• Journal of Gastric Cancer
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• 제18권4호
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• pp.339-347
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• 2018

Purpose: To evaluate the status of number 3b lymph node (LN) station in patients with adenocarcinoma of the esophagogastric junction (AEG) and to investigate the optimal indications for radical proximal gastrectomy (PG) for AEG. Materials and Methods: Data of 51 patients with clinically advanced Siewert types II and III AEG who underwent total gastrectomy (TG) between April 2010 and July 2017 were reviewed. The proportion of metastatic LNs at each LN station was examined. Number 3 LN station was separately classified into number 3a and number 3b. The risk factors for number 3b LN metastasis and the clinicopathological features of number 3b-positive AEG patients were investigated. Results: The incidences of LN metastasis were the highest in number 1 (47.1%), followed by number 2 (23.5%), number 3a (39.2%), and number 7 (23.5%) LN stations. LN metastasis in number 3b LN station was detected in 4 patients (7.8%). A gastric invasion length of more than 40 mm was a significant risk factor for number 3b LN metastasis. All 4 patients with number 3b-positive AEG had advanced cancer with a gastric invasion length of more than 40 mm. The 5-year survival rate of patients with a gastric invasion length of more than 40 mm was 50.0%. Conclusions: Radical PG may be indicated for patients with AEG with gastric invasion length of less than 40 mm.

• 한국정밀공학회지
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• 제21권1호
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• pp.71-79
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• 2004

The deformed layers generated in face milling works were comparatively investigated to type 316L and nitrogen(N)-added type 316LN stainless steels. In order to characterize mechanical properties between type 316L and type 316LN, high-temperature tensile tests were conducted with different temperatures: R.T to $700^{\circ}C$. The cutting forces of three components, Fx, Fy and Fz were measured using a tool dynamometer through the face milling cutting tests. The deformed layers were measured by micro-hardness tests along deformed layers. The results of mechanical properties showed that type 316LN was superior to type 316L. The deformed layers of two steels were generated in the 1501m-3001m ranges, and type 316L was higher than type 316LN. The reason for this is due to the high strength properties by nitrogen effect. It was found that deformed structures were well observed for type 316L, but were minutely observed for type 316LN in this cutting conditions.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2001년도 추계학술대회논문집A
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• pp.123-128
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• 2001

The creep constants which are used to the reference stress equations of creep damage were obtained to type 316LN stainless steel, and their determining methods were described in detail. Typical Kachanov and Rabotnov(K-R) creep damage model was modified into the damage equations with reference stress concepts, and the modified equations were applied practically to type 316LN stainless steel. In order to determine the reference stress value, a series of high-temperature tensile tests and creep tests were accomplished at $550^{\circ}C$ and $600^{\circ}C$. By using the experimental creep data, the creep constants used in reference stress equations could be obtained to type 316LN stainless steel, and a creep curve on rupture strain was predicted. The reference stress concept on creep damage can be utilized easily as a design tool to predict creep life because the process, which is quantified by the measurement of voids or micro cracks during creep, is omitted.

• 대한화학회지
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• 제26권1호
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• pp.24-30
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• 1982

란탄족 화합물인 Ln$(fod)_3$ (Ln = Pr, Nd, Eu 및 Yb)를 사용하여 contact-only (COM) 및 dipolar-only (DOM) 2성분계 혼합물을 만든 후 기질인 4-picoline의 $F_i$ 및 $G_i$값을 핵자기공명 이동으로 부터 측정하였다. 그 결과 Pr$(fod)_3$ 및 Eu$(fod)_3$의 혼합물인 COM 1 및 DOM 1으로 얻은 값들을 단일 Ln$(fod)_3$로 얻은 값들과 잘 일치하였다. 그러나 $(fod)_3$ 및 Yb$(fod)_3$의 혼합물인 COM 2 및 DOM 2로 얻을 값들을 단일 Ln$(fod)_3$로 얻은 값들과 상당한 오차를 나타내었다. 그 오차는 이테르븀(Yb) 착물에 기인하는 것으로 추정되었다.

