Edison Amah et al., Direct Numerical Simulation of Particles in Spatially Varying Electric Fields †, Fluids, 3 (2018) 52-18.
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Anon. (2009), Dielectric Properties, Electric Energy and Force , , 2009 pp. 1-25.
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I Prigogine, Advances in Chemical Physics, , 2018 pp. 1-552.
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Anon. (2005), Chapter 7 - Dielectrics in the Electrostatic Field, , 2005 pp. 1-21.
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G Kennedy and J Martins, An adjoint-based derivative evaluation method for time-dependent aeroelastic optimization of flexible aircraft, Arc.Aiaa.Org, .
The goal of this paper is to develop techniques to enable the use of aeroelastic constraints within a high-fidelity design optimization framework. As a first-step towards this goal we have developed a fully-coupled aeroelastic analysis tool that includes a coupled structural and aerodynamic analysis as well as rigid-body degrees of freedom. This work departs from previous efforts in two important ways: first, we use solution techniques that are tailored for high-performance parallel computing; second, we implement a fully-coupled adjoint method …
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Anon. (2009), Strong Permittivity Fluctuations , , 2009 pp. 1-25.
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Hoi Sung Chung et al., Experimental determination of upper bound for transition path times in protein folding from single-molecule photon-by-photon trajectories, Proceedings Of The National Academy Of Sciences Of The United States Of America, 106 (2009) 11837-11844.
Transition paths are a uniquely single-molecule property not yet observed for any molecular process in solution. The duration of transition paths is the tiny fraction of the time in an equilibrium single-molecule trajectory when the process actually happens. Here, we report the determination of an upper bound for the transition path time for protein folding from photon-by-photon trajectories. FRET trajectories were measured on single molecules of the dye-labeled, 56-residue 2-state protein GB1, immobilized on a glass surface via a biotin-streptavidin-biotin linkage. Characterization of individual emitted photons by their wavelength, polarization, and absolute and relative time of arrival after picosecond excitation allowed the determination of distributions of FRET efficiencies, donor and acceptor lifetimes, steady state polarizations, and waiting times in the folded and unfolded states. Comparison with the results for freely diffusing molecules showed that immobilization has no detectable effect on the structure or dynamics of the unfolded protein and only a small effect on the folding/unfolding kinetics. Analysis of the photon-by-photon trajectories yields a transition path time <200 μs, >10,000 times shorter than the mean waiting time in the unfolded state (the inverse of the folding rate coefficient). Szabo9s theory for diffusive transition paths shows that this upper bound for the transition path time is consistent with previous estimates of the Kramers preexponential factor for the rate coefficient, and predicts that the transition path time is remarkably insensitive to the folding rate, with only a 2-fold difference for rate coefficients that differ by 105-fold.
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Elena Bichoutskaia et al., Electrostatic analysis of the interactions between charged particles of dielectric materials, The Journal Of Chemical Physics, 133 (2010) 024105-11.
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Cem Civelek and Thomas Franz Bechteler, Lagrangian formulation of electromagnetic fields in nondispersive medium by means of the extended Euler–Lagrange differential equation, International Journal Of Engineering Science, 46 (2008) 1218-1227.
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Filippo Costa et al., Electromagnetic Characterisation of Materials by Using Transmission/Reflection (T/R) Devices, Electronics, 6 (2017) 95-27.
An overview of transmission/reflection-based methods for the electromagnetic characterisation of materials is presented. The paper initially describes the most popular approaches for the characterisation of bulk materials in terms of dielectric permittivity and magnetic permeability. Subsequently, the limitations and the methods aimed at removing the ambiguities deriving from the application of the classical Nicolson–Ross–Weir direct inversion are discussed. The second part of the paper is focused on the characterisation of partially conductive thin sheets in terms of surface impedance via waveguide setups. All the presented measurement techniques are applicable to conventional transmission reflection devices such as coaxial cables or waveguides.
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Michael E Crenshaw, The Theory of Electrodynamics in a Linear Dielectric, Arxiv.Org, 2013 1303.1412v3, physics.class-ph.
We adopt the continuum limit of a linear, isotropic, homogeneous, transparent, dispersion-negligible dielectric of refractive index n and examine the consequences of the effective speed of light in a stationary dielectric, c/n, for D'Alembert's principle and the Lagrange equations. The principles of dynamics in the dielectric-filled space are then applied to the electromagnetic Lagrangian and we derive equations of motion for the macroscopic fields. A direct derivation of the total energy--momentum tensor from the field strength tensor for the electromagnetic field in a dielectric is used to demonstrate the utility of the new theory by resolving the century-old Abraham--Minkowski electromagnetic momentum controversy in a way that preserves the principles of conservation of energy, conservation of linear momentum, and conservation of angular momentum.
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Vikram Jadhao et al., A variational formulation of electrostatics in a medium with spatially varying dielectric permittivity, The Journal Of Chemical Physics, 138 (2013) 054119-14.
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Felix M Kamenetsky, Equations of the electromagnetic field in dispersive media , , 2009 pp. 1-12.
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Armik Khachatourian et al., Electrostatic force between a charged sphere and a planar surface: A general solution for dielectric materials, The Journal Of Chemical Physics, 140 (2014) 074107-11.
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G Li and NR Aluru, A Lagrangian approach for electrostatic analysis of deformable conductors, Journal Of Microelectromechanical Systems, 2002.
Deformable conductors are frequently encountered in microelectromechanical systems (MEMS). For example, in electrostatic MEMS, microstructures undergo deformations because of electrostatic forces caused by applied potentials. Computational analysis of electrostatic MEMS requires an electrostatic analysis to compute the electrostatic forces acting on micromechanical structures and a mechanical analysis to compute the deformation of micromechanical structures. Typically, the mechanical analysis is performed …
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Per Linse, Electrostatics in the presence of spherical dielectric discontinuities, The Journal Of Chemical Physics, 128 (2008) 214505-14.
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S Habib Mazharimousavi and Ashkan Roozbeh, Electromagnetic wave propagation through inhomogeneous material layers, Psychological Perspectives, 27 (2013) 2065-2074.
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Tsymbal, Section 4: Electrostatics of Dielectrics, , 2015 pp. 1-16.
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Markus Zahn, Electromagnetic Field Theory - A Problem-Solving Approach – Chapter 3: Polarization and Conduction, , 2016 pp. 1-123.
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cline, Electric Fields in Dielectrics , , 2014 pp. 1-7.
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jew, Electrostatic Polarization, , 2010 pp. 1-23.
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senben, Chapter 5 Capacitance and Dielectrics, , 2003 pp. 1-46.
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