• 수산해양기술연구
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• 제36권4호
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• pp.287-298
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• 2000

본 연구에서는 측정거리의 정밀도가 3.5cm이내인 GPS 선간거리계측 시스템을 이용하여 권현망 조업선의 주선에 기준국을 종선에 이동국을 설치하여 주$.$종선의 양선간격의 변화와 침로에 따른 예망항적을 측정하고 예망중인 어구의 각부에 자기식 수온수심계를 부착하여 각부의 망고와 예망수층의 파악을 통한 어구의 수중형상을 비교 분석하여 어법 및 어구의 조업진단을 행하였다. 1. 양선간격 5m일 시에는 어구가 큰 폭으로 가라앉아 불안정한 형상을 나타내며 깔대기와 자루그물도 동일한 예망수층을 이루고 있어 입망된 어군의 도피 위험성이 가장 크다. 2. 양선간격이 l00m일 시에는 어구 각부의 망고가 다소 높아지며 앞창과 문턱, 깔대기의 예망수층의 경사가 커서 자루그물의 형상이 불안정하여 어군입망의 저해요인이 되어 어획효율은 크게 감소할 것으로 판단되므로 양선간격이 좁아질수록 예망속도의 증대가 필요하다. 3. 양선간격이 200m일 시에는 어구의 수중형상이 다소 안정된 상태를 보여 주고 있으나 자루 그물 뒤끝이 다소 들어올려지며 이는 깔대기가 상대적으로 아래쪽으로 내려앉아 어획효율이 좋지 않을 것으로 예상되며 자루그물의 예망수층의 개선이 필요하다. 4. 양선간의 거리가 300m일 시에는 오비기에서 자루그물까지의 연결이 비교적 완만하게 형성되고 깔대기와 자루그물의 형상도 양호하여 전체적인 어구의 형상이 안정되어 있으나 정상적인 망고를 이룰 수 있도록 개선이 요구된다. 5. GPS 선간거리계측 시스템을 권현망어 업에 적용하여 조업을 행한다면 어군의 기록분포에 따라 적정한 양선간격을 도출함과 동시에 정밀한 양선간격의 조절이 가능하여 보다 높은 어획효율을 얻을 수 있다.

• Current Optics and Photonics
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• 제7권4호
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• pp.354-361
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• 2023

We present the optical design and experimental verification of resolving performance of a 3× long wavelength infrared (LWIR) zoom camera for drones. The effective focal length of the system varies from 24.5 mm at the wide angle position to 75.1 mm at the telephoto position. The design specifications of the system were derived from ground resolved distance (GRD) to recognize 3 m × 6 m target at a distance of 1 km, at the telephoto position. To satisfy the system requirement, the aperture (f-number) of the system is taken as F/1.6 and the final modulation transfer function (MTF) should be higher than 0.1 (10%). The measured MTF in the laboratory was 0.127 (12.7%), exceeds the system requirement. Outdoor targets were used to verify the comprehensive performance of the system. The system resolved 4-bar targets corresponding to the spatial resolution at the distance of 1 km, 1.4 km and 2 km.

• Journal of the Korean Statistical Society
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• 제32권4호
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• pp.401-409
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• 2003

We consider a particle walking on the nonnegative integers and each unit of time it makes, given it is at site k, either a jump of size m distance units to the right with probability $p_{k}$ or it goes back (falls down) to its starting point 0, a retaining barrier, with probability $v_{k}\;=\;1\;-\;p_{k}$. This is a Markov chain on the integers $mZ^{+}$. We show that if $v_{k}$ has a nonzero limit, then the Markov chain is positive recurrent. However, if $v_{k}$ speeds to 0, then we may get transient Markov chain. A critical speeding rate to zero is identified to get transience, null recurrence, and positive recurrence. Another type of random walk on $Z^{+}$ is considered in which a particle moves m distance units to the right or 1 distance unit to left with probabilities $p_{k}\;and\;q_{k}\;=\;1\;-\;p_{k}$, respectively. A necessary condition to having a stationary distribution and positive recurrence is obtained.

• 한국산업보건학회지
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• 제8권1호
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• pp.146-154
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• 1998

