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Delta-T Antenna (T.E.C.)
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<blockquote data-quote="Sonix" data-source="post: 186501" data-attributes="member: 10954"><p>Apparently I wasn't the first person to think about the circumference orbit speed of a rotating electromagnetic field... <img src="data:image/gif;base64,R0lGODlhAQABAIAAAAAAAP///yH5BAEAAAAALAAAAAABAAEAAAIBRAA7" class="smilie smilie--sprite smilie--sprite38" alt=":)" title="Smile :)" loading="lazy" data-shortname=":)" /></p><p>Found this in Robert <a href="http://pcbs13.informatik.uni-stuttgart.de/~lagally/fun/ag_bibl.htm" target="_blank">Stirniman's Antigravity Bibliography,</a> both excerpts attributed to "Robert Shannon":</p><p></p><p>"Several key pharases keep popping up regarding rotating fields, powerful </p><p>magnetic pulsed fields, and 90 degree cross-field phase shifts. </p><p>For example, Preston Nicholes describes a device known as a Delta T </p><p>antenna in the Montauk series of books. The Delta T antenna is described </p><p>as a pyramidal structure, but lets just take two square loops, placed at </p><p>90 degrees to each other, and feed these two loops with an RF signal, </p><p>also with a 90 degree phase shift, we will produce a rotating magnetic </p><p>field within the loops (these loops share a common center point, and </p><p>each loop is in a plane 90 degrees from the other)</p><p>The speed of rotation of this magnetic field is a direct function of the </p><p>frequancy of the applied RF signal. At the center of the antenna, the </p><p>rotational velocity is zero, but as you move out from the center, and </p><p>rotational velocity increases. At some distance from center would reach </p><p>the speed of light, dependant of the frequancy used... </p><p>What effect would there be at the boundry where the rotational velocity </p><p>reached, and then exceeded the speed of light. How could the magnetic </p><p>field even propogate to the center of the antenna structure if it would </p><p>have to move faster than light to reach that space? If hemholtz coils </p><p>were used instead of loops, the magnetic field strength would be uniform </p><p>inside the structure, how could the field strenght be uniform if there is </p><p>not sufficient time for the field to propogate through the space inside </p><p>the structure itself?..."</p><p></p><p></p><p></p><p>"How fast do you want it rotated? It's fairly simple to construct a system </p><p>to produce rotating EM waves at whatever rotational velocity you wish by </p><p>feeding a pair of broadside dipole arrays with quatrature phased waves.</p><p>It is quite simple to construct a system that would have a rotational </p><p>velocity of C within the uniform field area. It might also be fairly easy </p><p>to do this with a Hemholtz coil arangement as well, but the broadside array </p><p>will be much easier to do at easily engineerable frequencies.</p><p>Some really interesting paradoxes come about when the rotational frequency </p><p>is high enough so that the rotational velocity exceeds C within the uniform </p><p>field area of the arrays or within the hemholtz coils.</p><p>-- Robert Shannon"</p></blockquote><p></p>
[QUOTE="Sonix, post: 186501, member: 10954"] Apparently I wasn't the first person to think about the circumference orbit speed of a rotating electromagnetic field... :) Found this in Robert [URL='http://pcbs13.informatik.uni-stuttgart.de/~lagally/fun/ag_bibl.htm']Stirniman's Antigravity Bibliography,[/URL] both excerpts attributed to "Robert Shannon": "Several key pharases keep popping up regarding rotating fields, powerful magnetic pulsed fields, and 90 degree cross-field phase shifts. For example, Preston Nicholes describes a device known as a Delta T antenna in the Montauk series of books. The Delta T antenna is described as a pyramidal structure, but lets just take two square loops, placed at 90 degrees to each other, and feed these two loops with an RF signal, also with a 90 degree phase shift, we will produce a rotating magnetic field within the loops (these loops share a common center point, and each loop is in a plane 90 degrees from the other) The speed of rotation of this magnetic field is a direct function of the frequancy of the applied RF signal. At the center of the antenna, the rotational velocity is zero, but as you move out from the center, and rotational velocity increases. At some distance from center would reach the speed of light, dependant of the frequancy used... What effect would there be at the boundry where the rotational velocity reached, and then exceeded the speed of light. How could the magnetic field even propogate to the center of the antenna structure if it would have to move faster than light to reach that space? If hemholtz coils were used instead of loops, the magnetic field strength would be uniform inside the structure, how could the field strenght be uniform if there is not sufficient time for the field to propogate through the space inside the structure itself?..." "How fast do you want it rotated? It's fairly simple to construct a system to produce rotating EM waves at whatever rotational velocity you wish by feeding a pair of broadside dipole arrays with quatrature phased waves. It is quite simple to construct a system that would have a rotational velocity of C within the uniform field area. It might also be fairly easy to do this with a Hemholtz coil arangement as well, but the broadside array will be much easier to do at easily engineerable frequencies. Some really interesting paradoxes come about when the rotational frequency is high enough so that the rotational velocity exceeds C within the uniform field area of the arrays or within the hemholtz coils. -- Robert Shannon" [/QUOTE]
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