AC Electrokinetic: Colloids and Nanoparticles - download pdf or read online

By Hywel Morgan, Nicolas G. Green

ISBN-10: 0585489491

ISBN-13: 9780585489490

ISBN-10: 0863802559

ISBN-13: 9780863802553

This ebook is an creation to the technology in the back of the recent expertise, and explains how the electrical box interacts with the debris. It describes how those micro-systems are synthetic and the way they're used to check homes of the debris. The authors supply a finished remedy of the underlying rules and governing idea for the AC electrokinetic habit of debris, overview the present state-of-the-art in AC electrokinetic manipulation and characterization of debris, and supply chapters on simulation, equipment layout and fabrication.

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Additional resources for AC Electrokinetic: Colloids and Nanoparticles

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P. On the orientation of non-spherical particles in an alternating electric field J. Chem. Phys. 43 3562-3569 (1965). A. Electromagnetic theory McGraw-Hill, New York (1941). Takashima S. Electrical Properties of Biopolymers and Membranes Adam Hilger, Philadelphia (1989). L. L. H. The behaviour of unicellular organisms in an electromagnetic field Exp. Cell Res. 20 548-564 (1960). , Pethig R. B. Relationship of dielectrophoretic and electrorotational behaviour exhibited by polarized particles J. Phys.

30) with σ% = iωε% . 4. Returning to the definition of the polarisation P, it can be seen that in reality, both conduction currents and displacement currents flow. 7 Energy in a dielectric In a lossy dielectric the total current is given by the sum of J c = σ E and J d = iωε E . 35) where δ is the angle between the conduction and displacement currents, referred to as the loss angle. In a perfectly insulating (non-lossy) dielectric, the loss angle is zero. If the complex permittivity is written as ε% = ε ′ − iε ′′ , the loss angle can also be written as tanδ = ε ′′ / ε ′ .

3 Sphere of radius a centred on the origin, with an applied electric field anti-parallel to the z-axis. The spherical polar co-ordinates are defined as shown, making the problem two dimensional in r and θ. 32) gives the same boundary condition but with the permittivities replaced by complex values. By extrapolation from Lorrain et al. f. 12). 7) This is the effective dipole moment of the sphere. 8) Using this equation, the magnitude of the dipole for a particle can be calculated. Taking for example a field of 106 V m−1, the dipole moment of a particle such as a cell is of the order of 10−19 C m.

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AC Electrokinetic: Colloids and Nanoparticles by Hywel Morgan, Nicolas G. Green

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