• 대한수의학회지
• /
• 제33권4호
• /
• pp.735-746
• /
• 1993

Electrocardiographic parameters of amplitude and the shape of waves on the unipolar precordial chest leads in the normal Korean native cattles have been measured with a 3 channel electrocardiograph built in a computed and analysis. The study was conducted on 98 heads of mean age of 17.6 months. The wave forms of P, T and QRS complex wave in all leads showed various types. The parameters of the amplitude in the wave types showed the most frequency in each lead that were analyzed as follow : 1. In P wave, amplitudes of positive type showed a frequency of 92.9% and 93.9% in leads $CV_6LU$ and $CV_6LL$ that were $83.8{\pm}31.0{\mu}V$ and $76.0{\pm}30.7{\mu}V$, and negative type showed a frequency of 97.9% in lead V 10 that were $-80.2{\pm}29.4{\mu}V$, respectively. But the plate type in leads $CV_6RU$ and $CV_6RL$ showed frequency of 48% and 58.3%, respectively. 2. Average amplitude of the QRS complex were in a range of $277.0{\pm}154.0{\mu}V$ to $648.2{\pm}146.2{\mu}V$(mean of $418.8{\pm}139.4{\mu}V$) in all leads that were manifested the Low-Voltage QRS complex(below 1 mV in unipolar precordial leads). Average amplitudes of each wave type in the QRS complex were $-250.0{\pm}139.8{\mu}V$ and $-399.2{\pm}226.8{\mu}V$ in the QS group types that showed a frequency of 50.0% and 82.5% in the leads $CV_6LU$ and $CV_6LL$, respectively. And average amplitudes of the R group types showed a frequency of 85.6%, 56.1% and 75.8% in the $CV_6RU$, $CV_6RL$ and $V_{10}$ that were $321.5{\pm}142.1{\mu}V$, $271.6{\pm}139.9{\mu}V$ and $552.4{\pm}132.7{\mu}V$, respectively. 3. In T waves, Amplitudes of the positive type showed a frequency of 60.2%, 46.9% and 83.7% in leads of $CV_6LL$, $CV_6RU$ and $CV_6RL$ that were respectively $184.7{\pm}93.7{\mu}V$ $103.7{\pm}64.43{\mu}V$ and $111.8{\pm}39.3{\mu}V$, the negative type showed a frequency of 62.2% and 93.7% in leads $CV_6LU$ and $V_{10}$ that were $142.2{\pm}82.1{\mu}V$ and $-280.3{\pm}107.2{\mu}V$, respectively. 4. Average amplitude of ST segment were $3.7{\pm}33.1{\mu}V$, $0.9{\pm}23.1{\mu}V$, $10.9{\pm}28.6{\mu}V$, $5.8{\pm}28.3{\mu}V$ and $-34.7{\pm}48.4{\mu}V$ in leads $CV_6LL$, $CV_6RU$, $CV_6RL$, $CV_6LU$ and $V_{10}$ respectively.

• 비파괴검사학회지
• /
• 제26권6호
• /
• pp.390-402
• /
• 2006

The elastic properties and thickness of mullite environmental barrier coatings grown through chemical vapor deposition (CVD) on silicon carbide substrates were measured using frequency domain photoacoustic microscopy. In this technique, extremely narrow bandwidth surface acoustic waves are generated with an amplitude modulated laser source. A photorefractive crystal based interferometer is used to detect the resulting surface displacement. The complex displacement field is mapped as a function of source-to-receiver distance in order to extract the wavelength of the surface acoustic wave at a given excitation frequency, and the phase velocity is determined. The coatings tested exhibited spatial variations in thickness and mechanical properties. The measured surface wave dispersion curves were used to extract an effective value for the elastic modulus and the coating thickness. Nanoindentation was used to validate the measurements of the effective elastic modulus. The average elastic modulus measured through the coating thickness using nanoindentation is compared to the effective modulus found using the photoacoustic system. Optical microscopy is used to validate the thickness measurements. The results indicate that the photoacoustic microscopy technique can be used to estimate the effective elastic properties in coatings exhibiting spatial inhomogeneities, potentially providing valuable feedback for the optimization of the CVD growth process.

