Os-coated cathode for very high emission-density applications

1987 ◽  
Vol 34 (5) ◽  
pp. 1193-1200 ◽  
Author(s):  
A. Shih ◽  
A. Berry ◽  
C.R.K. Marrian ◽  
G.A. Haas
Author(s):  
Boris Cheslavovich Djubua ◽  
Anatoly Pavlovich Makarov ◽  
Aleksander Andreevich Negirev ◽  
Stanislav Efimovich Rozhkov ◽  
Evgeny Mikhailovich Zemchikhin

Carbon ◽  
2013 ◽  
Vol 52 ◽  
pp. 356-362 ◽  
Author(s):  
V. Guglielmotti ◽  
E. Tamburri ◽  
S. Orlanducci ◽  
M.L. Terranova ◽  
M. Rossi ◽  
...  

2013 ◽  
Vol 734-737 ◽  
pp. 1743-1746
Author(s):  
Guo Qing Yin ◽  
Ling Li Xu ◽  
Xue Du

This paper uses Chinas statistical data by industry and by region in 1995-2010 to calculate the carbon emission caused by the fossil fuel consumption. The total amount of carbon emission in 2010 was about 1.9 billion tons and it shows an increase of 150% compared with that in 1995, which shows a rapid increase year by year.The differentiation of carbon emission by industry is significant, while the manufacturing and transportation are the major emitting sectors. The differentiation of carbon emissions by region is significant as well, while the developed region and resource-rich region are the high emission regions. Some areas like Inner Mongolia have a very high speed growth.


2012 ◽  
Vol 3 (2) ◽  
pp. 935-977 ◽  
Author(s):  
D. J. L. Olivié ◽  
G. P. Peters

Abstract. Emission metrics are necessary to determine the relative climate effect of emissions of different species, such as between CO2 and CH4. Most emission metrics are based on Impulse Response Functions (IRFs) derived from singe models. There is currently very little understanding on how IRFs vary across models, and how the model spread propagates into the metric values. In this study, we first derive three CO2 IRF distributions from Carbon-Cycle models in the inter-comparison projects C4MIP and LTMIP, and three temperature IRF distributions from AOGCMs in the inter-comparison projects CMIP3 and CMIP5. Each distribution is based on the behaviour of several models, and takes into account their spread. The derived IRF distributions differ considerably, which is partially related to differences among the underlying models, but also to the specific scenarios (experimental setup) used in the inter-comparison exercises. For example, the very high emission pulse in LTMIP leads to considerably higher CO2 IRFs, while the abrupt forcing scenario in CMIP5 leads to a relatively high temperature IRF the first four to five years. The spreads within the different IRF distributions are however rather similar. In a second part of the study, we investigate how differences among the IRFs then impact GWP, GTP and iGTP emission metric values for time horizons up to 100 yr. The spread in the CO2 IRFs causes rather similar impacts in all three metrics. The LTMIP IRF gives 20–35% lower metric values, while the C4MIP IRFs give up to 40% higher values for short time horizons shifting to lower values for longer time horizons. Within each derived CO2IRF distribution, underlying model differences give similar spreads on the metrics in the range of −15% to 25% (10–90% spread). The GTP and iGTP metrics are also impacted by spread in the temperature IRFs, and this impact differs strongly between both metrics. For GTP, the impact of the spread is rather strong for species with a short life time. For BC, depending on the time horizon, 50% lower to 85% higher values can be found using the CMIP5 IRF, and slightly lower variations are found when using the CMIP3 IRFs (10% lower to 40% higher). For CH4 the impact from spread in the temperature IRF is still considerable, but it becomes small for longer-lived species. On the other hand, the impact from spread in the temperature IRF on iGTP is very small for all species for time horizons up to 100 yr as it is an integrated metric. Finally, as part of the spread in IRFs is caused by the specific setup of the inter-comparison exercises, there is a need for dedicated inter-comparison exercises to derive CO2 and temperature IRFs.


2015 ◽  
Vol 36 ◽  
pp. 44-50 ◽  
Author(s):  
Pankaj M. Koinkar ◽  
Sandip S. Patil ◽  
Toshihiro Moriga ◽  
Mahendra A. More

Electrochemical synthesis of Polypyrrole (PPy) thin films on Sn substrates has been carried out under cyclic voltammetry (CV) mode. The structural, morphological and chemical properties of the as-synthesized PPy films were investigated using various characterization techniques like SEM, UV-Visible and FTIR. Furthermore, field emission (FE) behaviour of the PPy thin film emitter were carried out at base pressure of ~ 1×10-8 mbar and found to be interesting. The threshold field, required to draw emission current density of 1 μA/cm2, is observed to be 0.90 V/μm and very high emission current density of 12.87 mA/cm2 has been drawn at applied field of ~ 2.8 V/μm. The emission current stability investigated at preset values of 1, 10 and 100 μA/cm2 is observed to be fairly good over duration of more than three hours. The simplicity of the synthesis route coupled with the capability to deliver very high emission current density at relatively lower applied field make the PPy thin field emitter as a potential candidate for practical applications in field emission based devices


2015 ◽  
Vol 29 (06n07) ◽  
pp. 1540035 ◽  
Author(s):  
Kashmira Harpale ◽  
Mahendra A. More ◽  
Pankaj M. Koinkar ◽  
Sandip S. Patil ◽  
Kishor M. Sonawane

Polypyrrole (PPy) nanostructures have been synthesized on indium doped tin oxide (ITO) substrates by a facile electrochemical route employing cyclic voltammetry (CV) mode. The morphology of the PPy thin films was observed to be influenced by the monomer concentration. Furthermore, FTIR revealed formation of electrically conducting state of PPy. Field emission investigations of the PPy nanostructures were carried out at base pressure of 1×10-8 mbar . The values of turn-on field, corresponding to emission current density of 1 μA/cm2 were observed to be 0.6, 1.0 and 1.2 V/μm for the PPy films characterized with rod-like, cauliflower and granular morphology, respectively. In case of PPy nanorods maximum current density of 1.2 mA/cm2 has been drawn at electric field of 1 V/μm. The low turn on field, extraction of very high emission current density at relatively lower applied field and good emission stability propose the PPy nanorods as a promising material for field emission based devices.


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