On behalf of all other Renewable Energy forum members:
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Your analogy of harnessing the air turbulence of a passing vehicle without affecting the vehicle does have a parallel in Leedskalnin's PMH but you may want to note this relationship between a conductor and its field:
Meissner Effect (of Superconductivity) - Wikipedia
When a superconductor is placed in a weak external magnetic field H, and cooled below its transition temperature, the magnetic field is ejected. The Meissner effect does not cause the field to be completely ejected but instead the field penetrates the superconductor but only to a very small distance, characterized by a parameter λ, called the London penetration depth, decaying exponentially to zero within the bulk of the material. The Meissner effect is a defining characteristic of superconductivity. For most superconductors, the London penetration depth is on the order of 100 nm.
The Meissner effect is sometimes confused with the kind of diamagnetism one would expect in a perfect electrical conductor: according to Lenz's law, when a changing magnetic field is applied to a conductor, it will induce an electric current in the conductor that creates an opposing magnetic field. In a perfect conductor, an arbitrarily large current can be induced, and the resulting magnetic field exactly cancels the applied field.
Rest assured, threads don't die. Scroll down and rate or subscribe to this thread if you wish. Quite often related discussions exist on other threads so you may want to search for a particular member's postings. Be aware that thread titles are often vague and don't always reflect how a discussion may evolve. For these reasons I'd suggest advanced searching for a string and/or multiple terms using inurl:http://www.energeticforum.com/renewable-energy/
----------------------------------------------
Your analogy of harnessing the air turbulence of a passing vehicle without affecting the vehicle does have a parallel in Leedskalnin's PMH but you may want to note this relationship between a conductor and its field:
Meissner Effect (of Superconductivity) - Wikipedia
When a superconductor is placed in a weak external magnetic field H, and cooled below its transition temperature, the magnetic field is ejected. The Meissner effect does not cause the field to be completely ejected but instead the field penetrates the superconductor but only to a very small distance, characterized by a parameter λ, called the London penetration depth, decaying exponentially to zero within the bulk of the material. The Meissner effect is a defining characteristic of superconductivity. For most superconductors, the London penetration depth is on the order of 100 nm.
The Meissner effect is sometimes confused with the kind of diamagnetism one would expect in a perfect electrical conductor: according to Lenz's law, when a changing magnetic field is applied to a conductor, it will induce an electric current in the conductor that creates an opposing magnetic field. In a perfect conductor, an arbitrarily large current can be induced, and the resulting magnetic field exactly cancels the applied field.

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