• Composites Research
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• 제12권6호
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• pp.74-82
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• 1999

폴리 우레탄 폼 코아 샌드위치 복합재료의 정적 및 피로 특성에 대하여 연구하였다. 유리 섬유강화 스킨과 중합의 폼 코아를 갖는 비스티칭, 스티칭, 스티프너의 세 종류 시편이 사용되었다. 특히 스티칭 샌드위치 구조는 두께 방향에 대하여 폴리에스터와 유리섬유를 꼬아서 부가적인 구조 보강이 코아의 상하 표면을 통하여 꿰멘 구조로 층간분리를 최소화하기 위해 샌드위치 구조 패널을 스티칭하여 만들고 수지는 수지의 유동 온도에서 수지의 낮은 점도 특성을 이용하여 스티칭 섬유에 침투시켜 함께 경화하였다. 스티칭 섬유가 $50{\times}50{\;}mm$의 간격으로 스티칭된 시편 및 스티프너 시편의 굽힘강도는 비스티칭 시편과 비교하여 각각 50%및 10배 이상으로 향상되었다. 최대 하중의 20%크기로 $10^6$ 피로 사이클을 받은 후, 비스티칭 시편의 굽힘 피로강도는 정적 굽힘강도와 비교하여 27%까지 감소되었고, 스티칭된 시편은 39%,그리고 스티프너에 의하여 보강된 시편은 20%정도 감소되었다. 폴리우레탄 폼 코아의 에이징 효과를 입증하기 위해, 피로 시험 후 샌드위치 시편의 표면 적층의 손상은 초음파 C-scan장비를 사용하여 검출하였다. 초음파 C-scan결과로부터 피로 시험동안 손상 받은 어떤 결함도 없었다 이는 피로 사이클동안 폼 코아 샌드위치 구조에 대한 굽힘강도의 감소는 폴리우레탄 폼이 에이징되어 발생하는 것을 의미한다.

• 대한기계학회논문집A
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• 제27권12호
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• pp.2011-2018
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• 2003

To analyze the bending collapse behavior of an aluminum square tube beam under a bending load, a finite element simulation for the four-point bending test has been performed. Using an aluminum tube beam specimen partly inserted with two steel bars, the local buckling deformation near the center of the tube beam was induced. The maximum bending load and the bending collapse behavior obtained from the numerical simulation were in good agreement with experimental results. Using a combination of the four-point bending test and its finite element simulation, analysis of the local buckling and the accompanied bending collapse behavior of aluminum tube beam could be quantitative accomplished.

• 대한기계학회논문집
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• 제18권9호
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• pp.2396-2403
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• 1994

An experimental study on material characterization and mechanical properties of SMC(Sheet Molding Compounds) compression method parts was carried out. Simple compression test using grease oil as a lubricant was carried out to characterize flow stress of SMC at elevated temperatures. Two different mold temperatures, $130^{\circ}C{\;}and{\;}150^{\circ}C$ and two different mold speeds, 15, 45 mm/min were used for preparing the specimen of SMC compression molded parts. Surface roughness, tensile, and 3-point bending tests were used to determine the effects of molding temperatures and speeds on mechanical properties of compression molded SMC parts. Orientation and distribution of glass fiber in the compression molded SMC parts were also investigated by photographing the burnt flat specimen and taking SEM(Scanning Electron Microscope) of cross-sectional T-specimen.

• 대한기계학회논문집A
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• 제26권1호
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• pp.160-170
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• 2002

Many of aged and damaged concrete structure have been revitalized with composite reinforcement. Flexural behaviors of composite-patched concrete specimens are characterized by high-sensitivity moire interferometry. The three-mirror, four-beam interferometry system and a compact loading system are used for obtaining singe patterns representing whole-field contour maps of in-plane displacements. It is seen from the calibration test for the loading system that the measured bending displacement is in excellent agreement with the displacement calculated by the beam theory. The crack opening displacement as well as the bending and the horizontal displacement fur the notched and unnotched specimen are investigated. The results also show that the notched specimen reinforced by a composite sheet has sufficient stiffness and strength compared to the original concrete specimen.

• 수산해양기술연구
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• 제28권3호
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• pp.286-294
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• 1992

In this paper, the corrosion fatigue crack propagation behavior of structure rolled steel (SWS 41C) was investigated by changing the thickness, and this experiment was done by the three point bending corrosion fatigue tester. The main results obtained are as follows: 1) As the thickness of specimen becomes thicker, the corrosion sensitivity to initial stage crack becomes some sensitive, and that the fatigue life becomes more sensitive. 2) The crack growth rate to initial stage crack (da/dN) was retarded as the thickness of specimen becomes thicker. But after initial stage crack, as the thickness of specimen is more thicker, da/dN is more rapid. 3) As the corrosion fatigue crack length grows, the accelerative factor of thick specimen (t=12mm) is more higher than that of thin specimen (t=6mm). 4) As the corrosion fatigue crack length grows, the corroson potential of both thick specimen and thin specimen becomes more less noble potential, however thick specimen (t=12mm) tends to more less noble potential than that of thin specimen(t=6mm).

