• 사물인터넷융복합논문지
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• 제8권1호
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• pp.79-85
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• 2022

사물인터넷(IoT)은 다양한 플랫폼, 컴퓨팅 성능, 기능을 가지는 장치를 연결한다. 네트워크의 다양성과 IoT 장치의 편재로 인해 보안 및 개인 정보 보호에 대한 요구가 증가하고 있다. 따라서 암호화 메커니즘은 이러한 증가된 요구 사항을 충족할 만큼 충분히 강력해야 하고 동시에 저 사양의 장치에 구현될 수 있을 만큼 충분히 효과적이어야 한다. 논문에서는 IoT에서 사용할 수 있는 다양한 유형의 장치에 대한 최신 암호화 기본 요소 및 체계의 성능 및 메모리 제한 사항을 제시한다. 또한, IoT 네트워크에 자주 사용되는 저 사양의 장치에서 가장 일반적으로 사용되는 암호화 알고리즘의 성능에 대한 자세한 성능 평가를 수행한다. 데이터 보호 기능을 제공하기 위해 바이너리 링에서 암호화 비대칭 완전 동형 암호화와 대칭 암호화 AES 128비트를 사용했다. 실험 결과 IoT 장치는 대칭 암호를 구현하는데 충분한 성능을 가지고 있었으나 비대칭 암호 구현에서는 성능이 저하되는 것을 알 수 있다.

• Clinical and Experimental Pediatrics
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• 제52권2호
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• pp.242-246
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• 2009

13번 환염색체 증후군은 정신발달의 지체, 성장 장애, 안면부 기형, 중추신경계 기형, 심장기형, 손발의 기형, 골격계 기형 및 항문기형의 특징을 가진다. 많은 수의 13번 환염색체 증후군에 대한 보고가 있었지만 국내에서는 오직 6예의 임상증례 고가 있다. 이들 보고는 모두 순수한 13번 환염색체 증후군을 보고한 것으로 본 저자들은 13번 환염색체 모자이크 현상의 증례를 경험하였다. 산전진찰 상 자궁내 발육지연이 의심되었던 남아에서 안면부기형이 관찰되었으나 이 외에 이학적 검사상 심장 기형, 골격계 및 외부 생식기 기형은 특별히 관찰되지 않았다. 시행한 세포 유전학 검사상 13번 염색체의 ring/monosomy/dicentric 모자이크 현상이 나타났다. 이후에도 근력저하, 성장과 발달지연을 보이고 있다. 저자들은 안면부 기형, 소두증과 대칭성 자궁내 발육지연을 보인 남아에서 13번 환염색체의 모자이크 증후군을 경험하여 기존에 보고된 다른 증례들과 임상 양상을 비교하여 보고하는 바이다.

• 대한수학회보
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• 제22권1호
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• pp.11-15
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• 1985

Manddelberg [9] has shown that a Clifford algebra of a free quadratic space over an arbitrary semi-local ring R in Brawer-Wall group BW(R) is determined by its rank, determinant, and Hasse invariant. In this paper, we prove a corresponding result when R is a full ring.Throughout this paper, unless otherwise specified, we assume that R is a commutative ring having 2 a unit. A quadratic space (V, B, .phi.) over R is a finitely generated projective R-module V with a symmetric bilinear mapping B: V*V.rarw.R which is non-degenerate (i.e., the natural mapping V.rarw.Ho $m_{R}$(V,R) induced by B is an isomorphism), and with a quadratic mapping .phi.: V.rarw.R such that B(x,y)=1/2(.phi.(x+y)-.phi.(x)-.phi.(y)) and .phi.(rx) = $r^{2}$.phi.(x) for all x, y in V and r in R. We denote the group of multiplicative units of R by U9R). If (V, B, .phi.) is a free rank n quadratic space over R with an orthogonal basis { $x_{1}$,.., $x_{n}$}, we will write < $a_{1}$,.., $a_{n}$> for (V, B, .phi.) where the $a_{i}$=.phi.( $x_{i}$) are in U(R), and denote the space by the table [ $a_{ij}$ ] where $a_{ij}$ =B( $x_{i}$, $x_{j}$). In the case n=2 and B( $x_{1}$, $x_{2}$)=1/2 we reserve the notation [a $a_{11}$, $a_{22}$] for the space. A commutative ring R having 2 a unit is called full [10] if for every triple $a_{1}$, $a_{2}$, $a_{3}$ of elements in R with ( $a_{1}$, $a_{2}$, $a_{3}$)=R, there is an element w in R such that $a_{1}$+ $a_{2}$w+ $a_{3}$ $w^{2}$=unit.TEX>=unit.t.t.t.

