한국해양대학교

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이중 구리선을 이용한 THz 도파관의 전파특성

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dc.contributor.author 조정상 -
dc.date.accessioned 2017-02-22T06:52:41Z -
dc.date.available 2017-02-22T06:52:41Z -
dc.date.issued 2013 -
dc.date.submitted 57014-11-26 -
dc.identifier.uri http://kmou.dcollection.net/jsp/common/DcLoOrgPer.jsp?sItemId=000002175683 ko_KR
dc.identifier.uri http://repository.kmou.ac.kr/handle/2014.oak/9950 -
dc.description.abstract In this paper, we have described the various characteristics of the two-wire transmission lines. The lines consist of two 0.4mm (or 0.5mm) diameter copper wires with centers separated by 1.0mm. Scattering coupling is generally used in order to combine the THz wave with two-wire lines in the previous study. Instead of this method, we have used two tungsten probes with 1 μm diameter tips in near-contact with the pulse generating and receiving antennas. It can improve the coupling efficiency because the dipole antenna radiation pattern is similar to the propagation mode on two-wire transmission lines. We have made the waveguide holder with wide bandwidth, high efficiency by Teflon disk experiments of various forms. But, the remaining serious practical problem is how to support the wires and how to maintain their separation without disturbing the TEM mode propagation for long distance. To solve this problem, we have fabricated the two-wire lines using Teflon tube. The 150 μm thick Teflon covered two-wire lines are prepared by removing the two original stranded wires separated by 1.0 mm between the wire centers from the commercial Teflon covered two-wire lines and replacing them with the same solid Cu wire used in the air spaced two-wire lines. A single wire waveguide have high attenuation when the waveguide were curved, and Parallel-plate waveguide has the drawback of bending setup. Unlike other waveguide, two-wire waveguide has the advantage of bending experimental configuration with low attenuation. We also investigate the bend characteristics of two-wire waveguide. -
dc.description.tableofcontents 목 차 List of Figures ·································································································· iii Abstract ················································································································ v 1. 서 론 ············································································································· 1 2. 본 론 2.1 이중 구리선 도파관 ····························································································· 4 2.1.1 실험 장치 구성 ·························································································· 4 2.1.2 테플론 고정대의 형태에 따른 효율 ······················································ 7 2.1.3 이중 구리선 도파관의 전파 특성 ························································ 12 2.1.4 이중 구리선 도파관의 굽힘 특성 ························································ 18 2.1.5 이중 구리선 도파관의 굽힘 특성을 이용한 THz 분배기 ·············· 21 2.2 테플론 코팅된 이중 구리선 도파관 ······························································· 24 2.2.1 실험 장치 구성 ························································································ 24 2.2.2 도체에 따른 테플론 코팅된 이중 구리선 도파관의 특성 ·············· 26 2.2.3 테플론 코팅된 이중 구리선 도파관의 전파 특성 ···························· 29 2.2.4 테플론 코팅된 이중 구리선 도파관의 굽힘 특성 ···························· 33 3. 결론 ·················································································································· 37 참고문헌 ············································································································ 39 -
dc.language kor -
dc.publisher 한국해양대학교 -
dc.title 이중 구리선을 이용한 THz 도파관의 전파특성 -
dc.title.alternative Propagation Properties of Terahertz radiation on Two-Wire Waveguide -
dc.type Thesis -
dc.date.awarded 2013-02 -
dc.contributor.alternativeName Jeong sang Jo -
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전기전자공학과 > Thesis
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