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Auswahl der wissenschaftlichen Literatur zum Thema „Polar dielectric liquids“

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Zeitschriftenartikel zum Thema "Polar dielectric liquids"

1

Tabassum, Shagufta, and V. P. Pawar. "Complex permittivity spectra of binary polar liquids using time domain reflectometry." Journal of Advanced Dielectrics 08, no. 03 (2018): 1850019. http://dx.doi.org/10.1142/s2010135x18500194.

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The study of complex properties in a binary mixture of polar liquids has been carried out in the frequency range of 10[Formula: see text]MHz to 30 GHz at 293[Formula: see text]K and 298[Formula: see text]K temperatures using time domain reflectometry. The complex properties of polar liquids in binary mixture give information about the frequency dispersion in the dielectric permittivity ([Formula: see text]) and dielectric loss ([Formula: see text]). The information regarding the orientation of electric dipoles in a polar liquid mixture is given by Kirkwood parameters. The Bruggeman parameters are used as the indicator of liquid1 and liquid2 interaction. Molar entropy ([Formula: see text]) and molar enthalpy ([Formula: see text]) are also discussed at the end of the paper.
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2

Monder, Hila, Leo Bielenki, Hanna Dodiuk, Anna Dotan, and Samuel Kenig. "Poly (Dimethylsiloxane) Coating for Repellency of Polar and Non-Polar Liquids." Polymers 12, no. 10 (2020): 2423. http://dx.doi.org/10.3390/polym12102423.

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The wettability of poly (dimethylsiloxane) (PDMS) coating on plasma-treated glass was studied at room temperature using polar and non-polar liquids. The wettability was investigated regarding the liquids’ surface tensions (STs), dielectric constants (DCs) and solubility parameters (SPs). For polar liquids, the contact angle (CA) and contact angle hysteresis (CAH) are controlled by the DCs and non-polar liquids by the liquids’ STs. Solubility parameter difference between the PDMS and the liquids demonstrated that non-polar liquids possessed lower CAH. An empirical model that integrates the interfacial properties of liquid/PDMS has been composed. Accordingly, the difference between the SPs of PDMS and the liquid is the decisive factor affecting CAH, followed by the differences in DCs and STs. Moreover, the interaction between the DCs and the SPs is of importance to minimize CAH. It has been concluded that CAH, and not CA, is the decisive attribute for liquid repellency of PDMS coating.
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3

Useinova, S. "Application of the Variational Method in Studying of Polar Liquids and Their Concentrated Solutions." Bulletin of Science and Practice, no. 12 (December 15, 2022): 20–27. http://dx.doi.org/10.33619/2414-2948/85/02.

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The developed new variational method for measuring the permittivity ξ' and dielectric losses ξ'' of polar liquids is free from a number of shortcomings. At which the minimum amplitude of the reflected wave (ρ) or the standing wave coefficient η takes place, and the value of ηm at this liquid thickness is based on measuring the thickness of the liquid layer in the cell. A variant of this method was considered in the assumption of the active value of the initial resistance of the waveguide section with liquid at the layer thickness corresponding to the minimum value of (ρ) or η, justified only for the case of polar liquids with low dielectric losses. Thus, polar liquids — cyclopentanol, cyclopentanone and their concentrated solutions in each other were studied for the first time, and variational method found a worthy application as the results showed.
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4

de Souza, J. Pedro, Alexei A. Kornyshev, and Martin Z. Bazant. "Polar liquids at charged interfaces: A dipolar shell theory." Journal of Chemical Physics 156, no. 24 (2022): 244705. http://dx.doi.org/10.1063/5.0096439.

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The structure of polar liquids and electrolytic solutions, such as water and aqueous electrolytes, at interfaces underlies numerous phenomena in physics, chemistry, biology, and engineering. In this work, we develop a continuum theory that captures the essential features of dielectric screening by polar liquids at charged interfaces, including decaying spatial oscillations in charge and mass, starting from the molecular properties of the solvent. The theory predicts an anisotropic dielectric tensor of interfacial polar liquids previously studied in molecular dynamics simulations. We explore the effect of the interfacial polar liquid properties on the capacitance of the electrode/electrolyte interface and on hydration forces between two plane-parallel polarized surfaces. In the linear response approximation, we obtain simple formulas for the characteristic decay lengths of molecular and ionic profiles at the interface.
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5

Chandra, Amalendu, and Biman Bagchi. "Exotic dielectric behavior of polar liquids." Journal of Chemical Physics 91, no. 5 (1989): 3056–60. http://dx.doi.org/10.1063/1.456927.

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6

Matyushov, Dmitry V. "Nonlinear dielectric response of polar liquids." Journal of Chemical Physics 142, no. 24 (2015): 244502. http://dx.doi.org/10.1063/1.4922933.

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7

Woisetschläger, Jakob, Adam D. Wexler, Gert Holler, Mathias Eisenhut, Karl Gatterer, and Elmar C. Fuchs. "Horizontal bridges in polar dielectric liquids." Experiments in Fluids 52, no. 1 (2011): 193–205. http://dx.doi.org/10.1007/s00348-011-1216-x.

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8

del Castillo, L. F., L. A. Dávalos-Orozco, and L. S. Garcı́a-Colı́n. "Ultrafast dielectric relaxation response of polar liquids." Journal of Chemical Physics 106, no. 6 (1997): 2348–54. http://dx.doi.org/10.1063/1.473789.

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9

Kalmykov, Yurii P. "Dielectric relaxation in solutions of polar liquids." Journal of Molecular Liquids 49 (September 1991): 201–7. http://dx.doi.org/10.1016/0167-7322(91)80077-h.

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10

Chaube, Hemantkumar A., and Vipinchandra A. Rana. "Dielectric and Electrical Properties of Binary Mixtures of Anisole and Some Primary Alcohols in the Frequency Range 20 Hz to 2 MHz." Advanced Materials Research 665 (February 2013): 194–201. http://dx.doi.org/10.4028/www.scientific.net/amr.665.194.

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The complex relative dielectric function ε*(ω) = ε-jε of binary mixture of anisole (AN) with methanol (MeOH) ,1-propanol (1-PrOH), 1-butanol (1-BuOH), 1-heptanol (1-HeOH) of varying concentration have been measured using Precision LCR meter in the frequency range 20 Hz to 2 MHz at 303 K. The electrical/dielectric properties of the liquid samples are represented in terms of intensive quantities namely, complex relative dielectric function ε*(ω), electrical modulus M*(ω), and extensive quantities, i.e. complex admittance Y*(ω) and complex impedance Z*(ω). All of these presentations are used to explore various processes contributed in the electrical/dielectric properties of the mixtures of polar-polar liquids.
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