• 제목/요약/키워드: $A_0$ Mode

검색결과 4,019건 처리시간 0.035초

Combination of Quantitative Parameters of Shear Wave Elastography and Superb Microvascular Imaging to Evaluate Breast Masses

  • Eun Ji Lee;Yun-Woo Chang
    • Korean Journal of Radiology
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    • 제21권9호
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    • pp.1045-1054
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    • 2020
  • Objective: This study aimed to evaluate the diagnostic value of combining the quantitative parameters of shear wave elastography (SWE) and superb microvascular imaging (SMI) to breast ultrasound (US) to differentiate between benign and malignant breast masses. Materials and Methods: A total of 200 pathologically confirmed breast lesions in 192 patients were retrospectively reviewed using breast US with B-mode imaging, SWE, and SMI. Breast masses were assessed based on the breast imaging reporting and data system (BI-RADS) and quantitative parameters using the maximum elasticity (Emax) and ratio (Eratio) in SWE and the vascular index in SMI (SMIVI). The area under the receiver operating characteristic curve (AUC) value, sensitivity, specificity, accuracy, negative predictive value, and positive predictive value of B-mode alone versus the combination of B-mode US with SWE or SMI of both parameters in differentiating between benign and malignant breast masses was compared, respectively. Hypothetical performances of selective downgrading of BI-RADS category 4a (set 1) and both upgrading of category 3 and downgrading of category 4a (set 2) were calculated. Results: Emax with a cutoff value of 86.45 kPa had the highest AUC value compared to Eratio of 3.57 or SMIVI of 3.35%. In set 1, the combination of B-mode with Emax or SMIVI had a significantly higher AUC value (0.829 and 0.778, respectively) than B-mode alone (0.719) (p < 0.001 and p = 0.047, respectively). B-mode US with the addition of Emax, Eratio, and SMIVI had the best diagnostic performance of AUC value (0.849). The accuracy and specificity increased significantly from 68.0% to 84.0% (p < 0.001) and from 46.1% to 79.1% (p < 0.001), respectively, and the sensitivity decreased from 97.6% to 90.6% without statistical loss (p = 0.199). Conclusion: Combining all quantitative values of SWE and SMI with B-mode US improved the diagnostic performance in differentiating between benign and malignant breast lesions.

응력비 변화에 따른 혼합모드 피로균열 전파거동 (The Mixed Mode fatigue Crack Propagation Behavior with the Variation of Stress Ratio)

  • 송삼홍;최지훈;이정무
    • 대한기계학회논문집A
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    • 제26권11호
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    • pp.2287-2296
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    • 2002
  • Most cracks in the structure occur under mixed mode loading and those fatigue crack propagation behavior heavily depends on the stress ratio. So, it is necessary to study the fatigue behavior under mixed mode loading as the stress ratio changes. In this paper, the fatigue crack propagation behavior was respectively investigated at stress ratio 0.1, 0.3, 0.5, 0.7 and we changed the loading application angle into 0$^{\circ}$, 30$^{\circ}$, 60$^{\circ}$ to apply various loading mode. The mode I and II stress intensity factor of CTS specimen used in this study was calculated by the displacement extrapolation method using FEM (ABAQUS). Using both the experiment and FEM analysis, we have concluded the relationship between crack propagation rate and stress intensity factor range at each loading mode due to the variation of stress ratio. Also, when the crack propagated under given stress ratio and loading mode condition, we have concluded the dominant factors of the crack propagation rate at each case.

가상 탐지자 배열 모델을 이용한 직사각형 판에서 A0 램파 모드 시간반전과정 모사 (Simulating a Time Reversal Process for A0 Lamb Wave Mode on a Rectangular Plate Using a Virtual Sensor Array Model)

  • 박현우
    • 한국소음진동공학회논문집
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    • 제20권5호
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    • pp.460-469
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    • 2010
  • This paper presents the analysis of a time reversal process for $A_0$ Lamb wave mode($A_0$ mode) on a rectangular plate. The dispersion characteristic equation of the $A_0$ mode is approximated using the Timoshenko beam theory. A virtual sensor array model is developed to consider the effects of reflections occurring on the plate boundary on the time reversal process. The time reversal process is formulated in the frequency domain using the virtual sensor array model. The reconstructed signal is obtained in the time domain through an inverse fast Fourier transform. The validity of the proposed method is demonstrated through the comparison to the numerical simulation results computed by the finite element analysis.