• 한국지반공학회:학술대회논문집
• /
• 한국지반공학회 1993년도 학술발표집 지반진동 영향평가
• /
• pp.83-116
• /
• 1993

본 고는 쓰레기 매립장에서 동다짐을 시행할 시 발생하는 진동을 측정하고, 그 결과를 분석하여 쓰레기 매립지반의 동다짐 진동 특성을 고찰하였다. 진동특성은 크게 쓰레기 매립지반의 일반적 진동특성과 동다짐 조건 변화에 의한 진동특성의 2가지 측면으로 검토되었다. 그 결과 연구대상 쓰레기 매립지반의 기본적인 진동특성으로 충격지점 주위에서의 전단계수 G 행 17496~58320 t/m2, 감쇠비 D=14~58%, 탁월진동수 f=6~14 Hz 등으로 나타났다. 동다짐 조건 차이에 의한 진동특성으로는 타격회수가 증가될수록 cross hole시험에 의한 전단파 및 압축파의 속도가 중가하였으며, 타격지점으로 부터의 거리와 최대입자속도는 vPP = 5.08 [D/E]-1.4의 관계를 가지며, 쓰레기층 바닥에서는 반사파의 영향으로 진동의 진폭이 커지는 것으로 나타났다. 또한 진동에 의하여 지반이 개량되는 범위는 타격지점으로 부터 반경 약 6~10 m정도인 것으로 나타났다.

