• Title/Summary/Keyword: Information of emission

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Evaluating Vehicle Emission Reduction (CO, VOC and NOx) Using Real-time Traffic Information (실시간교통정보 이용에 따른 차량의 CO, VOC, NOx 저감효과 평가)

  • Kim, Jun-Hyung;Um, Jung-Sup
    • Journal of Environmental Impact Assessment
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    • v.20 no.2
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    • pp.217-226
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    • 2011
  • This paper was inspired by the fact that Real-time Traffic Information Service could play a key role in reducing incomplete combustion time remarkably since it can provide traffic jam information in real-time basis. Emission characteristics of experimental engines were studied with variable travel distances and speed of car in terms of traffic information provided. 12 Km distance road of Susung district in Daegu is taken as an experimental area to examine this new approach. The emission was tested while the driving was done at 8 AM, 3 PM, 6 PM which represents various traffic conditions. The reduced emission has been measured for a travel distance running at different loads (conventional shortest route and Real-time Traffic Information) and various loads (CO, VOC and NOx) are all inventoried and calculated in terms of existing emission factors. The emission has been shown to reduce linearly with travel distance : carbon monoxide (20.56%), VOC (29.21%), NOx(8.86%).

Enhanced Electron Emission of Carbon Nanotube Arrays Grown Using the Resist-Protection-assisted Positioning Technique

  • Ryu, Je-Hwang;Kim, Ki-Seo;Yu, Yi-Yin;Lee, Chang-Seok;Lee, Yi-Sang;Jang, Jin;Park, Kyu-Chang
    • Journal of Information Display
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    • v.9 no.4
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    • pp.30-34
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    • 2008
  • Field emitter arrays (FEAs) were developed using carbon nanotubes (CNTs) as electron emission sources. The CNTs were grown using a selective-positioning technique with a resist-protection layer. The light emission properties were studied through the electron emission of the CNTs on patterned islands, which were modulated with island diameter and spacing. The electron emission of CNT arrays with $5{\mu}m$ diameters and $10{\mu}m$ heights increased with increased spacing (from $10{\mu}m$ to $40{\mu}m$). The electron emission current of the $40-{\mu}m$-island-spacing sample showed a current density of 1.33 mA/$cm^2$ at E = 11 V/${\mu}m$, and a turn-on field of 7 V/${\mu}m$ at $1{\mu}A$ emission current. Uniform electron emission current and light emission were achieved with $40{\mu}m$ island spacing and $5{\mu}m$ island diameter.

A new model and testing verification for evaluating the carbon efficiency of server

  • Liang Guo;Yue Wang;Yixing Zhang;Caihong Zhou;Kexin Xu;Shaopeng Wang
    • KSII Transactions on Internet and Information Systems (TIIS)
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    • v.17 no.10
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    • pp.2682-2700
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    • 2023
  • To cope with the risks of climate change and promote the realization of carbon peaking and carbon neutrality, this paper first comprehensively considers the policy background, technical trends and carbon reduction paths of energy conservation and emission reduction in data center server industry. Second, we propose a computing power carbon efficiency of data center server, and constructs the carbon emission per performance of server (CEPS) model. According to the model, this paper selects the mainstream data center servers for testing. The result shows that with the improvement of server performance, the total carbon emissions are rising. However, the speed of performance improvement is faster than that of carbon emission, hence the relative carbon emission per unit computing power shows a continuous decreasing trend. Moreover, there are some differences between different products, and it is calculated that the carbon emission per unit performance is 20-60KG when the service life of the server is five years.

Effect of Current-Aging on Field Emission from Carbon Nanotube Field Emitter Arrays

  • Kim, Ki-Seo;Ryu, Je-Hwang;Lee, Chang-Seok;Manivannan, S.;Moon, Jong-Hyun;Ahn, Jung-Sun;Jang, Jin;Park, Kyu-Chang
    • 한국정보디스플레이학회:학술대회논문집
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    • 2007.08a
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    • pp.782-785
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    • 2007
  • We studied the effect of current-aging on field emission from carbon nanotubes field emitter arrays (CNT-FEAs) selectively patterned by the resist-assistan tpatterning(RAP) process. After sustaining the electric field when starting emission current density $(J_s)$ is $0.1\;mA/cm^2$ during 40 hrs, it was observed that the field emission property and uniformity were remarkably improved due to the elimination of oxygen atom and thus the reconstruction of carbon bonding at the tip of CNTs during field emission.

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Characteristics of transparent metal Cathode for top emission organic light emitting diode (Top emission 유기 발광 소자를 위한 투명 금속 cathode 특성 평가)

  • Lee, Chan-Jae;Moon, Dae-Gyu;Han, Jeong-In;Baik, Sung-Ho;Park, No-Hoon;Ju, Soung-Sam
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2003.04a
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    • pp.107-110
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    • 2003
  • 본 연구에서는 캐소드 방향으로 발광하는 Top emission 소자를 설계 제작하였다. 이를 위하여 반투명한 금속 박막을 제작하여 전기적 특성과 광학적 특성을 비교 평가하였다. 이를 바탕으로 제작한 Top emission 소자를 bottom emission 소자와 비교하였을 때 구동 전압은 다소 높았으며 색좌표 및 스펙트럼이 이동하였는데 이동 정도와 경향성은 파장에 따라 다르게 나타났다

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Measurement of Secondary Electron Emission Coefficient on Deposition Time of the Silicon Thin Films (실리콘박막의 증착시간에 따른 감마계수 측정법 개발)

  • Lee, Jung-Hui;Choi, Byoung-Jung;Yang, Sung-Chae
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2006.11a
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    • pp.330-331
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    • 2006
  • Recently, plasma display panels (PDPs) are highlighted for the flat type display device. Therefore, much attention has been paid to secondary electron emission coefficient of the electrode protective material of PDPs. As PDPs is developing, the concern about secondary electron emission coefficient ($\gamma$) which is related with PDPs electrode protection material is increasing continually. So the concern about the way to how to measure secondary electron emission coefficient is on the rise. At present, the way to how to measure secondary electron emission coefficient is developed by some research groups, which is giving some research part's advance help. In this research, we have studied how to measure secondary electron emission coefficient which is related with various thin films more conveniently than previous measurement method. We studied the method of measurement of secondary electron emission coefficient (${\gamma}$) of amorphous silicon films by using Paschen's curve.

