Download Bioengineering and Biophysical Aspects of Electromagnetic by Ben Greenebaum, Frank S. Barnes PDF

By Ben Greenebaum, Frank S. Barnes

Bioengineering and Biophysical facets of Electromagnetic Fields basically includes discussions at the physics, engineering, and chemical points of electromagnetic (EM) fields at either the molecular point and bigger scales, and investigates their interactions with organic structures. the 1st quantity of the bestselling and newly up to date instruction manual of organic results of Electromagnetic Fields, 3rd version, this e-book provides fabric describing contemporary theoretical advancements, in addition to new information on fabric homes and interactions with susceptible and robust static magnetic fields. Newly separated and improved chapters describe the exterior and inner electromagnetic environments of organisms and up to date advancements within the use of RF fields for imaging.Bioengineering and Biophysical facets of Electromagnetic Fields offers an available review of the present realizing at the clinical underpinnings of those interactions, in addition to a partial creation to experiments at the interactions themselves.

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Extra info for Bioengineering and Biophysical Aspects of Electromagnetic Fields (Handbook of Biological Effects of Electromagnetic Fields, 3Ed)

Example text

A logging device was used, which recorded the fields during two consecutive 24-h periods. 8 mT. 7 V=m. Hansson Mild et al. [20] compared the ELF fields in Swedish and Norwegian residential buildings. The overall mean values were as follows: E fields 54 V=m (SD ¼ 37) and 77 V=m (SD ¼ 58) in Sweden and Norway, respectively; the corresponding values for B fields were 40 nT (SD ¼ 37) and 15 nT (SD ¼ 17). 1 shows additional comparisons. Mccurdy et al. [21] measured women’s exposure in the United States by using personal magnetic field exposure meters that were worn during a working day or a day at home.

1 eV, which is only sufficient to excite vibrational modes in the target molecule. Apparently such excitation is sufficient to cause ionization if the collision process lasts long enough [28]. Except for some laboratory conditions where a sufficiently high potential difference can be applied directly across a biological membrane to bring about its destruction, collisional ionization is generally not a factor in the interaction of electromagnetic waves with tissue: The potential difference required for membrane destruction [29] is between 100 nV and 300 mV, corresponding to a field strength of the order of 2 Â 107 V=m, assuming a ˚ ; E ¼ V=d).

The maximum current in these cables is slightly above 1000 A, and the estimated normal load is about 30% or 400 A. Depending on the location of the return path, the DC magnetic field will range from a maximum disturbance of the geomagnetic field (with a return through water) to a minimal disturbance (with a return through a second cable as close as possible to the feed cable). 2, immediately above the cables (2 m), practically the same value as that obtained for a single wire. 2. Since the cables are shielded, no electric field will be generated outside the cable.

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