• The Korean Journal of Physiology
• /
• 제18권1호
• /
• pp.51-65
• /
• 1984

장기간(長期間) 체력단련(體力鍛鍊)이 심전도파고(心電圖波高) 및 심전도(心電圖) vector에 미치는 효과(效果)를 구명(究明)하고자 10명(名)의 운동선수군(運動選手群)과 13명(名)의 비운동선수군(非運動選手群)에서 rebounder운동전후(運動前後)의 심전도파고(心電圖波高)와 QRS vector의 길이를 측정(測定)하여 분절(分折)한 결과(結果)는 다음과 같다. 심전도파고(心電圖波高)에서 R파고(波高)는 선수군(選手群)이 $23.38{\pm}1.14\;mm$로서 비선수군(非選手群)의 $17.91{\pm}2.00$\;mm$에 비(比)해 유의(有意)하게 높았고, 운동후(運動後)에도 선수군(選手群)이 계속(繼續) 유의(有意)하게 높았다. S파고(波高)는 양군(兩群) 모두 운동후(運動後)는 안정시(安靜時)에 비(比)해 유의(有意)하게 높았으며, T파고(波高)는 운동후(運動後) 감소(減少)하였다. P파고(波高)는 양군(兩群) 모두 운동후(運動後) 증가(增加)하였으며 선수군(選手群)이 다소 낮았다. PQ분절(分節)의 파고(波高)는 선수군(選手群)은 0인데 비(比)해 비선수군(非選手群)은 negative를 나타냈으며 운동후(運動後)에 유의(有意)하게 감소(減少)하였다. J점(點)은 양군(兩群) 모두 안정시(安靜時) positive에서 운동후(運動後) 유의(有意)하게 감소(減少)하여 negative를 나타냈고, J+0.08초(秒)도 운동후(運動後) 양군(兩群) 모두 감소(減少)하였으며 선수군(選手群)이 다소 높았다. 그러므로 ST분절(分節)은 운동후(運動後) 감소(減少)함을 알 수 있다. $Rv_5$와 $Sv_1$의 합(合)은 선수군(選手群)이 $38.74{\pm}2.71\;mm$로서 비선수군(非選手群)의 $32.28{\pm}2.90\;mm$에 비(比)해 높았으며 운동후(運動後)에도 선수군(選手群)이 유의(有意)하게 높았다. QRS vector 각도(角度)에서 Frontal plane에서 선수군(選手群)이 $62.7{\pm}7.36^{\circ}$로서 비선수군(非選手群)과 별(別) 차이(差異)가 없었고, horizontalplane에서는 선수군(選手群)이 $-23.5{\pm}7.2^{\circ}$로서 비선수군(非選手群)의 $-38.8{\pm}8.2^{\circ}$에 비(比)해 유의(有意)하게 높았으며 운동후(運動後) 양군(兩群) 모두 유의(有意)하게 높았다. QRS vector 길이에서 Frontal plane에서 선수군(選手群)이 $13.86{\pm}1.44\;mm$로서 비선수군(非選手群)의 $9.62{\pm}0.97\;mm$에 비(比)해 유의(有意)하게 높았으며 운동후(運動後)에도 유의(有意)하게 높았다. Horizontal plane에서도 선수군(選手群)이 $19.82{\pm}2.10\;mm$로서 비선수군(非選手群)의 $16.90{\pm}1.39\;mm$에 비(比)해 유의(有意)하게 높았고 운동후(運動後)에도 선수군(選手群)이 유의(有意)하게 높았다. 이상(以上)을 종합(綜合)해 보면 선수군(選手群)의 R파고(波高)가 비선수군(非選手群)에 비(比)해 운동후(運動後) 계속(繼續) 유의(有意)하게 높았고, $Rv_5$와 $Sv_1$파고(波高)의 합(合)이 38.74mm정도(程度)로 좌심실(左心室)이 비대(肥大)함을 알 수 있으며, 선수군(選手群)의 PQ분절파고(分節波高)와 ST분절(分節) 파고(波高)가 비선수군(非選手群)에 비(比)해 높고 운동후(運動後)에 양군(兩群) 모두 감소(減少)한 점(點)은 주목(注目)할만한 사실(事實)이며, 특(特)히 선수군(選手群)의 QRS vector의 길이가 모두 비선수군(非選手群)에 비(比)해 유의(有意)하게 긴점등(點等)으로 좌심실기능(左心室機能)이 우수(優秀)한 스포츠심장(心臟)임을 알 수 있으며, 선수군(選手群)과 비선수군(非選手群)을 평가(評價)할 수 있는 중요(重要)한 지표(指標)가 될 것으로 사료(思料)되는 바이다.

• 대한기계학회:학술대회논문집
• /
• 대한기계학회 2003년도 추계학술대회
• /
• pp.90-96
• /
• 2003

Numerical analyses have been performed to obtain the absorption heat and mass transfer coefficients and the absorption mass flux from a falling film of LiBr solution. In the present study, the behavior of laminar-wavy falling film in the vertical absorber was studied analytically and experimentally. The change of absorption performance on mean film thickness, wave amplitude, wave celerity was analysed. The heat and mass transfer equations are solved simultaneously to give the temperature and concentration variations at the LiBr solution/refrigeration vapor interface and at the wall. Effects of uniform film, wavy film and film Reynolds number on the heat and mass transfer coefficients have been estimated. The analytical results of the uniform and wavy falling film in the bare tube was higher than experimental result for $Rd_{t}<100$. The absorption performance showed the maximum at the wavy film by the insert device(spring).

