• 한국전자파학회:학술대회논문집
• /
• 한국전자파학회 2005년도 종합학술발표회 논문집 Vol.15 No.1
• /
• pp.245-248
• /
• 2005

In this paper, small sized half-wavelength circular loop antenna which attached beneath a visor of helmet is designed and fabricated at the resonant frequency of 449MHz. To reduce the size of the antenna, double series-shorted stubs are inserted inside the loop for practical use of a vacant space of loop inside. Also, It is designed for the printed type to install the helmet easily. The size of antenna on helmet is reduced to 87.75%(diameter : 70mm, height :.36mm) compare with general type antenna(diameter : 200mm height 101mm). The return loss, -10dB bandwidth and gain are -13.2dB, 17.6MHz(3.9%), and -1.78dBd. And, radiation pattern is omni-directional pattern at H-plane. Therefore, it can be seen that the half-wavelength circular loop antenna using double series-shorted stubs is proper structure for the miniaturization and the installed antenna of the helmet.

• 한국전자파학회:학술대회논문집
• /
• 한국전자파학회 2003년도 종합학술발표회 논문집 Vol.13 No.1
• /
• pp.376-379
• /
• 2003

In this raper, proposed easy half-wavelength LPF and acceptor structure in actuality manufacture using EBG (Electromagnatic Bandgap) structure for application of micro-strip circuit. Because conventional half-wavelength LPF and acceptor is narrow line-width of High impedance, actuality manufacture is difficult. Width that in proposed structure narrow microstrip line of High impedance EBG structure use and has equal impedance embodied to wide microstrip line. Also, it is seen that actuality manufacture is available applying to half-wavelength LPF that have cut-off Frequency of 3GHz.

• 한국안광학회지
• /
• 제6권1호
• /
• pp.101-105
• /
• 2001

UV 차단 렌즈 UV solution을 이용한 dip method로 제작하여 광 투과율과 광 반사율을 측정하였다. 광 투과율의 half point 파장 및 edge 파장이 dip 시간의 존성인 exponetial decay형식에 잘 적용되었다. $$W=W_0+A_1{e}{x}{p}[-(x-x_1)/t_1]$$ 광 투과율의 half point 파장은 358 nm 에서 408 nm로 이용하였고, edge 파장은 340 nm에서 398 nm로 이동하였다. 광 반사율 주 peak 380 nm는 dip 시간이 클수록 세기는 작아지고 장파장 쪽으로 이동하였으며, dip 시간 10분에서 UV solution의 성분 peak가 나타나기 시작하였다.

• 한국소음진동공학회논문집
• /
• 제16권10호
• /
• pp.1057-1066
• /
• 2006

Acoustic streaming Induced by longitudinal vibration at 30 kHz is visualized for a test fluid flow between the stationary glass plate and ultrasonic vibrating surface with particle imaging velocimetry (PIV) To measure an increase in the velocity of air flow due to acoustic streaming, the velocity of air flow in a gap between the heat source and ultrasonic vibrator is obtained quantitatively using PIV. The ultrasonic wave propagating into air in the gap generates steady-state secondary vortex called acoustic streaming which enhances convective cooling of the stationary heat source. Heat transfer through air in the gap is represented by experimental convective heat transfer coefficient with respect to the gap. Theoretical analysis shows that gaps for maximum heat transfer enhancement are the multiple of half wavelength. Optimal gaps for the actual design are experimentally found to be half wavelength and one wavelength. A drastic temperature variation exists for the local axial direction of the vibrator according to the measurement of the temperature distribution in the gap. The acoustic streaming velocity of the test fluid in the gap is at maximum when the gap agrees with the multiples of half wavelength of the ultrasonic wave, which are specifically 6 mm and 12 mm.

• 한국전자파학회논문지
• /
• 제16권10호
• /
• pp.973-981
• /
• 2005

본 논문에서는 이동통신 단말기에 적합한 변형된 반 파장 로디드 라인 안테나를 설계 및 구현하였다. 제안된 안테나는 실험적인 PCB 위에 하나의 반 파장 로디드 라인 구조를 갖는 방사체, 유전체 기판, 급전봉과 두 개의 단락봉으로 구성되어져 있다. 두 개의 단락봉은 방사체의 양쪽 끝에 각각 배치되어 있으며, 집중형 인덕턴스 소자는 각각의 단락봉과 PCB 그라운드 사이에 놓여져 있다. 인덕터 값의 조절을 통하여 안테나의 공진 주파수와 입력 임피던스가 각각 조정되어질 수 있다. 제안된 안테나는 최대 12 nH의 인덕터 값의 범위 내에서 $1,470\~2,660\;MHz$의 넓은 동작 영역과 좋은 임피던스 정합 특성을 가지고 있다. 안테나의 최대 이득은 동작 영역내에서 $-0.45\~2.03\;dBi$로 측정되었다.

