• Title/Summary/Keyword: 크립 특성

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High Accurate Creep Compensation of the Loadcell using the Strain Gauge (스트레인 게이지식 로드셀의 고정밀 크립보상)

  • Seo, Hae-Jun;Jung, Haing-Sup;Ryu, Gi-Ju;Cho, Tae-Won
    • Journal of IKEEE
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    • v.16 no.1
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    • pp.34-44
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    • 2012
  • This paper proposes a practical compensation method by using digital signal processing over the creep error which is representative in strain gauge loadcell. The signal compensation method carry out the simulation by deciding compensation constant (time constant) and coefficient measuring the loadcell output response. Then, compensation constant and coefficient are stored on the microprocessor. By using calculated on microprocessor creep error compensation values, weighting value is showed as a digital signal by reducing error values measured through output signals of loadcell. In addition, we apply error compensation method in order to have a dedicated software for loadcell electronic scale. This technique is useful because it has great influence on error rate reduction that has been produced by conventional electronic scales (0.03%). As a result our technique gives better accuracy (0.01%~0.003%) as what is given by digital electronic scale, while it has less complex operation processing.

A Toolkit for Constructing Virtual Instruments to Augment User Interactions in Virtual Environments (가상환경에서의 사용자 인터랙션을 지원하기 위한 가상 계측 단말기 스크립팅 툴킷)

  • Kim, Seok-Hwan;Chung, Da-Young;Cho, Yong-Joo
    • Proceedings of the Korea Information Processing Society Conference
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    • 2005.05a
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    • pp.155-158
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    • 2005
  • 본 논문은 가상 계측 단말기 (Virtual Instrument) 제작을 위해 만들어진 가상 계기 스크립팅 툴킷 (VIST)의 구현과 설계를 보여준다. 가상 계기는 가상현실에서 휴대용 컴퓨터에 탑재되어 실행되는 응용 프로그램들을 일컫는다. 가상 계기는 가상환경의 특성에 대해 조사하고 보여주는 데 사용되고 가상환경에서 사용자와 가상현실 시스템의 상호 작용을 개선시키는 데에도 사용할 수 있다. VIST 는 가상 계기를 구성하는 컴포넌트를 쉽게 생성하도록 해주고, 그 컴포넌트들을 사용하여 프로토타입을 빠르게 제작할 수 있게 한다. 또한 가상환경 안에서 가상환경의 특성과 가상객체의 속성을 보여 주고 그것들을 쉽게 파악하도록 하는 메커니즘을 제공한다. 본 논문은 VIST 의 설계 원리와 구조를 기술하고, 실제로 어떻게 가상 계측 단말기를 제작하였는지 보여준다.

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Creep Behavior of a PZT Wafer Under Tensile Stress: Experiments and Modeling (인장하중을 받을 때 PZT 웨이퍼의 크립 거동: 실험과 모델링)

  • Kim, Sang-Joo;Lee, Chang-Hoan
    • Transactions of the Korean Society of Mechanical Engineers A
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    • v.34 no.1
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    • pp.61-65
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    • 2010
  • A commercially available soft PZT wafer that is poled in thickness direction is subjected to longitudinal tensile stress loading in both short and open-circuit conditions. Variations of electric displacement in thickness direction and in-plane strains are measured over time during the loading. Different material responses in the two electrical boundary conditions are explained by the effects of piezoelectrically produced internal electric field on linear material moduli and domain switching mechanisms. Finally, a free energy model of normal distribution is introduced to explain the observed creep behavior, and its predictions are compared with experimental observations.

Creep Characteristics of Unconsolidated Shale (미고결 셰일의 크립 특성)

  • Chang, Chan-Dong;Zoback, Mark
    • 한국지구물리탐사학회:학술대회논문집
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    • 2006.06a
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    • pp.195-200
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    • 2006
  • Laboratory creep experiments show that compaction of unconsolidated shale is an irrecoverable process caused by viscous time-dependent deformation. Using Perzyna's viscoplasticity framework combined with the modified Cam-clay theory, we found the constitutive equation expressed in the form of strain rate as a power law function of the ratio between the sizes of dynamic and static yield surfaces. We derived the volumetric creep strain at a constant hydrostatic pressure level as a logarithmic function of time, which is in good agreement with experimental results. The determined material constants indicate that the yield stress of the shale increases by 6% as strain rate rises by an order of magnitude. This demonstrates that the laboratory-based prediction of yield stress (and porosity) may result in a significant error in estimating the properties in situ.

