• 한국정밀공학회지
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• 제14권12호
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• pp.160-165
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• 1997

The instrumented Charpy impact test is generally used to evaluate the dynamic fracture toughnesses for varying engineering materials. However, the test is known to be difficult to evaluate the dynamic fracturetoughnesses for very brittle materials because of the small crack initiation load which may be engulfed by the inertia load of the instrumented tup. To evaluate the dynamic fracture toughnesses of very brittle materials, such as chalk or plaster,it is thus, necessary to develop a load sensitive instrumented tup. In this study, a polymer tup, which has very small Young's modulus comparing to one of the conventional steel tup, is used for the instrumented Charpy impact test, and a proper testing method to evaluate the dynamic fracture behavior of very brittle materials is developed. The results show that the developed method can measure rapidly changing loads from the moment of contact between the tup and the specimen to dynamic crack initiation of the very brittle materials.

• Ocean Systems Engineering
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• 제14권1호
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• pp.53-72
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• 2024

The interaction of the blade of surface-piercing propellers (SPPs) with the water/air surface is a physical phenomenon that is difficult to model mathematically, so that such propellers are usually designed using empirical approaches. In this paper, a newly developed mechanism for measuring the torque of SPPs in an open water circuit is presented. The mechanism includes a single-component load cell and a deformable torque sensor to detect the forces exerted on the propeller. Deformations in the sensor elements lead to changes in the strain gauge resistance, which are converted into voltage using a Wheatstone bridge. The amplified signal is then recorded by a 16-channel data recording system. The mechanism is calibrated using a 6-DoF calibration system and a Box-Behnken design, achieving 99% accuracy through multivariate regression and ANOVA. Finally, the results of performance tests on a 4-blade propeller were presented in the form of changes in the torque coefficient as a function of feed rate. The results show that the new mechanism is 8% more accurate than conventional empirical methods.

• 한국기계가공학회지
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• 제18권9호
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• pp.72-80
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• 2019

In this task, the tool dynamometer design and manufacture, and the Ansys S/W structural analysis program for tool attachment that satisfies the cutting force measurement requirements of the tool dynamometer system are used to determine the cutting force generated by metal cutting using 3-axis static structural analysis and the LabVIEW system. The cutting power in a cutting process using a milling tool for processing metals provides useful information for understanding the processing, optimization, tool status monitoring, and tool design. Thus, various methods of measuring cutting power have been proposed. The device consists of a strain-gauge-based sensor fitted to a new design force sensing element, which is then placed in a force reduction. The force-sensing element is designed as a symmetrical cross beam with four arms of a rectangular parallel line. Furthermore, data duplication is eliminated by the appropriate setting the strain gauge attachment position and the construction of a suitable Wheatstone full-bridge circuit. This device is intended for use with rotating spindles such as milling tools. Verification and machining tests were performed to determine the static and dynamic characteristics of the tool dynamometer. The verification tests were performed by analyzing the difference between strain data measured by weight and that derived by theoretical calculations. Processing test was performed by attaching a tool dynamometer to the MCT to analyze data generated by the measuring equipment during machining. To maintain high productivity and precision, the system monitors and suppresses process disturbances such as chatter vibration, imbalances, overload, collision, forced vibration due to tool failure, and excessive tool wear; additionally, a tool dynamometer with a high signal-to-noise ratio is provided.

• 대한기계학회논문집
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• 제8권2호
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• pp.154-161
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• 1984

본 연구에서는 고정밀 아날로그-디지탈 변환기와 마이크로 프로세서(micropr- ocessor) Intel 8085를 사용하여 비정상 아날로그(analog)신호를 왜곡이 없이 디지탈 량으로 직접 변환하여 자료처리하였다. 또한 비정상 열선법은 열선에 전류를 가하여 열선이 열원이며 동시에 온도계의 두 가지 역할을 하므로, 전기전도성이 있는 액체는 적합하지 못한 단점이 있다. 이를 해결하기 위하여 열선에 얇은 절록피복층을 입혀 전기전도성 액체의 열전도율을 측정할 수 있는 가능성에 대한 연구를 시도하였다.

