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Livros sobre o tema "Non thermal plasma (NTP)"

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Autor: Grafiati

Publicado: 6 de julho de 2024

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1

Penetrante, Bernie M., e Shirley E. Schultheis, eds. Non-Thermal Plasma Techniques for Pollution Control. Berlin, Heidelberg: Springer Berlin Heidelberg, 1993. http://dx.doi.org/10.1007/978-3-642-78476-7.

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2

1960-, Penetrante Bernie M., Schultheis Shirley E. 1957-, North Atlantic Treaty Organization. Scientific Affairs Division. e NATO Advanced Research Workshop on Non-Thermal Plasma Techniques for Pollution Control (1992 : Cambridge, England), eds. Non-thermal plasma techniques for pollution control. Berlin: Springer-Verlag, 1993.

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3

Engineers, Society of Automotive, e International Fall Fuels & Lubricants Meeting & Exposition (1999 : Toronto, Ont.), eds. Non-thermal plasma for exhaust emission control--NOx, HC, and particulates. Warrendale, PA: Society of Automotive Engineers, 1999.

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4

Sun, Yongxia. Degradation of air pollutants in non-thermal plasma generated by electron beam: Experimental and theoretical study. Warszawa: Institute of Nuclear Chemistry and Technology, 2013.

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5

Engineers, Society of Automotive, e International Fall Fuels & Lubricants Meeting & Exposition (2000 : Baltimore, Md.), eds. Non-thermal plasma. Warrendale, PA: Society of Automotive Engineers, 2000.

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6

Non-Thermal Plasma Emission Control Systems. Society of Automotive Engineers (SAE), 2001.

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7

Non-Thermal Plasma Technology for Polymeric Materials. Elsevier, 2019. http://dx.doi.org/10.1016/c2016-0-03254-0.

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8

Mildažienė, Vida, e Božena Šerá, eds. Effects of Non-thermal Plasma Treatment on Plant Physiological and Biochemical Processes. MDPI, 2022. http://dx.doi.org/10.3390/books978-3-0365-4206-5.

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9

Penetrante, Bernie M. Non-Thermal Plasma Techniques for Pollution Control : Part B: Electron Beam and Electrical Discharge Processing. Springer, 2011.

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10

Penetrante, Bernie M., e Shirley E. Schultheis. Non-Thermal Plasma Techniques for Pollution Control : Part B: Electron Beam and Electrical Discharge Processing. Springer London, Limited, 2013.

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11

Thomas, Sabu, Miran Mozetic, Uros Cvelbar, Petr Spatenka e Praveen K. M. Non-Thermal Plasma Technology for Polymeric Materials: Applications in Composites, Nanostructured Materials and Biomedical Fields. Elsevier, 2018.

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12

Thomas, Sabu, Miran Mozetic, Uros Cvelbar, Petr Spatenka e K. M. Praveen. Non-Thermal Plasma Technology for Polymeric Materials: Applications in Composites, Nanostructured Materials, and Biomedical Fields. Elsevier Science & Technology Books, 2018.

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13

Non-Thermal Plasma for Exhaust Emission Control: Nox, Hc, and Particulates (S P (Society of Automotive Engineers)). Society of Automotive Engineers Inc, 1999.

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14

Morent, Rino. Chapter 8 Non-thermal Plasma Technology for the Improvement of Scaffolds for Tissue Engineering and Regenerative Medicine - A Review. InTechOpen, 2016.

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15

Horing, Norman J. Morgenstern. Random Phase Approximation Plasma Phenomenology, Semiclassical and Hydrodynamic Models; Electrodynamics. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198791942.003.0010.

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Resumo:

Chapter 10 reviews both homogeneous and inhomogeneous quantum plasma dielectric response phenomenology starting with the RPA polarizability ring diagram in terms of thermal Green’s functions, also energy eigenfunctions. The homogeneous dynamic, non-local inverse dielectric screening functions (K) are exhibited for 3D, 2D, and 1D, encompassing the non-local plasmon spectra and static shielding (e.g. Friedel oscillations and Debye-Thomas-Fermi shielding). The role of a quantizing magnetic field in K is reviewed. Analytically simpler models are described: the semiclassical and classical limits and the hydrodynamic model, including surface plasmons. Exchange and correlation energies are discussed. The van der Waals interaction of two neutral polarizable systems (e.g. physisorption) is described by their individual two-particle Green’s functions: It devolves upon the role of the dynamic, non-local plasma image potential due to screening. The inverse dielectric screening function K also plays a central role in energy loss spectroscopy. Chapter 10 introduces electromagnetic dyadic Green’s functions and the inverse dielectric tensor; also the RPA dynamic, non-local conductivity tensor with application to a planar quantum well. Kramers–Krönig relations are discussed. Determination of electromagnetic response of a compound nanostructure system having several nanostructured parts is discussed, with applications to a quantum well in bulk plasma and also to a superlattice, resulting in coupled plasmon spectra and polaritons.

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