Journal articles: 'Non-ideal behavior'

1

Thio, Y., and L. Frost. "Non-ideal plasma behavior of railgun arcs." IEEE Transactions on Magnetics 22, no. 6 (November 1986): 1757–62. http://dx.doi.org/10.1109/tmag.1986.1064721.

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2

Iliuk, Itamar, José Manoel Balthazar, Angelo Marcelo Tusset, Jorge Luiz Palácios Felix, and Bento Rodrigues de Pontes. "On Non-ideal and Chaotic Energy Harvester Behavior." Differential Equations and Dynamical Systems 21, no. 1-2 (June 20, 2012): 93–104. http://dx.doi.org/10.1007/s12591-012-0127-5.

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3

Lawryshyn, Yuri, and Kuang-ping Chiu. "UV Reactor Validation: Implications of Non-ideal Reactor Behavior." Proceedings of the Water Environment Federation 2002, no. 16 (January 1, 2002): 750. http://dx.doi.org/10.2175/193864702784246621.

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4

Demana, Tshenge, Chang-Yuh Chen, and Michael D. Morris. "Non-ideal behavior in analyte velocity modulation capillary electrophoresis." Journal of High Resolution Chromatography 13, no. 8 (August 1990): 587–89. http://dx.doi.org/10.1002/jhrc.1240130817.

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5

Pospíšil, Rudolf, Tomáš Sommer, Martin Zapletal, Jiří Krupka, and Jiří Trejbal. "Influence of non-ideal behavior on esterification kinetics modeling." Reaction Kinetics, Mechanisms and Catalysis 130, no. 2 (June 13, 2020): 617–32. http://dx.doi.org/10.1007/s11144-020-01796-7.

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6

Kristensen, Eric W., David H. Igo, R. C. Elder, and William R. Heineman. "Non-ideal behavior of Nernstian plots from spectroelectrochemistry experiments." Journal of Electroanalytical Chemistry and Interfacial Electrochemistry 309, no. 1-2 (July 1991): 61–72. http://dx.doi.org/10.1016/0022-0728(91)87004-n.

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7

Moldover, Michael R. "D. Yu. Ivanov: Critical Behavior of Non-Ideal Systems." International Journal of Thermophysics 31, no. 6 (June 2010): 1220–22. http://dx.doi.org/10.1007/s10765-010-0812-y.

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8

Mahal, M. K., Asami Murao, Gwynn R. Johnson, Ann E. Russo, and Mark L. Brusseau. "Non-ideal Behavior During Complete Dissolution of Organic Immiscible Liquid: 2. Ideal Porous Media." Water, Air, & Soil Pollution 213, no. 1-4 (March 30, 2010): 191–97. http://dx.doi.org/10.1007/s11270-010-0377-1.

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9

Sandoval-Ibarra, Federico D., Arturo A. Garcia-Figueroa, José L. López-Cervantes, and Jesús Gracia-Fadrique. "SAC: Surface activity coefficient, a function to unveil surface and bulk’s ideal - non ideal behavior." Fluid Phase Equilibria 546 (October 2021): 113120. http://dx.doi.org/10.1016/j.fluid.2021.113120.

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10

Chacón, R., and A. Martínez García-Hoz. "Chaotic behavior in a dissipative non-ideal periodically kicked rotator." Physics Letters A 281, no. 4 (March 2001): 231–39. http://dx.doi.org/10.1016/s0375-9601(01)00134-7.

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11

Willis, C. "WE-D-330D-02: Non-Ideal Behavior of DR Systems." Medical Physics 33, no. 6Part20 (June 2006): 2242. http://dx.doi.org/10.1118/1.2241752.

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12

Chiroiu, Veturia, and Dan Dumitriu. "On the chaotic behavior of the non-ideal vibrating systems." PAMM 15, no. 1 (October 2015): 245–46. http://dx.doi.org/10.1002/pamm.201510113.

