Composition Determination of Vehicle Dismantling Waste

2014 ◽  
Vol 878 ◽  
pp. 83-89
Author(s):  
Shao Hong Peng ◽  
Sha Liang ◽  
Jian Li ◽  
Mei Yu ◽  
Yan Huang

In recent years, a large number of toxic and hazardous substances were discharged into environment because of the simple landfill and accumulation of vehivle dismantling waste. Therefore, it is very important to develop the recycling technology of vehivle dismantling waste for the harmless, stability, reduction and resource utilization of vehivle dismantling waste. In this paper, the compositions of vehicle dismantling waste from two different dismantling processes were investigated by manual sorting, infrared spectroscopy and X-ray fluorescence spectrometer, experimental results showed that the vehicle waste from manual dismantling contained more polyurethane, foamed plastic and rubber with low value and the size of waste is lager, the vehicle waste from mechanical dismantling contained more metal and brittle polymer and their size was smaller. The concentration of metal in two kinds of wastes are less than 1%, the total concentration of carbon and hydrogen reach about 70%, so vehicle dismantling waste was suital for recovering ernergy, but the pollution of chlrone from polyvinyl chloride need to be prevented.

2004 ◽  
Vol 59 (5) ◽  
pp. 567-572 ◽  
Author(s):  
Claus Mühle ◽  
Andrey Karpov ◽  
Jürgen Nuss ◽  
Martin Jansen

Abstract Crystals of K2Pt(CN)4Br2, K2Pt(CN)4I2 and K2Pt(CN)4Cl2 ·2H2O were grown, and their crystal structures have been determined from single crystal data. The structure of K2Pt(CN)4Cl2 has been determined and refined from X-ray powder data. All compounds crystallize monoclinicly (P21/c; Z = 2), and K2Pt(CN)4X2 with X = Cl, Br, I are isostructural. K2Pt(CN)4Cl2: a = 708.48(2); b = 903.28(3); c = 853.13(3) pm; β = 106.370(2)°; Rp = 0.064 (N(hkl) = 423). K2Pt(CN)4Br2: a = 716.0(1); b = 899.1(1); c = 867.9(1) pm; β = 106.85(1)°; R(F)N′ = 0.026 (N’(hkl) = 3757). K2Pt(CN)4I2: a = 724.8(1); b = 914.5(1); c = 892.1(1) pm; β = 107.56(1)°; R(F)N′ = 0.025 (N’(hkl) = 2197). K2Pt(CN)4Cl2 ·2H2O: a = 763.76(4); b = 1143.05(6); c = 789.06(4) pm; β = 105.18(1)°; R(F)N′ = 0.021 (N’(hkl) = 2281). Raman and infrared spectroscopy data are reported.


2013 ◽  
Vol 544 ◽  
pp. 445-449
Author(s):  
Ran Yan ◽  
Yu Bing Liu ◽  
Ping Dai

When an X-ray photon which is generated by the sample enters into the detector, pulses can be produced and recorded. The detector is unable to respond to another photon that enters at the same time when a photon is being detected. The time that the detector takes to respond to a photon is regarded as dead time. For the x-ray fluorescence detector, the recorded count is less than the real count impulse due to dead time. Hence, to correct x-ray intensity of samples whose element content is vastly different, determination of dead time is necessary. In this paper, a new and complete way to determine dead time is proposed, which can be summarized as “intensity pair method”. Three “intensity pairs” were used for determining dead time, which were “intensity pair” of collimators (S2 and S4), “intensity pair” of spectral lines (Kα and Kβ) and “intensity pair” of beads with different flux-sample ratio (higher SH and lower SL analyte content in the beads). It comes to a conclusion that dead time obtained from “intensity pair” of beads is the most practical method for correcting X-ray fluorescence intensity. As for routine analysis, the dead time of proportional counter can be accurate to 1×10-9s, which can make intensity correction error less than 0.1%.


RSC Advances ◽  
2016 ◽  
Vol 6 (11) ◽  
pp. 9002-9006 ◽  
Author(s):  
Xiaofeng Lin ◽  
Shun-Xing Li ◽  
Feng-Ying Zheng

An integrative field analytical system was developed for the determination of Pb(ii) and Cd(ii).


2017 ◽  
Vol 726 ◽  
pp. 85-89
Author(s):  
Lei Zhang ◽  
Man Li ◽  
Hai Jian Li ◽  
Xin Song

Energy dispersive X-ray fluorescence spectrometry (EDXRF) allows a rapid determination of the concentration of elemental constituents or the thickness of thin film, it has been widely used in the industry of thin film thickness. But for multilayer film, especially the middle layer, with the absorption and enhance effect of other layers, the thickness and intensity of the middle layer is not a linear relationship. This paper reports a quantitative analysis of multilayer film thicknesses based on the use of EDXRF and fundamental parameters method. The thickness of multilayer film can be easily determined with the CTCFP software because it requires a minimum number of pure elementals only. Analysis of double-layer thin films using the CTCFP software shows that the inter-element and inter-layer X-ray absorptions and enhancements in a specimen have been determined properly. Results obtained on the standards confirmed the accuracy of the method.


2011 ◽  
Vol 99 (2) ◽  
pp. 332-338 ◽  
Author(s):  
Yong Suk Choi ◽  
Jong-Yun Kim ◽  
Suk Bon Yoon ◽  
Kyuseok Song ◽  
Young Jin Kim

2016 ◽  
Vol 9 (6) ◽  
pp. 061102 ◽  
Author(s):  
Yuichi Oshima ◽  
Elaheh Ahmadi ◽  
Stefan C. Badescu ◽  
Feng Wu ◽  
James S. Speck

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