• 대한기계학회논문집A
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• 제35권7호
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• pp.779-784
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• 2011

본 논문은 첨가제 $SiO_2$를 가지는 3종류의 SiC 세라믹스의 연마판 거칠기에 따르는 균열 치유 연구를 실시하였다. 혼합물은 질소가스 분위기에서 2053 K, 35 MPa, 1시간 동안 소결하였다. SiC 세라믹스 시험편의 최적 균열 치유 조건은 1373 K에서 1시간이다. 균열부의 치유 물질은 SiC와 $O_2$의 산화반응에 의한 유리상 $SiO_2$이다. 최적 치유 조건에서 미연마 SiC 세라믹스의 굽힘 강도는 완전하게 회복되지 않았다. 그러나 SAY, SAYS-1 및 SAYS-2 시험편에서 경제적인 면을 고려하면 1시간 열처리에서 상온 굽힘 강도가 가장 높게 나타난 SAY 시험편이 우수하다. $125\;{\mu}m$ 연마판의 연마 시험편은 결함의 수나 크기가 줄어들었으나, 열처리 후에도 표면 미세 결함이 완전하게 치유되지 못하였다. $40\;{\mu}m$ 연마판의 연마 시험편은 1시간 열처리 후 표면 결함이나 기공은 거의 없었으며, 굽힘 강도는 $6\;{\mu}m$ 연마판 경면 시험편의 강도만큼 회복하였다.

• 소성∙가공
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• 제3권4호
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• pp.401-414
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• 1994

Springback for the three point bending is anlayzed and experimented. Neutral axis is assumed to remain at the midthickness for large ratio of radius of curvature to thickness. Pure bending theory is used to be extended to the analysis of the springback for three point bending. The specimen is thought to be divided into numerous small elements. The theory for pure bending is then adopted for analysis of each element to obtain springback in terms of the relationship between initial and final deflections. the boundary conditions between neighborhood elements are the deflection and slope which should be the same. Deflection is calculated by summing up the deflections of each element. Experiments have been performed for different conditions which are punch radius, span length, and initial deflections. Comparisons between the analytical solution and experimental results show the same trends.

• 대한기계학회논문집A
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• 제38권12호
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• pp.1387-1394
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• 2014

광탄성 실험법에 의해 측정된 등색프린지 차수를 응력으로 변환시키기 위해서는 광탄성 재료 응력 프린지 상수를 알아야 한다. 광탄성 재료 응력 프린지 상수는 단순 인장시편 또는 압축하중을 받는 원형디스크를 이용하여 측정하는 방법 등이 있다. 이들 방법에서는 시편에 여러 하중을 가하여 하중에 응답하는 프린지 차수의 관계를 최소자승법 등을 이용하여 재료 상수를 결정한다. 본 논문에서는 4점 굽힘 시편에 하중을 가하여 나타나는 프린지로부터 재료 응력 프린지 상수를 결정하였다. 4점 굽힘 시편의 순수 굽힘 구간에서는 주응력 방향이 일정하므로 4단계 위상이동법의 적용이 가능하다. 이 방법은 원형편광기에서 검광판을 0, ${\pi}/4$, ${\pi}/2$, 그리고 $3{\pi}/4$ 라디안 회전시켜 얻은 4개의 광탄성 프린지를 필요로 한다. 4점 굽힘 시편을 이용한 재료의 프린지 상수를 결정하는 방법에서는 일정 하중을 가하여 서로 다른 위치에서도 측정할 수 있는 장점이 있다. 이 방법으로 측정된 재료 응력 프린지 상수는 제조회사에서 제시한 범위이내에 분포하였다.

• Nuclear Engineering and Technology
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• 제52권7호
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• pp.1579-1586
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• 2020

Dissimilar metal joints (DMJs) are more common in the application of piping system of many industries. A 2- D and 3-D finite element analysis (FEA) is carried out on dissimilar metal Single Edged Notch Bending (DMSENB) specimens fabricated from ferritic steel, austenitic steel and Inconel - 182 alloy to study the behavior of DMJs with constraints by using linear elastic fracture mechanics (LEFM) principles. Studies on DMSENB specimens are conducted with respect to (i) dissimilar metal joint width (DMJW) (geometrical constraints) (5 mm, 10 mm, 20 mm, 30 mm and 50 mm) (ii) strength mismatch (material constraints) and (iii) crack lengths (16 mm, 20 mm and 24 mm) to study the DMJ behavior. From the FEA investigation, it is observed that (i) SIF increases with increase of crack length and DMJWs (ii) significant constraint effect (geometry, crack tip and strength mismatch) is observed for DMJWs of 5 mm and 10 mm (iii) stress distribution at the interfaces of DMSENB specimen exhibits clear indication of strength mismatch (iv) 3-D FEA yields realistic behavior (v) constraint effect is found to be significant if DMJW is less than 20 mm and the ratio of specimen length to the DMJW is greater than 7.4.

• 한국의류학회지
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• 제20권3호
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• pp.519-526
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• 1996

To investigate the relationship between plane and side drape coefficient, the drape tester designed in which coordinate of projected outline of draped specimen could be recorded. By using this drape tester, the three dimensional shape, plane and side drape coefficient were obtained from coordinate of plane projected shape, and furthermore examined the tendency in changes of drape coefficient in terms of diameter of specimen, deflection angle, and bending rigidity. The side drape coefficients were constant regardless of changes in diameter of specimen. The plane drape coefficients, however, made a little difference according to changes in diameter of specimen. The experimental drape coefficient agreed well with the theoretical drape coefficient according to deflection angle. In the meanwhile, when the plane drape coefficients were regressed with the side drape coefficents, regression equation was $y=0.375x-0.002x^2+6.9\times10^{-5}x^3$. When the $\overline{\theta_s}$ is mean of deflection angle of selected points which have the longest and shortest distance from center point in the node, the theoretical drape coefficient calculated from $\overline{\theta_s}$ has high correlation with experimental drape coefficient. The plane and side drape coefficient changed linearly with increasing the bending length, $\sqrt[3]{EI/w}$.