• 제목/요약/키워드: Distribution amplitude

검색결과 478건 처리시간 0.047초

AE 진폭분포를 이용한 고장력강의 파괴특성평가 (Evaluation of Fracture Behavior of High Tension Steel by AE Amplitude Distribution)

  • 서정원;석창성;김영진;박지우
    • 한국정밀공학회지
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    • 제16권5호통권98호
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    • pp.175-185
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    • 1999
  • Acoustic emission(AE) measurement was carried out to evaluate the fracture behavior of high tension steel. Fracture toughness $K_{AE}$ could be determined reasonably by using the load value corresponding to an abrupt change of the accumulated AE counts AE emitted from the test specimens. AE characteristics of the base metal, the weld metal and the heat-affected zone could be distinguished using a constant value b which represented the AE amplitude distribution, Consequently the structure integrity can be evaluated by variation of the constant b at the load level. In addition it was found that AE signals due to crack growth have high amplitude but low rise time and duration.

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대퇴부 모델에서의 초음파 압력분포에 관한 유한요소 해석 (Finite Element Analysis of Pressure Distribution by Ultrasound in Human Thigh Model)

  • 최호선
    • 정보학연구
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    • 제8권1호
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    • pp.43-50
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    • 2005
  • Quantitative analysis for distribution of penetrating ultrasound in vivo is very important to determine the treatment region and method. In this paper, we constructed a simplified 2-D femoral region model that consists of skin-fat-muscle-bone layered system, and simulated the pressure distribution in the model in case of applying ultrasound using Finite Element Method(FEM). The ultrasound used in the simulation was assumed to be pulse wave and the pressure distribution was analyzed during only one period of pulse wave. In order to find the penetration depth, amplitude of pressure and sphere that ultrasound reaches in the model, we performed the simulation with varying the applied frequency, transducer size and amplitude of transducer's output. The result showed that applied frequency is inversely proportional to the penetration depth and amplitude of pressure but the amplitude of transducer's output is proportional to the amplitude of pressure in the model. Also, the sphere that ultrasound reaches was widened and the amplitude of pressure became larger as the transducer size became larger. This results were similar to that obtained from the previous model consisting of fat-muscle-bone layered system, but we observed that the pressure of ultrasound is decreased due to the decrements of pressure by the absorption coefficient of skin and the interference that depends on the reflection of ultrasound caused by the difference of acoustic impedance of skin and fat. Finally, we can infer that the model proposed in this study is closer to the realistic model than the previous ones. It shows that the results obtained from this study can be useful in designing the ultrasound treatment instrument or in setting up the treatment plan.

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SFCFOS Uniform and Chebyshev Amplitude Distribution Linear Array Antenna for K-Band Applications

  • Kothapudi, Venkata Kishore;Kumar, Vijay
    • Journal of electromagnetic engineering and science
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    • 제19권1호
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    • pp.64-70
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    • 2019
  • In this study, a compact series-fed center-fed open-stub (SFCFOS) linear array antenna for K-band applications is presented. The antenna is composed of a single-line 10-element linear array. A symmetrical Chebyshev amplitude distribution (CAD) is used to obtain a low sidelobe characteristic against a uniform amplitude distribution (UAD). The amplitude is controlled by varying the width of the microstrip patch elements, and open-ended stubs are arranged next to the last antenna element to use the energy of the radiating signal more effectively. We insert a series-fed stub between two patches and obtain a low mutual coupling for a 4.28-mm center-to-center spacing ($0.7{\lambda}$ at 21 GHz). A prototype of the antenna is fabricated and tested. The overall size of the uniform linear array is $7.04{\times}1.05{\times}0.0563{\lambda}_g^3$ and that of the Chebyshev linear array is $9.92{\times}1.48{\times}0.0793{\lambda}_g^3$. The UAD array yields a ${\mid}S_{11}{\mid}$ < -10 dB bandwidth of 1.33% (20.912-21.192 GHz) and 1.45% (20.89-21.196 GHz) for the CAD. The uniform array design gives a -23 dB return loss, and the Chebyshev array achieves a -30.68 dB return loss at the center frequency with gains of 15.3 dBi and 17 dBi, respectively. The simulated and measured results are in good agreement.

