• 한국재료학회지
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• 제26권4호
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• pp.182-186
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• 2016

Zircon, having excellent thermal, chemical, and mechanical properties, is utilized in refractory materials, electronic materials, chemical machines, structural materials, etc. However, zircon generally shows thermal dissociation to zirconia($ZrO_2$) and silica($SiO_2$) around the sintering temperature of $1540^{\circ}C$, and when zircon particles are small and impurities are present, thermal dissociation is known to occur at around $1100^{\circ}C$. This reduces the mechanical properties of $ZrSiO_4$. In this research, the effect of adding $SiO_2$ and 3Y-TZP to $ZrSiO_4$ has been studied in order to suppress dissociation and improve the mechanical properties. Addition of $SiO_2$ suppressed the dissociation of $ZrSiO_4$ at lower temperatures. It also enabled optimum packing between the particles, resulting in a dense microstructure and good mechanical properties. When 3Y-TZP was added, recombination with the dissociated $SiO_2$ resulted in good mechanical properties by suppressing the generation of pores and the densification of the microstructure.

• Bulletin of the Korean Chemical Society
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• 제35권3호
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• pp.770-774
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• 2014

The bond dissociation energy (BDE) of the chemical bond between the carbon and oxygen atoms of a simple TEMPO-derivative is calculated by employing the density functional theory, the $2^{nd}$ order M${\phi}$ller-Plesset (MP2) perturbation theory, and complete basis set (CBS) methods. We find that BDE of the positive ion of the TEMPO-derivative is larger at least by 7 kcal/mol than that of the negative ion, which implies that the dissociation reaction rate of the positive ion should be slower than that of the negative ion. Such theoretical predictions are contrary to the results of our previous experiments (Anal. Chem. 2013, 85, 7044), in which the larger energy was required for negative o-TEMPO-Bz-C(O)-peptides to undergo the dissociation reactions than for the positive ones. By comparing our theoretical results to those of the experiments, we conclude that the dissociation reaction of o-TEMPO-Bz-C(O)-peptide should occur in a complicated fashion with a charge, either positive or negative, probably being located on the amino acid residues of the peptide.

• 대한화학회지
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• 제30권2호
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• pp.152-158
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• 1986

치환나프톨류(4-Cl-1-naphthol, 6-Br-2-naphthol and $8-NH_2-2-naphthol)$의 해리상수를 온도(25 ~ 40${\circ}C$)와 압력(1~2000bar)을 변화시키면서 분광학적 방법으로 측정했다. 이들의 해리상수는 치환기가 들어가므로서 모두 감소했다. 이것은 치환기의 I-효과로서 설명이 가능했으며 또 온도와 압력이 증가하면 해리상수도 증가하였다. 이들 해리상수로부터 반응의 열역학적 성질을 계산하여 반응의 성질을 알아보았다.

• 대한화학회지
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• 제33권4호
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• pp.343-349
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• 1989

${\omega}$-아미노산인 ${\beta}$-alanine과 ${\gamma}$-aminobutyric acid의 해리상수를 전도도법을 이용하여 온도($20{\sim}40^{\circ}C$)와 압력($1{\sim}2500$ bar)을 변화시키면서 측정하였다. 각각 아미노산의 두 가지 해리상수는 온도가 증가하면 증가하지만 압력이 증가하면 $K_1$은 증가하지만 $K_2$는 감소하였다. 해리상수를 이용하여 여러 가지 열역학적 성질들을 계산하고 이들로부터 해리반응의 특성을 알아보았다. ${\omega}$-아미노산의 해리상수를 해리기와 치환기간의 거리의 상관관계로 알아보았다. 반응특성을 알아보기 위해 Hammett 법칙을 적용하여 반응의 치환기 상수와 압력에 따른 반응상수를 계산하였다. ${\omega}$-아미노산의 특성을 치환기 효과로 설명하고 반응유형을 반응상수로서 알아보았다.

• Journal of Yeungnam Medical Science
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• 제4권1호
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• pp.17-23
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• 1987

백서심장조직을 trypsin과 collagenase 두가지의 효소를 사용하여 분리하면서 각 효소의 분리효과와 두가지 효소의 복합적 세포분리효과를 조사하였으며 이와 동시에 dimethyl sulfoxide가 세포분리과정 및 단기간 배양중에 세포에 미치는 효과를 조사한 결과를 다음과 같이 요약할 수 있다. 1. 백서심장조직에서 세포를 분리할 때 $4^{\circ}C$ trypsin 18시간 전처치후 $37^{\circ}C$ collagenase 처치한 군에서 세포생존율 세포수확량 및 심근세포 생존율이 가장 높았다. 즉 단일 효소 처리보다는 효소 복합연속 처리가 더 효율적이었다. 2. $37^{\circ}C$ trypsin만으로 세포분리를 하였을 때 세포생존율과 수확량이 가장 낮았다. 3. 백서심장세포의 분리과정과 초기 배양 과정에 세포회복이나 보호에 대한 DMSO의 효과는 인정되지 않았으며 오히려 세포파괴 효과가 높음을 알 수 있었다.