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13

Arora, Rajan, and Mohd Junaid Siddiqui. "Evolutionary behavior of weak shocks in a non-ideal gas." Journal of Theoretical and Applied Physics 7, no. 1 (2013): 14. http://dx.doi.org/10.1186/2251-7235-7-14.

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14

Dubin, Paul L., Shun L. Edwards, Mamta S. Mehta, and Donald Tomalia. "Quantitation of non-ideal behavior in protein size-exclusion chromatography." Journal of Chromatography A 635, no. 1 (April 1993): 51–60. http://dx.doi.org/10.1016/0021-9673(93)83113-7.

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15

Kaminski, A., J. J. Marchand, and A. Laugier. "Non ideal dark I–V curves behavior of silicon solar cells." Solar Energy Materials and Solar Cells 51, no. 3-4 (February 1998): 221–31. http://dx.doi.org/10.1016/s0927-0248(97)00216-x.

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16

Moya, Cristian, Maria Gonzalez-Miquel, Francisco Rodriguez, Ana Soto, Hector Rodriguez, and Jose Palomar. "Non-ideal behavior of ionic liquid mixtures to enhance CO2 capture." Fluid Phase Equilibria 450 (October 2017): 175–83. http://dx.doi.org/10.1016/j.fluid.2017.07.014.

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17

Pereyra, Romina B., Guillermo A. Durand, Marcos Fernández Leyes, Hernán Ritacco, and Erica P. Schulz. "Homologous mixed micellar systems with non-ideal and asymmetric thermodynamic behavior." Colloids and Surfaces A: Physicochemical and Engineering Aspects 594 (June 2020): 124626. http://dx.doi.org/10.1016/j.colsurfa.2020.124626.

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18

Yang, Chane-Yuan, Yu-Shu Chien, Jun-Hong Chou, Hsing-Ya Li, and Chau Wei Hsieh. "Application of Cholette’s model in non-ideal mixing CSTR: a simulation study on dynamic behavior." International Journal of Chemical Reactor Engineering 19, no. 4 (February 23, 2021): 341–67. http://dx.doi.org/10.1515/ijcre-2020-0197.

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Abstract Non-ideal mixing phenomena are widely found in industrial chemical reactors. In this work we derived the bifurcation formulas for a non-adiabatic CSTR with an irreversible exothermic first order reaction with the non-ideal mixing effect. This is investigated via dynamic behavior simulations based on Chollete’s model. The results show that the non-ideal mixing parameter n (the fraction of the feed entering the perfect mixing zone) determines the variation between six classified regions and dominates the dynamic behavior patterns in the steady-state response diagram. On the other hand, the phase portraits of examples verify the formulas derived in this work. We note that the non-ideal mixing effect has significant importance in CSTR design and control steps. For example, in the safe operating region for an ideal mixing CSTR, non-linear dynamics are obtained by the system under non-ideal mixing conditions (n ≠ 1). The present study has significance and help for chemical reactor design and CSTR control.

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19

Fadhil, Maytham, and Jawad Mahmood. "PLC-HMI BASED SIMULATION of PV CELL and ARRAY BEHAVIOR." Iraqi Journal for Electrical and Electronic Engineering 15, no. 2 (December 1, 2019): 130–37. http://dx.doi.org/10.37917/ijeee.15.2.14.

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This paper presents the PLC-HMI based simulation of electrical-based PV cell/array model in laboratory platform to give the opportunity to students and users who haven't clear knowledge to study PV cell and array behavior with respect to change of environment conditions and electrical parameters. This simulation process covers the cell models under ideal and non-ideal ones. In non-ideal one, the series resistance and the shunt resistance are covered.

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20

da Costa Ferreira, Douglas, Fábio Roberto Chavarette, Cláudio Henrique Cerqueira Costa Basquerotto, and Nelson José Peruzzi. "Non-Ideal Excitation Approach for Piezoelectric Vibration Based Energy Harvesting." Advanced Materials Research 936 (June 2014): 2160–64. http://dx.doi.org/10.4028/www.scientific.net/amr.936.2160.