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Comparative Evaluation of Interpolation Accuracy for $CO_2$ Emission using GIS (GIS를 활용한 이산화탄소 농도 보간 정확도 비교평가)

  • Kim, Jun-Hyun;Choi, Jin-Ho;Kim, Chung-Sil
    • Journal of Environmental Impact Assessment
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    • v.19 no.6
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    • pp.647-656
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    • 2010
  • As the $CO_2$ from buildings take up approximately 25% of the total $CO_2$ emission, the need for regulating and managing this emission is urgently required. Thus this study recognizes $CO_2$ emission status for diverse purposes and suggests accurate interpolation method for visualizing $CO_2$ emission as the basic data for regulating and managing $CO_2$ emission by applying IDW, Spline, and Kringing method. Results showed that Gaussian Function application among the Kriging methods had the highest accuracy in its estimations, with 3.049 with RMSE standards. This could be used as the basic data when visualizing $CO_2$ emission status, which is a necessity for many local and federal governments that are to regulate and manage $CO_2$ emission. This study shows that the interpolation is very appropriative method in recognizing $CO_2$ emission characteristics for regional climate change measures.

Layer Thickness-dependent Electrical and Optical Properties of Bottom- and Top-emission Organic Light-emitting Diodes

  • An, Hui-Chul;Na, Su-Hwan;Joo, Hyun-Woo;Kim, Tae-Wan
    • Transactions on Electrical and Electronic Materials
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    • v.10 no.1
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    • pp.28-30
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    • 2009
  • We have studied organic layer-thickness dependent electrical and optical properties of bottom- and top-emission devices. Bottom-emission device was made in a structure of ITO(170 nm)/TPD(x nm)/$Alq_3$(y nm)/LiF(0.5 nm)/Al(100 nm), and a top-emission device in a structure of glass/Al(100 nm)/TPD(x nm)/$Alq_3$(y nm)/LiF(0.5 nm)/Al(25 nm). A hole-transport layer of TPD (N,N'-diphenyl-N,N'-di(m-tolyl)-benzidine) was thermally deposited in a range of 35 nm and 65 nm, and an emissive layer of $Alq_3$ (tris-(8-hydroxyquinoline) aluminum) was successively deposited in a range of 50 nm and 100 nm. Thickness ratio between the hole-transport layer and the emissive layer was maintained to be 2:3, and a whole layer thickness was made to be in a range of 85 and 165 nm. From the current density-luminance-voltage characteristics of the bottom-emission devices, a proper thickness of the organic layer (55 nm thick TPD and 85 nm thick $Alq_3$ layer) was able to be determined. From the view-angle dependent emission spectrum of the bottom-emission device, the peak wavelength of the spectrum does not shift as the view angle increases. However, for the top-emission device, there is a blue shift in peak wavelength as the view angle increases when the total layer thickness is thicker than 140 nm. This blue shift is thought to be due to a microcavity effect in organic light-emitting diodes.

A Study on the Analysis Method of Emission Intensity of GHGs utilizing Real World Vehicle Driving Information (실차 운행정보를 활용한 온실가스 배출지표 분석 방법에 대한 연구)

  • Kim, Yong Beom;Kim, Pil Su;Han, Yong Hee;Lee, Heon Ju;Jang, Young Kee
    • Journal of Climate Change Research
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    • v.7 no.1
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    • pp.19-29
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    • 2016
  • In this study, the emission intensity calculation method of GHGs was developed by considering the characteristics of the models and time series. The telematics device was installed on the car (OBD-II) to collect information on the operation conditions from each sample vehicle of public authorities. Based on emission intensity of GHGs, it presented a methodology of quantitative comparison of GHGs emission by vehicles. Collected driving information of vehicle was used for operating characteristics analysis of the target vehicle, and it was confirmed different operating characteristics through comparison of the results and previous study. GHGs emission intensity were analyzed considering characteristics of vehicle type by passenger car, van, cargo, and considering characteristics of the time series by summer, winter, and intermediate. From the analysis result, it was calculated GHGs emission intensity based on mileage ($g\;CO_2\;eq./km$) and operating time ($g\;CO_2\;eq./sec$).

Numerical Calculation Study on the Generalized Electron Emission Phenomenon

  • Kim, Hee-Tae;Yu, Soon-Jae
    • Journal of Information Display
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    • v.10 no.4
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    • pp.158-163
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    • 2009
  • There are two kinds of well-known electron emissions from metal: field and thermionic emission. For thermionic emission, electrons come out of a metal due to the thermal energy, whereas for field emission, electrons tunnel out of a metal through the strong electric field. In this study, the most general electron emission caused by the temperature and electric field with a free electron gas model was considered. The total current density of electron emission comes from the field emission effect, where the electron energy is lower than vacuum, and from the thermionic-emission effect, where the electron energy is higher than vacuum. The total current density of electron emission is shown as a function of the temperature for a constant electric field, and as a function of the electric field for a constant temperature.