• 한국콘텐츠학회논문지
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• 제12권9호
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• pp.389-395
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• 2012

본 연구는 전통적인 태권도 정권지르기 기술인 끊어지르기를 어깨를 앞으로 밀어 넣는 밀어지르기와 비교하여 최대 충격력과 주먹의 최고 속도 및 최고속도가 발현된 지점에 대해 규명하였다. 피험자는 남성 태권도 유단자 7명으로 구성하였다. 최대 충격력은 PS2142 force platform[10]을 수직으로 세워 측정하였고, 주먹의 최고속도는 PS2103A motion sensor[12]를 이용하였다. 측정 데이터는 PASCO사에서 제공한 data studio를 통해 수집되었고, SAS 9.1 패키지를 활용해 지르기 방식에 따른 t-test를 실시하였다. 본 실험절차를 통해 나타난 결론은 다음과 같다. 첫째, 최고 충격력에 있어서는 끊어지르기가 밀어지르기 보다 유의한 수준에서(p<.01) 더 높은 것으로 나타났다. 둘째, 주먹의 최고속도는 밀어지르기가 끊어지르기 보다 유의하게(p<.01) 빠른 것으로 제시되었다. 셋째, 최고속도의 발현지점에 있어서는 끊어지르기가 주먹 전체길이의 69.1%, 밀어지르기는 76.6%로 나타났고, 통계적으로 유의한(p<.001) 차이가 있었다.

• International Journal of Fluid Machinery and Systems
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• 제3권2호
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• pp.113-121
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• 2010

LES(Large Eddy Simulation) with a cavitation model was performed to calculate an unsteady flow for a mixed flow pump with a closed type impeller. First, the comparison between the numerical and experimental results was done to evaluate a computational accuracy. Second, the torque acting on the blade was calculated by simulation to investigate how the cavitation caused the fluctuation of torque. The absolute pressure around the leading edge on the suction side of blade surface had positive impulsive peaks in both the numerical and experimental results. The simulation showed that those peaks were caused by the cavitaion which contracted and vanished around the leading edge. The absolute pressure was predicted by simulation with -10% error. The absolute pressure around the trailing edge on the suction side of blade surface had no impulsive peaks in both the numerical and experimental results, because the absolute pressure was 100 times higher than the saturated vapor pressure. The simulation results showed that the cavitation was generated around the throat, then contracted and finally vanished. The simulated pump had five throats and cavitation behaviors such as contraction and vanishing around five throats were different from each other. For instance, the cavitations around those five throats were not vanished at the same time. When the cavitation was contracted and finally vanished, the absolute pressure on the blade surface was increased. When the cavitation was contracted around the throat located on the pressure side of blade surface, the pressure became high on the pressure side of blade surface. It caused the 1.4 times higher impulsive peak in the torque than the averaged value. On the other hand, when the cavitation was contracted around the throat located on the suction side of blade surface, the pressure became high on the suction side of blade surface. It caused the 0.4 times lower impulsive peak in the torque than the averaged value. The cavitation around the throat caused the large fluctuation in torque acting on the blade.

• 한국소음진동공학회:학술대회논문집
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• 한국소음진동공학회 2006년도 춘계학술대회논문집
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• pp.1260-1264
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• 2006

Shock-type vibrations are usually experienced in vehicles excited by impulsive forces. Fifteen subjects used magnitude estimation to judge the discomfort of vertical shock-type vibration generated on a rigid seat. The shocks had different frequencies and magnitudes and were produced from the response of a 1 degree-of-freedom model to a half-sine force input. The magnitudes of the shocks, expressed in terms of both peak-to-peak value and un-weighted vibration dose values, VDVs, were correlated with magnitude estimates of the discomfort. In this study, equivalent comfort contour of shock-type vibration were obtained. From the contour, it was investigated that shock-type vibration at frequency below 0.8 Hz and between 4.0 Hz and 10.0 Hz is highly sensitive to the discomfort than at other frequencies.

• 한국구조물진단유지관리공학회 논문집
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• 제9권1호
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• pp.189-196
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• 2005

임펄스 비와 하중최대치의 비로 작성된 손상곡선을 이용하여 충격하중의 임펄스와 하중의 크기가 구조물의 거동에 미치는 영향을 분석하였다. 단기에 종료하는 충격하중의 경우 관성력의 영향으로 하중의 크기보다는 임펄스가 구조물 손상에 주요변수가 되며, 관성력을 극복할 충분한 시간을 갖는 장기하중이 작용하는 경우에는 임펄스보다는 하중의 크기가 구조물 손상에 주요변수가 된다. 지반충격에 의한 구조물의 손상은 단기인 경우에는 지반의 최대입자속도가 그러나 장기인 경우에는 최대입자가속도가 손상의 주요 변수가 된다.

