• Proceedings of the KAIS Fall Conference
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• 2000.04a
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• pp.19.2-19
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• 2000

• 한국정보통신설비학회:학술대회논문집
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• 2002.08a
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• pp.137-139
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• 2002

본 논문은 FTTC용 공유급전시스템을 구성하기 위한 광동복합케이블 연구에 관련한 것이다. 광섬유 및 구리 도체를 하나의 케이블에 포함한 복합케이블은 공유급전 시스템에서 포설 비용 절감 및 서비스의 운용 및 유지 보수의 효율 향상을 가능하게 한다. KT 운용시스템연구소의 공유급전 시스템 구성에 따라서 세 가지 type의 광동복합 케이블을 설계하였다. 구리 도체로는 200Vdc 출력 전력을 최대 500m까지 급전을 지원하는 0.65mm 직경의 구리 도체가 선정되었으며 KT 규격을 만족하는 일반 단일모드 광섬유가 적용되었다. 케이블 구조는 다심화에 유리하고 중간분기가 용이한 loose tube형 구조를 채택하였으며, 다심 케이블에서는 stranding된 3층의 집합 코아를 가지도록 설계하였다. 다심의 광동복합케이블은 32심 광섬유와 18페어(pair)의 동선을 실장하여, 두 조의 케이블로 32개의 ONU의 광신호전송 및 전력 공급이 가능하도록 하였다. 또한 포설 및 중간 분기 작업시 광섬유로의 접근이 용이하게 하기 위해 광섬유 튜브를 최외층에 배치하였다. 복합케이블은 상용 loose tube형 광케이블과 동일한 공정으로 제작되었으며, 기계적 및 환경적 특성에서 KT 규격을 만족하는 것을 확인하였다.

• Korean Journal of Optics and Photonics
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• v.17 no.2
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• pp.127-135
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• 2006

We implement numerical simulations for the distributed optical fiber sensor system that uses the spatially-selective Brillouin scattering, by treating the superposition of the optical-frequency-modulated pump/probe waves in the time domain. We obtain temporal and spatial distributions of Brillouin gain for various cases. Simulations are applied to the case of concatenated optical fibers of different kinds and the case of distributed temperature along the fiber, which give reasonable results for the distributed sensor. The result of using a triangular wave instead of a sinusoidal one as a modulation waveform shows that the triangular wave modulation has an advantage in spatial resolution.

• Journal of the Korean Recycled Construction Resources Institute
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• v.6 no.3
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• pp.69-78
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• 2011

As recent concrete products changed to pursue high class, high quality, and high strength, as translucent concrete was developed to meet esthetic effects and exhibition purpose of structures. This study aims at introducing fabrication methods of various shapes of translucent concrete and evaluating feasibility of using mineral admixture such as fly ash, ground granulated blast furnace slag and granulated glass throughout experimental tests. As the result, it was found that compressive strength of translucent concrete block at 28 days is 32.2MPa and higher elastic modulus and Poisson's ratio than ordinary concrete block, which means that translucent concrete is widely applicable to structural purpose. Application of fly ash as a replacement of cement showed lower strength of 85 to 96% than Portland cement. In the meanwhile, ground granulated blast furnace slag showed 82 to 96% depending on the amount of replacement. The use of granulated glass as replacement of optical fiber was not applicable due to invisibility of light in concrete.

• Proceedings of the Optical Society of Korea Conference
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• 1989.02a
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• pp.140-142
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• 1989

1.54um 파장에서 최대 형광을 나타내는 ZrF4-BaF2-LaF3-AlF3-NaF : ErF3 유리를 built-in-casting 법에 의해 제조하였다. Er+3 이온을 0.2몰부터 4몰까지 첨가하였으며, Er+3 이온의 4I13/2 준위의 lifetime 은 Er+3 이온 0.2몰부터 2몰까지 28msec로 최대값을 갖으며 4몰일때는 급격히 감소하였다.

• Composites Research
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• v.13 no.5
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• pp.1-9
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• 2000

An intensity-based optical fiber vibration sensor is applied to monitor the structural vibration and detect impact locations on a plate. Optical fiber vibration sensor is constructed by placing two cleaved fiber end, one of which is cantilevered in a hollow glass tube. The movement of the cantilevered section lags behind the rest of the sensor in response to an applied vibration and the amount of light coupled between the two fibers is thereby modulated. For vibration sensing, optical fiber vibration sensor is mounted on the carbon fiber composite beam and its response is investigated to free and forced vibration. In impact location detection, four optical fiber vibration sensors whose location is predetermined are placed at chosen positions and the different arrival times of impact-generated vibration signal are recorded by an FFT analyzer. Impact location can be calculated from these time delays. Experimental results show that optical fiber vibration sensor signals coincide with gap sensor in vibration sensing. The precise location of impact can be detected on an acrylate plate.

