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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
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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 inte
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3

Zhi, Huiqiang, Youquan Bao, Lu Wang, and Yixing Mi. "Extinguishing performance of alcohol-resistant firefighting foams on polar flammable liquid fires." Journal of Fire Sciences 38, no. 1 (2019): 53–74. http://dx.doi.org/10.1177/0734904119893732.

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The protection of polar flammable liquid storage tanks from fire is an important matter related to the safe production of enterprises and to the safety of people’s lives and property. Although the foam fire-extinguishing system has long been the main means for the fire protection of flammable liquid storage tanks, the influence of the physical properties of polar flammable liquids on the fire-extinguishing characteristics of alcohol-resistant foams has not been well studied, which causes many problems for engineering design. In the present work, 14 kinds of polar flammable liquids were used to
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4

Tregubov, Dmytro, Ilgar Dadashov, Vitalii Nuianzin, Olena Khrystych, and Natalya Minska. "Relationship Between Properties of Floating Systems and Flammable Liquids in the Stopping Their Burning Technology." Key Engineering Materials 954 (August 31, 2023): 145–55. http://dx.doi.org/10.4028/p-krzrd9.

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The contributions balance of isolation and cooling effects relative to the liquids surface to slow down their evaporation and to achieve safe vapor concentrations is determined. The influence of liquids characteristic temperatures and their water solubility on this process is considered. It is proven that the long-term effect of such means is provided by systems based on closed-pore floating solid materials (for example, foam glass). It is proposed to increase the foam glass low isolation and cooling capacity either by coating it with an inorganic gel or by wetting it with water. Smaller evapo
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5

Bolotov, Alexander, and Georgy Burdo. "Magnetic fluid method for sealing liquid media." E3S Web of Conferences 383 (2023): 04081. http://dx.doi.org/10.1051/e3sconf/202338304081.

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Magnetic fluid seals for sealing gas environments are widely used in various industries due to their undeniable advantages. However, such seals are not capable of reliable sealing of liquid media with different polarities. The paper analyses physicochemical processes that lead to destructing magnetic fluid in a seal under the influence of a liquid medium in contact with it. There are results of experimental studies on sealing using magnetic seals of non-magnetic fluids with different polarity. The authors studied the tightness of a magnetic fluid seal capacity in contact with weakly polar liqu
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6

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 f
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7

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 th
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8

Useinova, S. "Application of the Variational Method in Studying of Polar Liquids and Their Concentrated Solutions." Bulletin of Science and Practice 8, no. 12 (2023): 20–27. https://doi.org/10.33619/2414-2948/85/02.

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The developed new variational method for measuring the permittivity &xi;&#39; and dielectric losses &xi;&#39;&#39; of polar liquids is free from a number of shortcomings. At which the minimum amplitude of the reflected wave (&rho;) or the standing wave coefficient &eta; takes place, and the value of <em>&eta;<sub>m</sub></em> at this liquid thickness is based on measuring the thickness of the liquid layer in the cell. A&nbsp;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 correspon
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9

Fukaya, Yukinobu, Takuro Nakano, and Hiroyuki Ohno. "Rheopectic Gel Formation of Stimuli-Responsive Ionic Liquid/Water Mixtures." Australian Journal of Chemistry 70, no. 1 (2017): 74. http://dx.doi.org/10.1071/ch16228.

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A new class of hydrophobic and polar ionic liquids was prepared by coupling hydrophobic tetraoctylphosphonium cation and polar phosphonate-derived anions. Mixtures of these ionic liquids and water showed lower critical solution temperature-type phase behaviour. Furthermore, these mixtures displayed thermoreversible, however, non-linear viscosity change despite their large content of water. The abrupt increase in the viscosity was explained by the occurrence of rheopectic gelation of the ionic liquid/water mixtures by external stimuli such as shear stress.
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10

Agathopoulos, Simeon, M. Nedea, Brandusa Ghiban, José Maria F. Ferreira, and P. Nikolopoulos. "Surface Energies Acting at the Interfaces of Ceramics and Glasses while in Contact with Organic and Biological Liquids." Key Engineering Materials 284-286 (April 2005): 1023–26. http://dx.doi.org/10.4028/www.scientific.net/kem.284-286.1023.

