Chlorobenzene Release During Thermal Drying of Sludge: Mechanism and Source

Dai, Zhixi; Tian, Liwen; Liu, Chongxuan; Weng, Huan-Xin

doi:10.1007/s11270-017-3554-7

Cited by 6 publications

(3 citation statements)

References 16 publications

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“…gases was obtained following the technique of the pressure decrease [38] performed before the cross-section measurements. Although the quadratic behavior given by equation (1) has been observed, in the current work, the normalization procedure was performed in a lower-pressure regime (P < 0.3 Torr), so the mean-free path of the atoms/molecules was comparable or greater than the collimating gas tube diameter. In such a low-pressure condition the second-order contribution in equation ( 1) was made negligible and the DCS for the chlorobenzene can then be determined as [21] DCS(E 0 , θ) X = DCS(E 0 , θ)…”

Section: Comparison Of Csuf and Ufscar Rft Applicationsmentioning

confidence: 90%

“…In industry, chlorobenzene (C 6 H 5 Cl) is an important chemical reactant and is used as an intermediate in the production of commodities such as herbicides, dye stuffs, and rubber [1]. Biologically, chlorobenzene and its derivatives are highly toxic.…”

Section: Introductionmentioning

confidence: 99%

“…Biologically, chlorobenzene and its derivatives are highly toxic. They can inhibit the central nervous system, irritate eyes, affect the upper respiratory system, cause skin sclerosis, and various blood diseases [1,2] and can even cause cancer. Therefore, such compounds have been ranked as priority (dangerous) pollutants by the United States Environmental Protection Agency and the European Union Environmental Agency [3].…”

Section: Introductionmentioning

confidence: 99%

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Elastic electron scattering from chlorobenzene

Mata¹,

Hlousek²,

Bardela³

et al. 2020

J. Phys. B: At. Mol. Opt. Phys.

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We report a joint theoretical–experimental investigation on elastic electron scattering by chlorobenzene in the low- and intermediate-energy ranges as a part of a collaborative project established between the Federal University of São Carlos (UFSCar) and the California State University (CSUF). More specifically, experimental elastic differential cross sections (DCS), in the incident electron energy range of 1.0 to 800 eV and scattering angle range of 10° to 130°, were measured using the crossed-beam relative-flow technique. Integral and momentum-transfer cross sections were determined from the numerical integration over the experimental DCS. Theoretically, elastic differential, integral, and momentum-transfer cross sections were calculated using a combination of a molecular complex optical potential model with the Padé approximant technique for impact energies ranging from 1.0 to 150 eV. Further calculations of DCS were performed at an energy range of 20 to 500 eV using the independent-atom model. Our results, which significantly extend available electron scattering cross sections for this target, are compared to existing theoretical and experimental data in the literature.

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Section: Comparison Of Csuf and Ufscar Rft Applicationsmentioning

confidence: 90%

Section: Introductionmentioning

confidence: 99%