and sintered $Mg_{5}Ta_{4}O_{15}$ powder. Also $Mg_{5}Ta_{4}O_{15}$ phase added with increasing sintering temperature. In the case of calcined and sintered $Mg_{5}Nb_{4}O_{15}$ powder, single phase of $Mg_{5}Nb_{4}O_{15}$ were appeared. The bulk density and quality factor of the $Mg_{5}B_{4}O_{15}$ (B=Ta, Nb) ceramics were increased with sinteming temperature in $1400^{\circ}C{\sim}1450^{\circ}C$, but these were decreased in another sintering temperature. Dielectric constant of the $Mg_{5}Ta_{4}O_{15}$ ceramics was increased continuously with increasing of sintering temperature. And the dielectric constant of the $Mg_{5}Nb_{4}O_{15}$ ceramics was increased in $1400^{\circ}C{\sim}1450^{\circ}C$ but decreased in $1475^{\circ}C$. In the case of the $Mg_{5}Ta_{4}O_{15}$ and $Mg_{5}Nb_{4}O_{15}$ ceramics sintered at $1450^{\circ}C$ for 5h, the dielectric constant, quality factor, and temperature coefficient of the resonant frequency (TCRF) were 8.2, 259,473 GHz, -10.91 $ppm/^{\circ}C$ and 14, 37,350 GHz, -52.3 $ppm/^{\circ}C$, respectively.

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A Study on the magnetic properties of Mn-Zn Ferrite (Mn-Zn Ferrite의 자기적 특성에 관한 연구)

  • Kim Do-Hwan;Choi Young-Ji;Kwon Oh-Heung
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2006.05a
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    • pp.898-901
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    • 2006
  • In this paper, effect of ceramic processing was investigated on the magnetic properties of low loss Mn-Zn ferrite. High frequency characteristics, high saturated magnetic flux density and high magnetic permeability and low magnetism loss are required for the development of Mn-Zn ferrite, which is parts in the communication. therefore, in order to improve Mn-Zn ferrite with a high frequency , it is important to have a minimal change of particles and to control the eddy current loss caused by high resistance of the stratum of particles and to reduce the hysteresis loss by uniform change of detailed structure. In this paper, we added $V_2O_5\;and\;CaCo_3$ to Mn-Zn Ferrite to achieve a high efficiency, low loss core material. The compositions are MnO : ZnO : $Fe_2O_3$ = 21 : 10 : 69 mol%. They were sintered at $1250^{\circ}C$ for Three hours. Initial permeability was measured at 0.1MHz. At 50mT, Power loss was measured by temperature changing at 100kHz.

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Sintering and Dielectric Properties of LTCC Zero Shrinkage Substrate by Glass Infiltration (Glass Infiltration법에 의한 LTCC 무수축 기판의 소결특성 및 유전특성)

  • You, Jung-Hun;Yeo, Dong-Hun;Shin, Hyo-Soon;Kim, Hyo-Tae;Kim, Jong-Hee;Yoon, Ho-Gyu
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.06a
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    • pp.49-49
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    • 2007
  • Glass infiltration 방법을 이용하여 '$A_2O_3$/Glass/$Al_2O_3$' 구조의 무수축 LTCC 기판을 제조하였다. Glass infiltration 법에 의한 무수축 기판 제조에 있어 가장 중요한 요소로는 Glass의 점성은 낮고, alumina에 대한 Glass의 젖음성 (wettability)이 좋으며. 낮은 반응성이 요구되기 때문에 Glass의 조성 선정이 무엇보다 중요하다. 본 연구에서는 Na, Pb, Mg 계열의 각기 다른 glass들의 alumina에 대한 젖음성을 평가하여 젖음성 및 치밀성이 우수한 Pb 계열의 Glass를 이용하여 LTCC 기판으로 적용 가능한 온도인 $700{\sim}900^{\circ}C$에서 '$A_2O_3$/Glass/$Al_2O_3$'구조의 glass infiltration 특성을 고찰하였다. 소성 후 수축율은 x-y축 0.2%, Z축 40%, 밑도 $3.8g/cm^3$, 유전율 6.8, 품질계수 552로 무수축 기판으로서의 적용 가능성을 확인하였다.

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The structural properties of the $(Bi_xBa_{0.6-x}Sr_{0.4})TiO_3$[BBST] ceramics with the sintering temperature and addition of $Bi2O_3$ ($Bi2O_3$ 첨가량 및 소결온도에 따른$(Bi_xBa_{0.6-x}Sr_{0.4})TiO_3$[BBST] 세라믹스의 구조적 특성)

  • Nam, Sung-Pill;Lee, Sang-Chul;Lim, Sung-Su;Lee, Sung-Gap;Lee, Young-Hie
    • Proceedings of the KIEE Conference
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    • 2002.11a
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    • pp.85-87
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    • 2002
  • The $(Ba_xBi_{0.6-x}Sr_{0.4})TiO_3$[x=0.1, 0.2, 0.3] ceramics were prepared by conventional mixed oxide method The structural properties of the $(Ba_xBi_{0.6-x}Sr_{0.4})TiO_3$[x=0.1, 0.2, 0.3] ceramics with the sintering temperature($1200^{\circ}C,\;1250^{\circ}C,\;1300^{\circ}C$) were investigated by XRD, SEM, EDS. Increasing the sintering temperature, the intensity of the $Ba_{0.5}Sr_{0.5}TiO_3$ (100), (110), (111), (200), (310) peaks and $SrBi_4Ti_4O_{15}$ (319), (040) peaks were increased. The gram of the $(Bi_{0.2}Ba_{0.4}Sr_{0.4})TiO_3$ ceramics sintered at $1250^{\circ}C$ were fine and uniform. Increasing the sintering temperature. the average gram size of the $(Bi_{0.2}Ba_{0.4}Sr_{0.4})TiO_3$ ceramics were decreased. The density of $(Bi_{0.1}Ba_{0.5}Sr_{0.4})TiO_3$ ceramics sintered at $1250^{\circ}C$ was 5.4524 [$g/cm^2$].

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Microwave Dielectric Properties of $0.8Mg_4Ta_2O_9-0.2CaTiO_3$ Ceramics with Sintering Temperatuer (소결온도에 따른 $0.8Mg_4Ta_2O_9-0.2CaTiO_3$ 세라믹스의 마이크로파 유전 특성)

  • Kim, Jae-Sik;Choi, Eui-Sun;Lee, Moon-Kee;Ryu, Ki-Won;Lee, Young-Hie
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2004.07b
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    • pp.659-662
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    • 2004
  • The microwave dielectric properties of the $0.8Mg_4Ta_2O_9-0.2CaTiO_3$ ceramics with sintering temperature were investigated. All the sample of the $0.8Mg_4Ta_2O_9-0.2CaTiO_3$ ceramics prepared by conventional mixed oxide method and sintered at $1400^{\circ}C-1450^{\circ}C$. According to X-ray diffraction patterns of the $0.8Mg_4Ta_2O_9-0.2CaTiO_3$ ceramics, major phase of the hexagonal $Mg_4Ta_2O_9$ phase were showed. Porosity of the $0.8Mg_4Ta_2O_9-0.2CaTiO_3$ ceramics were reduced with increasing sintering temperature, but the bulk density was increased. In the case of $0.8Mg_4Ta_2O_9-0.2CaTiO_3$ ceramics sintered at $1425^{\circ}C$, dielectric constant, quality factor and temperature coefficient of resonant frequency(TCRF) were 13.69, 63,754GHz and -29.37 $ppm/^{\circ}C$, respectively.

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