• 대한전기학회논문지:전기물성ㆍ응용부문C
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• 제54권6호
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• pp.255-261
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• 2005

Recently, the RF inductive discharge or inductively coupled plasma continues to attract growing attention as an effective plasma source in many industrial applications, the best known of which are plasma processing and lighting technology. To the point of lighting sources, the ring-shaped electrodeless fluorescent lamps utilizing an inductively coupled plasma have been objects of interest and research during the last decades, mainly because of their potential for extremely long life, high lamp efficacies, rapid power switching response. In this paper, maxwell 3D finite element analysis program (Ansoft) was used to obtain electromagnetic properties associated with the coil and nearby structures. The electromagnetic emitting properties were presented by 3D simulation software operated at 250 kHz and some specific conditions. The electromagnetic field in the ferrite core was shown to be high and symmetric. An LS-100 luminance meter and a Darsa-2000 spectrum analyzer were used in the experiment. According to data on the lamp tested using high magnetic field ferrite, the optical and thermal wave fields were shown to be high around the ring-shaped electrodeless fluorescent lamp. The optical or light field was high at the center of the bulb rather than around the ferrite core. The light conditions of the bulb were assumed to be complex, depending on the condition of the filler gas, the volume of the bulb, and the frequency of the inverter. Our results have shown coupling between the gas plasma and the field of the light emitted to be nonlinear.

• 대한기계학회논문집B
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• 제29권10호
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• pp.1101-1110
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• 2005

In this paper we present the numerical results of the behavior of the horizontal vortex generated by ejecting a liquid vertically upward from an orifice into the bulk fluid above the orifice. The numerical calculation has been performed for the axi-symmetric Navier-Stokes equation. A simple flow-visualization experiment was also conducted to qualitatively verify the numerical solutions. Three cases of the flow configurations studied in this paper are; firstly, the vortex was generated without any background rotation, secondly, the vortex was made under a full background rotation, and thirdly, the vortex was made during the spin-up process such that only the region adjacent to the side wall was set into motion viewed in the inertial frame of reference. It was shown that the swirl flow at the inlet boundary affects considerably the formation and development of the vortex for the second case. In the third case, it was remarkable to see that the vortex cannot penetrate into the region near to the side wall of the tank, because of the strong swirl flow and corresponding high pressure gradient in the region.

• 대한수학회논문집
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• 제22권1호
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• pp.41-51
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• 2007

Let R be a ring with left identity e and suitably-restricted additive torsion, and Z(R) its center. Let H : $R{\times}R{\times}R{\rightarrow}R$ be a symmetric 3-additive mapping, and let h be the trace of H. In this paper we show that (i) if for each $x{\in}R$, $$n=<<\cdots,\;x>,\;\cdots,x>{\in}Z(R)$$ with $n\geq1$ fixed, then h is commuting on R. Moreover, h is of the form $$h(x)=\lambda_0x^3+\lambda_1(x)x^2+\lambda_2(x)x+\lambda_3(x)\;for\;all\;x{\in}R$$, where $\lambda_0\;{\in}\;Z(R)$, $\lambda_1\;:\;R{\rightarrow}R$ is an additive commuting mapping, $\lambda_2\;:\;R{\rightarrow}R$ is the commuting trace of a bi-additive mapping and the mapping $\lambda_3\;:\;R{\rightarrow}Z(R)$ is the trace of a symmetric 3-additive mapping; (ii) for each $x{\in}R$, either $n=0\;or\;<n,\;x^m>=0$ with $n\geq0,\;m\geq1$ fixed, then h = 0 on R, where denotes the product yx+xy and Z(R) is the center of R. We also present the conditions which implies commutativity in rings with identity as motivated by the above result.

