• 자연과학논문집
• /
• 제4권
• /
• pp.85-93
• /
• 1991

$BaCO_3$와 $TiO_2$ 등 mole비 혼합물의 고상반응은 $BaCO_3 + TiO_2\longrightarrow$ $BaTiO_3 + CO_2$의 반응식에 따라 $CO_2$ gas가 발생된다. 이 분해과정을 DTA-TG를 사용하여 속도론적으로 고찰하였다. 그 결과는 다음과 같다. 1. $TiO_2$와 공존하는 $BaCO_3$는 순수한 $BaCO_3$보다 낮은 온도에서 분해된다. 그 이유는 생성물의 free energy가 감소되기 때문이다. 2. $BaCO_3$ 분해과정의 속도론적 고찰에 사용되는 식은 Jander's식보다는 Carter's식이 더욱 의미가 있으며 Carter's식에 의해 구해진 분해 활성화 에너지는 42.8Kcal/mol이다.

• 한국결정성장학회지
• /
• 제19권5호
• /
• pp.223-227
• /
• 2009

침전법, 수열 반응법, 리간드 보조법을 사용하여 다양한 형태의 $BaCO_3$ 결정을 합성하였다. 수용액에서 $Ba(NO_3)_2$과 $Na_2CO_3$를 단순 침전시키면 불규칙한 입자 형태의 $BaCO_3$ 마이크로 결정이 얻어졌다. 수열 반응으로 $Ba(NO_3)_2$와 urea를 반응시켜 육각형 막대 피라미드 형태의 $BaCO_3$를 합성하였으며, 리간드 보조 수열 반응법을 사용하여 육각형 막대형의 $BaCO_3$를 합성하였다. 리간드 농도가 증가 할수록 $BaCO_3$ 육각형 막대의 종횡비가 증가하였다.

• The Korean Journal of Ceramics
• /
• 제5권4호
• /
• pp.379-385
• /
• 1999

Minute boehmite crystals with high aspect rations, which were hydrothermally synthesized from gibbsite in $Ba(OH)_2$ solution, occluded Ba with the Ba/Al molar ratio of about 0.03 in their interlayers. Their surface areas were about 14$\m^2$/g. The Ba-intercalated bohemite samples were partly used for producing $BaAl_{12}O){19}$ with low sinterability by externally supplementing $Ba(OH)_2$, and for forming transient aluminas. The surface area of $BaAl_{12}O){19}$ obtained by firing at $1500^{\circ}C$ for 3 h was 5.3$\m^2$/g, which was significantly lower than 12$\m^2$/g of the sol-gel origin. While a mixture ${\gamma}$-alumina and BaO is known to from $BaAl_{12}O){19}$ at $1200^{\circ}C$, solid state reaction between η-alumina transformed from the Ba-intercalated boehmite and BaO formed from $Ba(OH)_2$ deposited on the boehmite started above $1300^{\circ}C$. This suggests that large sized $Ba^{2+}$ ion occluded in η-alumina considerably suppresses the diffusion of $Al^{3+}$ ion. The surface area of the Ba-intercalated boehmite fired at $1400^{\circ}C$ for 3h was as high as 14$\m^2$/g indicative of its potential applicability to combustion catalysts. But it was decreased to 5.0$\m^2$/g after firing at $1500^{\circ}C$ for 3 h, accompanied by abrupt formations of $\alpha$-alumina and $BaAl_{12}O){19}$ as main products. The suppression of $\alpha$-alumina formation up to $1400^{\circ}C$ also suggests the significant blocking effect of $Ba^{2+}$ ion on the diffusion of the component ions.

• 한국세라믹학회지
• /
• 제19권3호
• /
• pp.223-228
• /
• 1982

For the preparation of ferroxidure BaO.5.5 $Fe_2O_3$ with high coercive force, the green and calcined coprecipitates, which were obtained by neutralizing the mixed salt solution $FeCl_2-BaCl_2$ and $FeCl_3-BaCl_2$ with alkali solution $NaOH-Na_2CO_3$, were investigated about the thermal reaction, crystal growth, and the magnetic properties of the sintered specimens. The very single-domain crystallites of Ba-ferrite with high coercive force are formed from the coprecipitate of amorphous $Fe(OH)_3$ and amorphous $BaCO_3$ at lower temperature than that of subnucleus crystalline $\delta$-FeOOH and amorphous $BaCO_3$.

