• Title/Summary/Keyword: mmWave

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MMB System and Channel Model for 5th Generation Mobile Communication (5세대 이동통신을 위한 MMB 시스템 및 채널 모델)

  • Moon, Sangmi;Kim, Bora;Malik, Saransh;Kim, Jihyung;Lee, Moon-Sik;Kim, Daejin;Hwang, Intae
    • Journal of the Institute of Electronics and Information Engineers
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    • v.51 no.8
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    • pp.3-10
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    • 2014
  • Millimeter wave (mmWave) has attracted great interest recently and the necessity of Millimeter Mobile Broadband (MMB) system has appeared based on the 4 Generation Long Term Evolution-Advanced (LTE-A) Specification. Currently, there are many studies about the mmWave communication channel. And it is subject of interest to analyze the performance in MMB channel environments. In this paper, we design the MMB system for 5th Generation mobile communication and propose channel models through the analysis of the mmWave propagation characteristics. Also, we have analyzed the performance of the MMB system of 28 GHz band in MMB channel environments.

Acoustic Characteristics of Sand Sediment with Circular Cylindrical Pores in Water (수중 원통형 다공성 모래퇴적물의 음향특성)

  • 윤석왕;이용주;노희설
    • The Journal of the Acoustical Society of Korea
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    • v.21 no.2
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    • pp.110-119
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    • 2002
  • Acoustic characteristics of water sediment were experimentally studied in laboratory. Water saturated sand sediment less than the grain size of 0.5 mm diameter is uniformly distributed in an acryl box (100 mm×100mm×42mm) with material thickness 1 mm. Pores in the acryl box are modeled as the structure of cylindrical pore tubes (diameter 3 mm and length 42 mm) filled with water. Cylindrical pore tubes have porosities 0%, 5%, 11%, 18% and 26 % controlled by the tube numbers. Transmitted acoustic waves through sand sediment specimen are analyzed as the functions of porosity and frequency from 0.3 MHz to 4 MHz. Transmitted acoustic waves are mixed with the first-kind wave from whole specimen and the second-kind wane from cylindrical pore tubes. For the center frequency 1 MHz, the first kind wave is dominant but for the center frequency 2.25 MHz, the second kind wave is dominant. In the case of the first-kind wave, as the porosity increases, the transmission coefficient decreases and the sound speed decreases to the sound speed of water. As the frequency increases, the transmission coefficient decreases but the sound speed is almost constant. In the case of the second-kind wave, as the porosity increases, the transmission coefficient increases but the sound speed is almost constant. The transmission coefficient and the sound speed are almost constant as a function of frequency.

DC ∼ 45 GHz CPW Wideband Distributed Amplifier Using MHEMT (MHEMT를 이용한 DC ∼ 45 GHz CPW 광대역 분산 증폭기 설계 및 제작)

  • Jin Jin-Man;Lee Bok-Hyung;Lim Byeong-Ok;An Dan;Lee Mun-Kyo;Lee Sang-Jin;Ko Du-Hyun;Beak Yong Hyun;Oh Jung-Hun;Chae Yeon-Sik;Park Hyung-Moo;Kim Sam-Dong;Rhee Jin-Koo
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.41 no.12
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    • pp.7-12
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    • 2004
  • In this paper, CPW wideband distributed amplifier was designed and fabricated using 0.1 $\mum$ InGaAs/InAlAs/GaAs Metamorphic HEMT(High Electron Mobility Transistor). The DC characteristics of MHEMT are 442 mA/mm of drain current density, 409 mS/mm of maximum transconductance. The current gain cut-off frequency(fT) is 140 GHz and the maximum oscillation frequency(fmax) is 447 GHz. The distributed amplifier was designed using 0.1 $\mum$ MHEMT and CPW technology. We designed the structure of CPW curve, tee and cross to analyze the discontinuity characteristics of the CPW line. The MIMIC circuit patterns were optimized electromagnetic field through momentum. The designed distributed amplifier was fabricated using our MIMIC standard process. The measured results show S21 gain of above 6 dB from DC to 45 GHz. Input reflection coefficient S11 of -10 dB, and output reflection coefficient S22 of -7 dB at 45 GHz, respectively. The chip size of the fabricated CPW distributed amplifier is 2.0 mm$\times$l.2 mm.

