• 한국군사과학기술학회지
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• 제3권1호
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• pp.207-217
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• 2000

A fire fighting characteristic by a single evaporating droplet in the case of a fire of military enclosure space was studied experimentally. Transient cooling of solid surface by water droplet evaporation has been investigated through controlled experiments using a heated brass cylinder. Quantitative predictions of droplet evaporation time and in-depth transient temperature distribution in solid have been made. The particular interest was in the removal of thermal energy from the heated cylinder by evaporative cooling. A $10{\mu}1$ single droplet is deposited on a horizontal brass surface with initial temperatures in the range of $90^{\circ}C{\sim}130^{\circ}C.$ The results can be summarized as follows; Evaporating droplet was divided into three different configuration. Evaporation time was predicted as a function of initial surface temperature ($t_c=492.62-6.89T_{s0}+0.0248T_{s0}^2).$ The contact temperature was predicted as a function of initial surface temperature( $T_{i}$=0.94 $T_{s0}$+1.4), The parameter ${\beta}_o$ was predicted as a function of initial surface temperature( ${\beta}_0$ : 0.O0312 $T_{s0}+0.932$)>)>)

• 설비공학논문집
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• 제8권3호
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• pp.437-450
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• 1996

A set of stability equations is formulated for natural convection flows adjacent to a vertical isothermal surface melting in cold pure water. It takes account of the nonparallelism of the base flows. The melting rate is regarded as a blowing velocity at the ice surface. The numerical solutions of the linear stability equations which constitute a two-point boundary value problem are accurately obtained for various values of the density extremum parameter $R=(T_m-T_{\infty})/(T_0-T_{\infty})$ in the range $0.3{\leq}R{\leq}0.6$, by using a computer code COLNEW. The blowing effects on the base flow becomes more significant as ambient temperature ($T_{\infty}$) increases to $T_{\infty}=10^{\circ}C$. The maximum decrease of heat transfer rate is about 6.4 percent. The stability results show that the melting at surface causes the critical Grashof number $G^*$ and the maximum frequency of disturbances to decrease. In comparision with the results for the conventional parallel flow model, the nonparallel flow model has a higher critical Grashof number but has lower amplification rates of disturbances than does the parallel flow model. The spatial amplification contours exhibit that the selective frequency $B_0$ of the nonparallel flow model is higher than that of the parallel flow model and that the effects of melting are rather small. The present study also indicates that the selective frequency $B_0$ can be easily predicted by the value of the frequency parameter $B^*$ at $G^*$, which comes from the neutral stability results of the nonparallel flow model.

• 한국자기학회지
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• 제1권2호
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• pp.15-21
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• 1991

고온초전도체 $Y_{1}Ba_{2}Cu_{3-x}Sn_{x}O_{7-y}$에서 Cu 대신에 Sn 을 치환하면서 이들의 조성변화에 따른 자기적 특성을 vibrating sample magnetometer(VSM)와 torque magnetometer를 이용 하여 측정하였다. Cu 대신에 Fe, Ni 등의 원소를 치환했을 때와는 달리 x=0.36 까지 되어도 초전도 전이온도가 90 K 이상을 나타냄을 알 수 있었다. 온도와 외부자기장에 따른 자기 모우먼트 측정을 통하여 각 조성에 따른 lower critical field ($H_{c1}(T)$)과 upper critical field ($H_{c2}(T)$)를 측정하였다. 이 결과를 이용해 $H_{c1}(0)$과 $H_{c2}(0)$를 계산했으며, 간섭길이 (${\varepsilon}_{0}$), 침투깊이 (${\lambda}_{0}$), Ginzburg-Landau 상수 k등을 얻을 수 있었으며, 시료의 flux pinning 효과도 확인할 수 있었다.