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The surface energy components which govern the interfacial interactions between bioinert solid substrates of partial stabilized ZrO2 (with 3 mol% Y2O3) and a glass with a composition of 55SiO2×10Na2O×35MgO in contact with organic and biological liquids under equilibrium regime, were determined. The experimental results indicated that the interfacial bonding between zirconia and the polar liquids is result of interactions due to dispersion forces. In the case of the glass, polar forces significantly contribute to solid/liquid interfacial interactions.
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11

Prasanna, Thushara Haridas, Mridula Shantha, Anju Pradeep, and Pezholil Mohanan. "Identification of polar liquids using support vector machine based classification model." IAES International Journal of Artificial Intelligence (IJ-AI) 11, no. 4 (2022): 1507. http://dx.doi.org/10.11591/ijai.v11.i4.pp1507-1516.

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&lt;div align="left"&gt;The dispersive nature of polar liquids creates ambiguity in their identification process. It requires a long time and effort to compare the measured values with the available standard values to identify the unknown liquid. Nowadays machine learning techniques are being used widely to assist the measurement techniques and make predictions with great accuracy and less human effort. This paper proposes a support vector machine (SVM) based classification model for the identification of six polar liquids- butan-1-ol, dimethyl sulphoxide, ethanediol, ethanol, methanol and pro
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12

Thushara, Haridas Prasanna, Shantha Mridula, Pradeep Anju, and Mohanan Pezholil. "Identification of polar liquids using support vector machine based classification model." International Journal of Artificial Intelligence (IJ-AI) 11, no. 4 (2022): 1507–16. https://doi.org/10.11591/ijai.v11.i4.pp1507-1516.

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The dispersive nature of polar liquids creates ambiguity in their identification process. It requires a long time and effort to compare the measured values with the available standard values to identify the unknown liquid. Nowadays machine learning techniques are being used widely to assist the measurement techniques and make predictions with great accuracy and less human effort. This paper proposes a support vector machine (SVM) based classification model for the identification of six polar liquids-butan-1- ol, dimethyl sulphoxide, ethanediol, ethanol, methanol and propan-1-ol for a temperatu
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13

Hallett, Jason P., and Tom Welton. "How Polar are Ionic Liquids?" ECS Transactions 16, no. 49 (2019): 33–38. http://dx.doi.org/10.1149/1.3159305.

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14

Fukaya, Yukinobu, and Hiroyuki Ohno. "Hydrophobic and polar ionic liquids." Physical Chemistry Chemical Physics 15, no. 11 (2013): 4066. http://dx.doi.org/10.1039/c3cp44214d.

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15

Rips, Ilya, Joseph Klafter, and Joshua Jortner. "Solvation dynamics in polar liquids." Journal of Chemical Physics 89, no. 7 (1988): 4288–99. http://dx.doi.org/10.1063/1.454811.

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16

Lagerwall, S. T. "Can liquids be macroscopically polar?" Journal of Physics: Condensed Matter 8, no. 47 (1996): 9143–66. http://dx.doi.org/10.1088/0953-8984/8/47/005.

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17

Fragiadakis, D., and C. M. Roland. "Are polar liquids less simple?" Journal of Chemical Physics 138, no. 12 (2013): 12A502. http://dx.doi.org/10.1063/1.4769262.

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18

Bressanini, D., E. S. Fois, A. Gamba, and G. Morosi. "Charge layering in polar liquids." Chemical Physics Letters 200, no. 3 (1992): 333–36. http://dx.doi.org/10.1016/0009-2614(92)80019-8.

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19

Rawat, Bachan S., and Indar B. Gulati. "Cohesive energy density of polar and non-polar liquids." Journal of Applied Chemistry and Biotechnology 27, no. 3 (2007): 459–64. http://dx.doi.org/10.1002/jctb.5020270306.