• 한국자기학회지
• /
• 제24권6호
• /
• pp.165-170
• /
• 2014

본 연구에서는 두께가 다른 비정질 CoFeB 박막 재료에서 측정한 강자성 및 스핀파 공명 신호를 비교 분석하였다. 강자성 공명 자기장($H_{FMR}$)은 두께에 거의 무관하게 일정한 값을 갖는 반면 스핀파 공명 자기장($H_{SWR}$)은 CoFeB의 두께에 의존하는 스핀파 모드들에 대한 이론 값과 일치하였다. 수평면에서 자기장 각도에 따른 $H_{FMR}$ 측정 결과로부터 CoFeB 재료의 일축이방성 자기장은 37 Oe였다. 한편 $H_{SWR}$은 $H_{FMR}$과 동일한 각도 의존성을 보였으며, 스핀파 공명 신호의 크기는 강자성 공명 신호에 비하여 약 5.7배 증가하였다. 이러한 증가는 비정질 재료의 작은 감쇠 상수에 의한 저감이 작은 스핀파의 진행 특성 및 균일한 자화에 의한 이상적인 정상파 형성 조건에 기인함을 알 수 있었다.

• 비파괴검사학회지
• /
• 제30권5호
• /
• pp.458-463
• /
• 2010

음향 비선형성은 재료 물성의 미세한 변화에 민감하기 때문에, 이를 측정하는 비선형 초음파 기술은 재료의 열화나 피로를 평가할 수 있는 기법으로 연구되어 왔다. 하지만 벌크파를 이용하는 일반적인 비선형 초음파 기법은 얇은 판재에 적용하는 것에는 여러 한계가 있다. 이와 같은 경우에는 비선형 Lamb 파의 사용을 생각할 수 있지만, Lamb 파는 벌크파와 매우 다른 전파 특성을 가지고 있어 그 비선형 특성에 대한 별도의 연구를 필요로 한다. 이를 위해 본 연구에서는 Lamb 파에서 비선형성에 의해 전파하면서 누적 성장할 수 있는 2차 고조파 모드의 발생 조건을 분석하였으며, 그 결과 네 가지 조건, 즉 (1) phase matching, (2) non-zero power flux, (3) group velocity matching, (4) non-zero out-of-plane displacement 를 제시하였다. 그리고 제시된 조건으로 알루미늄 판재에 대책 실험한 결과 이론 예측과 동일하게 전파 거리에 따라 2차 고조파 성분의 크기와 비선형 파라미터가 증가하였고, Al6061-T6 과 Al1100-H14에서 측정된 상대적인 비선형 파라미터의 비율이 이론적인 비율과 근접함을 보였다.

• Ocean Systems Engineering
• /
• 제10권1호
• /
• pp.87-110
• /
• 2020

Catamaran has recently been a choice to support a typical vertical axis turbine in floating tidal current energy conversion system. However, motion responses associated with the catamaran can reduce the turbines efficiency. The possibility to overcome this problem isto change the catamaran parameter by varying and simulating the demi-hull separations to have lower motion responses. This simulation was undertaken by Computational Fluid Dynamic (CFD) using potential flow analysis. Cases of demi-hull separation were considered, with ratios of demi-hull separation (S) to the breadth of demi-hull (B), ^S/_B of 3.45, 4.95, 6.45, 7.2 and 7.95. In order to compare to the previous works in the literature, the regular wave was set with wave height of 0.8 m. Furthermore, the analysis was carried out by irregular waves with significant wave height, H_s, of about 0.09 to 1.5 m and the wave period, T, of about 1.5 to 6 s or corresponding to the wave frequency, ω, of about 1.1 to 4.2 rad/s. The wave spectrum was derived from the equation of the International Towing Tank Conference (ITTC). For the case of turbines-loaded catamaran under consideration, the new finding is that the least significant amplitude response can be satisfied at the ratio ^S/_B of 7.2. This study indicates that selecting a right choice of demi-hull separation ratio could contribute in reducing motion responses of the tidal current turbines-loaded catamaran.