Channel Modeling and RF Performance Verification in mmWave Bands Based on NS-3 (NS-3 기반의 mmWave 대역 채널 모델링 및 RF 성능 검증)

  • Seung-Min Lee;Jun-Seok Seo;Hong-Je Jang;Myung-Ryul Choi
    • Journal of IKEEE
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    • v.27 no.4
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    • pp.650-656
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    • 2023
  • This paper implements a channel model for mmWave bands using an NS-3-based 5G system-level simulator and analyzes the reliability and validity of the implemented model through RF performance verification. The channel model for RF performance verification in the mmWave bands consider parameters such as characteristics defined in 3GPP TR 38.901, beam-forming, antenna configuration, scenarios, among others. Furthermore, the simulation results verify compliance within the ranges permitted by the 3GPP standards and verify reliability in indoor environmental scenarios by exploiting the Radio Environment Map (REM). Therefore, the channel model implemented in this study is applicable to the actual design and establishment of 5G networks, presenting a method to evaluate and validate RF performance by adjusting various parameters.

Study on Stress Waves for Development of Glulam from Domestic Small Diameter Log(I) - Effect of MC on Stress Wave in Glulam Member - (국산 소경재를 이용한 집성재 개발을 위한 응력파 연구(I) - Glulam 부재의 응력파에 대한 함수율 영향 -)

  • Cha, Jae-Kyung
    • Journal of the Korean Wood Science and Technology
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    • v.24 no.3
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    • pp.90-100
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    • 1996
  • 두께가 20mm 와 30mm 이고, 폭이 40mm 와 60mm인 600mm 길이의 낙엽송 제재목에 응력파 시험을 실시하였다. 모든 시험편은 생재 상태로 구입 후 함수율 27%, 22%, 17%과 12%조건으로 조습 처리하였다. 함수율 변화에 따른 응력파 속도와 영계수를 구하기 위한 응력파 시험을 4종류의 함수율 조건에서 실시하였다. 응력파 속도와 응력파 시험으로부터 구한 영계수는 시편의 함수율, 치수, 그리고 시험편의 옹이와 옹이 주변 목리의 상호작용에 의해 영향을 받았다. 모든 함수율 및 각 함수율 조건에서 응력파 속도는 응력파에 의해 구한 영계수와 양호한 상관관계를 나타냈다. 응력파 속도와 응력파 시험으로 구한 영계수는 함수율이 증가할 때 비선형적으로 감소하였으나, 함수율 25% 이상에서는 응력파에 의해 구한 영계수의 변화가 거의 없었다.

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Development of Electromagnetic Wave Absorbers far Mobile Phone Using Sendust (Sendust를 이용한 휴대전화용 전파 흡수체의 개발)

  • Choi Jung-Hyun;Kim Dong-Il;Song Jae-Man;Jung Jae-Hyun
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
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    • v.16 no.8 s.99
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    • pp.842-847
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    • 2005
  • In this paper, we fabricated sheet-type EM wave absorbers for mobile phones by using sendusts and tested EM wave absorption of it. The band-width of EM wave absorbers coated with $Al_2O_3$ were larger than non-coated EM wave absorbers. Particle size decreased with increasing milling time, which made the result of increasing of EM wave absorption. The fabricated EM wave absorbers show a reflection coefficient 17.4 dB at 946 MHz for a 4 mm sample and 5 dB at 1.8 GHz for a 1 mm sample.

A Millimeter-Wave LC Cross-Coupled VCO for 60 GHz WP AN Application in a 0.13-μm Si RF CMOS Technology

  • Kim, Nam-Hyung;Lee, Seung-Yong;Rieh, Jae-Sung
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.8 no.4
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    • pp.295-301
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    • 2008
  • Recently, the demand on mm-wave (millimeter-wave) applications has increased dramatically. While circuits operating in the mm-wave frequency band have been traditionally implemented in III-V or SiGe technologies, recent advances in Si MOSFET operation speed enabled mm-wave circuits realized in a Si CMOS technology. In this work, a 58 GHz CMOS LC cross-coupled VCO (Voltage Controlled Oscillator) was fabricated in a $0.13-{\mu}m$ Si RF CMOS technology. In the course of the circuit design, active device models were modified for improved accuracy in the mm-wave range and EM (electromagnetic) simulation was heavily employed for passive device performance predicttion and interconnection parasitic extraction. The measured operating frequency ranged from 56.5 to 58.5 GHz with a tuning voltage swept from 0 to 2.3 V. The minimum phase noise of -96 dBc/Hz at 5 MHz offset was achieved. The output power varied around -20 dBm over the measured tuning range. The circuit drew current (including buffer current) of 10 mA from 1.5 V supply voltage. The FOM (Figure-Of-Merit) was estimated to be -165.5 dBc/Hz.