• 대한기계학회논문집A
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• 제25권2호
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• pp.296-303
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• 2001

Kachanov-Rabotnov(K-R) creep damage theory was reviewed, and applied to design a creep curve for type 316LN stainless steel. Seven coefficients used in the theory, i.e., A, B, k, m, λ, r, and q were determined, and their physical meanings were analyzed clearly. In order to quantify a damage parameter ($\omega$), cavity amount was measured in the crept specimen taken from interrupted creep test with time variation, and then the amount was reflected into K-R damage equations. Coefficient λ, which is regarded as a creep tolerance feature of a material, increased with creep strain. Mater curve with λ=2.8 was well coincided with an experimental one to the full lifetime. The relationship between damage parameter and life fraction was matched with the theory at exponent ${\gamma}$=24 value. It is concluded that K-R damage equation was reliable as the modelling equation for type 316LN stainless steel. Coefficient data obtained from type 316LN stainless steel can be utilized for life prediction of operating material.

• 방사성폐기물학회지
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• 제19권3호
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• pp.353-366
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• 2021

The solubilities of different multicomponent lanthanide oxide (Ln₂O₃) solid solutions including binary (Ln₁ and Ln₂ = La, Nd, Eu, or Tm), ternary (Ln₁, Ln₂, and Ln₃ = La, Nd, Eu, or Tm), and higher systems (Ln = La, Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, and Lu) were studied after aging for four weeks at 60℃. Our recent study revealed that the phase transformations in binary ((La, Nd) and (La, Eu)) and ternary (La, Nd, Eu) systems are responsible for the formation of (La, Nd)(OH)₃, (La, Eu)(OH)₃, and (La, Nd, Eu)(OH)₃ solid solutions, respectively. The variations in the mole fractions of La³⁺, Nd³⁺, and Eu³⁺ in the sample solutions of these hydroxide solid solutions indicated that a thermodynamic equilibrium might account for the apparent La, Nd, and Eu solubilities. Conversely, the binary and ternary systems containing Tm₂O₃ as the heavy lanthanide oxide retained the oxide-based solid solutions, and their solubility behaviors were dominated by their congruent dissolutions. In the higher multicomponent system, the X-ray diffraction patterns of the solid phases, before and after contact with the aqueous phase indicated the formation of a stable oxide solid solution and their solubility behavior was explained by its congruent dissolution.

• 공업화학
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• 제4권3호
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• pp.474-481
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• 1993

무극성, 극성 용매 중 무극성, 극성용질의 무한희석 활동도계수를 가스 크로마토그래피에 의하여 $60^{\circ}C$로부터 $100^{\circ}C$ 범위에서 측정하였다. 무극성용매(n-octadecane)와 극성용매(n-hexadecyl alcohol)에 있어서 무극성용질(alkanes, cyclohexane, benzene, toluene과 $CCl_4$)의 $ln{\gamma}{\infty}$는 1/T 따라 비례하여 증가하였으며, 일정온도에서 동족렬의 $ln{\gamma}{\infty}$는 용질의 탄소수 증가에 따라 비례하여 증가하였다. 극성용질(alcohols, esters and ketones)과 약극성용매(di-2-ethyl adiphate and di-2-ethylhexylsebacate)계에서, 용질의 $ln{\gamma}{\infty}$는 1/T 증가에 따라 변화율이 증가하였으며, 또 일정온도에서 동족렬 용질의 $ln{\gamma}{\infty}$는 탄소수 증가에 따라 반비례하여 감소하였다. 극성용질(alcohols, esters and ketones)은 극성이 큰 용매(triphenyl-phosphate and tricresyl phosphate)계에 있어서, $ln{\gamma}{\infty}$는 1/T 증가에 따라 변화율이 증가하였으며, 일정온도에서 동족렬의 $ln{\gamma}{\infty}$는 용질의 탄소수 증가에 따라 비례하여 증가하였다.