This study was designed to investigate the workers' exposure level to electromagnetic field(EMF) in accordance with the VDT arrangement in the work place and distance from VDT. Author compared the exposure strength of EMF in line group(workers exposed to EMF from both front and back side) and in shielding group(workers exposed to EMF exclusively from front side). The levels of EMF at 30cm and 50cm from front side and at 30cm from back side of VDT were also measured. The result were as follows: 1. Mean distance between a monitor and a worker in shielding group ($47.7{\pm}8.7cm$) significantly longer than that in line group($44.3{\pm}7.2cm$). Strength of EMF in shielding group [$1.3{\pm}0.7V/m$ (electric field) and $18.2{\pm}11.5mA/m$ (magnetic field) were lower than in line group [$1.4{\pm}0.6V/m$ and $26.6{\pm}11.6mA/m$, respectively] at the workers' position. 2. The strength of EMF was decreased with the distance from VDT. The strength at 70cm from VDT was nearly the same as the background strength in the ordinary office rooms. 3. Working distance from 9 inch monitor was significantly shorter than that from 14 inch and wider sized monitors. 4. The strength of EMF in extremely low frequency spectrum of color monitors was higher then that of black and white monitor. 5. Metal coated filters significantly decreased the electric field strength of EMF when earth line was connected. Metallic shield was effectively decreased the EMF strength from VDT, but wooden shield was not. From the above results, line type arrangement of VDT in the work place using metallic shield at the back side of VDT, and metal coated filter to monitor with application of earth line were recommended. It is also recommended to maintain workers position to be 60cm or more distance from monitor and 140cm or more between VDTs for minimizing workers' exposure to EMF.

• 화약ㆍ발파
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• 제8권1호
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• pp.3-16
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• 1990

The cautious blasting works had been used with emulsion explosion electric M/S delay caps. Drill depth was from 3m to 6m with Crawler Drill $\varphi{70mm}$ on the calcalious sand stone(sort-moderate-semi hard Rock). The total numbers of feet blast were 88. Scale distance were induces 15.52-60.32. It was applied to propagation Law in blasting vibration as follows. Propagtion Law in Blasting Vibration $V=K(\frac{D}{W^b})^n$ where V : Peak partical velocity(cm/sec) D : Distance between explosion and recording sites (m) W : Maximum Charge per delay-period of eighit milliseconds or more(Kg) K : Ground transmission constant, empirically determind on th Rocks, Explosive and drilling pattern ets. b : Charge exponents n : Reduced exponents Where the quantity $D/W^b$ is known as the Scale distance. Above equation is worked by the U.S Bureau of Mines to determine peak particle velocity. The propagation Law can be catagrorized in three graups. Cabic root Scaling charge per delay Square root Scaling of charge per delay Site-specific Scaling of charge per delay Charge and reduction exponents carried out by multiple regressional analysis. It's divided into under loom and over loom distance because the frequency is verified by the distance from blast site. Empirical equation of cautious blasting vibration is as follows. Over 30m----under l00m----- $V=41(D/3\sqrt{W})^{-1.41}$ -----A Over l00m-----$V= 121(D/3\sqrt{W})^{-1.66}$-----B K value on the above equation has to be more specified for furthur understang about the effect of explosives, Rock strength. And Drilling pattern on the vibration levels, it is necessary to carry out more tests.

• 천문학회지
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• 제28권2호
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• pp.169-175
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• 1995

Deep V I CCD photometry of the Pegasus dwarf irregular galaxy shows that the tip of the red giant branch (RGB) is located at I = $21.15{\pm}0.10$ mag and (V - I) = $1.58{\pm}0.03$. Using the I magnitude of the tip of the RGB (TRGB), the distance modulus of the Pegasus galaxy is estimated to be $(m\;-\;M)_o\;=\;25.13{\pm}0.11$ mag (corresponding to a distance of d = $1060{\pm}50$ kpc). This result is in a good agreement with the recent distance estimate based on the TRGB method by Aparicio [1994, ApJ, 437, L27],$ (m\;-\;M)_o$ = 24.9 (d = 950 kpc). However, our distance estimate is much smaller than that based on the Cepheid variable candidates by Hoessel et al.[1990, AJ, 100, 1151], $(m\;-\;M)_o\;=\;26.22{\pm}0.20$ (d = $1750{\pm}160$ kpc) mag. The color-magnitude diagram illustrates that the Cepheid candidates used by Hoessel et al.are not located in the Cepheid instability strip, but in the upper part of the giant branch. This result shows that the Cepheid candidates studied by Hoessel et al.are probably not Cepheids, but other types of variable stars. Taking the average of our distance estimate and Aparicio's, the distance to the Pegasus galaxy is d= $1000{\pm}80$ kpc. Considering the distance and velocity of the Pegasus galaxy with respect to the center of the Local Group, we conclude that the Pegasus galaxy is probably a member of the Local Group.

• 한국정밀공학회지
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• 제24권8호통권197호
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• pp.41-49
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• 2007

In this paper, we proposed a new ultrasonic distance measurement system with high accuracy and long range. To improve accuracy and enlarge range, the time of flight of ultrasonic is calculated by the period detecting method. In the proposed ultrasonic distance measurement system, the ultrasonic transmitter and receiver are separated but synchronized by RF(Radio frequency) module. The experiment has been implemented from short distance 1m to maximum available distance 30m. And the period detecting method is compared with the conventional threshold level method. Experimental results show the accuracy and range of the distance measurement are improved by this period detecting method.

