• Journal of Korean Society of Coastal and Ocean Engineers
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• v.15 no.4
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• pp.232-241
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• 2003

The interaction of incident monochromiatic waves with N bottom-mounted porous circular cylinders is investigated in the frame of three-dimensional linear potential theory. The fluid domain is divided into N+l regions i.e. a single exterior region and N interior regions, and the diffraction potential in each fluid region is expressed by an eigenfunction expansion method (Williams and Li,2000). The analytic results show that the porous structure reduces both the wave forces and the run-up wave around the cylinder. To verify the developed model, the systematic model test with a line array of porous cylinders is conducted at the wave tank (30m$\times$7m$\times$1.5m). The analytic results are in good agreement with the experimental results within measured frequency range. It is concluded that the breakwater constructed with an array of porous circular cylinders shows the performance of an effective wave barrier together with the seawater-exchange effect and is considered to have vast potentials for the use of seawater-exchanging breakwater in the future.

• Journal of Ocean Engineering and Technology
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• v.23 no.6
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• pp.23-31
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• 2009

The interaction of incident monochromatic waves with a bottom-mounted vertical porous circular cylinder is investigated using the framework of the three-dimensional linear potential theory. The porosity of the circular cylinder is uniform vertically but varies in the circumferential direction. By adjusting the porosities of the circular cylinder, both the wave blocking performance of a porous semi-circular breakwater and the wave responses inside a circular harbor with an entrance are applied as calculation examples. It is found that the reflected waves, wave run-up, and wave forces are significantly reduced due to wall porosity, which are positive factors for a breakwater, and the amplification factor of a circular harbor at resonant frequencies is greatly reduced by a porous sidewall.

• Proceedings of the Korean Vacuum Society Conference
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• 2016.02a
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• pp.346.1-346.1
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• 2016

본 연구에서는 열처리(Thermal Dewetting Process)와 빗각 증착(Oblique angle deposition)을 이용하여 비주기 서브파장 구조물을 마이크로 렌즈 형태의 유리 기판 상부에 제작하였다. 먼저 $2{\times}2cm2$ 크기의 유리 기판에 기존 리소그래피 공정으로 원기둥 형태의 감광액을 형성한다. 이후 Hot-plate로 $180^{\circ}C$에서 90초간 열을 가해 지름이 $20{\mu}m$인 반구형태로 변형시킨 뒤 반응성이온식각 공정을 진행하여 마이크로 렌즈를 제작한다. 렌즈의 표면에 나방 눈 구조를 형성하기 위해 전자빔 증착으로 15nm의 은 박막을 쌓은 뒤 $500^{\circ}C$에서 1분간 열처리 공정을 진행하였다. 열이 가해졌을 때 은 박막은 표면자유에너지를 최소화하기 위해 나노 크기의 덩어리진 입자 형태로 변화한다. 여기서 형성되는 나노입자의 크기가 렌즈 표면 중심에서 가장자리로 갈수록 작아진다는 것을 주사전자현미경을 통해 확인하였다. 증착 각도가 증가할수록 열처리 공정 후의 은 나노입자의 크기가 점점 작아진다는 것을 검증하기 위해 은 박막의 증착 각도를 $0^{\circ}$, $35^{\circ}$, $55^{\circ}$, $70^{\circ}$로 증착 후 열처리 공정을 진행하여 확인하였다. 비스듬하게 증착되어 형성된 박막은 다공형태로 낮은 밀도를 가지는데 이는 박막 두께 감소를 일으킨다. 따라서 증착 각도가 증가할수록 열처리 공정 후의 은 나노입자의 크기는 점점 작아진다. 이후 은 나노입자를 마스크로 하여 다시 반응성이온식각 공정을 진행하였으며 식각 후 나머지 은 나노입자들은 HNO3용액에서 1분간 처리하여 제거하였다. 제작된 구조물의 평균 직경과 크기는 각각 ~220nm 및 ~250nm인 것으로 확인하였다. 위와 같은 공정을 통해 다양한 크기를 가진 비주기 서브파장 구조물을 제작할 수 있다. 구조물의 주기가 파장 길이보다 짧을 경우 분산이 최소화되며 넓은 파장 대역에서 무반사 효과를 얻을 수 있다. 이 공정은 마스크를 통한 리소그래피의 한계를 극복할 수 있으며 여러 곡면형 표면에 적용가능한 장점이 있다. 또한 프리즘, 렌즈, 광섬유와 같은 광소자의 광투과율을 향상시키는데 이용될 수 있다.

• Journal of the Korean Society of Radiology
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• v.14 no.3
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• pp.279-287
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• 2020

Recently, interest in radiation protection is increasing because of the occurrence of accidents related to exposure dose. So, the nuclear safety act provides to install the shields to avoid exceeding the dose limit. In particular, when the worker conducts the non-destructive testing (NDT) without the fixed shielding structure, we should monitor the access to the workplace based on a constant dose rate. However, when we apply for permits for NDT work in these work environments, the consideration factors to the estimation of the distance and exposure dose are not legally specified. Therefore, we developed the excel model that automatically calculates the distance, exposure dose, and cost if we input the factors. We applied the assumption data to this model. As a result of the application, the distance change rate was low when the thickness of the lead blanket and collimator is above 25 mm, 21.5 mm, respectively. However, we didn't consider the scattering and build-up factor. And, we assumed the shape of the lead blanket and collimator. Therefore, if we make up for these limitations and use the actual data, we expect that we can build a database on the distance and exposure dose.

• The Journal of Korean Society for Radiation Therapy
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• v.21 no.2
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• pp.89-95
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• 2009

Purpose: The purpose is to evaluate efficiency of the CT simulator QA phantom manufactured for daily QA. Materials and Methods: We made holes ($1{\times}100{\times}1\;mm$) to verify accuracy between image and real measurement in polystyrene phantom and made 1 mm holes to verify table movement accuracy at superior and inferior 100 mm to the center of the phantom and inserted radiopacity material. To evaluate laser alignment, we made cross mark on the right and left side at phantom and to evaluate CT number accuracy we made 3 cylindrical holes and inserted equivalence material of bone, water, air in them. After CT scanning the phantom, We evaluated accuracy between image and real measurement, accuracy of table movement, laser, and CT number using exposed image. Results: It was measured that the accuracy between image and real measurement was ${\pm}0.3\;mm$, table movement accuracy was ${\pm}0.3\;mm$, laser accuracy was ${\pm}0.5\;mm$ from 7th January to 7th March in 2008 as within the reference point ${\pm}1\;mm$. In the CT number accuracy of bone was ${\pm}10\;HU$, air was ${\pm}5\;HU$, water was ${\pm}5\;HU$ as within the reference point is ${\pm}10\;HU$. Conclusion: We was able to perform CT simulator QA and laser equipment QA more conveniently and fast using manufactured phantom at the same time. We will be able to make more accurate treatment plan that added to QA procedures using images at previous daily QA.