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The Characteristics of Thermoluminescence from $^{137}$ Cs Irradiated Beta-Eucryptite ($^{137}$ Cs으로 조사된 베타-유크립타이트의 열자극발광 특성)

  • 김태규;이병용;박영우;추성실;황정남
    • Progress in Medical Physics
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    • v.3 no.2
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    • pp.23-31
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    • 1992
  • The thermally stimulated luminecence (Thermoluminescence:TL) of manufactured beta-eucryptite was studied for dose range of 200cGy-20000Gy. The TL spectrum from cesium irradiated beta-eucryptite was measured over the temperature range of 300K to 600K. The linearity of TL intensity vs irradiation dose is valid up to 50Gy and beyond higher dose supralinearity and saturation come out. At the dose of 2000Gy, the net number of supralinearity is maximum. The net amount of supralinearity form newly formed trapping center by photon irradiation and totally calculated TL intensity are accord with the experimental results except for the 50Gy range that supralinearity appears.

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Effect of HAZ Softening Zone on Creep Rupture Properties of 1.0Cr-1.0Mo-0.25V Turbine Rotor Steels - Part I : Creep Rupture Life- (1.0Cr-1.0Mo-0.25V 터어빈 로터강의 열영향부 연화층이 크립 파단 특성에 미치는 영향 -Part I : 크립 파단 수명 -)

  • ;Indacochea, J. E.
    • Journal of Welding and Joining
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    • v.15 no.1
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    • pp.92-100
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    • 1997
  • Weld repair of ASTM A-470 class 8 high pressure (HP) steam turbine rotor steel has been performed to extend the service life of older fossil units. Microhardness measurements were conducted across the weldment from unaffected base metal (BM) to weld metal (WM). The hardness of the BM was VHN 253, however it dropped up to VHN 227 at the heat affected zone (HAZ) close to unaffected BM for multipass SAW. This area of hardness drop is called "siftening zone" and has a width of 0.5-0.6mm. During creep rupture test, failure occurred around the softening zone and rupture time was 772.4hr at 19Ksi (132 Mpa) and 593.deg. C. Multipass MIG and TIG welding have been employed to reduce the softening zone width. The softening zone width for MIG was 0.3-0.4mm and for TIG was zero-0.4mm depending on heat inputs. However creep rupture time was decreased as softening zone width reduced. Creep rupture time also showed a close relationship with heat inputs in TIG process. The higher heat input, the longer rupture time. Most failure occurred at intercritical HAZ (ICHAZ), however rupture location was shifted to coarse grained HAZ (CGHAZ) as heat input decreased. The rupture surface showed tearing and dimple which indicated transgranular fracture. fracture.

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A Study on the High Temperature Creep Crack Growth Properties for Steam Turbine Rotor Steel under Static and Cyclic Loading Condition (화력 발전용 고압 로터강의 정하중 및 변동하중하의 고온 크립 균열전파 특성에 관한 연구)

  • O, Se-Gyu;Jeong, Sun-Eok
    • Journal of Ocean Engineering and Technology
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    • v.5 no.2
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    • pp.207-207
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    • 1991
  • The crack length measurements by electrical potential(EP) method for 1% Cr-Mo-V and 12%Cr steel of 0.5T-CT specimen were performed at $500^{\circ}C, 600^{\circ}C 700^{\circ}C$, and an applicability of stress intensity factor($K_I$), net section stress($\sigma_{net}$), $C^*$-ingegral and $C_t$ parameter was studied to measure creep crack growth rate(da/dt) with side groove and without side groove under static and cyclic loading condition. The experimental result could be summarized as follows: 1) Crack measurement by EP method was available and coincided with the Johnson,s analytical equation. 2) da/dt by $K_I$ and $\sigma_{net}$ was not adequate because of the wide scatter band according to load and temperature, but $C^*$-integral, except for transition region, was adequate. 3) $C_t$ parameter showed the best fitted line through total creep region without relating with both temperature and load condition. 4) Under the cyclic loading condition, $C_t$ parameter was proper to extimate da/dt. And it was shown that da/dt for 1% Cr-Mo V steel under the static condition(R=1) was 1.16 times faster than the case under cyclic loading(R=0), and for 12% Cr steel, 1.43 times.