• 대한기계학회논문집A
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• 제34권5호
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• pp.619-628
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• 2010

차세대 의료기기 시장을 변화시킬 것으로 기대되는 형상기억합금(SMA) 기반의 최소침습용 의료기기는 시술자의 손동작과 같은 유연성과 섬세함을 구현할 수 있는 장점이 있다. 그러나 SMA의 비선형 열전기적 특성으로 인해 SMA 기반 차세대 의료기기 엑추에이터는 자유로운 방향조종 구현이 제한적이고 상용화에 있어서 큰 한계성으로 작용한다. 본 논문은 SMA의 효과적인 온도제어를 위해 전류-온도간의 개방루프 계단응답을 분석하고 1차 미분방정식 해와 비교하여 온도제어에 필요한 파라미터 $t_1$을 도출한 뒤 실험적으로 그 기능을 검증하였다. 또한 $t_1$은 전류를 입력으로 온도를 출력으로 하는 시불변 선형계의 특성함수의 폴(pole)이므로 주파수에 의한 온도제어에 관계된 파라미터인 것으로 나타났다. 본 논문의 결과는 SAM 기반의 차세대 의료기기 액추에이터의 효과적인 위치제어 설계에 응용될 수 있다.

• 소성∙가공
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• 제10권1호
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• pp.42-52
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• 2001

The static softening mechanisms of 304 stainless steel were studied by hot torsion test. The interrupted deformation tests were performed In the range of 900~$1100^{\circ}C$ and 5.0$\times$$10^{-2}$- 5.0$\times$$10^0$/sec. The metadynamic recrystallization (MDRX) could be distinguished from the static recrystallization (SRX). Comparison of the softening kinetics between MDRX and SRX showed that the rate of MDRX was more rapid than that of SRX for the same deformation variables. To the exact prediction of MDRX, the MDRX parameter, which could be simultaneously estimated by the interpass time and Zener-Hollomon parameter, was developed. The time lot 50% MDRX, $t_{0.5} was modeled using the deformation parameters : $t_{0.5} = 1.33\times10^{-11}$ $\.\varepsilon^{-0.41}$ D exp(230.3kJ/mol/RT) and the predicted value was very correspondent with the measurement. It was found that the static parameters such as interpass time can control the dynamic states in the several successive deformation process.

• 대한수학회보
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• 제51권6호
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• pp.1649-1654
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• 2014

A tournament T is an orientation of a complete graph and an arc in T is called pancyclic if it is contained in a cycle of length l for all $3{\leq}l{\leq}n$, where n is the cardinality of the vertex set of T. In 1994, Moon [5] introduced the graph parameter h(T) as the maximum number of pancyclic arcs contained in the same Hamiltonian cycle of T and showed that $h(T){\geq}3$ for all strong tournaments with $n{\geq}3$. Havet [4] later conjectured that $h(T){\geq}2k+1$ for all k-strong tournaments and proved the case k = 2. In 2005, Yeo [7] gave the lower bound $h(T){\geq}\frac{k+5}{2}$ for all k-strong tournaments T. In this note, we will improve his bound to $h(T){\geq}\frac{2k+7}{3}$.

• 한국안전학회지
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• 제8권4호
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• pp.27-40
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• 1993

