• 제목/요약/키워드: Micro Plasma

검색결과 507건 처리시간 0.028초

Upregulation of MicroRNA 181c Expression in Gastric Cancer Tissues and Plasma

  • Cui, Mei-Hua;Hou, Xiao-Lin;Lei, Xiao-Yan;Mu, Fang-Hong;Yang, Gui-Bin;Yue, Lin;Fu, Yi;Yi, Guo-Xing
    • Asian Pacific Journal of Cancer Prevention
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    • 제14권5호
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    • pp.3063-3066
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    • 2013
  • Objective: To test the microRNA-181c (miR-181c) expression in tissues and plasma of gastric cancer (GC) cases, analyze any correlations, and explore the possibility of miR-181c as a potential molecular marker for GC diagnosis. Materials and Methods: Relative miR-181c expression levels in cancers and plasma from 30 GC patients was tested using reverse transcription-real-time fluorescent quantitation PCR and compared to that in samples from 30 gastric ulcer and 30 chronic gastritis patients. Results: The miR-181c expression level in the GC tissues was significantly higher than that in the gastric ulcer and chronic gastritis tissues (P = 0.000), as was the miR-181c expression level in the GC plasma (P = 0.000). We determined that miR-181c expression in GC plasma was positively correlated to its expression in the GC tissues (P = 0.000). Conclusions: The expression of miR-181c is upregulated in GC tissues and plasma, and the miR-181c expression level in GC plasma is positively correlated to that in the corresponding cancer tissues. Plasma miR-181c is possibly a new serological marker for GC diagnosis.

Micro-discharged plasma density, electron temperature and excited xenon density for enhancement of vacuum ultraviolet luminous efficiency in alternating current plasma display panel

  • Choi, Eun-Ha;Oh, Phil-Yong;Seo, Yoon-Ho;Cho, Guang-Sup;Uhm, Han-S
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2005년도 International Meeting on Information Displayvol.I
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    • pp.161-166
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    • 2005
  • The plasma ion density in AC-PDP has shown to be increased from $5.6{\times}10^{11}cm^{-3}$ to $9.0{\times}10^{11)cm^{-3}$ as the Xe mixture ratio to neon increase from 1 % to 10 %, respectively, at fixed pressure of 400 Torr, by using the micro-Langmuir probe. It is noted that the plasma ion density is density increases as the gas pressure increases in this experiment. The electron temperature decreases from 2.3 to 1.2 eV as the Xe mole fraction increases from 1 % to 10 % at fixed pressure of 400 Torr, which is measured by the micro Langmuir probe and high-speed ICCD camera in this experiment. It is noted that the electron temperature decreases as the gas pressure increases from 150 to 400 Torr in this experiment. It is also observed that the exited Xe atom density and the plasma ion density are in strong correlation sharp between each other in this experiment. It is noted that $5.2{\times}10^{12}cm^{-3}$ in the $1s_5$ metastable state and $1.2{\times}10^{12}cm^{-3}$ in the $1s_4$ resonance state for the PDP cell with gap of 50 um distances under the fixed gas pressure of 400 Torr and Xe content ratio of 10 %.

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Atmospheric Pressure Micro Plasma Sources

  • Brown, Ian
    • 한국표면공학회지
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    • 제34권5호
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    • pp.384-390
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    • 2001
  • The hollow cathode discharge is a kind of plasma formation scheme in which plasma is formed inside a hollow structure, the cathode, with current to a nearby anode of arbitrary shape. In this scheme, electrons reflex radially within the hollow cathode, establishing an efficient ionization mechanism for gas within the cavity. An existence condition for the hollow cathode effect is that the electron mean-free-path for ionization is of the order of the cavity radius. Thus the size of this kind of plasma source must decrease as the gas pressure is increased. In fact, the hollow cathode effect can occur even at atmospheric pressure for cathode diameters of order 10-100 $\mu\textrm{m}$. That is, the "natural" operating pressure regime for a "micro hollow cathode discharge" is atmospheric pressure. This kind of plasma source has been the subject of increasing research activity in recent years. A number of geometric variants have been explored, and operational requirements and typical plasma parameters have been determined. Large arrays of individual tiny sources can be used to form large-area, atmospheric-pressure plasma sources. The simplicity of the method and the capability of operation without the need for the usual vacuum system and its associated limitations, provide a highly attractive option for new approaches to many different kinds of plasma applications, including plasma surface modification technologies. Here we review the background work that has been carried out in this new research field.