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20

Kano, S., and H. Mekaru. "Impedance Response of Insulator Nanoparticle Films with Condensed Chemical Vapor: Structural Isomers and Aprotic Chemicals." ECS Journal of Solid State Science and Technology 12, no. 5 (2023): 057005. http://dx.doi.org/10.1149/2162-8777/acd1ad.

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Rapid electrical analysis of chemical liquids is a promising technique for on-site evaluation. In this study, the electrical impedance response of insulator nanoparticle films with condensed chemical vapors was investigated in structural isomers and polar aprotic chemical liquids. Headspace vapor was condensed in the nanoscale void between the nanoparticles, and ionic conduction subsequently occurred under an AC voltage. The transient electrical impedance response depends on the vapor pressure and conductivity of the liquid isomers. A chemical liquid of the structural isomers was identified by
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21

OGOLO, NAOMI A., KINGSLEY AMACHREE, and MIKE O. ONYEKONWU. "Clay stability with nanoparticles in a polar and non-polar liquid." Journal of Engineering Sciences and Innovation 9, no. 2 (2024): 141–48. https://doi.org/10.56958/jesi.2024.9.2.141.

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Clay dispersed in polar or non-polar liquids has various industrial uses. In the petroleum industry, clay suspended in oil-based mud is used in drilling sensitive formations. In crude oil refining, clay serves as catalysts in dehydrating ethanol and for other purposes. Clay stability in fluids is critical, necessitating deployment of additives to maintain stability. It is speculated that some nanoparticles have the potential to stabilize clays in fluids. This work therefore focuses on identifying types of nanoparticles that can promote clay stability in polar and non-polar liquids. Nine kinds
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22

Pavlovica, S., E. Gzibovska, A. Zicmanis, P. Mekss, and M. Klavins. "Hydrophilic Ionic Liquids in the Synthesis of Hantzsch Ester." Latvian Journal of Chemistry 50, no. 3-4 (2011): 277–83. http://dx.doi.org/10.2478/v10161-011-0064-6.

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Hydrophilic Ionic Liquids in the Synthesis of Hantzsch Ester Hantzsch ester synthesis was investigated using (2-hydroxyethyl)-ammonium carboxylates, polar and hydrophilic ionic liquids possessing low toxicity and high biodegradability. The reaction rates and yields of the products in ionic liquids were greater than those in common organic solvents. The relationship between the structure of the ionic liquid used and the structure of the heterocyclic compound was investigated.
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23

Taghiyari, Hamid R., Roya Majidi, Mahnaz Ghezel Arsalan, et al. "Penetration of Different Liquids in Wood-Based Composites: The Effect of Adsorption Energy." Forests 12, no. 1 (2021): 63. http://dx.doi.org/10.3390/f12010063.

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The penetration properties of three different liquids on the surface of medium-density fiberboard (MDF) and particleboard panels were studied. Water, as a polar liquid, was compared to two other less polar liquids (namely, ethanol and kerosene) with significantly larger molecules. Measurement of penetration time and wetted area demonstrated significantly higher values for water in comparison with the other two liquids, in both composite types. Calculation of adsorption energies, as well as adsorption distances, of the three liquid molecules on hemicellulose showed higher potentiality of water
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24

Taghiyari, Hamid R., Roya Majidi, Mahnaz Ghezel Arsalan, et al. "Penetration of Different Liquids in Wood-Based Composites: The Effect of Adsorption Energy." Forests 12, no. 1 (2021): 63. http://dx.doi.org/10.3390/f12010063.