High temperature tensile tests, steady state creep tests, Internal stress tests and creep rupture tests using A17075 alloy( $T_{6}$ ) were performed over the temperature range of 9$0^{\circ}C$~50$0^{\circ}C$ (0.4 $T_{m}$ ~0.85 $T_{m}$ ) and stress range of 0.64~17.2(kgf/$\textrm{mm}^2$). The main results obtained in this paper were as follows. (1) The activation energies for yielding at the temperature of 0.4 $T_{m}$ ~0.75 $T_{m}$ were calculated to be 25.7~36.5kcal/mol, which were nearly equal to the activation energies for creep. (2) At around the temperature of 9$0^{\circ}C$~12$0^{\circ}C$ and under the stress level of 10~17.2(kgf/$\textrm{mm}^2$), and at around the temperature of 200~41$0^{\circ}C$ and under the stress level of 1.53~9.55(kgf/$\textrm{mm}^2$) and again at around the temperature of 470~50$0^{\circ}C$ and under the stress level of 0.62~l.02(kgf/$\textrm{mm}^2$), the applied stress dependence of steady state creep rate $n_{measu}$ measured were, respectively, 3.15, 6.62 and 1.1, which were in good agreement the calculated stress dependence $n_{ealeu}$ obtained by the difference of the applied stress dependence of the Internal stress and the ratio of the internal stress to the applied stress. (3) At the temperature range of 0.4~0.43 $T_{m}$ , and at the temperature range of 0.52~0.75 $T_{m}$ and again at the temperature range of 0.82~0.85 $T_{m}$ , the activation energies $Q_{measu}$ obtained by steady state creep rate, respective, 26. 16, 34.9, 36.2 and 36.1kcal/mol, which were in good agreement with those obtained with the activation energies under constant effective stress and the temperature dependence of Internal stress. (4) At the temperature range of the 0.52~0.73 $T_{m}$ and under the stress level of 1.53~9.55(kgf/$\textrm{mm}^2$), the stress dependence of rupture life(n’) measured was 6.3~6.6, which was in good agreement with the stress dependence of steady state creep rate(n). And at the same condition the activation energy for rupture( $Q_{f}$ ) measured was 32.0~36.9kca1/mol, which was also in good agreement with the activation energy obtained by steady state creep rate ( $Q_{c}$ ). (5) The rupture life( $t_{f}$ ) might be represented by athermal process attributed to the difference of the applied stress dependence of the internal stress and the ratio of the internal stress to the applied stress, and the thermal activated process attributied to the temperature dependence of the internal stress as $t_{f}$ = A'$\sigma$$_{a}$ ｛n(1-d $\sigma$$_{i}$ /d $\sigma$$_{a}$ )/(1-$\sigma$$_{i}$ / $\sigma$$_{a}$ )｝.exp[｛ $Q_{c}$ $^{*}$-( $n_{o}$ R $T^2$/ $E_{(T)}$) (d $E_{(T)}$/dT) - ( $n_{0}$ R $T^2$/ $\sigma$$_{a}$ - $\sigma$$_{i}$ ) (d $\sigma$$_{i}$ /dT)｝/RT]. (6) The relationship betwween Larson-Miller rupture parameter and logarithmic stress was linearly decreased, so creep rupture life of Al 7075 alloy seemed to be predicted exactly with Larson-Miller parameter.meter.

• International Journal of Reliability and Applications
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• 제12권1호
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• pp.61-77
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• 2011

One of the most important problems in the estimation of the parameter of the failure model, is the cost of experimental sampling units, which can be reduced by using any prior information available about ${\theta}$, and devising a two-stage pooling shrunken estimation procedure. We have proposed an estimator of the reliability function (R(t)) of the exponential model using two-stage time censored data when a prior value about the unknown parameter (${\theta}$) is available from the past. To compare the performance of the proposed estimator with the classical estimator, computer intensive calculations for bias, mean squared error, relative efficiency, expected sample size and percentage of the overall sample size saved expressions, were done for varying the constants involved in the proposed estimator (${\tilde{R}}$(t)).

• 한국수산과학회지
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• 제8권2호
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• pp.47-60
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• 1975