• 대한전기학회:학술대회논문집
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• 대한전기학회 1989년도 추계학술대회 논문집 학회본부
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• pp.87-90
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• 1989

The force acting on high Tc superconductors at 77K is measured and analyzed numerically. Both values are compared, and the difference between them is discussed. The forces, acting on a superconducting disk (thickness:1[mm], diameter:12[mm]) in an axially-symmetric magnetic field produced by a solenoid or a permanent magnet ring, are measured at 77K. The disk is an YBCO high Tc superconductor. The discrete surface current method(DSCM) is formalized for an axially-symmetric magnetic field. The forces of the superconducting disk in the magnetic field are analyzed using the DSCM, assuming that the disk is a perfect diamagnetic body. When the bottom side of the disk is separated 8[mm] from the top side of the solenoid, and the magnetic field applied on the center of the bottom side of the disk is 96[G], the measured value and the calculated value of the force are 96 and 496[mgf], respectively. The difference between them is caused by a non-perfect diamagnetism of the high Tc superconductor at 77K. It is proposed that a real force acting on high Tc superconductors at 77K can be estimated on the basis of a measured magnetic susceptibility of the high Tc superconductor at 77K and a calculated force of a perfect diamagnetic body.

• 대한기계학회논문집
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• 제16권11호
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• pp.2082-2089
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• 1992

본 연구에서는 모델링재료를 이용한 AISI4130축대칭 도움형상의 열간 단조 공 정 설계 방안을 이룩하기 위한 실험을 수행하였다. 본 실험에 사용된 모델링 재료는 Van Akan International사 제품의 Plastalina를 이용하였다. 모델링재료와 실제 재 료 사이의 상사성을 검토하기 위해 압축실험을 수행하였는데 압축 실험시 모델링재료 와 평다이 사이의 마찰력을 줄이기 위해 베이비파우더, 휴지, 바셀린, 테프론테잎 등 을 이용하였으며 램 속도, 온도, 그리고 변형률도에 따른 응력 변화를 검토해 보았다. 열간 공정시에 수반되는 금형과 공작물 사이의 마찰력을 알아보기 위해 앞에 열거한 윤활제를 이용한 링실험을 수행하여 전단마찰계수(m) 값의 변화를 알아보고 폐쇄단조 시 주요한 설계방안을 검토하기 위해 플래쉬를 갖는 폐쇄단조 실험을 수행하였다. 이 실험에서는 폐쇄단조시 중요한 설계변수 중의 하나인 플래쉬 두께 대 폭비, 플래쉬 부를 통한 체적손실, 그리고 원기둥모양의 초기 단조 시편 형상비 등에 따른 설계방안 을 검토하여 기존 참고문헌에 나와 있는 결과들과 유사성을 검토하였다. 이와같은 실험 결과를 체계적으로 확립하고 고강도강 대형 단조품생산에 필요한 단조하중 예측, 예비성형체 설계, 성형성 연구등에 대한 응용성을 검토하고자 한다.

• 한국기계가공학회지
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• 제19권5호
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• pp.91-97
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• 2020

A split-die design for the cold forging of symmetric parts such as those having a hexagonal cross-section is presented in this paper. Parts with a hexagonal cross-section, such as bolt heads and nuts, should be forged with a die that has a hexagonal-shaped hole. A split type die is required to mitigate the buildup of stress concentrations located at the corners of the hexagonal hole. Generally, the insert of a hexagonal die is made by cutting each corner of a cylinder using a hexagonal hole and then combined with the die and shrink-fitted. However, split dies face problems when extruding material at the corners of the hexagonal split die. To address this problem, two types of split dies were evaluated: rounded hexagonal dies and angular hexagonal dies. The effects of the pre-stress ring on the dies were compared and analyzed and results show that using the angular split hexagonal die can extend the lifetime of forging dies.

• Bulletin of the Korean Chemical Society
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• 제35권4호
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• pp.989-993
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• 2014

The molecular structures of 2,6-diaza-1,3,5,7-tetraoxaspiro[3,3]heptane (1) and its dinitro derivative, 2,6-dinitro-2,6-diaza-1,3,5,7-tetraoxaspiro[3,3]heptane (2), were fully optimized without symmetry constraints at $HF/6-31G^*$ level of theory. A bisected conformation with respect to the ring is preferred with a $C_2$ symmetric structure. The density of each molecule in the crystalline state was estimated to 1.12 and 2.36 $g/cm^3$ using PM3/VSTO-3G calculations from the molecular volume. The heat of formation was calculated for two compounds at the CBS-4M level of theory. The detonation parameters were computed using the EXPLO5 software: D = 6282 m/s, $P_{C-J}$ = 127 kbar for compound 1, D = 7871 m/s, $P_{C-J}$ = 307 kbar for compound 2, and D = 6975 m/s, $P_{C-J}$ = 170 kbar for 60% compound 2 with 40% TNT. Specific impulse of compound 1 in aluminized formulation when used as monopropellants was very similar to that of the conventional ammonium perchlorate in the same formulation of aluminum.