• 대한기계학회논문집B
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• 제29권5호
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• pp.633-642
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• 2005

Nucleate pool boiling experiments for R11 under a constant wall temperature condition were carried out. A microscale heater array was used for the heating and the measurement of high temporal and spatial resolution by the Wheatstone bridge circuit. Very sensitive heat flow rate data were obtained by the control for the surface condition with high time resolution. The measured heat flow rate shows a discernable peak at the initial growth stage and reaches an almost constant value. In the thermal growth region, bubble shows a growth proportional to $t^{\frac{1}{5}}$. The bubble growth behavior is analyzed with a dimensionless parameter to compare with the previous results in the same scale. As the wall superheat increases, the departure diameter and the departure time increase, and the waiting time decreases. But the asymptotic growth rate is not affected by the wall superheat change. The effect of the wall superheat is resolved into the suggested growth equation. Dimensionless parameters of time and bubble radius characterize the thermal growth behavior well, irrespective of wall condition. The comparison between the result of this study and the previous results shows a good agreement at the thermal growth region. The quantitative analysis for the heat transfer mechanism is conducted with the measured heat flow rate behavior and the bubble growth behavior. The required heat flow rate for the volume change of the observed bubble is about twice as much as the instantaneous heat flow rate supplied from the wall.

• 대한기계학회논문집B
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• 제29권5호
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• pp.643-652
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• 2005

Saturated nucleate pool boiling experiments for binary mixtures, which are consisted of refrigerant R11 and R113, were performed with constant wall temperature condition. Results for binary mixtures were also compared with pure fluids. A microscale heater array and Wheatstone bridge circuits were used to maintain the constant temperature of the heating surface and to obtain heat flow rate measurements with high temporal and spatial resolutions. Bubble growth images were captured using a high speed CCD camera synchronized with the heat flow rate measurements. The departure time for binary mixtures was longer than that for pure fluids, and binary mixtures had a higher onset of nucleate boiling (ONB) temperature than pure fluids. In the asymptotic growth region, the bubble growth rate was proportional to a value between $t^{\frac{1}{6}}$ and $t^{\frac{1}{4}}$. The bubble growth behavior was analyzed to permit comparisons with binary mixtures and pure fluids at the same scale using dimensionless parameters. There was no discernable difference in the bubble growth behavior between binary mixtures and pure fluids for a given ONB temperature. And the departure radius and time were well predicted within a ${\pm}30{\%}$ error. The minimum heat transfer coefficient of binary mixtures occurred near the maximum ${\mid}y-x{\mid}$ value, and the average required heat flux during bubble growth did not depend on the mass fraction of R11 as more volatile component in binary mixtures. Finally, the results showed that for binary mixtures, a higher ONB temperature had the greatest effect on reducing the heat transfer coefficient.

• 대한기계학회논문집B
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• 제29권2호
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• pp.169-179
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• 2005

Nucleate boiling experiments on heating surface of constant wall temperature were performed using R113 for almost saturated pool boiling conditions. A microscale heater array and Wheatstone bridge circuits were used to maintain a constant wall temperature condition of heating surface and to measure the heat flow rate with high temporal and spatial resolutions. Bubble images during the bubble growth were taken as 5000 frames per second using a high-speed CCD camera synchronized with the heat flow rate measurements. The bubble growth behavior was analyzed using the new dimensionless parameters for each growth regions to permit comparisons with previous experimental results at the same scale. We found that the new dimensionless parameters can describe the whole growth region as initial and later (thermal) respectively. The comparisons showed good agreement in the initial and thermal growth regions. In the initial growth region including surface tension controlled, transition and inertia controlled regions as divided by Robinson and Judd, the bubble growth rate showed that the bubble radius was proportional to $t^{2/3}$ regardless of working fluids and heating conditions. And in the thermal growth region as also called asymptotic region, the bubble showed a growth rate that was proportional to $t^{1/5}$, also. Those growth rates were slower than the growth rates proposed in previous analytical analyses. The required heat flow rate for the volume change of the observed bubble was estimated to be larger than the heat flow rate measured at the wall. Heat, which is different from the instantaneous heat supplied through the heating wall, can be estimated as being transferred through the interface between bubble and liquid even with saturated pool condition. This phenomenon under a saturated pool condition needs to be analyzed and the data from this study can supply the good experimental data with the precise boundary condition (constant wall temperature).