• 한국운동역학회지
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• 제13권1호
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• pp.63-72
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• 2003

This study is examine and analysis of the most flying and run distance during swing three times with six balls between two amateurs and pro-golfers in golf field in Sungnam airport. During down swing, kinetics variances are velocity of club-head and balls, vertical angular velocity. this scientic data present amateur golfers with recognition of long flying distances for golf balls. Through this study, the conclusions are as follows. 1. Before impact the balls, The club-head velocity of amateur golfers and pro-golfers show 33.34 - 39.53m/s, 39.04 - 42.82m/s respectively during the down swing. But The club-head velocity, flight and Run distances comparative $K_1$ amateur golfer with the pro-golfer are similar. 2. After impact the balls, The balls velocity if amateur golfers show 53.04 - 61.57m/s, The pro-golfers show 62.32 - 63.4m/s respectively during the down swing. In case of $K_3$,$K_4$, After the impact balls velocity comparative The RA brand with other brand are similar, Flight and Run distance are difference. 3. After impact the balls, The balls velocity are difference to other brand but The long flight and Run distance arrange RA, BIG, TITL. 4. In the vertical flight angle of the ball after impact, amateur golfer showed 16.75 - $18.73^{\circ}$. The pro-golfer showed 15.03 - $16.04^{\circ}$. In the vertical flight angle of the balls ideal $12-13^{\circ}$, The long flight and Run distance approach In the vertical flight angle the balls $12-13^{\circ}$.

• 설비공학논문집
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• 제12권1호
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• pp.59-66
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• 2000

In a previous paper, we have examined the effects of nozzle configuration and jet to jet spacing on the heat transfer of 1 row of circular water jets. In this paper, experiments have been conducted to obtain the effects of nozzle to target plate distances on the heat transfer of 1 row of 3 jets and 1 row of 5 jets. The nozzle configurations are Cone type, Reverse cone type and Vertical circular type. Nozzle to target plate distance H was varied from 16 mm(H/D=2) to 80mm(H/D=10). For fixed value of mass flow rate and nozzle to target plate distance, larger values of average Nusselt number were obtained for the smaller jet to jet spacing. For the array of water jets, the average heat transfer was decreased slightly with increasing nozzle to target plate distance at low jet velocity of $\textrm{V}_{o}$=3 m/s. However, except for $\textrm{V}_{o}$=8 m/s of 1 row of 5 jets, it was increased with increasing nozzle to target plate distance at high jet velocity of $\textrm{V}_{o}$$\geq$6m/s. We proposed to apply the nozzle configuration of maximum average heat transfer to each nozzle to target plate distance for 1 row of 3 jets, and, it was Reverse cone type nozzle for 1 row of 5 jets(Reynolds number$\geq$36000).

• 한국식생활문화학회지
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• 제2권1호
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• pp.1-8
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• 1987

한식을 편의식화하기 위해서 10개 품목의 양목표(量目表) 및 가공 순서를 정했다. $62.8m^2$와 $32.4m^2$의 상업용 식당과 모델 식당에서, 주방기기류의 배치에 따른 작업원의 작업동선, 소요 에너지를 측정한 결과는 다음과 같다. 1. $62.8m^2$식당의 경우 C-스토아에서 작업원의 동선, 소요시간 및 소요 에너지는 각각 1,922m, 2,986분 및 4,704kcal였고 T-스토아는 각기 2,134m, 3,173분 및 5,001.7kcal였으며 모델 식당에서는 1,704m, 2,808분 및 4,414.5kcal로 기존 주방들에 비해서 289.5kcal(6.6%)와 587.2kcal(13.3%)의 에너지가 절약되었다. 2. $32.4m^2$식당의 경우 S-스토아에서 작업동선, 소요시간 및 소요 에너지는 각각 1,277m, 2,926분 및 4,588kcal였고 H-음식점에서는 1,425m, 3,108분 및 4,873.8kcal였으며 모델 주방에서는 1,167m, 2,798분 및 4,381.4kcal로 기존 주방에 비해서 206.6kcal(4.7%) 및 492.4kcal(11.2%)가 절약되었다. 3. 4개 품목은 직접 생산하고 6개 품목은 편의식화할 경우 S-스토아에서 작업동선, 소요시간 및 소요 에너지는 각기 554.7m, 972분 및 1,586kcal였고 H-음식점에서는 각각 684.7m, 991분 및 1,579.2kcal였으며 모델 주방에서는 각기 523.1m, 938분 및 1,479.5kcal로 기존 주방들에 비해서 106.5kcal(7.2%)와 99.7kcal(6.7%)의 에너지 절약 효과가 있었다. 4. 동선 절약형 시스템 주방의 경우 모델 주방에 비해서 동선은 42%, 소요 에너지는 20.4%가 절약 되었다.