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Common solution for energy harvester device is project design according harmonic excitation around natural frequency matching excitation source. Environment vibration is random and wide band causing short time of resonance in disagreement of project objectives. Control driven of energy harvesting to take advantage of the higher vibration range can results in greater energy converted. This study investigates a non-ideal excitation behavior and their efficiency in convert electricity via piezoelectric direct effect from the available system energy compared to harmonic excitation source. Numeric evaluation was performed based in bimorph piezoelectric beam in dimensionless consideration. Chaos behavior and harvest energy capability were compared from non-ideal to harmonic excitation. Results demonstrate considerable higher quantity of energy available for non-ideal approach compared to harmonic resonant design and encourages advance study to control and enhance energy from random and wide band vibration source.

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21

Jung, Hojung, Mukul M. Sharma, Dave D. Cramer, Sean Oakes, and Mark W. McClure. "Re-examining interpretations of non-ideal behavior during diagnostic fracture injection tests." Journal of Petroleum Science and Engineering 145 (September 2016): 114–36. http://dx.doi.org/10.1016/j.petrol.2016.03.016.

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22

Mediwaththe, Chathurika P., and David B. Smith. "Game-Theoretic Electric Vehicle Charging Management Resilient to Non-Ideal User Behavior." IEEE Transactions on Intelligent Transportation Systems 19, no. 11 (November 2018): 3486–95. http://dx.doi.org/10.1109/tits.2017.2784418.

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23

KOUDYMOV, ALEXEI, and MICHAEL SHUR. "NON-IDEAL CURRENT TRANSPORT IN HETEROSTRUCTURE FIELD EFFECT TRANSISTORS." International Journal of High Speed Electronics and Systems 18, no. 04 (December 2008): 935–47. http://dx.doi.org/10.1142/s0129156408005898.

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We describe a new analytical model of a Heterostructure Field Effect Transistors (HFETs) that accounts for electron trapping in the gate-drain spacing of the device and for related non-ideal device behavior. Under conditions of a very strong trapping, the electron velocity saturates outside the gate, in the trapping region, and the negative trapped charge leads to relatively large differential output conductance at the drain voltages exceeding the knee voltage. Also under the conditions of severe trapping, the negative trapped charge leads to the positive offset of the output current-voltage (I-V) characteristic. The model describes quite well numerous experimental data for passivated and unpassivated AlGaN / GaN HFETs with and without field plates (FP) under different bias conditions.

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24

Beauregard, Paul. "Behavior of Particle Size Distributions, Means and BET Values in Ideal and Non-Ideal Morphology Systems in a TEM." Microscopy Today 12, no. 1 (January 2004): 30–33. http://dx.doi.org/10.1017/s1551929500051798.

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Historically, one of the first jobs performed by the new instrument called a “transmission electron microscope” (TEM) was the determination of particle size and distribution. Particle size is still important in controlling the properties of sub-micron and nanoparticle products. The width and average particle size can determine the light scattering properties of a pigment like TiO2, for example. The cost of installing a TEM facility and TEM sample preparation issues makes TEM analysis expensive and labor intensive. So decades ago, nitrogen BET (Brunauer, Emmett, and Teller) surface area determinations were used on sub-micron powders and pigments to minimize these costs. The BET measurement of the exposed external surface area of a material is made by detecting and measuring the amount of nitrogen given off after absorption, assuming one atomic layer of nitrogen is adsorbed.

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25

Krenn, C. R., D. Roundy, J. W. Morris, and Marvin L. Cohen. "The non-linear elastic behavior and ideal shear strength of Al and Cu." Materials Science and Engineering: A 317, no. 1-2 (October 2001): 44–48. http://dx.doi.org/10.1016/s0921-5093(01)01178-9.