일정 및 변동하중하의 레일강의 피로특성 (Fatigue Properties of Rail Steel Under Constant Amplitude Loading and Variable Amplitude Loading)

  • 김철수;김정규
    • 대한기계학회논문집A
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    • 제25권4호
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    • pp.654-661
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    • 2001
  • In this study, fatigue growth behavior of the transverse crack, which was the most dangerous damage among the various types of rail defects, was investigated using the notched keyhole specimen under constant amplitude loadings. Fatigue limit of smooth specimen in rail steel at R=0 was 110MPa, and the fatigue crack initiation life in the region of the low stress amplitude (ie. long life) occupied the major portion of the total fatigue life. The fatigue strength under variable amplitude loading was converted to the equivalent fatigue strength based upon. Miners rule, which was estimated approximately 9% lower than that under constant amplitude loading. Also, in the low ΔK(sub)rms region ($\leq$21MPa√m), fatigue crack growth rate (da/dN) under constant amplitude loading was higher than that under variable amplitude loading, whereas the tendency was reversed in the high ΔK(sub)rms region. It is believed that this behavior is due to the transition of fracture appearance.

음향방출법에 의한 SM45C 고주파 열처리 강의 기계적 특성 평가 (The Estimation of Mechanical Properties of the High Frequency Induction Hardening SM45C Steel by Acoustic Emission)

  • 이장규;김봉각
    • 대한안전경영과학회:학술대회논문집
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    • 대한안전경영과학회 2009년도 추계학술대회
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    • pp.471-481
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    • 2009
  • This study is deal with the high frequency induction hardening (HF at $850^{\circ}C$, 120kHz & 50kW condition) SM45C steel. (1) The HF specimen which was tempered at $150^{\circ}C$, did not appear any tempering effect. A brittle fracture occurred at rounded area of the tensile specimen. AE amplitude distribution showed between 45~60dB. (2) The HF specimen which was tempered at $300^{\circ}C$, slip and fracture occurred at the hole area of the tensile specimen. As it passes the yield point, the AE energy increased intermittently and AE amplitude distribution showed between 70~85dB. In addition, after the maximum tensile load, it showed high amplitude and energy distribution. The AE amplitude showed between 45~70dB. (3) The HF specimen which was tempered at $450^{\circ}C$, a brittle fracture occurred as if it is torn in the direction of $45^{\circ}$ on parallel area over the both sides of the tensile specimen, which led to several peak to be appeared in AE energy. It was found that the AE amplitude was relatively low and the AE energy was high.

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음향방출법에 의한 SM45C 고주파 열처리 강의 기계적 특성 평가 (The Analysis of Mechanical Properties of the High Frequency Induction Hardening SM45C Steel by Acoustic Emission)

  • 이장규
    • 한국기계기술학회지
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    • 제13권2호
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    • pp.93-100
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    • 2011
  • This study deals with the high frequency induction hardening (HF at $850^{\circ}C$, 120kHz & 50kW condition) SM45C steel. (1) The HF specimen, which was tempered at $150^{\circ}C$, did not show any tempering effect. A brittle fracture occurred at rounded area of the tensile specimen. AE (acoustic emission) amplitude distribution showed between 45dB and 60dB. (2) A slip and fracture occurred at the hole area of the HF specimen which was tempered at $300^{\circ}C$. As they pass the yield point, the AE energy is increased intermittently and AE amplitude distribution exists between 70dB and 85dB. In addition, after imposing the maximum tensile load, AE signals showed high amplitude and energy distribution. The AE amplitude showed between 45dB and 70dB. (3) A brittle fracture occurred at HF specimen which was tempered at $450^{\circ}C$ as if it is torn in the direction of $45^{\circ}$ on parallel area over the both sides of the tensile specimen, which lead to several peak appeared in AE energy. It was found that the AE amplitude was relatively low and the AE energy was high.

