Hourly emission inventories for air toxic emissions for eastern Australian electricity generators derived from energy distribution data

Author(s):  
M. Garg ◽  
J. D. Silver ◽  
R. Schofield ◽  
R. G. Ryan
Author(s):  
Fatin Amani Mohd Ali ◽  
Samsul Ariffin Abdul Karim ◽  
Sarat Chandra Dass ◽  
Vaclav Skala ◽  
Mohammad Khatim Hasan ◽  
...  

The work to be described is a continuation of the experiments dealt with in the papers listed in the footnote. For brevity, these papers will be referred to in the sequel by the corresponding numbers. It may be recalled that the results of (5) exhibited a conflict with those of the earlier papers of which (3) is the most important. In the range of partial pressure of COCl 2 used in (5), which extended from about 0.05 to 0.001 mm. of mercury, the electron currents were found to be independent of that pressure; whereas in the earlier experiments, which employed smaller currents, these had been varied by controlling the rate of evaporation of the source of COCl 2 , which was kept in a bath of liquid air. In addition, some 50 determinations of the apparent temperature of the emitted electrons in the range of pressure 0.001 to 0.01mm., as deduced from the energy distribution data, gave values none of which differed by as much as 5 per cent. from 2368°K., whereas in the earlier work values in the neighbourhood of about 3300°K., which were though to be accurate to about 10 per cent., had been obtained. In the earlier experiments, the pressures used were not known, but were thought to be much lower than those in (5). The present experiments have been carried to much lower pressure, with the result that satisfactory progress has been made towards the removal of the discrepancies referred to.


Author(s):  
Valeriy YUFEREV ◽  
Natalya TKACHENKO

Studies of the thermodynamic characteristics of semi-desert landscapes were carried out with the PSR-1100 Spectroradiometer in the range from 320 to 1100 nm. Energy distribution data for the parts of the spectrum for plant phytocenosis Poa bulbosa, Descurainia Sophia were obtained from the energy brightness distribution spectrogram at the Tavn-Gashun test site.


2020 ◽  
Vol 501 (1) ◽  
pp. 157-167
Author(s):  
Rachel C Zhang ◽  
Bing Zhang ◽  
Ye Li ◽  
Duncan R Lorimer

ABSTRACT Fast radio bursts (FRBs) are millisecond-duration radio transients from cosmological distances. Their isotropic energies follow a power-law distribution with a possible exponential cut-off, but their intrinsic redshift distribution, which contains information about the FRB sources, is not well understood. We attempt to constrain both distributions by means of Monte Carlo simulations and comparing the simulations results with the available FRB specific fluence distribution, dispersion measure (DM) distribution, and the estimated energy distribution data. Two redshift distribution models, one tracking the star formation history of the Universe and another tracking compact binary mergers, are tested. For the latter model, we consider three merger delay time-scale distribution (Gaussian, lognormal, and power-law) models. Two FRB samples detected by Parkes and the Australian Square Kilometre Array Pathfinder, respectively, are used to confront the simulation results. We confirm the ∼−1.8 power-law index for the energy distribution but the exponential cut-off energy of the distribution, if any, is unconstrained. For the best energy distribution model, none of the redshift distributions we considered are rejected by the data. A future, larger, uniform FRB sample (such as the one collected by the Canadian Hydrogen Intensity Mapping Experiment) can provide better constraints on the intrinsic FRB redshift distribution using the methodology presented in this paper.


Author(s):  
Tamotsu Ohno

The energy distribution in an electron; beam from an electron gun provided with a biased Wehnelt cylinder was measured by a retarding potential analyser. All the measurements were carried out with a beam of small angular divergence (<3xl0-4 rad) to eliminate the apparent increase of energy width as pointed out by Ichinokawa.The cross section of the beam from a gun with a tungsten hairpin cathode varies as shown in Fig.1a with the bias voltage Vg. The central part of the beam was analysed. An example of the integral curve as well as the energy spectrum is shown in Fig.2. The integral width of the spectrum ΔEi varies with Vg as shown in Fig.1b The width ΔEi is smaller than the Maxwellian width near the cut-off. As |Vg| is decreased, ΔEi increases beyond the Maxwellian width, reaches a maximum and then decreases. Note that the cross section of the beam enlarges with decreasing |Vg|.


2008 ◽  
Vol 42 (2) ◽  
pp. 125-128
Author(s):  
J. F. Al-Sharab ◽  
J. E. Wittig ◽  
G. Bertero ◽  
T. Yamashita ◽  
J. Bentley ◽  
...  

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