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26

Lee, Ahra, Hyoungho Ko, Dong-il “Dan” Cho, and Gunn Hwang. "Non-ideal behavior of a driving resonator loop in a vibratory capacitive microgyroscope." Microelectronics Journal 39, no. 1 (January 2008): 1–6. http://dx.doi.org/10.1016/j.mejo.2007.10.025.

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27

Skaugen, G., M. Hammer, and M. Aa Gjennestad. "Investigation of Non-ideal Behavior of Plate-fin Heat Exchangers in LNG Services." Energy Procedia 64 (2015): 13–22. http://dx.doi.org/10.1016/j.egypro.2015.01.004.

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28

Chavarette, Fábio Roverto. "On an Optimal Linear Control of a Chaotic Non-Ideal Duffing System." Applied Mechanics and Materials 138-139 (November 2011): 50–55. http://dx.doi.org/10.4028/www.scientific.net/amm.138-139.50.

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In this work, we use a nonlinear control based on Optimal Linear Control. We used as mathematical model a Duffing equation to model a supporting structure for an unbalanced rotating machine with limited power (non-ideal motor). Numerical simulations are performed for a set control parameter (depending on the voltage of the motor, that is, in the static and dynamic characteristic of the motor) The interaction of the non-ideal excitation with the structure may lead to the occurrence of interesting phenomena during the forward passage through the several resonance states of the system. Chaotic behavior is obtained for values of the parameters. Then, the proposed control strategy is applied in order to regulate the chaotic behavior, in order to obtain a periodic orbit and to decrease its amplitude. Both methodologies were used in complete agreement between them. The purpose of the paper is to give suggestions and recommendations to designers and engineers on how to drive this kind of system through resonance.

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29

Fedosov, Dmitry A., Ankush Sengupta, and Gerhard Gompper. "Effect of fluid–colloid interactions on the mobility of a thermophoretic microswimmer in non-ideal fluids." Soft Matter 11, no. 33 (2015): 6703–15. http://dx.doi.org/10.1039/c5sm01364j.

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Thermophoretic Janus colloids offer promising prospects as artificial microswimmers. Their swimming behavior is investigated numerically for different fluid–colloid interactions, boundary conditions, and temperature-controlling strategies in non-ideal and ideal-gas-like fluids.

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30

CAMERON, I. "A MECHANISTIC VIEW OF THE NON-IDEAL OSMOTIC AND MOTIONAL BEHAVIOR OF INTRACELLULAR WATER." Cell Biology International 21, no. 2 (February 1997): 99–113. http://dx.doi.org/10.1006/cbir.1996.0123.

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31

Rocha, Rodrigo Tumolin, Jose Manoel Balthazar, Angelo Marcelo Tusset, Silvio Luiz Thomaz de Souza, Frederic Conrad Janzen, and Hassan Costa Arbex. "On a non-ideal magnetic levitation system: nonlinear dynamical behavior and energy harvesting analyses." Nonlinear Dynamics 95, no. 4 (January 29, 2019): 3423–38. http://dx.doi.org/10.1007/s11071-019-04765-5.

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32

Kang, Won Jun, Kyung Su Kim, Cheol Hyoun Ahn, Sung Woon Cho, Da Eun Kim, Bora Kim, Hyung Koun Cho, and Yunseok Kim. "Non-ideal current drop behavior in ultra-thin inorganic a-InGaZnO thin film transistors." Journal of Materials Science: Materials in Electronics 28, no. 11 (February 15, 2017): 8231–37. http://dx.doi.org/10.1007/s10854-017-6534-1.

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33

Sun, Wendell Q. "86. Non-ideal phase behavior of freeze-concentrated ice/amorphous system during freeze drying." Cryobiology 53, no. 3 (December 2006): 404. http://dx.doi.org/10.1016/j.cryobiol.2006.10.087.