• Mass Spectrometry Letters
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• 제13권4호
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• pp.177-183
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• 2022

The monomer and dimer structures of the amyloid fragment Aβ(1-16) sequence formed in H₂O were investigated using electrospray ionization mass spectrometry (MS) and tandem MS (MS/MS). Aβ16 monomers and dimers were indicated by signals representing multiple proton adduct forms, [monomer+zH]ⁿ⁺ (=M^z+, z = charge state) and [dimer+zH]^z+ (=D^z+), in the MS spectrum. Fragment ions of monomers and dimers were observed using collision-induced dissociation MS/MS. Peptide bond dissociation was mostly observed in the D1-D7 and V11-K16 regions of the MS/MS spectra for the monomer (or dimer), regardless of the monomer (or dimer) charge state. Both covalent and non-covalent bond dissociation processes were indicated by the MS/MS results for the dimers. During the non-covalent bond dissociation process, the D³⁺ dimer complex was separated into two components: the M¹⁺ and M²⁺ subunits. During the covalent bond dissociation of the D³⁺ dimer complex, the b and y fragment ions attached to the monomer, (M+b_10-15)^z+ and (M+y_9-15)^z+, were thought to originate from the dissociation of the M²⁺ monomer component of the (M¹⁺+M²⁺) complex. Two different D³⁺ complex geometries exist; two distinguished interaction geometries resulting from interactions between the M¹⁺ monomer and two different regions of M²⁺ (the N-terminus and C-terminus) are proposed. Intricate fragmentation patterns were observed in the MS/MS spectrum of the D⁵⁺ complex. The complicated nature of the MS/MS spectrum is attributable to the coexistence of two D⁵⁺ configurations, (M¹⁺+M⁴⁺) and (M²⁺M³⁺), in the Aβ16 solution.

• Bulletin of the Korean Chemical Society
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• 제32권11호
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• pp.3873-3879
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• 2011

The potential energy surface (PES) for the isomerizations and dissociations of the acrylonitrile radical cation was determined from the CBS-QB3 and CBS-APNO calculations. The Rice-Ramsperger-Kassel-Marcus model calculations were performed based on the PES in order to predict the competitions among the dissociation channels. The mechanisms for the loss of $H^{\bullet}$, $H_2$, $CN^{\bullet}$, HCN, and HNC were proposed. The $C_3H_2N^+$ ion formed by loss of $H^{\bullet}$ was predicted as a mixture of $CH{\equiv}C-C=NH^+$, $CH{\equiv}C-N{\equiv}CH^+$, and $CH_2=C-C{\equiv}N^+$. Furthermore $CH{\equiv}C-C{\equiv}N^{+{\bullet}}$ was formed mainly by a consecutive 1,2-H shift and 1,2-H2 elimination.

• Bulletin of the Korean Chemical Society
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• 제21권8호
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• pp.779-784
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• 2000

Comparing the adsorption properties and dissociation on a Pt(111) iththat ona Fe(111) surface, we have con-sidered seven coordination modes of the adsorbed binding site: $di-${\sigma}$${\Delta}$\mu\pi/\mu$, 1-fbld,2-fold, and 3-fbld sites. On the Pt(111) surface, t he adsorbed binding site of carbon dioxide was strongestat the1-fold site and weakest at the $\pi/\mu-site.$ The adsorbed binding site on the Fe(111) surface was strongest at the di-бsite and weakest at the 3-fold site. We have found that the binding energy at each site that excepted 3-fold on the Fe(111) surface was stronger than the binding energy on the Pt(111) surface and that chemisorbed $CO_2bends$ because of metal mixing with $2\piu${\rightarrow}$6a_1CO_2orbital.$, The dissociation reaction occured in two steps, with an intermediate com-plex composed of atomic oxygen and ${\pi}bonding$ CO forming. The OCO angles of reaction intermediate com-plex structure for the dissociation reaction $were115^{\circ}Con$ the Pt(111), and $117^{\circ}C$ on the Fe(111) surface. We have found that the $CO_2dissociation$ rea11) surface proceeds easily,with an activationenergy about 0.2 eV lower than that on the Pt(111) surface.

• 대한화학회지
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• 제30권2호
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• pp.145-151
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• 1986

3-CN, 4-CN, $3-NH_2$ 및 $4-NH_2$ 치환피리딘의 해리상수를 온도(15 ∼ 40${\circ}C$)와 압력(1-2500bar)을 변화시키면서 측정하였다. 측정방법은 전도도법을 적용했으나 낮은 해리상수를 가진 물질에서도 적용되는 피리딘류의 염용액의 전도도를 측정하므로 계산가능한 방법을 모색하여 응용하였다. 이 방법은 어떤 조건에서의 해리상수를 알고 있어야 하는 것과 실험값을 외삽하여 피리딘염의 전도도를 알아야 하는 번거로움도 있으나 측정이 가능하다는 것을 확인할 수 있다. 이들 치환체의 해리상수는 온도가 증가하면 커지고 압력이 높아지면 해리상수는 작아진다는 것을 알 수 있었다. 또 반응의 열역학적 성질을 계산하여 반응성도 고찰하였다.

• Bulletin of the Korean Chemical Society
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• 제26권11호
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• pp.1682-1688
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• 2005

Using the ASED-MO (Atom Superposition and Electron Delocalization-Molecular Orbital) theory, we investigated carbon formation and carbon hydrogenation for $CO_2$ methanation on the Ni (111) surface. For carbon formation mechanism, we calculated the following activation energies, 1.27 eV for $CO_2$ dissociation, 2.97 eV for the CO, 1.93 eV for 2CO dissociation, respectively. For carbon methanation mechanism, we also calculated the following activation energies, 0.72 eV for methylidyne, 0.52 eV for methylene and 0.50 eV for methane, respectively. We found that the calculated activation energy of CO dissociation is higher than that of 2CO dissociation on the clean surface and base on these results that the CO dissociation step are the ratedetermining of the process. The C-H bond lengths of $CH_4$ the intermediate complex are 1.21 $\AA$, 1.31 $\AA$ for the C${\cdot}{\cdot}{\cdot}H_{(1)}$, and 2.82 $\AA$ for the height, with angles of 105${^{\circ}}$ for ∠ $H_{(1)}$CH and 98${^{\circ}}$ for $H_{(1)} CH _{(1)}$.