• 대한화학회지
• /
• 제38권4호
• /
• pp.309-318
• /
• 1994

La$_2O_3$-변형 BaTi$O_3$의 안정한 결함구조와 단일상 영역을 X-선 회절분석기와 주사전자현미경을 사용하여 연구하였다. La$_2O_3$-변형 BaTi$O_3$의 안정한 결함구조는 La$^{3+}$ 이온이 격자구조내의 Ba$^{3+}$ 이온을 치환하고 Ti빈자리가 전하 불균형을 보상하기 위한 결함으로 생성된 [($Ba^x_{Ba})_{1-2x}(La{\cdot}_{Ba})_{2x}][Ti^x_{Ti})_{1-x/2}(V""_{Ti})_{x/2}]O_3$이다. 안정한 결함구조가 형성되도록 BaTi$O_3$에 La$_2O_3{\cdot}3/2TiO_3$를 혼입할 때 단위격자는 약 3 mol%가 혼입될 때부터 정방정에서 입방정으로 변하였고, 고용한계는 약 14 mol%이었다. La2$O_3{\cdot}3/2TiO_2$를 고용한계 이상으로 혼입할 때는 이차상으로 La_4Ba_2Ti_5O){18}$가 생성되었다. La$_2O_3$-변형 BaTi$O_3$ 조성에서 BaO가 과량 존재하면 소결성이 나쁘지만, Ti$O_2$가 과량으로 존재하면 액상소결에 의하여 소결성이 좋아짐을 확인할 수 있다.

• 전기학회논문지
• /
• 제57권4호
• /
• pp.625-628
• /
• 2008

Ba-Zn ferrite powders for electromagnetic insulator were synthesized by self-propagating high-temperature synthesis(SHS) with a reaction of $xBaO_2+(1-x)ZnO+0.5Fe_2O_3+Fe{\rightarrow}Ba_xZn_{1-x}Fe_2O_4$. In this study, phase indentification of SHS products was carried out by using x-ray diffractometry and quasi-nano sized Ba-Zn powders were prepared by a pulverizing process. SHS mechanism was studied by thermodynamical analysis about oxidation reaction among $BaO_2,\;ZnO,\;Fe_2O_3$, and Fe. As oxygen pressure increases from 0.25 MPa to 1.0 MPa, the SHS reactions occur well and make clearly the SHS products. X-ray analysis shows that final SHS products formed with the ratio of $BaO_2/ZnO$ of 0.25, 1.0 and 4.0, are mainly $Ba_xZn_{1-x}Fe_2O_4$. Based on thermodynamical evaluation, the heat of formation increases in the order of $ZnFe_2O_4,\;BaFe_2O_4$, and $Ba_xZn_{1-x}Fe_2O_4$. This supports that $Ba_xZn_{1-x}Fe_2O_4$ phase is predominately formed during SHS reaction. The SHS reactions to form $Ba_xZn_{1-x}Fe_2O_4$ depends on oxygen partial pressure, and the heat of formation during the SHS reaction. The SHS reactions tends to occur well with increasing the oxygen partial pressure and BaO2/ZnO ratio in the reactants This means that the SHS reaction for the formation of Ba-Zn ferrite includes the reduction of BaO2/ZnO and the oxidation of Fe. $Ba_xZn_{1-x}Fe_2O_4$ powders after pulverizing is agglomeratedwith a size of about $50{\mu}m$, in which quasi-nano sized particles with about 300nm are present.

• 한국세라믹학회지
• /
• 제38권10호
• /
• pp.881-885
• /
• 2001

Kinetics and mechanisms of intermediate phases formation in $Ba(Mg_{1/3}Ta_{2/3})O_3$, obtained by a solid state reaction were studied. $Ba{Ta_2}{O_6}$ and ${Ba_4}{Ta_2}{O_9}$ as intermediate products were first formed at $700^{\circ}C$. $Ba(Mg_{1/3}Ta_{2/3})O_3$ was appeared at $800^{\circ}C$. Several reactions take place on heating process. $Ba{Ta_2}{O_6}$ is found at the first stage of the reaction, and then $Ba{Ta_2}{O_6}$ or ${Ba_4}{Ta_2}{O_9}$ react with MgO to form $Ba(Mg_{1/3}Ta_{2/3})O_3$. The reaction of $Ba(Mg_{1/3}Ta_{2/3})O_3$ formation does not complete until fired at $1350^{\circ}C$ for 60 min. The kinetics of solid-state reaction between powdered reactants was controlled by diffusion mechanism, and can be explained by the Jander's model for three-dimensional diffusion.