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The penetration properties of three different liquids on the surface of medium-density fiberboard (MDF) and particleboard panels were studied. Water, as a polar liquid, was compared to two other less polar liquids (namely, ethanol and kerosene) with significantly larger molecules. Measurement of penetration time and wetted area demonstrated significantly higher values for water in comparison with the other two liquids, in both composite types. Calculation of adsorption energies, as well as adsorption distances, of the three liquid molecules on hemicellulose showed higher potentiality of water
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25

Kolmachikhina, E. B., E. A. Ryzhkova, and D. V. Dmitrieva. "Influence of Zinc Sulfide Wetting in Surfactants Presence on Leaching Parameters." Solid State Phenomena 284 (October 2018): 737–42. http://dx.doi.org/10.4028/www.scientific.net/ssp.284.737.

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This paper is describing an investigation of surfactants influence on zinc sulfide wetting by non-polar liquids and sphalerite concentrates pressure leaching parameters. Zinc sulfide preferential wettability by oil was tested in presence anionic surfactants with different chemical structures. Interfacial tension was determinated by the maximum liquid drop volume method. It allows to determine surfactant potential effectivity on pressure leaching of sphalerite concentrate. It is found that SDBS decreases zinc sulfide wettability by non-polar liquids in a greater degree than SDS and Ls. Combined
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26

Wiącek, Agnieszka Ewa, and Monika Sujka. "Physicochemical Characteristics of Porous Starch Obtained by Combined Physical and Enzymatic Methods—Part 2: Potential Application as a Carrier of Gallic Acid." Molecules 29, no. 15 (2024): 3570. http://dx.doi.org/10.3390/molecules29153570.

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Wettability measurements were performed for aqueous dispersions of native and modified corn, potato, and pea starch granules deposited on glass plates by the thin layer method using test liquids of a different chemical nature (polar water and formamide or non-polar diiodomethane). High values of the determination coefficient R2 confirm that the linear regression model describes the relationship between the wetting time and the square of the penetration distance very well, indicating the linear nature of the Washburn relationship. A change in free energy (enthalpy) during the movement of the li
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27

Cho, Minhaeng. "Vibrational relaxation rates of a polar molecule in polar liquids." Journal of Chemical Physics 105, no. 24 (1996): 10755–65. http://dx.doi.org/10.1063/1.472883.

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28

Georgiev, Georgi As, Stanislav Baluschev, Petar Eftimov, Mihaela Bacheva, and Katharina Landfester. "Addressing the Apparent Controversies Between the Contact Angle-Based Models for Estimation of Surface Free Energy: A Critical Review." Colloids and Interfaces 8, no. 6 (2024): 62. http://dx.doi.org/10.3390/colloids8060062.

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The most popular contact angle (CA)-based approaches for determination of solid surface free energy (SFE) are considered: (i) single liquid methods, mainly of Neumann and Chibowski, (ii) the multiple liquids approach of Owens–Wendt–Rabel–Kaelble (OWRK), and (iii) van Oss-Chaudhury–Good (vOCG) acid–base model. Evaluations based on Neumann and Chibowski models agree between each other. Under the assumption of equilibrium “wet wetting” (i.e., presence of saturated precursor film ahead of the drop), the model of Chibowski transforms in Lipatov’s interfacial equilibrium rule, i.e., the Antonow rule
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29

Tie, Lu, Jing Li, Zhiguang Guo, Yongmin Liang, and Weimin Liu. "An all superantiwetting surface in water–oil–air systems." Journal of Materials Chemistry A 7, no. 12 (2019): 6957–62. http://dx.doi.org/10.1039/c8ta12521j.

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Six superantiwetting states, superhydrophobicity, superoleophobicity, underoil superhydrophobicity, underwater superoleophobicity, and underoil and underwater superaerophobicity, are realized on one surface. The all superantiwetting surface can be extended to polar liquid–nonpolar liquid–air systems and be used for on-demand separation of immiscible organic liquids.
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30

Kurnia, Kiki Adi, Pranesh Matheswaran, Choo Jia How, Mohd Hilmi Noh, and Yuly Kusumawati. "A comprehensive study on the impact of chemical structures of ionic liquids on the solubility of ethane." New Journal of Chemistry 44, no. 26 (2020): 11155–63. http://dx.doi.org/10.1039/d0nj02221g.