• 수산해양기술연구
• /
• 제46권2호
• /
• pp.173-183
• /
• 2010

In a split beam echo sounder, the transducer design needs to have minimal side lobes because the angular position and level of the side lobes establishes the usable signal level and phase angle limits for determining target strength. In order to suppress effectively the generation of unwanted side lobes in the directivity pattern of split beam transducer, the spacing and size of the transducer elements need to be controlled less than half of a wavelength. With this purpose, a 50 kHz tonpilz type transducer with a half-wavelength diameter in relation to the development of a split beam transducer was designed using the equivalent circuit model, and the underwater performance characteristics were measured and analyzed. From the in-air and in-water impedance responses, the measured value of the electro-acoustic conversion efficiency for the designed transducer was 51.6%. A maximum transmitting voltage response (TVR) value of 172.25dB re $1{\mu}Pa/V$ at 1m was achieved at 52.92kHz with a specially designed matching network and the quality factor was 10.3 with the transmitting bandwidth of 5.14kHz. A maximum receiving sensitivity (SRT) of -183.57dB re $1V/{\mu}Pa$ was measured at 51.45kHz and the receiving bandwidth at -3dB was 1.71kHz. These results suggest that the designed tonpilz type transducer can be effectively used in the development of a split beam transducer for a 50kHz fish sizing echo sounder.

• 대한전자공학회논문지
• /
• 제23권2호
• /
• pp.264-268
• /
• 1986

A thchnique has been studied for the measurement of the spectral loss and the cut-off wave length, at which the first high-order mode disappears. The near-field patterns of a fiber which is excited by a variable wavelength source are used for the measurement of cut-off wavelength. Because of the absorptive phenomenon of OH- molecular vibration, spectral loss of a single mode optical fiber sample is 5.6dB/km at 1380 nm wavelength and 1dB/km at 1240 nm wavelength. From the near field intensity patterns and the mode field diameter graph for the half power width, the cut-off wavelength of the fiber is measured to be 1120 nm.

• 조명전기설비학회논문지
• /
• 제24권12호
• /
• pp.33-37
• /
• 2010

In this paper, we have demonstrated absolute wavelength tuning in an optical fiber comb filter based on a polarization-diversity loop configuration by controlling the current injected into enameled wires wound on polarization-maintaining fibers (PMF's), that is, adjusting Joule heat generated from enameled wires. The proposed fiber comb filter consists of a polarization beam splitter, a half-wave plate, a quarter-wave plate, and PMF's. And we observed wavelength change of spectral dips in transmission spectra of the fabricated filter by varying an input current applied to enameled wires. The absolute wavelength of the filter could be controlled in proportional to the square of the input current with good linearity, and the rate of the wavelength shift with respect to the input current was measured as 36.79[nm/$A^2$].

• 대한전자공학회논문지SD
• /
• 제37권8호
• /
• pp.48-56
• /
• 2000

회절격자의 인접한 반주기 길이 사이에 음의 상관관계가 있는 회절격자 반주기의 랜덤 변이가 QWS-DFB 레이저의 특성에 미치는 영향을 유효 굴절률 전달 매트릭스 방법을 이용하여 해석하였다. 상관계수가 0에서 -1로 가까이 감에 따라 랜덤 변이에 의한 회절격자 주기의 오차가 감소하면서 단일모드 안정성과 파장 정확도의 저하가 덜 심각해진다. 이는 랜덤 변이의 크기가 같다면 상관관계가 없는 전자빔 lithography 법으로 회절격자를 만들기보다는 optical lithography 법으로 만드는 것이 회절격자 주기 랜덤 변이의 영향을 줄이는 데에 유리함을 의미한다. 그리고 전자빔 lithography를 이용하여 DFB 레이저를 만들 때에 랜덤 변이의 영향을 줄이려면 분해능을 높이거나, 인접 반주기 길이의 랜덤 변이에 음의 상관관계를 주어야 한다.

• Journal of electromagnetic engineering and science
• /
• 제16권3호
• /
• pp.159-163
• /
• 2016

In this paper, a frequency tunable double band-stop resonator (BSR) with voltage control by varactor diodes is suggested. It makes use of a half-wavelength shunt stub as its conventional basic structure, which is replaced by the distributed LC block. Taking advantage of the nonlinear relationship between the frequency and electrical length of the distributed LC block, a dual-band device can be designed easily. With two varactor diodes, the stop-band of the resonator can be easily tuned by controlling the electrical length of the resonator structure. The measurement results show the tuning ranges of the two operating frequencies to be 1.82 GHz to 2.03 GHz and 2.81 GHz to 3.03 GHz, respectively. The entire size of the resonator is $10mm{\times}11mm$, which is very compact.