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34

Zavitsas, Andreas A. "Ideal Behavior of Water Solutions of Strong Electrolytes and Non-electrolytes at High Concentrations." Journal of Solution Chemistry 39, no. 3 (March 2010): 301–17. http://dx.doi.org/10.1007/s10953-010-9503-3.

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35

Hoarau, Jean-Christophe, Paola Cinnella, and Xavier Gloerfelt. "Large Eddy Simulations of Strongly Non-Ideal Compressible Flows through a Transonic Cascade." Energies 14, no. 3 (February 1, 2021): 772. http://dx.doi.org/10.3390/en14030772.

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Transonic flows of a molecularly complex organic fluid through a stator cascade were investigated by means of large eddy simulations (LESs). The selected configuration was considered as representative of the high-pressure stages of high-temperature Organic Rankine Cycle (ORC) axial turbines, which may exhibit significant non-ideal gas effects. A heavy fluorocarbon, perhydrophenanthrene (PP11), was selected as the working fluid to exacerbate deviations from the ideal flow behavior. The LESs were carried out at various operating conditions (pressure ratio and total conditions at inlet), and their influence on compressibility and viscous effects is discussed. The complex thermodynamic behavior of the fluid generates highly non-ideal shock systems at the blade trailing edge. These are shown to undergo complex interactions with the transitional viscous boundary layers and wakes, with an impact on the loss mechanisms and predicted loss coefficients compared to lower-fidelity models relying on the Reynolds-averaged Navier–Stokes (RANS) equations.

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36

Bellini, Stefano, Yu Sun, Fausto Gallucci, and Alessio Caravella. "Thermodynamic Aspects in Non-Ideal Metal Membranes for Hydrogen Purification." Membranes 8, no. 3 (September 16, 2018): 82. http://dx.doi.org/10.3390/membranes8030082.

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In this paper, an overview on thermodynamic aspects related to hydrogen-metal systems in non-ideal conditions is provided, aiming at systematically merging and analyzing information achieved from several different studies present in the open literature. In particular, the relationships among inner morphology, dissolved hydrogen and internal stresses are discussed in detail, putting in evidence the conformation complexity and the various types of dislocations induced by the presence of H-atoms in the lattice. Specifically, it is highlighted that the octahedral sites are preferentially occupied in the FCC metals (such as palladium), whereas tetrahedral sites are more energetically favored in BCC-structured ones (such as vanadium). These characteristics are shown to lead to a different macroscopic behavior of the two classes of metals, especially in terms of solubility and mechanical failure due to the consequent induced stresses. Furthermore, starting from the expression of the chemical potential generally presented in the literature, a new convenient expression of the activity of the H-atoms dissolved into the metal lattice as a function of the H-concentration is achieved. Such an activity expression is then used in the dissolution equilibrium relationship, which is shown to be the overall result of two different phenomena: (i) dissociative adsorption of molecular hydrogen onto the surface; and (ii) atomic hydrogen dissolution from the surface to the metal bulk. In this way, the obtained expression for equilibrium allows a method to calculate the equilibrium composition in non-ideal conditions (high pressure), which are of interest for real industrial applications.

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37

Malik, O., V. Grimalsky, and J. De la Hidalga-W. "Behavior of an optical sensor based on non-ideal silicon capacitors: From amplification to generation." Sensors and Actuators A: Physical 130-131 (August 2006): 208–13. http://dx.doi.org/10.1016/j.sna.2006.01.014.

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38

Bell, Katherine Young, and Eugene J. LeBoeuf. "Mechanistic Investigation of Non-Ideal Sorption Behavior in Natural Organic Matter. 1. Vapor Phase Equilibrium." Environmental Science & Technology 46, no. 12 (June 11, 2012): 6689–97. http://dx.doi.org/10.1021/es204726p.

