• Title/Summary/Keyword: Surface phase change

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Impact of Sea Surface Scattering on Performance of QPSK (해면산란이 QPSK 성능에 미치는 영향)

  • Xue, Dandan;Seo, Chulwon;Park, Jihyun;Yoon, Jong Rak
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.18 no.8
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    • pp.1818-1826
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    • 2014
  • Time-variant sea surface causes a forward scattering and Doppler spreading in received signal on underwater acoustic communication system. This results in time-varying amplitude, frequency and phase variation of the received signal. In such a way the channel coherence bandwidth and fading feature also change with time. Consequently, the system performance is degraded and high-speed coherent digital communication is disrupted. In this paper, quadrature phase shift keying (QPSK) performance is examined in two different sea surface conditions. The impact of sea surface scattering on performance is analyzed on basis of the channel impulse response and temporal coherence using linear frequency modulation (LFM) signal. The impulse response and the temporal coherence of the rough sea surface condition were more unstable and less than that of the calm sea surface condition, respectively. By relating these with time variant envelope, amplitude and phase of received signal, it was found that the bit error rate (BER) of QPSK are closely related to time variation of sea surface state.

Phase Change Characteristics of Ge-Se-Te Thin Film for PRAM (PRAM을 위한 Ge-Se-Te 박막의 상변환 특성)

  • Shin, Jae-Ho;Kim, Byung-Cheul;Yeo, Jong-Bin;Lee, Hyun-Yong
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.24 no.12
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    • pp.982-987
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    • 2011
  • In this study, $Ge_8Se_{(2+x)}Te_{(6-x)}$ thin film amorphous-to-crystalline phase-change rate was evaluated in using a nano-pulse scanner. The focused laser beam with a diameter <10 ${\mu}m$ was illuminated in the power (P) and pulse duration (t) ranges of 1-31 mW and 10-460 ns, respectively, with subsequent detection of the responsive signals reflected from the film surface. We also evaluated the material characteristics, such as optical absorption and energy gap, crystalline phases, and sheet resistance of as-deposited and annealed films. The result of experiments showed that the thermal stability of the Ge-Se-Te film is largely improved by adding Se.

Probing of Microscale Phase-Change Phenomena Based on Michelson Interforometry (Michelson 간섭계를 응용한 미세 상변화 현상 계측)

  • Kim, Dong-Sik;Park, Hee-K.;Grigoropoulos, Costas P.
    • Proceedings of the KSME Conference
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    • 2001.06d
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    • pp.348-353
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    • 2001
  • Experimental schemes that enable characterization of phase-change phenomena in the micro scale regime is essential for understanding the phase-change kinetics. Particularly, monitoring rapid vaporization on a submicron length scale is an important yet challenging task in a variety of laser-processing applications, including steam laser cleaning and liquid-assisted material ablation. This paper introduces a novel technique based on Michelson interferometry for probing the liquid-vaporization process on a solid surface heated by a KrF excimer laser pulse (${\lambda}=248nm,\;FWHM=24\;ns$) in water. The effective thickness of a microbubble layer has been measured with nanosecond time resolution. The maximum bubble size and growth rate are estimated to be of the order of $0.1{\mu}m\;and\;1\;m/s$, respectively. The results show that the acoustic enhancement in the laser induced vaporization process is caused by bubble expansion in the initial growth stage, not by bubble collapse. This work demonstrates that the interference method is effective for detecting bubble nucleation and microscale vaporization kinetics.

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Probing of Microscale Phase-Change Phenomena Based on Michelson Interforometry (Michelson 간섭계를 응용한 미세 상변화 현상 계측)

  • Kim, Dong-Sik;Park, Hui-Gwon;Grigoropoulos, Costas-P.
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.25 no.8
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    • pp.1140-1147
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    • 2001
  • Experimental schemes that enable characterization of phase-change phenomena in the microscale regime are essential for understanding the phase-change kinetics. Particularly, monitoring rapid vaporization on a submicron length scale is an important yet challenging task in a variety of laser-processing application, including steam laser cleaning and liquid-assisted material ablation. This paper introduces a novel technique based on Michelson interferometry for probing the liquid-vaporization process on a solid surface heated by a KrF excimer laser pulse(λ=248nm, FWHM=24ns) in water. The effective thickness of a microbubble layer has been measured with nanosecond time resolution. The maximum bubble size and growth rate are estimated to be of the order of 0.1㎛ and 1m/s, respectively. The results show that the acoustic enhancement in the laser induced vaporization process is caused by bubble expansion in the initial growth stage, not by bubble collapse. This work demonstrates that the interference method is effective for detecting bubble nucleation and microscale vaporization kinetics.

