"From the inception of the wireless system I saw that this new art of applied electricity would be of greater benefit to the human race than any other scientific discovery, for it virtually eliminates distance.  The majority of the ills from which humanity suffers are due to the immense extent of the terrestrial globe and the inability of individuals and nations to come into close contact. . . ." edit


Work edit

WP:WikiProject Energy
WT:WikiProject Energy

WP:WikiProject_Physics
WT:WikiProject_Physics

WP:WikiProject_Electrical_engineering
WT:WikiProject_Electrical_engineering

Microphonic contact edit



Heterodyning edit

A signal processing technique developed by inventor-engineers Reginald Fessenden and Nikola Tesla between 1892 and 1901 that creates a new output frequency by combining or mixing two other input frequencies. . . . Cite error: The <ref> tag has too many names (see the help page).[1][2][3]

  1. ^ Christopher E. Cooper (January 2001). Physics. Fitzroy Dearborn Publishers. pp. 25–. ISBN 978-1-57958-358-3. Retrieved July 27, 2013.
  2. ^ United States Bureau of Naval Personnel (1973). Basic Electronics. USA: Courier Dover. p. 338. ISBN 0-486-21076-6.
  3. ^ Graf, Rudolf F. (1999). Modern dictionary of electronics, 7th Ed. USA: Newnes. p. 344. ISBN 0-7506-9866-7.


Beat receiver/receptor edit

 
Machines of this character have been in use since 1892.


Wireless power transfer edit

Magneto-inductive coupling or inductive coupling, Magneto-inductive phenomena edit

Resonant inductive coupling edit

Electro-inductive coupling or Capacitive coupling, Electro-inductive phenomena edit

Capacitive coupling (electro-inductive coupling), is the conjugate equivalent of inductive coupling (magneto-inductive coupling). 

Resonant capacitive coupling edit


Electrical Conduction edit

Atmospheric plasma channel coupling edit

Earth transmission line coupling edit

EXCITATION AND USE OF GUIDED SURFACE WAVE MODES ON LOSSY MEDIA



Jagadish Chandra Bose's experiments edit



Mahlon Loomis' experiments edit



Nikola Tesla's experiments edit

https://en.wikipedia.org/w/index.php?title=Wireless_power_transfer&oldid=746613847#Tesla

https://en.wikipedia.org/w/index.php?title=Wireless_power_transfer&oldid=744688956#Tesla.27s_experiments

https://en.wikipedia.org/w/index.php?title=Wireless_power_transfer&oldid=744636501#Nikola_Tesla.27s_experiments

https://en.wikipedia.org/w/index.php?title=Wireless_power_transfer&oldid=742685327#Nikola_Tesla.27s_experiments

https://en.wikipedia.org/w/index.php?title=Wireless_power_transfer&oldid=735272016#Tesla.27s_experiments



The Leyh-Kenan Demonstrations edit



Corum & Corum, et al. edit

. . .



Near-field and non-radiative technologies edit



Nikola Tesla's experiments supplemental edit

Two widely different experiments edit

The Experiment presented as evidence. edit

The true C/S magnifier specifications. edit



Tesla wireless system feasibility edit



Earth electrical resonance and Stationary terrestrial waves edit



Articles edit

Wireless energy transmission
Wireless power transfer
Wireless power
Wireless power
Wireless power
Wireless power


Wardenclyffe Tower


Tesla coil


Magnifying transmitter
Merge article into World Wireless system or Wardenclyffe tower?


Terrestrial stationary waves
Terrestrial stationary waves

Tesla Experimental Station


Tesla Science Center at Wardenclyffe


Beat receptor
Heterodyne


Annex


World Wireless system or Tesla wireless system
World Wireless

Revision as of 22:10, 21 November 2014
[1], [2], [3], [4]



Prodigal Genius: The Life of Nikola Tesla edit




Lightning in His Hand : The Life Story of Nikola Tesla edit




Longitudinal electromagnetic wave edit

 
The E-field of a Zenneck surface wave at an air-silver interface.
 
Plane pressure pulse wave




Surface Impedance Boundary Condition (SIBC) edit

Surface Impedance Boundary Conditions (SIBC) allow efficient modeling of conductors with a sufficiently strong skin effect. The direct modeling of such conductors with an appropriate MMP expansions for the field inside the conductor and with usual boundary conditions on the surface of the conductor is possible, but numerically very inefficient. First of all, the wavelength inside a good conductor is short and the field varies rapidly. Therefore, a high matching point density on the boundary and a large number of multipole expansions in the close vicinity of the boundary are required for accurately modeling the field. Note that the field outside the conductor can vary much less rapidly. Therefore, fewer matching points and a simpler MMP expansions are required for the exterior field. The distance between matching points can even be much greater than the wavelength inside the conductor. [1]



Leontovich boundary condition edit

The classical electrodynamics Leontovich boundary condition relates the tangential components of the electric Et and magnetic Ht fields on the surface of well-conducting bodies. [Landau and Lifshits, 1982.], [M. A. Leontovich, On the approximate boundary conditions for the electromagnetic field on the surface of well conducting bodies. Moscow: Academy of Sciences of USSR, 1948.]



Trichel pulse edit




Dogma of the Circle edit

"The postulate of ancient science on the perfection of circular motion which set abstractions on the facts of astronomical observations and for a long time determined not only the nature of the first theories of celestial mechanics, but also the approach to the mathematical description of physical phenomena by means of exponentials."[1]

The Greek philosopher Plato is credited with the introduction of the dogma of the circle.  It was expressed by Claudius Ptolemy as follows:  "We believe that the object which the astronomer must strive to achieve is this: to demonstrate that all the phenomena in the sky are produced by uniform and circular motions."



Kenneth Alva Norton edit

A United States War Department engineer. a former Federal Communications Commission engineer . . . Winner of The Franklin Institute Ballantine Award in 1954 for contributions in the field of radio propagation. The Norton ground wave is named after this individual.

Norton published a set of flat earth radio propagation curves in 1936.[1] The final Norton curves give normalized ground wave field strength vs. distance for various conductivities, fixed permittivity (εr = 15), and a selection of frequencies. Norton’s plots for 540-1640 kHz, ultimately ended up as the 20 famous charts in the FCC Rules and Regulations.[2]

1. K. A. Norton, “The Propagation of Radio Waves over the Surface of the Earth and in the Upper Atmosphere – Part I,” Proceedings of the IRE, 24, 1936, pp. 1367-1387.
2. FCC Rules and Regulations, Volume III, Part 73, US Government Printing Office, March 1980. See §73.184, Graphs 1-19A, “Ground Wave Field Intensity vs. Distance” and Graph 20, “Relative Field Intensity F(p)/p vs. Numerical Distance p”.
3. K. A. Norton, “The Propagation of Radio Waves over the Surface of the Earth and in the Upper Atmosphere: Part II,” Proceedings of the IRE, 25, 1937, pp. 1203-1236. [See: Corrections,” by R. J. King, Radio Science, 4, No. 3, March 1969, p. 267.]
4. Kenneth A. Norton. Transmission Loss in Radio Propagation. We will be concerned primarily with the transmission loss encountered in the propagation of ...



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