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39

An, Ning, Yufeng An, Zhongai Hu, Bingshu Guo, Yuying Yang, and Ziqiang Lei. "Graphene hydrogels non-covalently functionalized with alizarin: an ideal electrode material for symmetric supercapacitors." Journal of Materials Chemistry A 3, no. 44 (2015): 22239–46. http://dx.doi.org/10.1039/c5ta05812k.

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Alizarin (AZ) with a multi-electron redox center is selected to functionalize three-dimensional self-assembled graphene hydrogels (SGHs) through non-covalent modification and the electrode material shows a good self-synergy and potential self-matching behavior.

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40

Obregón, Octavio, José López, and Marco Ortega-Cruz. "On Quantum Superstatistics and the Critical Behavior of Nonextensive Ideal Bose Gases." Entropy 20, no. 10 (October 9, 2018): 773. http://dx.doi.org/10.3390/e20100773.

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We explore some important consequences of the quantum ideal Bose gas, the properties of which are described by a non-extensive entropy. We consider in particular two entropies that depend only on the probability. These entropies are defined in the framework of superstatistics, and in this context, such entropies arise when a system is exposed to non-equilibrium conditions, whose general effects can be described by a generalized Boltzmann factor and correspondingly by a generalized probability distribution defining a different statistics. We generalize the usual statistics to their quantum counterparts, and we will focus on the properties of the corresponding generalized quantum ideal Bose gas. The most important consequence of the generalized Bose gas is that the critical temperature predicted for the condensation changes in comparison with the usual quantum Bose gas. Conceptual differences arise when comparing our results with the ones previously reported regarding the q-generalized Bose–Einstein condensation. As the entropies analyzed here only depend on the probability, our results cannot be adjusted by any parameter. Even though these results are close to those of non-extensive statistical mechanics for q ∼ 1 , they differ and cannot be matched for any q.

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41

Yang, Yang, Guo Dong Sun, Ming Xin Song, and Zhi Ming Wang. "A Sigma-Delta Modulator System Design with 2-2 Mash Structure." Advanced Materials Research 981 (July 2014): 121–24. http://dx.doi.org/10.4028/www.scientific.net/amr.981.121.

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Σ-Δ modulator structure is increasingly becoming complex, it is very necessary to improve the design efficiency by the level of behavior model in the simulation. The paper discussed several important Σ-Δ modulators with ideal factors, and gives corresponding behavior model. Then, the paper shows a behavior level design with non-ideal factors. Under the condition that sample rate is 256 and input signal frequency is 250 KHz, the SNR can get 105 dB, the effective bit can get 16 bit. It can be used in audio and electronic equipment.

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42

Asatryan, Rubik, Eli Ruckenstein, and Johannes Hachmann. "Revisiting the polytopal rearrangements in penta-coordinate d7-metallocomplexes: modified Berry pseudorotation, octahedral switch, and butterfly isomerization." Chemical Science 8, no. 8 (2017): 5512–25. http://dx.doi.org/10.1039/c7sc00703e.

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43

Liao, Wang, Lang Cheng Lei, and Xiao Dan Zhou. "A 14-Bit Pipeline ADC Behavior Model Using Verilog-A for SOC." Applied Mechanics and Materials 644-650 (September 2014): 3663–66. http://dx.doi.org/10.4028/www.scientific.net/amm.644-650.3663.

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This paper presents the advantage of behavior model. This is useful for the SOC fast verification. A 14 bit pipeline ADC is constructed with simulation of behavior model and the noise model. A comparison of result is illustrated, between the ideal 14 bit ADC behavior model and the 14 bit pipeline ADC with non-idealities.

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44

Grieshammer, Steffen. "The effect of defect interactions on the reduction of doped ceria." Physical Chemistry Chemical Physics 23, no. 17 (2021): 10321–25. http://dx.doi.org/10.1039/d1cp00925g.