Thermal Storage and Thermodynamic Characteristics of Phase Change Materials Slurries

  • Kwon, Ki-Hyun;Jeong, Jin-Woong;Kim, Jong-Hoon;Kim, Yong-Joo;Choi, Chang-Hyun
    • Food Science and Biotechnology
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    • v.18 no.6
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    • pp.1392-1397
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    • 2009
  • This study was aimed at developing a low cost cold storage system for agricultural products. Three kinds of slurries: $K_1$, $K_2$, and $K_3$ slurries were developed using phase change materials (PCMs) such as tetradecane, octadecane, and sodium polyacrylate to maintain the desired temperature ranges. The slurries were manufactured by in-situ polymerization. Tetradecane and octadecane were capsulated in a core with melamine at the surface. The thermodynamic characteristics of the slurries were measured and analyzed. The latent heats of the $K_1$, $K_2$, and $K_3$ slurries at the melting points were 206.41, 186.88, and 147.91 kJ/kg, respectively. A transportable cold storage container was built to investigate the performance of the slurries as thermal storage media. The temperatures at the insides of the container could be maintained in the ranges of 0-5, 5-10, and $10-15^{\circ}C$ for more than 23, 27, and 60 hr with the $K_1$, $K_2$, and $K_3$ slurries, respectively.

Phase Changes of the STS 431 Martensitic Stainless Steel after High Temperature Gas Nitriding Treatment (STS 431 마르텐사이트계 스테인리스강의 고온 가스 질화 열처리에 따른 상변화)

  • Yoo, D.K.;Kong, J.H.;Lee, H.W.;Kang, C.Y.;Kim, Y.H.;Sung, J.H.
    • Journal of the Korean Society for Heat Treatment
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    • v.21 no.5
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    • pp.244-250
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    • 2008
  • This study has investigated the surface phase change, hardness variation, surface precipitates, nitrogen content and corrosion resistance in STS 431 (17Cr-2Ni-0.2C-0.01Nb) martensitic stainless steel after high temperature gas nitriding (HTGN) treatment at the temperature range between $1050^{\circ}C$ and $1150^{\circ}C$. The HTGN-treated surface layer appeared $Cr_2N$ of rod type, carbo-nitride of round type and fine precipitates in the austenite matrix. On the other hand the interior region where the nitrogen was not permeated, exhibited martensite phase. The surface hardness showed 250~590 HV, depending on the HTGN treatment conditions, while the interior martensitic phase represented 520 HV. The permeation depth of nitrogen increased with increasing the HTGN-treated temperature. The nitrogen concentration of the surface layer appeared approximately ~0.17% at $1100^{\circ}C$. On comparing the corrosion resistance between solution-annealed and HTGN-treated steels, the corrosion resistance of HTGN-treated steel was superior to that of solution-annealed specimens.

A phase transformation model for burning surface in AP/HTPB propellant combustion (AP추진제의 연소면 형성 및 전파 모델링 연구)

  • Jung, Tae-Yong;Doh, Young-Dae;Yoo, Ji-Chang;Yoh, Jack Jai-Ick
    • Journal of the Korean Society for Aeronautical & Space Sciences
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    • v.38 no.4
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    • pp.363-368
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    • 2010
  • In the solid rocket propellant combustion, the dynamic phase change from solid to liquid to vapor occurs across the melt layer. During the surface burning, liquid and gas phases are mixed in the intermediate zone between the propellant and the flame to form micro scale bubbles. The known thickness of the melt layer is approximately 1 micron at $10^5$ Pa. In this paper, we present a model of the melt layer structure and the dynamic motion of the melt front derived from the classical phase field theory. The model results show that the melt layer grows and propagates uniformly according to exp(-1/$T_s$) with $T_s$ being the propellant surface temperature.