잡음에 강인한 음성인식을 위한 Generalized Gamma 분포기반과 Spectral Gain Floor를 결합한 음성향상기법 (Speech Estimators Based on Generalized Gamma Distribution and Spectral Gain Floor Applied to an Automatic Speech Recognition)

  • 김형국;신동;이진호
    • 한국ITS학회 논문지
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    • 제8권3호
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    • pp.64-70
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    • 2009
  • 본 논문은 잡음에 강인한 음성인식 성능을 획득하기 위해 generalized Gamma 분포기반의 음성향상 기법을 제안한다. 우수한 음성향상을 위해서 제안된 방식에서는 generalized Gamma분포와 spectral gain floor를 이용한 음성추적 기법에 스펙트럼 최소잡음성분에 의한 희귀적인 평균 스펙트럼 값으로부터 유도되는 잡음추정을 결합하여 음질을 향상시켜 음성인식에 적용하였다. Spectral component, spectral amplitude 그리고 log spectral amplitude에 기반하여 제안된 음성향상 기법을 잡음환경에서의 음성인식에 적용하여 그 성능을 측정하였다.

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일정진폭하중하의 피로균열전파의 통계적 특성 (A Statistical Analysis of Fatigue Crack Growth under Constant-Amplitude Loads)

  • 정현철;임영규;김선진
    • 한국해양공학회:학술대회논문집
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    • 한국해양공학회 2002년도 춘계학술대회 논문집
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    • pp.104-109
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    • 2002
  • In this paper, a statistical analysis of fatigue crack growth behavior under constant amplitude loads has been carried out. Fatigue crack growth tests were conducted on sixteen pre-cracked compact tension (CT) specimens of the pressure vessel (SPV50) steel in controlled identical load and environmental conditions. The assessment of the statistical distribution of fatigue crack growth experimental data obtained from SPV50 steel was studied and also the correlation of the parameter C and m in the Paris-Erdogan law was discussed. The probability distribution function of fatigue crack growth life seems to follow the 3-parameter Weibull. The fatigue crack growth rate seems to follow the 3-parameter Weibull and the log-normal distribution. The coefficient of variation (COV) of fatigue crack growth life was observed to decrease as the crack grows. A strong negative linear correlation exists between the coefficient C and the exponent m in Paris model. Fatigue crack growth rate data shows a normal distribution for both m and logC.

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Stiles - Crawford 효과가 결상에 미치는 영향 (The Influence of the Stiles - Crawford Effect on the Image)

  • 박성종
    • 한국안광학회지
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    • 제5권2호
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    • pp.175-180
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    • 2000
  • 입사 광량과 동공 직경의 관계는 Stiles-Crawford 효과에 의해서 동의 중앙에서 가장자리로 갈수록 입사 광량이 감소하는 경향을 갖는다. 본 논문에서는 여러 가지 영향에 의하여 임의의 방향으로 입사광의 실수 진폭 분포가 편위되었을 때 상면에서의 착락원 형태 변화를 조사하였다. 입사광의 실수 진폭 분포가 편위되지 않았을 때는 상면에서 착락원은 원형 대칭성을 나타냈지만 입사광의 실수 진폭 분포가 편위되었을 때는 상면에서의 착락원 형태는 비대칭의 타원 형태로 변화되었다. 또한 입사광의 실수 진폭 분포의 편위 방향과 상면에서 착락원의 장축 방향이 일치하였으며 입사광의 실수 진폭 분포의 편위 방향이 서로 반대 방향(${\Delta}{\phi}$${\Delta}{\phi}+{\pi}$)일지라도 상면에서의 강도 분포와 착락원의 형태는 동일하게 나타나 상질에 동일한 영향을 미침을 알 수 있었다.

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잔류수차가 있는 유한 가우스 동의 회절진폭 분포 (Diffraction Amplitude Distribution of Finite Gaussian Pupil with Residual Aberrations)

  • 송영란;이민희;이상수
    • 한국광학회지
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    • 제9권3호
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    • pp.142-145
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    • 1998
  • 가우스 함수로 진폭변조한 우인한 가우스 동에 작은 Seidel 제 1차 수차가 있을때의 회절진폭 분포를 해석적으로 구하였다. 즉, 무수차 가우스 동의 회절진폭 분포와 수차에 의한 회절효과의 함으로 구하였다. 각 수차의 표현은 파면수차함수의 환산좌표를 공간각주파구로 대치하여, 수차에 의한 회절상을 되풀이 공식(recurrence formula)으로 구하였다.

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