고효율, Temperature/voltage 변화에 둔감한 Triple-mode CMOS DC-DC Converter (A High-Efficiency, Robust Temperature/voltage Variation, Triple-mode DC-DC Converter)

  • 임지훈;하종찬;김상국;위재경
    • 대한전자공학회논문지SD
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    • 제45권6호
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    • pp.1-9
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    • 2008
  • 본 논문에서는 temperature/voltage에 둔감한 triple-mode CMOS DC-DC Converter를 제안한다. 제안된 triple-mode DC-DC converter는 단일 배터리의 수명에 따른 전압변화(3.3-5.5V)로부터 일정 또는 다양한 출력전압(0.6-2.2V)을 생성한다. 제안된 triple-mode CMOS DC-DC converter는 Pulse Width Modulator(PWM) 모드, Pulse Frequency Modulator(PPM) 모드, 그리고 Low Drop-Out(LDO) 모드, 이렇게 세 가지 모드로 동작한다. 또한, 제안된 회로는 temperature/voltage 변화에 의한 칩의 오동작을 방지하기 위해 temperature/voltage 변화에 둔감한 저 전력 1MHz CMOS ring oscillator를 사용한다. 제안된 triple-mode DC-DC converter는 단일 입력 전원소스(3.3-5.5V)에서 출력 전압(0.6-2.2V)을 생성하며, 출력 전압 ripple은 PWM mode에서 10mv, PFM mode에서 15mV, 그리고 LDO mode에서는 4mV 이하이다. 또한, 제안된 회로의 효율은 PWM mode에서 93% 이상이며, $-25-80^{\circ}C$의 온도변화에도 각 모드에서의 출력 전압 레벨의 오차는 단지 0.8% 이하로 유지한다 제안된 회로의 검증을 위해 CMOS $0.35{\mu}m$ 공정을 이용한 시뮬레이션 및 칩 테스트를 수행하였다.

선형방식과 스위칭 방식의 레귤레이터를 함께 구동하기 위한 Mode Selector (A Mode Selector for Operation with Linear and Switching Regulator)

  • 조한희;박경현;정준모;구용서
    • 전기전자학회논문지
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    • 제19권2호
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    • pp.260-264
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    • 2015
  • 본 논문에서는 부하전류를 감지하여 스위칭 방식과 선형 방식의 레귤레이터를 동작하기 위한 mode selector를 제안한다. 제안된 mode selector는 선형 방식과 스위칭 방식으로의 모드 전환이 가능하며, 경부하 조건에서 낮은 효율을 갖는 스위칭 방식의 레귤레이터의 단점을 보완하고자 제안되었다. 경부하 조건에서는 선형 방식의 레귤레이터로 mode를 전환함으로써 경부하 상태에서도 높은 효율을 제공할 수 있다. 설계한 mode selector는 동부 하이텍의 $0.18{\mu}m$ CMOS 공정을 이용하였다.

Attenuation of Fundamental Longitudinal Guided Wave Mode in Steel Pipes Embedded in Soil

  • Lee, Ju-Won;Shin, Sung-Woo;Na, Won-Bae
    • 비파괴검사학회지
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    • 제30권6호
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    • pp.539-547
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    • 2010
  • In this study, characteristics of the fundamental longitudinal guided wave mode, L(0,1), which is a usual mode employed in the inspection of the above-ground pipe, of the buried pipe were numerically investigated considering property changes in the surrounding soil. Results showed that soil conditions are significantly affecting the attenuation of L(0,1) mode in the pipe embedded in soil. Especially, if the soil is partially saturated, the attenuation of L(0,1) mode is larger and is very similar regardless of the degree of water saturation in the surrounding soil. However, when the soil is fully saturated, the attenuation of L(0,1) mode is less and show different trend with its partially saturated counterparts.

Treatment Plan Delivery Accuracy of the ViewRay System in Two-Headed Mode

  • Park, Jong Min;Park, So-Yeon;Wu, Hong-Gyun;Kim, Jung-in
    • 한국의학물리학회지:의학물리
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    • 제27권3호
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    • pp.169-174
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    • 2016
  • The aim of this study is to investigate the delivery accuracy of intensity-modulated radiation therapy (IMRT) plans in the two-headed mode of the ViewRay$^{TM}$ system in comparison with that of the normal operation treatment plan of the machine. For this study, a total of eight IMRT plans and corresponding verification plans were generated (four head and neck, two liver, and two prostate IMRT plans). The delivered dose distributions were measured using ArcCHECK$^{TM}$ with the insertion of an ionization chamber. We measured the delivered dose distributions in three-headed mode (normal operation of the machine), two-headed mode with head 1 disabled, two-headed mode with head 2 disabled, and two-headed mode with head 3 disabled. Therefore, a total of four measurements were performed for each IMRT plan. The global gamma passing rates (3%/3 mm) in three-headed mode, head 1 disabled, head 2 disabled, and head 3 disabled were $99.9{\pm}0.1%$, $99.8{\pm}0.3%$, $99.6{\pm}0.7%$, and $99.7{\pm}0.4%$, respectively. The difference in the gamma passing rates of the three- and two-headed modes was insignificant. With 2%/2 mm, the rates were $96.6{\pm}3.6%$, $97.2{\pm}3.5%$, $95.7{\pm}6.2%$, and $95.5{\pm}4.3%$, respectively. Between three-headed mode and head 3 disabled, a statistically significant difference was observed with a p-value of 0.02; however, the difference was minimal (1.1%). The chamber readings showed differences of approximately 1% between three- and two-headed modes, which were minimal. Therefore, the treatment plan delivery in the two-headed mode of the ViewRay$^{TM}$ system seems accurate and robust.