Changes of Surface Electromyography on Frontalis Muscle during Electro-Acupuncture Stimulation of Abdomen or Legs - A Pilot Study for Clinical Approach to Autonomic Nervous System Changes - (복부 및 사지 부위의 전기침 자극이 전두근에서 측정한 SEMG 변화에 미치는 영향 - 자율신경계의 변화에 대한 임상적 접근을 위한 사전 연구 -)

  • Je, Jun-Tae;Choi, San-Ho;Shin, Sun-Ho;Lim, Jin-Young;Lee, Sang-Kwan
    • The Journal of Internal Korean Medicine
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    • v.33 no.1
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    • pp.14-25
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    • 2012
  • Objectives : To observe physiological changes during clinical acupuncture treatment. Methods : We recruited 40 healthy volunteers who had experienced an acupuncture treatment at least once within the past three years. The experimental group was divided into four groups according to the needling site and frequency of electrical stimulation. Sites consisted of abdomen and legs. Frequencies consisted of 100 Hz and 2 Hz. The procedures of experimental treatment consisted of seven phases, Resting I phase (Resting I), Needle insertion phase (Insertion), Maintenance of needle insertion I phase (Maintain I), Electrical stimulation phase (ES), Maintenance of needle insertion II phase (Maintain II), Needle removal phase (Removal) and Resting II phase (Resting II). We measured the surface electromygraphy (SEMG) through an electrode on the frontalis muscle during all phases consecutively. Results : When SEMGs of all seven phases were analyzed, they significantly increased or decreased according to phases. SEMGs of Insertion, Maintain I, ES and Maintain II phase significantly increased more than RestingI in abdomen and legs groups. SEMGs of the abdomen group were measured as being $4.78{\pm}0.74{\mu}V$ on Resting I, $16.48{\pm}3.97{\mu}V$ on Insertion, $46.31{\pm}10.56{\mu}V$ on Maintain I, $45.88{\pm}9.72{\mu}V$ on ES, $45.56{\pm}9.69{\mu}V$ on Maintain II, $18.76{\pm}3.05{\mu}V$ on Removal, and $3.75{\pm}0.65{\mu}V$ on Resting II. SEMGs of the legs group were measured as being $3.34{\pm}0.35{\mu}V$ on Resting I, $12.11{\pm}1.76{\mu}V$ on Insertion, $36.74{\pm}6.99{\mu}V$ on Maintain I, $33.57{\pm}6.30{\mu}V$ on ES, $32.66{\pm}6.03{\mu}V$ on Maintain II, $14.08{\pm}2.15{\mu}V$ on Removal, and $2.88{\pm}0.32{\mu}V$ on Resting II. Conclusions : SEMG changed differently according to processes of acupuncture. Electrical stimulation showed different change of SEMG. Thus, acupuncture treatment may change the status of the autonomic nervous system.

Surface acoustic wave gas sensors by assembling gas chromatography column (가스 크로마토그래피를 부착한 표면탄성파 가스 센서)

  • Yoo, Beom-Keun;Park, Yong-Wook;Kang, Chong-Yun;Yoon, Seok-Jin;Choi, Doo-Jin;Kim, Jin-Sang
    • Journal of Sensor Science and Technology
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    • v.16 no.1
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    • pp.39-43
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    • 2007
  • This paper presents characteristics of surface acoustic wave (SAW) gas sensor for detecting volatile gases such as acetone, methanol, and ethanol by measuring phase shift of output signal. A delay-line by combining with a center frequency of 200 MHz was fabricated on S-T Quartz substrates. Using gas chromatography column, the selectivity of the SAW gas sensor were introduced. Experimental results, which show the phase change of output signal under the absorption of volatile gas on sensor surface, were presented. This SAW gas sensor system may be well suited for a high performance electronic nose system.

Development of viscosity sensor using surface acoustic wave (탄성 표면파를 이용한 점도 센서의 개발)

  • Chong, Woo-Suk;Kim, Gi-Beum;Kang, Hyung-Sub;Hong, Chul-Un
    • Journal of Sensor Science and Technology
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    • v.17 no.4
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    • pp.289-294
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    • 2008
  • The purpose of this study is to materialize the viscosity sensor by using the SH-SAW sensor of which the center frequency is operated at higher than 50 MHz. In order to measure the viscosity, SAW sensor of which the center frequency is operated at 100 MHz is developed. By using the developed sensor, phase shift, delay time, insertion loss, and frequency variation are measured at different viscosity. The result shows that the phase shift difference between the viscosity variations is such that the difference between the distilled water and the 100 % glycerol solution is approximately $45^{\circ}$, the change of the insertion loss is approximately 9 dB, and the difference of frequency variation is approximately 5.9 MHz. Therefore, it is shown that viscosity of unknown solution can be measured with the surface acoustic wave sensor.