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The solubility of ethane is not only governed by the electrostatic–misfit of the solute toward ionic liquids, but also the existence of a preferential site for ethane to interact with the ionic liquid's non-polar moiety.
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31

Rossky, P. J. "The Structure of Polar Molecular Liquids." Annual Review of Physical Chemistry 36, no. 1 (1985): 321–46. http://dx.doi.org/10.1146/annurev.pc.36.100185.001541.

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32

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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33

Zhang, Q., and J. P. Badiali. "Optical birefringence in inhomogeneous polar liquids." Molecular Physics 75, no. 2 (1992): 325–31. http://dx.doi.org/10.1080/00268979200100261.

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34

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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35

Khrapak, A. G., and W. F. Schmidt. "Negative ions in non-polar liquids." International Journal of Mass Spectrometry 277, no. 1-3 (2008): 236–39. http://dx.doi.org/10.1016/j.ijms.2008.04.011.

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36

Mechetti, H., and E. Zakowicz. "Critical number density in polar liquids." Chemical Physics Letters 128, no. 5-6 (1986): 563–64. http://dx.doi.org/10.1016/0009-2614(86)80674-1.

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37

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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38

Selin Tosun, B., Boris D. Chernomordik, Aloysius A. Gunawan, et al. "Cu2ZnSnS4 nanocrystal dispersions in polar liquids." Chemical Communications 49, no. 34 (2013): 3549. http://dx.doi.org/10.1039/c3cc40388b.

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39

Rips, Ilya. "Electron solvation dynamics in polar liquids." Chemical Physics Letters 245, no. 1 (1995): 79–84. http://dx.doi.org/10.1016/0009-2614(95)00963-5.

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40

Kroh, H. J., and B. U. Felderhof. "Electromagnetodynamics of polar liquids and suspensions." Zeitschrift f�r Physik B Condensed Matter 66, no. 1 (1987): 1–6. http://dx.doi.org/10.1007/bf01312756.

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41

Thagard, Selma Mededovic, Kazunori Takashima, and Akira Mizuno. "Electrical Discharges in Polar Organic Liquids." Plasma Processes and Polymers 6, no. 11 (2009): 741–50. http://dx.doi.org/10.1002/ppap.200900017.

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42

Kloubek, Jan. "Interactions of components and elements of the surface free energy at interfaces." Collection of Czechoslovak Chemical Communications 56, no. 2 (1991): 277–95. http://dx.doi.org/10.1135/cccc19910277.

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A new hypothesis is suggested for the evaluation of the components (γd and γab) and the elements (γa and γb) of the surface free energy. The respective equations are introduced for the interactions at interfaces between a non-polar acid and non-polar base, a polar phase and non-polar acid or base, and two polar phases. The dispersion component, γd, equals the total surface free energy of non-polar phases. However, they can interact at the interface as an acid or a base through their single permanent elements γa or γb, respectively. Otherwise, induced elements γia and γib can also be effective.
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43

Nikitin, Pavel A., and Vitold E. Pozhar. "Evaluation of the Acousto-Optic Figure of Merit and the Maximum Value of the Elasto-Optic Constant of Liquids." Materials 17, no. 12 (2024): 2810. http://dx.doi.org/10.3390/ma17122810.

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The elasto-optic properties of liquids on the basis of the first principles of acousto-optics were theoretically investigated. A relationship for calculating the elasto-optic constant of liquids using only the refractive index was obtained. The refractive index values corresponding to the maximum elasto-optic constant for polar and nonpolar liquids were determined. Calculations for about 100 liquids were performed and compared with known experimental data. This study significantly extends our understanding of the acousto-optic effect and has practical applications for predicting the elasto-opt
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44

Lenhard, Robert J., and Royal H. Brooks. "Comparison of Liquid Retention Curves with Polar and Nonpolar Liquids." Soil Science Society of America Journal 49, no. 4 (1985): 816–21. http://dx.doi.org/10.2136/sssaj1985.03615995004900040005x.