• 한국세라믹학회지
• /
• 제26권6호
• /
• pp.783-788
• /
• 1989

The reason of abnormal expansion in BaTiO3 synthesized in the equimolecular mixture and synthesized in Ba-rich region were investigated at the point of crystal and microstructure. The shrinkage and the expansion of the mixtures in BaCO3-TiO2 system were determined by the mass of BaCO3 added to the equimolecular BaCO3 and TiO2, Ba2TiO4 which was much formed and BaTi2O3 were important crystal in the reaction of Ba-rich region. Sintering phenomena of unreacted BaCO3 activity and the secondary phase caused to generate microcracks in the specimens.

• 방사성폐기물학회지
• /
• 제14권2호
• /
• pp.101-112
• /
• 2016

본 연구는 고방사성해수폐액 (HSW)으로부터 Barium (Ba)이 함침된 4A 제올라이트 (BaA)에 의한 고방사성핵종 중에 하나인 Sr의 흡착 제거를 수행하였다. BaA에 의한 Sr의 흡착 (BaA-Sr)은 Ba의 함침농도 20.2wt% 이상에서 Ba의 함침농도가 증가할수록 감소하며 Ba 함침농도는 20.2wt% 정도가 적당하였다. 그리고 BaA-Sr 흡착은 BaA 내 4A에 의한 Sr 흡착 (4A-Sr)에 $BaSO_4$ 침전에 따른 Sr 공침이 첨가되어, Sr의 농도가 0.2 mg/L 이하 (HSW 내 실제 Sr 농도 수준)에서 BaA는 m/V (흡착제량/용액 부피)=5 g/L, 4A는 m/V >20 g/L에서 99% 이상의 Sr 제거가 가능하였다. 이는 흡착제 단위 g 당 Sr의 처리용량 및 2차 고체폐기물 (폐흡착제 등) 발생량 저감화 차원에서 BaA-Sr 흡착이 4A-Sr 흡착보다 우수함을 나타낸다. 또한 BaA-Sr 흡착이 증류수보다 해수폐액에서 Sr의 제거능이 우수하여 HSW로부터 직접 Sr을 제거하는 데 효과적일 것으로 보인다. 반면에 BaA에 의한 Cs의 흡착 (BaA-Cs)은 주로 BaA 내 4A에 의해서 이루어지고 있어 함침 Ba의 영향은 거의 없는 것 같다. 한편 BaA-Sr 흡착속도는 유사 2차 속도식으로 표현할 수 있으며, Sr의 초기농도 및 V/m 비 증가에 따라서 속도상수 ($k_2$)는 감소하지만 평형흡착량 ($q_e$)은 증가하고 있다. 그러나 용액의 온도증가에 따라서는 반대로 $k_2$는 증가하지만 $q_e$는 감소하고 있다. BaA-Sr 흡착 활성화에너지는 약 38 kJ/mol 로 강력한 결합 형태를 이룬 화학흡착은 아니더라도 물리적 흡착보다 화학적 흡착이 지배적일 것으로 보인다.

• 한국세라믹학회지
• /
• 제35권8호
• /
• pp.775-782
• /
• 1998

This experiment is third study concerning BaO-{{{{ { { Pr}_{ 2} O}_{3 } }}-{{{{ { TiO}_{2 } }} (Ln=Sm, Nd, Pr, La..) system which is known to show a high dielectric constant and Q value in microwave dielectric materials. The process of cry-stallization and the microwave dielectric properties of the specimens sintered at 1220-140$0^{\circ}C$ for 2 hr was investigated in the BaO-(Na,{{{{ { { Pr})_{2 }O }_{3 } }}-{{{{ { TiO}_{2 } }} as well as BaO-{{{{ { { Pr}_{ 2} O}_{3 } }}-{{{{ { TiO}_{2 } }} system. The single phase BaPr2Ti5O14 and Ba(Nd,{{{{ { { Pr})_{2 }O }_{3 } }}Ti5O14 was finally formed from the Pr2Ti2O7 (Nd, Pr)2Ti2O7 as a secondary phase in the BaO-{{{{ { { Pr}_{ 2} O}_{3 } }}-{{{{ { TiO}_{2 } }} and BaO-(Nd, {{{{ { { Pr})_{2 }O }_{3 } }}-{{{{ { TiO}_{2 } }} system respectively The dielectric constant of the specimens sint-ered at 1280~131$0^{\circ}C$ showed the maximum value as 105(BaO-{{{{ { { Pr}_{ 2} O}_{3 } }}-{{{{ { TiO}_{2 } }} system) and 88 (BaO-(Nd,{{{{ { { Pr})_{2 }O }_{3 } }}-{{{{ { TiO}_{2 } }} system) and the Q values of them showed higher value than 1800 which are due to the maximum den-sity. However the dielectric properties of the specimens sintered at higher temperature than 131$0^{\circ}C$ were reduced due to the increases of pore which were resulted from the sudden grain growth.