• 한국임상수의학회지
• /
• 제14권2호
• /
• pp.319-337
• /
• 1997

The electrocardiographic (ECG) parameters in the normal Korean black goat have been measured with a 3-channel Electrocardiograph and computed, analyzed. ECG in 243 black goats were made with the limb leads (I, II, III, aVR, aVL, aVF), that were recorded conduction parameters of wave and interval, and were analyzed as to shape and amplitude of the P and T waves and the components of the QRS complex. Heart rate were recorded by the ECG which were a mean of 106.1$\pm $21.8 beats/min. Average conduction times in the PR, the QRS complex and the QTc interval were recorded 103.9$\pm $34.9 msec., 58.3$\pm $23.2 msec. and 302.6$\pm $67.8 msec., in the P and T wave duration recorded 24.8$\pm $6.4 msec. and 51.7$\pm $10.8 msec. respectively. The shape of wave in each leads were observed various types, and any spacial wave type appeared the highest frequency in each lead that ware shown less than 60%, and these frequent rate and average amplitudes as fallow: 1. In P waver the frequent rate and average amplitudes of the positive type showed in leads I, II and aVL that were 54.8% (93.0$\pm $ 33.2 $\mu $V), 50.5% (90.1$\pm $30.5 $\mu $V) and 41.7% (58.5$\pm $ 31.1 $\mu $V). Average amplitude of the negative type showed the frequent rate of 49.8% in lead aVE which was -77.6$\pm$ 25.2 $\mu $V. Biphasic type in leads III and aVF were 46.1% (108.4 $\mu $V, -90.2 $\mu $V.) and 45.7% (137.4 $\mu $V, -105.4 $\mu $V.), and amplitudes between positive and negative of it were significant difference. 2. The highest amplitudes of the QRS complex in all leads were 534.8$\pm $ 232.3 $\mu $V of lead II. The frequent rate and amplitudes of the R wave type in the I, II, III and aVF were 30.2% (277.8 $\pm $131.3 $\mu $V), 45.1% (393.1$\pm $114.2 $\mu $V), 48.5% (349.3$\pm $178.3 $\mu $V) and 54.9% (334.4$\pm $129.7 $\mu $V), and QS ways type in the lead aVL was 49.5% (359.2$\pm $195.5$\mu $V), and RS and QS wave types in the lead a VR were 43.3% (312.4 $\mu $V, -212.7 $\mu $V.) and 41.1% (399.2$\pm $92.2 $\mu $V), respectively. 3. In T wave, the frequent rata and amplitudes of the positive type in the leads I, II, III and aVF were 44.6% (207.9$\pm $ 97.1 $\mu $V), 41.6% (245.1$\pm $92.1 $\mu $V), 46.9% (189.8$\pm $ 82.7 $\mu $V) and 53.0% (195.4197.8 $\mu $V), and the negative in the lead aVR was 41.2% (-230.7$\pm$ 103.1 $\mu $V), respectively. The positive and negative types in the lead aVe appeared with same frequent rate of 43.2%.4. Frontal plane vectors for P, QRS, and T were found to lie at 38.1$\pm $ 21.5, 142.0$\pm $ 57.2, and 117.2$\pm $ 63.9 degrees, respectively. These results in ECG of goats may be served to the limited purposes as to conduction parameters, arrhythmias except abnormal ECG because of waveforms, amplitudes and electrical axis of it were variability.

• 대한기계학회논문집A
• /
• 제26권8호
• /
• pp.1487-1494
• /
• 2002

In this study, to propose the prediction method of the crack growth under flight-simulation loading, crack growth tests are conducted on 2124-7851 aluminum alloy specimens. The prediction of crack growth under flight-simulation loading is performed by the stochastic crack growth model which was developed in previous study. First of all, to reduce the complex load history into a number of constant amplitude events, rainflow counting is applied to the flight-simulation loading wave. The crack growth, then, is predicted by the stochastic crack growth model that can describe the load interaction effect as well as the variability in crack growth process. The material constants required in this model are obtained from crack growth tests under constant amplitude loading and single tensile overload. The curves predicted by the proposed model well describe the crack growth behavior under flight-simulation loading and agree with experimental data. In addition, this model well predicts the variability of fatigue lives.