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마이크로 추진장치 (Micro Propulsion System)

  • 전재영;윤영빈;허환일
    • 한국추진공학회지
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    • 제5권3호
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    • pp.100-107
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    • 2001
  • Miro propulsion device is a literally very small propulsion system The reason why such a small propulsion system is required is that micro satellites are considered as substitutions for conventional satellites to reduce cost; the fabrication of micro satellites enables us to produce mass production Microrockets have relatively high values of thrust/weight ratio due to the cube law; weight is proportional to volume and thrust is proportional to area. Accordingly, downsizing makes the ratio of thrust/weight ratio high However, conventionally ignorable facts are not negligible any more in small scale systems. for chemical micro rockets, downsizing causes lots of heat loss as surface to volume ratio increases, which results in the destruction of radical ions. For thrusters using plasma, the generation of strong magnetic field for plasma is very difficult. Also, in the aspect of flow dynamics, the effects of drag and viscosity are important parameters in low Re flows. When these problems are solved, micro propulsion systems can be commercialized and result in spin-off effects in many fields.

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마이크로 플라즈마 전극가공을 위한 FIB 연구

  • 최헌종;강은구;이석우;홍원표
    • 한국반도체및디스플레이장비학회:학술대회논문집
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    • 한국반도체및디스플레이장비학회 2004년도 춘계학술대회 발표 논문집
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    • pp.229-233
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    • 2004
  • The application of focused ion beam (FIB) technology in micro/nano machining has become increasingly popular. Its use in micro/nano machining has advantages over contemporary photolithography or other micro/nano machining technologies such as small feature resolution, the ability to process without masks and being accommodating for a variety of materials and geometries. This paper was carried out some experiments of the micro plasma electrode fabrications using FIB. The sputtering of FIB has one major problem that is redeposited by sputtered material including $Ga^+$ ion source. Therefore we have verified the effect of the reposition by EDX. And the optimal condition is suggested to machine the micro plasma electrode.

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Electron Temperature, Plasma Density and Luminous Efficiency in accordance with Discharge Time in coplanar AC PDPs

  • Jeong, S.H.;Moon, M.W.;Oh, P.Y.;Jeong, J.M.;Ko, B.D.;Park, W.B.;Lee, J.H.;Lim, J.E.;Lee, H.J.;Han, Y.G.;Son, C.G.;Lee, S.B.;Yoo, N.L.;Choi, E.H.
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2005년도 International Meeting on Information Displayvol.II
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    • pp.1203-1206
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    • 2005
  • Electron temperature and plasma density in coplanar alternating-current plasma display panels (AC-PDP's) have been experimentally investigated in accordance with discharge time by a micro-probe in this experiment. The resolution of a step mortor to move in micro-Langmuir probe is 10um.[1-3] The used gas in this experiment is He-Ne-Xe (4%) mixure gas. And sustain voltage is 320V which is above of firing voltage for degradation. The electron temperature and plasma density can be obtained from current-voltage (I-V) characteristics of micro Langmuir probe, in which negative to positive bias voltage was applied to the probe. And Efficiency is calculated by formula related discharge power and light emission. Those experiments operated as various discharge time ($0{\sim}72$ Hours). As a result of this experiment, Electron Temperature was increased from 2eV to 5eV after discharge running time of 20 hours and saturates beyond 20 hours. The plasma density is inversely proportional to the square root of electron temperature. So the plasma density was decreased from $1.8{\times}10^{12}cm^{-3}$ to $8{\times}10^{11}cm^{-3}$ at above discharge running time. And the Efficiency was reduced to 70% at 60hours of discharge running time.

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이단 마이크로 플라즈마 추력기의 개념 설계에 대한 실험적 연구 (Experimental Investigation on Conceptual Design of Dual Stage Micro Plasma Thruster)

  • 호 티 탄 트랑;신지철
    • 한국추진공학회:학술대회논문집
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    • 한국추진공학회 2011년도 제37회 추계학술대회논문집
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    • pp.540-543
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    • 2011
  • 이단 마이크로 플라즈마 추력기 (${\mu}PT$)의 개념 설계를 위하여 실험적 연구가 수행되었다. 운전 조건 및 노즐의 설계조건에 따른 전극 간격 및 출구 면적의 변화에 대한 추력기의 성능 최적화 연구가 수행되었다. 운전 압력은 $10^{-1}$ Torr에서 $10^{-4}$ Torr의 진공 조건이며 아르곤 가스의 유량은 5 sccm에서 300 sccm에 대하여 추력기의 성능 검증 연구가 이루어 졌다. 소모전력 약 1 watt에서 5 watt의 운전 상태에서 약 3000에서 4000정도의 비추력이 예상된다. 마이크로 플라즈마 추력기에 의해 발생된 토출 제트의 사진 및 전기적 특성에 대한 결과를 포함하였다.