부직포가 복합적층판의 층간파괴인성에 미치는 효과 (Effect of non-woven tissues on interlaminar fracture toughness of composite laminate)

  • 김영배;정성균;강진식;김태형
    • 한국복합재료학회:학술대회논문집
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    • 한국복합재료학회 2000년도 추계학술발표대회 논문집
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    • pp.110-114
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    • 2000
  • The Interlaminar fracture behavior of hybrid composite with non-woven carbon tissue was investigated under Mode I (DCB) and Mode II (ENF) loading condition. Hybrid composites were manufactured by means of inserting a non-woven tissue between prepreg layers. Two kinds of specimens were prepared from [0]$_{24}$ and [$0_{12}/0_{12}$]. Where, the symbol "/" means that a non-woven carbon tissue was located at 0/0 mid-plane of the specimen. The interlaminar fracture toughness of hybrid composites was compared with that of CFRP. The fracture surfaces of the specimens were observed using optical microscope and SEM, and the failure mechanism was discussed. The hybrid laminates, which are made by inserting non-woven carbon tissue between layers, were shown to be effective to remarkably improve Mode II fracture toughness.toughness.

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혼합모드(I+II)에서 피로 하중에 의한 균열진전 거동 (Crack Growth Behavior by Fatigue Load under Mixed Mode(I+II))

  • 공병채;최성대
    • 한국생산제조학회지
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    • 제21권2호
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    • pp.276-282
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    • 2012
  • This study looked for Mode status of each for fatigue crack growth behavior about the repeat load of mode I and the static load of mode II. The experiment was performed in the state of the repetition frequency of the sine wave 10Hz, the stress ratio 0.1, maximum load 300kg.f, a static load 0, 100, 200, 300kg.f, As the experimental results, in mode of static load, while the load value increases, the crack growth rate is slower as the energy of a crack mixing grows. Mode I and the power mode II get an influence each other in the direction of crack propagation path, but as they eventually get closer to the breaking point of the crack growth, it is dominated by the mode I.

Burst형과 고빈도형 경피신경전기자극치료가 실험적 동통역치와 체온에 미치는 영향 비교 (A Study Comparing the Effects of Burst Mode and High Rate Mode Transcutaneous Electrical Nerve Stimulation on Experimental Pain Threshold and Skin Temperature)

  • 김선엽;최흥식;권오윤
    • 대한물리치료과학회지
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    • 제2권2호
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    • pp.465-479
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    • 1995
  • We randomly assigned 61 healthy subjects(male 14, female 47) to compare the experimental pain threshold and skin temperature between high mode TENS and burst mode TENS. In this study, 61 subjects were divided into three groups ; high mode TENS(n=20), burst mode TENS (n=20), and control group(n=21). Experimental pain thresholds and skin temperatures were measured before, immediately after cessation of stimulation, and at 30 minutes post stimulation. Stimulation was applied to the dorsal surface of the forearm(L14, LI10). Pain thresholds were measured by chronaxie meter. Skin temperature were measured by electrical digital thermometer. The results are as follows ; 1. There were no statistical difference in the pain threshold and skin temperature at before TENS stimulation among the three groups(p>0.05). 2. The pain threshold and skin temperature in burst mode TENS group was significantly higher and longer effect than that in high mode TENS group and control group(p<0.01). 3. The pain threshold in burst mode TENS group decreased to prestimulation levels by 30 minutes poststimulation. 4. The skin temperature in burst mode TENS group decreased to prestimulation levels by 20 minutes poststimulation. 5. The skin temperature was significantly difference among three group at immediately after, and at 30 minutes poststimulation and the skin temperature in burst mode TENS group was significantely higher than that in two groups(p<0.001). 6. The increasing rate of pain threshold in high mode TENS group after immediately cassation of stimulation was 24.3%(p<0.001). 7. The increasing rate of pain threshold in burst mode TENS group after immediately cessation of stimulation was 93.5% (p<0.001).

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