Bioeffects and Therapeutic Applications of Electromagnetic - download pdf or read online

By Riadh Habash

ISBN-10: 1420062840

ISBN-13: 9781420062847

From cellphones to treating melanoma, EM power performs a component in lots of of the recommendations that we take with no consideration daily. A simple strength of nature, like nuclear strength or gravity, this power might be harnessed and used, yet nonetheless holds the aptitude to be destructive. The query is still, how secure are EM items? Bioeffects and healing purposes of Electromagnetic strength presents a assessment of state of the art study in EM healthiness results and EM remedy besides rising parts of bioengineering and biomedical engineering.

The e-book helps you to

·         comprehend the mandatory EM idea within the context of its interplay with the human physique

·         evaluation state of the art study on EM wellbeing and fitness results and EM treatment

·         discover innovations constructed to make sure sufficient EM and thermal dosimetry required for healthiness results and thermal remedy

·         develop your knowing of the quickly rising parts of bioengineering and biomedical engineering

Taking a transdisciplinary technique drawn from a number of highbrow streams that come with physics, epidemiology, medication, setting, hazard evaluate, and numerous disciplines of engineering, this booklet ventures into the conflicting stories to entry study on bioeffects and healing functions of EM power. it's the merely source at the moment to be had that covers bioeffects and chance overview of either super low frequency (ELF) fields and radiofrequency radiation (RFR) besides the hot advancements in thermal remedy and imaging ideas.

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Extra info for Bioeffects and Therapeutic Applications of Electromagnetic Energy

Example text

Low-energy photons (such as radiofrequency radiation or RFR) behave more like waves, while higher-energy photons (such as x-rays) behave more like particles. In the near-field region (distance less than one wavelength from the source), magnetic fields are decoupled. When a transmission line is energized without a load, it creates an E field and when the current flows, an H field comes into existence. At the far-field region (distance greater than one wavelength from the source), primarily at high frequencies, both E and H are related with the assumption that the characteristic impedance of the plane wave is 377 Ω.

6. A magnetic field with magnetic flux density B is normal to the plane of the loop. If the direction of B is upward and decreasing in value, a current I will be generated in the upward direction. If B is directed upward but its value is increasing in magnitude, the direction of the current will be opposite. 6a. 6b. Therefore, the induced current in the loop is always in such a direction as to produce flux opposing the change in B. This phenomenon is called Lenz’s law. 6 Induced currents due to magnetic flux density B.

As the energy required for ionization by breaking a chemical bond is typically 1 eV, it is clear that low-frequency fields do not cause ionization. Ionizing and nonionizing radiation are separated on the EM spectrum. The division between them is generally accepted to be at wavelengths around 1 nm in the far-UV region. Above that frequency is ionizing radiation, which contains enough energy to physically alter the atoms it strikes and change them into charged particles called ions. Below visible light is the nonionizing radiation.

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Bioeffects and Therapeutic Applications of Electromagnetic Energy by Riadh Habash

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