• 공업화학
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• 제32권4호
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• pp.478-482
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• 2021

고정층 상압 유통식 반응기를 사용하여 Ln(1)-Ni(5)/SBA-15 (Ln = Dy, Eu, Pr, Tb) 촉매상에서 메탄의 부분 산화 반응을 수행하여 수소의 수율을 조사하였다. X-ray photoelectron spectroscopy (XPS) 분석으로 Ni(5)/SBA-15 촉매에 1 wt%의 Eu를 첨가함으로써 Eu(1)-Ni(5)/SBA-15의 O1s와 Si2p의 핵심 전자 수준의 화학적 이동이 있었으며, O1s, Ni2p_3/2, Si2p의 원자의 비가 1.284, 1.298, 1.058로 증가하였다. 촉매 표면상에 O^-, O^2-의 산소와 Eu³⁺, Ni⁰, Ni²⁺, Si⁴⁺의 이온이 존재함을 알 수 있었다. Eu(1)-Ni(5)/SBA-15 촉매상에서 수소의 수율은 57.2%이었으며, Ln(1)-Ni(5)/SBA-15 (Ln = Dy, Pr, Tb)보다 우수한 수소 수율을 보여주었고 25 h의 반응에서 안정된 촉매 활성을 유지하였다. Eu를 Ni(5)/SBA-15에 1wt%를 첨가함으로서 금속과 담체 간에 강한 상호 작용에 의한 SMSI 효과로 산소 빈자리를 만들고 촉매 표면상에 Ni⁰, N²⁺의 나노입자의 분산을 증가시켜 촉매 활성을 유지시켰다.

• Journal of Ecology and Environment
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• 제48권2호
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• pp.196-206
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• 2024

Background: Most of the biomass equations were developed using sample trees collected mainly from pan-tropical and tropical regions that may over- or underestimate biomass. Site-specific models would improve the accuracy of the biomass estimates and enhance the country's measurement, reporting, and verification activities. The aim of the study is to develop site-specific biomass estimation models and validate and evaluate the existing generic models developed for pan-tropical forest and newly developed allometric models. Total of 140 trees was harvested from each diameter class biomass model development. Data was analyzed using SAS procedures. All relevant statistical tests (normality, multicollinearity, and heteroscedasticity) were performed. Data was transformed to logarithmic functions and multiple linear regression techniques were used to develop model to estimate aboveground biomass (AGB). The root mean square error (RMSE) was used for measuring model bias, precision, and accuracy. The coefficient of determination (R² and adjusted [adj]-R²), the Akaike Information Criterion (AIC) and the Schwarz Bayesian information Criterion was employed to select most appropriate models. Results: For the general total AGB models, adj-R² ranged from 0.71 to 0.85, and model 9 with diameter at stump height at 10 cm (DSH₁₀), ρ and crown width (CW) as predictor variables, performed best according to RMSE and AIC. For the merchantable stem models, adj-R² varied from 0.73 to 0.82, and model 8) with combination of ρ, diameter at breast height and height (H), CW and DSH₁₀ as predictor variables, was best in terms of RMSE and AIC. The results showed that a best-fit model for above-ground biomass of tree components was developed. AGB_Stem = exp {-1.8296 + 0.4814 natural logarithm (Ln) (ρD²H) + 0.1751 Ln (CW) + 0.4059 Ln (DSH₃₀)} AGB_Branch = exp {-131.6 + 15.0013 Ln (ρD²H) + 13.176 Ln (CW) + 21.8506 Ln (DSH₃₀)} AGB_Foliage = exp {-0.9496 + 0.5282 Ln (DSH₃₀) + 2.3492 Ln (ρ) + 0.4286 Ln (CW)} AGB_Total = exp {-1.8245 + 1.4358 Ln (DSH₃₀) + 1.9921 Ln (ρ) + 0.6154 Ln (CW)} Conclusions: The results demonstrated that the development of local models derived from an appropriate sample of representative species can greatly improve the estimation of total AGB.

• 대한수학회지
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• 제43권2호
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• pp.271-281
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• 2006

The commutative products of the distributions $x^r\;ln^p\;{\mid}x{\mid}\;and\;x^{-r-1}ln^q\;{\mid}x{\mid}$ and of sgn x $x^r\;ln^p\;{\mid}x{\mid}\;and\;sgn\;x\;x^{-r-1}ln^q\;{\mid}x{\mid}$ are evaluated for $r=0,\;\pm1,\;\pm2,...\;and\;p,\;q=0,1,2,....$