자원해석은 일반적으로 시계열적 견지에 입각하고 있으나, 본 연구에서는 단면적인 견지에서, 2년간의 자원변동을 극수적인 관계에서 파악하여 자원해석을 하였으며, 이것으로 각년의 가입량을 추정하는 방법 시도하였다. 이를 요약하면 다음과 같다. 1. 단일 population에 있어서 t 시기(년 또는 어기)와 t+1 시기와의 초기자원량(미수)의 관계는 $N_{0,\;t+1}=N_{0,\;t}(1-m_t)-C_t+R_{t+1}$ 단, $N_0$ : 초기자원량 (미수), C : 어획미수, R : 가입미수, m : 자연사망률 이다. 위의 식에서 다음의 관계가 성립된다. $\phi_{t+1}=\frac{(1-\varrho^{-z}{t+1})Z_t}{(1-\varrho^{-z}t)Z_{t+1}}-\frac{1-\varrho^{-z}t+1}{Z_{t+1}}\phi_t-a'\frac{1-\varrho^{-z}t+1}{Z_{t+1}}C_t+a'\frac{1-\varrho^{-z}t+1}{Z_{t+1}}R_{t+1}$ 단, $\phi$ : 밀도지수, M : 자연사망계수, Z : 감소계수, a' : 평균자원량에 대한 밀도지수 이 식에서 $\phi$ 및 $C_t$를 독립변수, $\phi_{t+1}$를 종속변수라해서 중회귀분석하여 $\phi_t$ 및 $C_t$ 의 각 계수를 구하고, 이 각 계수로서 저연사망계수 M, 단위노력당 어획계수 a'을 구하여 t+1연의 가입량추정치 $\hat{R}_{t+1}$를 구할 수 있다. 중회귀분석하는 데 있어서는 $R_{t+1}$이 거의, 같으며 $X_{t+1}$에 심한 차이가 없는 시기를 선정하여 취급할 수 있다. 2. 각 시기의 추정된 가입량은 가입량의 상대치로서 인정하는 것이 안전하다. 3. 밀도지수 대신으로 자원량지수를 사용하여도 같은 추정방법으로 가입량이 추정된다. 단, 어장면적을 고려해야 한다. 4. 변동관계를 미수로서 취급할 때는 이론적으로 가입량의 절대치를 구할 수 있으나, 중량으로 취급할 때는 이론적으로 가입량의 상대치를 구하게 된다. 그러나 어느 경우나 같은 추정방법이 적용된다. 5. 인도양의 bigeye tuna에 대하여 수전(1970)의 자료를 이용하여 본 추정방법에 적용시켜 보았다. 수전(1970)가 구한 M,q(단위노력당 어획계수)로서 계산된 각년의 가입량의 변화와 본연구에서 구한 각년의 가입량의 변화와는 극히 비례적이었다(Table 2, Fig.2). 6. 한국동안의 꽁치에 있어서 해황어황 주간예보 ($1964.3\~1974.8$ : 국립수산진흥원 포항지원)의 자료를 이용하여 어느 해의 춘하기의 밀도지수와 그해의 추동기의 밀도지수와의 관계에서 각년의 추기의 가입량을 추정하고 어느 해의 추동기의 밀도지수와 다음해의 춘하기의 밀도지수와의 관계에서 각년의 춘하기의 가입량을 추정하였다(Table4, Fig.5, Fig.7). 그 결과, 년금의 폭이 좁은 이 꽁치 군단에 있어서 각년의 밀도지수와 가입량이 상당히 비례적이었다.

• 대한수학회지
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• 제33권4호
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• pp.763-775
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• 1996

For $Q = [0,S] \times [0,T]$ let C(Q) denote Yeh-Wiener space, i.e., the space of all real-valued continuous functions x(s,t) on Q such that x(0,t) = x(s,0) = 0 for every (s,t) in Q. Yeh [10] defined a Gaussian measure $m_y$ on C(Q) (later modified in [13]) such that as a stochastic process ${x(s,t), (s,t) \epsilon Q}$ has mean $E[x(s,t)] = \smallint_{C(Q)} x(s,t)m_y(dx) = 0$ and covariance $E[x(s,t)x(u,\upsilon)] = min{s,u} min{t,\upsilon}$. Let $C_\omega \equiv C[0,T]$ denote the standard Wiener space on [0,T] with Wiener measure $m_\omega$. Yeh [12] introduced the concept of the conditional Wiener integral of F given X, E(F$\mid$X), and for case X(x) = x(T) obtained some very useful results including a Kac-Feynman integral equation.