• Journal of Sensor Science and Technology
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• v.9 no.2
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• pp.96-105
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• 2000

Fiber optic TR-EFPI(total reflected extrtinsic Fabry-Perot interferometric) sensor was developed to measure the strain of structures, such as building, bridge, aircraft, etc. It has been difficult to distinguish the increase and decrease of the strain from the conventional fiber optic EFPI sensor because their signals only have a sinusoidal wave pattern related to the change of strain. Also, the absolute strain could not be measured by the simple fiber optic EFPI sensor. In this study, in order to measure the magnitude of strain with the direction of strain, the fiber optic sensor was simply constructed with the total reflected EFPI sensor probe. This probe was manufactured with a single mode fiber and a mirror coated fiber in a silica glass capillary tube. The output signal of this fiber optic TR-EFPT sensor can give the information about the magnitude and the direction of strain. The loading-unloading test was performed by the universal testing machine with alluminum beam specimen to compare the strain from fiber optic TR-EFPI sensor with the value from electrical strain gauge. In the result of this experiment. the strain from fiber optic TR-EFPI sensor had a good agreement with the values from the electrical strain gauge.

• Proceedings of the KAIS Fall Conference
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• 2000.10a
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• pp.169-172
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• 2000

본 실험에서는 광Link로 응용될 Core Glass와 Clad Glass 및 Clad용 Polymer의 조성을 개발하고, Core용 Glass 와 Clad용 Glass의 match 및 Core Glass와 Clad용 Polymer의 효과적으로 접합 성형하여 반도체제조 설비내의 모든 Data 송ㆍ수신 Link를 Optical Fiber로 대체하여 기존 전선케이블이 전자기장의 영향으로 인한 Noise 와 Data 송ㆍ수신 오류를 일으키는 것을 방지하고자 한다. 따라서, 이에 대한 연구로 우선 유리를 사용한 기초 실험을 실시하였다. 실험 과정에 있어서는 Batch 실험과 용해 실험 및 물성 측정을 통하여 최적 조건의 유리를 선정하였다. 제조된 모유리를 사용하여 유리의 열적, 기계적 성질을 측정하였다. 또한 Glass core/Glass clad 파이버를 제조하여 광학적성질, 기계적성질, 구조적 특성을 평가하였다.

• Journal of the Korean Ceramic Society
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• v.39 no.12
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• pp.1158-1163
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• 2002

An Ge/B-doped optical fiber with high photosensitivity was fabricated to induce large second-order optical nonlinearity by UV poling. It was found that long period fiber gratings were inscribed on the fiber by the 248 nm KrF excimer laser irradiation with pulse energy of 116 mJ/$cm^2$ and pulse frequency of 10 Hz without hydrogen loading treatment. The photosensitivity was measured by use of the long period fiber grating pair method and the refractive index change of 3.3$10{\times}^{-3}$ was found to be induced in the core of the optical fiber by the KrF excimer laser irradiation of 8.67 kJ/$cm^2$. An H-shaped optical fiber was also fabricated for the UV poling through optimization of the fiber drawing condition.

• Journal of computational fluids engineering
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• v.16 no.1
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• pp.22-29
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• 2011

In this study, the glass fiber drawing from a silica preform in the furnace for the optical fiber manufacturing process is numerically simulated by considering the radiative heating of cylindrically shaped preform. The one-dimensional governing equations of the mass, momentum, and energy conservation for the heated and softened preform are solved as a set of the boundary value problems along with the radiative transfer approximation between the muffle tube and the deformed preform shape, while the furnace heating is modeled by prescribing the temperature distribution of muffle tube. The temperature-dependent viscosity of silica plays an important role in formation of preform neck-down profile when the glass fiber is drawn at high speed. The calculated neck-down profile of preform and the draw tension are found to be reasonable and comparable to the actual results observed in the optical fiber industry. This paper also presents the effects of key operating parameters such as the muffle tube temperature distribution and the fiber drawing speed on the preform neck-down profile and the draw tension. Draw tension varies drastically even with the small change of furnace heating conditions such as maximum heating temperature and heating width, and the fine adjustment of furnace heating is required in order to maintain the appropriate draw tension of 100~200 g.