• 한국기계가공학회지
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• 제17권4호
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• pp.97-103
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• 2018

Force is a crucial element to be measured in various industries, especially the machine tool industry. Mega units of force are required in fields such as the heavy and ship industries. Micro/nano units of force are required for microparticles. The detection of force generates a physical transformation due to the force imposed from the outside, atlrnd electrical voltage signals are obtained from the system. For the detection of force, an octagonal ring load cell based on circular ring theory is designed and produced. To design the octagonal strain ring, theoretical values with data from the ANSYS program are compared to determine the size of the octagonal strain ring. An octagonal strain ring of the chosen size is made with the SCM415 material. The strain gauges are attached to the octagonal strain ring, designed to construct a full Wheatstone bridge. The LabVIEW program is used to measure the data, and strain values are found. With the octagonal ring load cell completed in this way, experiments are conducted by imposing forces on the tangential axis and radial axis. Experiments are performed to verify if the octagonal ring load cell conducts measurements properly, and theoretical values are analyzed to find any differences. The data will later be used in further research to develop a machine-tool dynamometer.

• 융합신호처리학회논문지
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• 제9권2호
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• pp.146-153
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• 2008

본 연구에서는 $0.8{\mu}m$ 아날로그 혼합 CMOS 기술에 의한 2단 연산 증폭기를 가진 집적화된 습도센서 시스템을 설계 및 제작하였다. 시스템은 28핀 및 $2mm{\times}4mm$의 크기를 가졌으며, 휘스톤 브릿지형 습도센서, 저항형 습도센서, 온도센서 및 신호의 증폭과 처리를 위한 연산증폭기를 단일 칩에 구성하였다. 기존의 CMOS 공정에 트렌치형의 감지 영역을 형성하기 위해 폴리-질화 에치 스탑 공정을 시도하였다. 이러한 수정된 기술은 CMOS 소자의 특성에 영향을 주지 않았고, 표준 공정으로 동일 칩 상에 센서와 시스템을 제작할 수 있도록 하였다. 연산증폭기는 이득 폭이 5.46 MHz 이상, 슬루율이 10 V/uS 이상으로 센서를 동작하기에 안정된 특성을 보였다. N형 습도감지 전계효과 트랜지스터의 드레인 전류는 상대습도가 10%에서 70%로 변화할 때 0.54mA에서 0.68 mA로 변화하였다.

• 한국자기학회지
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• 제14권3호
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• pp.109-113
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• 2004

구형파의 디지털 자료를 전송하기에 적합한 구조의 휘트스톤 브리지 형태로 GMR 아이솔레이터를 모델링하고, 여기에서 입력전류에 대한 출력전압특성을 시간영역에서 조사하였다. GMR 아이솔레이터를 자기적 부분과 전기적 부분으로 나누고 제조된 스핀벨브 소자의 측정결과를 대입하여 출력전압을 구할 수 있는 모델링 순서도를 설정하였다. 자기적 모델링으로는 평판코일의 3차핀 모델을 FEM방법으로 해석하여 입력전류에 의해 생성되는 자장의 세기를 구하였다. 전기적 모델링을 위해 평판코일의 저항과 인덕턴스 그리고 정전용량을 계산하여, 시간영역에서 입력전류파형과 이에 따른 자기장파형을 구하였다. 마지막으로 스핀밸브의 MR-H 측정곡선과 평판코일에서 발생된 자장의 세기를 조합하여 아이솔레이터의 출력전압파형을 계산하였다. 여기에서 GMR 아이솔레이터의 입력전류파형에 비해 코일전류파형의 진폭이 최고 100％ 정도 증가하거나 90 ％ 정도 감소하고, 주기의 10％ 정도에 해당하는 지연이 발생하였다. 그럼에도 출력전압 파형은 스핀밸브의 히스테리시스 특성 때문에 400 Mbit/s 이상의 전송속도에서 입력전류파형과 비슷하게 복원되어 전달될 수 있음을 예측할 수 있었다.