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Spark Plasma Sintering of Stainless Steel Powders Fabricated by High Energy Ball Milling

  • Chang, Si Young;Oh, Sung-Tag;Suk, Myung-Jin;Hong, Chan Seok
    • 한국분말재료학회지
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    • 제21권2호
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    • pp.97-101
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    • 2014
  • The 304 stainless steel powders were prepared by high energy ball milling and subsequently sintered by spark plasma sintering, and the microstructural characteristics and micro-hardness were investigated. The initial size of the irregular shaped 304 stainless steel powders was approximately 42 ${\mu}m$. After high energy ball milling at 800 rpm for 5h, the powders became spherical with a size of approximately 2 ${\mu}m$, and without formation of reaction compounds. From TEM analysis, it was confirmed that the as-milled powders consisted of the aggregates of the nano-sized particles. As the sintering temperature increased from 1073K to 1573K, the relative density and micro-hardness of sintered sample increased. The sample sintered at 1573K showed the highest relative density of approximately 95% and a micro-hardness of 550 Hv.

Nitrogen Porosimeter를 이용한 산소 플라즈마 처리 PET의 미세구조 분석 (The Analysis of the Micro-structure of Oxygen Plasma Treated PET Using a Nitrogen Porosimeter)

  • 김병인;김태경;조규민;임용진
    • 한국염색가공학회지
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    • 제11권6호
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    • pp.1-6
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    • 1999
  • The porosities of PET fibers were investigated using a nitrogen porosimeter according to oxygen plasma treatment and dyeing with a disperse dye, and they were discussed in terms of the change of internal micro-structure of the PET fiber. The total pore volume, surface area and average pore size of the plasma treated PET fibers increased expectably compared with the untreated sample. The PET fibers treated with oxygen plasma and then dyed with a disperse dye were increased significantly in the surface area and the total pore volume comparing with those of plasma treated only, but decreased in the average pore size. The increase of the surface area, after dyeing, of the plasma treated PET fibers was due to addition of the surface area of the dye itself to that of the PET fiber. The increase of the total pore volume of the plasma treated PET fibers by dyeing, which is the opposite result to the general idea that the pore volume of fibers would be reduced by occupation of dye molecules in the pores, could be explained by the free-volume model. This is that the amorphous region in the fiber expanded by occupation of dye molecules, and the marginal space surrounding dyes was generated as many smaller pores, and the decrease of the average pore size of the dyed sample also could be explained The decrease of the average pore size was caused by the splitting of a larger pore into smaller pores.

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플라즈마 표면처리에 의한 Silk/PLA 바이오복합재료의 계면접착 (Interfacial Adhesion of Silk/PLA Biocomposites by Plasma Surface Treatment)

  • 추보영;권미연;이승구;조동환;박원호;한성옥
    • 접착 및 계면
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    • 제5권4호
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    • pp.9-16
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    • 2004
  • 견섬유와 폴리라틱산(PLA) 사이의 계면접착 특성을 향상시키기 위하여 천연섬유 표면을 아르곤과 에틸렌 플라즈마로 각각 처리하였다. 플라즈마 표면처리 후, 견섬유의 표면 모폴로지와 접착이 크게 변화하였다. 다음의 여러 플라즈마 처리조건이 본 연구에 사용되었다: 10, 25, 50 그리고 150 W의 전력, 1, 3, 5, 7 그리고 10분의 처리시간 및 10과 50 sccm의 가스흐름속도, 플라즈마 처리된 Silk/PLA 바이오복합재료의 계면전단강도는 단섬유 micro-droplet debonding 시험방법으로 측정하였다. 결과는 Silk/PLA 바이오복합재료의 계면접착을 향상시키기 위한 최적의 플라즈마 처리 조건을 제공하여 주었다.

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