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45

Pereira, Matheus M., Kiki A. Kurnia, Filipa L. Sousa, et al. "Contact angles and wettability of ionic liquids on polar and non-polar surfaces." Physical Chemistry Chemical Physics 17, no. 47 (2015): 31653–61. http://dx.doi.org/10.1039/c5cp05873b.

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46

Magsumov, Timur I., and Igor A. Sedov. "Nanoheterogeneity in Protic and Aprotic Alkylimidazolium Bistriflimide Ionic Liquids." Liquids 4, no. 3 (2024): 632–46. http://dx.doi.org/10.3390/liquids4030035.

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Many ionic liquids, including alkylimidazolium salts, form a nanoheterogeneous structure with polar and apolar domains in their liquid phase. Using molecular dynamics simulations, the influence of the structure of the cations of a series of aprotic ([CnC1Im][TFSI], [CnCnIm][TFSI]) and protic ([HCnIm][TFSI]) alkylimidazolium bistrilimides on the domain structure of their liquid phase was studied. The characteristic sizes of domains and the extent of domain segregation in different liquids have been compared. It has been shown that the latter, but not the former, is a key factor determining the
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Yadav, Ranjit Prasad. "Analysis of Dielectric Properties of Some Polar and Non-Polar Liquids." Academic Voices: A Multidisciplinary Journal 8, no. 1 (2018): 70–77. https://doi.org/10.3126/av.v8i1.74053.

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The study of dielectric behavior of polar, non polar liquids and their binary mixtures at various temperatures is very interesting. In this article the values of dielectric constant of polar, non polar &amp; their binary mixtures has been experimentally determined and study their properties at various temperatures 288k, 298k, 308k &amp; 318 K. In this experiment the dielectric constant of the mixture of carbon tetra chloride - ethyl acetate and carbon tetra chloride – dimethyl ether was calculated at different temperatures in different concentrations. The results are discussed in the light of
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Collins, Liam, Stephen Jesse, Jason I. Kilpatrick, et al. "Kelvin probe force microscopy in liquid using electrochemical force microscopy." Beilstein Journal of Nanotechnology 6 (January 19, 2015): 201–14. http://dx.doi.org/10.3762/bjnano.6.19.

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Conventional closed loop-Kelvin probe force microscopy (KPFM) has emerged as a powerful technique for probing electric and transport phenomena at the solid–gas interface. The extension of KPFM capabilities to probe electrostatic and electrochemical phenomena at the solid–liquid interface is of interest for a broad range of applications from energy storage to biological systems. However, the operation of KPFM implicitly relies on the presence of a linear lossless dielectric in the probe–sample gap, a condition which is violated for ionically-active liquids (e.g., when diffuse charge dynamics ar
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49

Samantaray, B., M. K. Praharaj, B. R. Das, and S. P. Das. "Comparative Study of Molecular Interaction in Ternary Liquid Mixtures of Polar and Non-Polar Solvents." Journal of Scientific Research 14, no. 3 (2022): 917–29. http://dx.doi.org/10.3329/jsr.v14i3.57587.

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Ultrasonic velocity measurements, density measurements, and viscometric studies were conducted for the ternary mixture of pyridine and toluene separately with N, N-dimethylformamide (DMF) in butanol, at different temperatures and for different concentrations of component liquids. Using these basic experimental data, various acoustic and thermodynamic parameters, such as adiabatic compressibility (β), free length (Lf,), free volume (Vf), etc. were calculated. Also, Excess thermo-acoustical parameters were calculated from the experimentally measured data. The outcomes were expressed in terms of
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50

Hoang, Hai, and Guillaume Galliero. "Predictive Tait equation for non-polar and weakly polar fluids: Applications to liquids and liquid mixtures." Fluid Phase Equilibria 425 (October 2016): 143–51. http://dx.doi.org/10.1016/j.fluid.2016.05.026.

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