A Study on the Reliability of Detecting Reinforcement Embedded in Concrete in Various Factors Using Electromagnetic Induction Method and Electromagnetic Wave Method (전자기유도법과 전자파레이더법을 이용한 각종인자에 따른 철근탐사의 신뢰성에 관한 연구)

  • Kim, Jong-Ho;Oh, Kwang-Chin;Park, Seung-Bum
    • Journal of the Korea institute for structural maintenance and inspection
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    • v.12 no.4
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    • pp.179-186
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    • 2008
  • Probing inside of concrete structures is one of the important steps in assessing condition of the structure. For the assessment, electromagnetic induction method and electromagnetic wave method are currently applied to the measurement of cover depth, and the detection of reinforcement embedded in concrete. To determine detection capability of locating reinforcement embedded in concrete, commercially available nondestructive testing (NDT) equipments have been tested. The equipments include electromagnetic wave system and electromagnetic induction system. In the tests, nine concrete specimens which have the dimensions of 1,000mm(length))${\times}$300mm(width) with thickness varying from 125mm to 150mm are used. The reinforcement are located at 45, 60, 100mm depth from the concrete surface. Horizontal reinforcement spacing has been set over 100mm. From the outcome, it is shown that error is increased as the diameter of reinforcement enlarge in case of using electromagnetic induction method. In case of using electromagnetic wave method, the detection of reinforcement embedded in deep is good in the view of reliability because of using the relative permittivity on the real cover depth.

COMPARISON OF APICAL SEALING EFFICACIES USING DIFFERENT PLUGGING DEPTH IN CONTINUOUS WAVE OF OBTURATION TECHNIQUE (Continuous wave of obturation technique에서 플러거의 다양한 적용 깊이에 따른 근단부 폐쇄효율 비교)

  • Lee, Sang-Jin;Park, Jeong-Kil;Hur, Bock;Kim, Hyeon-Cheol
    • Restorative Dentistry and Endodontics
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    • v.32 no.6
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    • pp.491-497
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    • 2007
  • The purpose of this study was to compare apical sealing ability of continuous wave canal filling technique according to various heat source plugging depths. Eighty one extracted human premolars with straight root were cleaned and shaped to size 35 using .06 taper rotary NiTi file. After cleansing and shaping, the teeth were divided into 5 groups following the heat source probing depths from the apex; 3, 4, 5, 6 and 7 mm. All specimens were filled using E&Q plus with #35/.06 tapered gutta-percha cone. The positive control teeth were not filled. All teeth were coated with nail varnish except the apical 1 mm around the apical foramen. Negative control teeth were completely sealed include the apical foramen. All specimens were immersed in 1% methylene blue solution for 72 hours. Then the specimens were sectioned horizontally at 1, 2 and 3 mm from the root apex. Each sectioned surface was photographed using a digital camera attached to the stereomicroscope at $12.5{\times}2.5$ fold magnification. All points at 1, 2 and 3 mm were summed as final score of one specimen. Statistical analysis of the collected data was performed. Under the condition of this study. there was no significant difference between the heat source plugging depths of 3, 4, 5, 6 and 7 mm in apical sealing ability. All of apical heat source plugging depth from 3 to 7 mm including Buchanan's protocol -from 5 to 7 mm- seems to be acceptable in clinical application.

Inspection on the acoustic output of the focused extracorporeal focused shock wave therapeutic devices approved by MFDS (식약처에서 허가된 집속형 ESWT 치료기의 음향 출력 분석)

  • Choi, Min Joo;Jeon, Sung Joung;Kwon, Oh Bin;Lee, Min Young;Cho, Jin Sik;Kim, Han Soo;Maeng, Eun Ho
    • The Journal of the Acoustical Society of Korea
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    • v.39 no.4
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    • pp.303-317
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    • 2020
  • Extracorporeal Shock Wave Therapy (ESWT) is an innovative treatment in chronic musculoskeletal pain management and cardiovascular diseases. In this study, we surveyed the acoustic shock wave outputs from the domestically used focal type ESWT devices. The survey data were collected through 30 technical documents registered to the Ministry of Food and Drug Safety (MFDS), Rep. Korea. The results show that the focusing geometry varies largely, 5 mm to 65 mm in the focal length, 3 mm to 30 mm in focal width, and 4 mm to 108 mm in focal depth. The maximum positive pressure (P+) ranges from 7 MPa to 280 MPa, the focal Energy Flux Density (EFD) from 0.0035 mJ/㎟ to 35 mJ/㎟, and the energy per pulse (E) from 0.737 mJ to 80.86 mJ. All domestic PE-type (five) and one EM-type domestic devices included in the analysis of the correlation between P+ and EFD are shown to be far beyond the usual ranges and do not comply with expected correlation so that the reliability of their data was suspected. For the suspected, post-performance tests are required by a recognized testing agency. MFDS guidelines need to be revised so that the pass criteria for the shock wave acoustic outputs can be based on the clinical tests for indications.