• 한국운동역학회지
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• 제27권3호
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• pp.181-187
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• 2017

Objective: The aim of the study was to compare & analyze on the variations of ground reaction force during ascending and descending of bus stair. Method: Simulated wooden stair of bus (raiser: 37.66 cm, width: 109 cm, tread: 29 cm) and GRF system (AMTI-OR-7/ AMTI., USA) was set up within experimental room. Adult female (n=8) performed ascending & descending of simulated bus stair, and variables analyzed consisted of TT (transfer-time), PVF (peak vertical force), LR (loading rate), DR (decay rate), CV (coefficient of variation) and AI (asymmetry index). Sample data from GRF cut off at 1,000 Hz. Results: TT showed shortest variation at phase 1 during descending, but longest variation at phase 1 during ascending of stair. PVF19 (Fz2, 100%) showed large pattern during descending than that of ascending, but rather showed small pattern during ascending of stair in case of PVF2 (Fz4). LR showed larger pattern during descending than that of ascending, but rather during ascending of stair in case of DR. Variation of CV (%) did not show difference between LR and DR, but showed higher possible occurrence of variation during descending of stair. Also AI (%) showed higher index during ascending than that of descending of stair. Conclusion: Because introduction of lowered bus stair has various realistic problems, if lined up at designated bus stopage exactly, rather can solve problems of inconvenience, reduce impulsive force and secure a stability of COG during ascending & descending of stair.

• 한국소음진동공학회논문집
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• 제16권6호
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• pp.658-664
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• 2006

Shock vibrations are usually experienced in vehicles excited by impulsive input, such as bumps. The frequency weighting functions of the current standards in ISO 2631 and BS 6841 are to help objectively predict the amount of discomfort of stationary vibration. This experimental study was designed to develop frequency weighting shape for shock vibration having various fundamental frequencies from 0.5 to 16Hz. The specks were produced from the response of single. degree-of-freedom model to a half-sine force input. Fifteen subjects used the magnitude estimation method to judge the discomfort of vertical shock vibration generated on the rigid seat mounted on the simulator. The magnitudes of the shocks, expressed in terms of both peak-to-peak value and un-weighted vibration dose values (VDVs) , were correlated with magnitude estimates of the discomfort. The frequency weighting shapes from the correlation were developed and investigated having nonlinearity due to the magnitude of the shock.

• 지질공학
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• 제23권1호
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• pp.29-36
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• 2013

스크린 공막힘에 의하여 채수량이 감소된 지하수 관정은 여러 방법을 통하여 재생시켜주면 지하수 채수량을 개선시켜 관정의 수명을 연장할 수 있다. 본 논문에서는 화약이나 압축 유체를 사용하는 기존의 공막힘 재생기술을 대신할 수 있는 고전압 펄스 방전에 의한 지하수 관정 스크린 공막힘의 재생법에 대하여 연구하였다. 본 기술은 수중에 삽입된 전극에 순간적으로 고전압의 전기에너지를 주입하여 이 때 전극 사이에서 발생하는 고온, 고압의 플라즈마의 팽창력에 의하여 발생하는 수중 충격파를 이용하는 기술로, 기존 기술 대비 취급이 용이하며 구조가 간단하고 충격압의 크기 조절이 용이하다는 장점을 갖는다. 본 연구에서는 축전기 방전형 펄스 발생장치를 사용하여 약 200 J의 전기에너지를 수중에 삽입된 전극에 순간적으로 주입함으로써 전극으로부터 6 cm 떨어진 곳에서 약 10.7MPa의 수중 충격압을 얻었다. 이 충격압의 크기는 축전기의 충전 전압을 바꿔줌으로써 손쉽게 조절이 가능하였으며, 다양한 전압에서의 실험을 통하여 방전 전류의 첨두치와 선형적인 관계를 갖고 있음을 알았다. 또한 지하수 관정에 사용되는 스크린과 유사한 시료에 대한 모의실험을 통하여 이 기술을 이용한 지하수 관정의 세척 가능성을 확인하였다.

• Structural Engineering and Mechanics
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• 제50권5호
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• pp.589-603
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• 2014

Expressions for determining the value of the impact force as reported in the literature and incorporated into code provisions are essentially quasi-static forces for emulating deflection. Quasi-static forces are not to be confused with contact force which is generated in the vicinity of the point of contact between the impactor and target, and contact force is responsible for damage featuring perforation and denting. The distinction between the two types of forces in the context of impact actions is not widely understood and few guidelines have been developed for their estimation. The value of the contact force can be many times higher than that of the quasi-static force and lasts for a matter of a few milli-seconds whereas the deflection of the target can evolve over a much longer time span. The stiffer the impactor the shorter the period of time to deliver the impulsive action onto the target and consequently the higher the peak value of the contact force. This phenomenon is not taken into account by any contemporary codified method of modelling impact actions which are mostly based on the considerations of momentum and energy principles. Computer software such as LS-DYNA has the capability of predicting contact force but the dynamic stiffness parameters of the impactor material which is required for input into the program has not been documented for debris materials. The alternative, direct, approach for an accurate evaluation of the damage potential of an impact scenario is by physical experimentation. However, it can be difficult to extrapolate observations from laboratory testings to behaviour in real scenarios when the underlying principles have not been established. Contact force is also difficult to measure. Thus, the amount of useful information that can be retrieved from isolated impact experiments to guide design and to quantify risk is very limited. In this paper, practical methods for estimating the amount of contact force that can be generated by the impact of a fallen debris object are introduced along with the governing principles. An experimental-calibration procedure forming part of the assessment procedure has also been verified.