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45

Calandra, Pietro, Vincenzo Turco Liveri, Noemi Proietti, Donatella Capitani, Domenico Lombardo, Catalin Gainaru, Roland Böhmer, et al. "Non-ideal mixing behavior in dibutyl phosphate-propylamine binary liquids: Dielectric and nuclear magnetic resonance investigations." Journal of Molecular Liquids 323 (February 2021): 114963. http://dx.doi.org/10.1016/j.molliq.2020.114963.

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46

Tuteja, Anish, Michael E. Mackay, Craig J. Hawker, and Brooke Van Horn. "Effect of Ideal, Organic Nanoparticles on the Flow Properties of Linear Polymers: Non-Einstein-like Behavior." Macromolecules 38, no. 19 (September 2005): 8000–8011. http://dx.doi.org/10.1021/ma050974h.

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47

Reyhanian, Ehsan, Benedikt Dorschner, and Ilya Karlin. "Kinetic Simulations of Compressible Non-Ideal Fluids: From Supercritical Flows to Phase-Change and Exotic Behavior." Computation 9, no. 2 (January 30, 2021): 13. http://dx.doi.org/10.3390/computation9020013.

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We investigate a kinetic model for compressible non-ideal fluids. The model imposes the local thermodynamic pressure through a rescaling of the particle’s velocities, which accounts for both long- and short-range effects and hence full thermodynamic consistency. The model is fully Galilean invariant and treats mass, momentum, and energy as local conservation laws. The analysis and derivation of the hydrodynamic limit is followed by the assessment of accuracy and robustness through benchmark simulations ranging from the Joule–Thompson effect to a phase-change and high-speed flows. In particular, we show the direct simulation of the inversion line of a van der Waals gas followed by simulations of phase-change such as the one-dimensional evaporation of a saturated liquid, nucleate, and film boiling and eventually, we investigate the stability of a perturbed strong shock front in two different fluid mediums. In all of the cases, we find excellent agreement with the corresponding theoretical analysis and experimental correlations. We show that our model can operate in the entire phase diagram, including super- as well as sub-critical regimes and inherently captures phase-change phenomena.

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48

Docampo-Álvarez, Borja, Víctor Gómez-González, Trinidad Méndez-Morales, Julio R. Rodríguez, Oscar Cabeza, Mireille Turmine, Luis J. Gallego, and Luis M. Varela. "The effect of alkyl chain length on the structure and thermodynamics of protic–aprotic ionic liquid mixtures: a molecular dynamics study." Physical Chemistry Chemical Physics 20, no. 15 (2018): 9938–49. http://dx.doi.org/10.1039/c8cp00575c.

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49

TENTELIER, CÉDRIC, THOMAS GUILLEMAUD, SARAH FERRY, and XAVIER FAUVERGUE. "Microsatellite-based parentage analysis reveals non-ideal free distribution in a parasitoid population." Molecular Ecology 17, no. 9 (March 25, 2008): 2300–2309. http://dx.doi.org/10.1111/j.1365-294x.2008.03743.x.

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50

Alişverişçi, G. Füsun. "The Nonlinear Analysis of Vibrational Conveyers with Non-Ideal Crank-and-Rod Exciters." Applied Mechanics and Materials 706 (December 2014): 44–53. http://dx.doi.org/10.4028/www.scientific.net/amm.706.44.

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With the crank-and-rod exciters, the vibrational conveyers have a trough supported on elastic stands which are rigidly fastened to the trough and a supporting frame. The trough is oscillated by a common crank drive. This vibration causes the load to move forward and upward. The movement is strictly related to vibrational parameters. In this study is the transitional behavior across resonance, during the starting of a single degree of freedom vibratory system excited by non-ideal DC motor. The mechanical system depends on the motion of the DC motor. The working rang of vibrational conveyers with cubic nonlinear spring and non-ideal vibration exciter has been analyzed analytically for primary resonance by the Method of Multiple Scales. Lyapunov exponents are numerically calculated and the results of numerical simulation are ploted.

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Journal articles on the topic 'Non-ideal behavior'

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