Color's Kapanadze forum, FE builds circuits and comments

[Jeg]

Hi color
Thanks for answering. It is not that nobody is experimenting. It is just difficult to understand/interpret things that you are not used of. I'll watch again your images. This vacuum idea is really very cool!!! 

[color]

Kapanadze, Akula, Ruslan의 발전기가 사용하는 접지 에너지를 Zenneck Surface wave가 아니라고 하는 이유는 세 가지다.

①
첫 번째는,
Zenneck wave는 용어의 통일이다.
용어의 통일은 특허와 관계있다.
특허는 곧 돈이다.
https://translate.google.com/translate?hl=ko&sl=en&tl=ko&u=https%3A%2F%2Fpatents.justia.com%2Finventor%2Fjames-f-corum&anno=2
2019년 1월경에 대부분 특허됐다.
그래서 Zenneck wave 용어를 주장하는 자들은 돈에 따라간다.

그러나 예전에 비슷한 실험들이 있었다.

대표적인 것이 Norton Surface Wave이다.

②
두 번째는,
까빠나제 발전기가 사용하는 접지 에너지는 전하의 불균형과 균형에 의해서만 에너지가 이동한다.
이것은 표면파가 아니라 양전하의 움직임이다.
도약으로 해석해도 무방하다.
기존에 사용하는 용어가 있다.
단지 특허와 관계된 용어로 통일하려는 움직임일 뿐이다.

③
그리고 마지막 세 번째 이유는,
Kapanadze, Akula, Ruslan의 발전기는 접지를 이용하지만 요크 변압기 공진이 에너지를 생산하는 주력이다.
특수한 기술을 접목해서 접지를 사용하지 않고도 자유 발전기가 작동한다.

2~3km 상공에서도 작동한다는 뜻이다.
이것은 Zenneck Surface wave나 Norton Surface Wave와 절대 무관하다.

이것은 비밀이라 코멘트하지 않겠다.

그리고 나의 언어가 영어로 정확하게 표현되지 않았다.


There are three reasons why Kapanadze, Akula, and Ruslan's generators are not using Zenneck surface waves as ground energy.

①
at first,
The Zenneck wave is the unification of terms.
The unification of terms is related to patents.
Patents are money soon.
https://translate.google.com/translate?hl=en&sl=en&tl=en&u=https%3A%2F%2Fpatents.justia.com%2Finventor%2Fjames-f-corum&anno=2
Most were patented in January 2019.
So those who claim Zenneck wave terms go with money.

But there were similar experiments in the past.

A typical example is Norton Surface Wave.

②
second is,
The ground energy used by the generator is transferred only by the imbalance and balance of charge.
This is not the surface wave but the movement of positive charge.
It can be interpreted as a leap.
There are existing terms.
It is merely a move to unify in terms related to patents.

③
And the last third,
The generator of Kapanadze, Akula and Ruslan uses ground but the resonance of the yoke transformer is the main force that produces energy.
The free generator works without any grounding by combining special technology.
 
It means that it works even in the sky over 2 ~ 3km.
This is absolutely irrelevant to the Zenneck Surface wave or Norton Surface Wave.
 
This is a secret and I will not comment.

And my language was not correctly represented in English.

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마찬가지로.. 용어 통일... surface wave, Zenneck wave, plasmons .....

표면 모드에 대해서 생각을 한번 해 보겠습니다.

좀더 구체적으로는 우리가 관심이 있는 표면 플라즈몬 폴라리톤 모드의 물리적 정의와 loss 문제에 대해서 생각해 보겠습니다.

간단하게

lossless dielectric
--------------------------
lossy metal

과 같은 구조에서 경계면에 존재하는 표면모드를
Maxwell 방정식으로 부터 구할 때의 물리적인 조건, 즉
'Maxwell 방정식에서 표면모드 해를 얻기 위해 사용되는
표면모드의 물리적 조건으로 부터 구체화된 수학적 조건'
을 말로 풀어보면

" 표면을 중심으로 전자장의 phase-velocity가 모두 바깥을
향하는 모드"

입니다. 이러한 조건으로 해를 얻고 나면 필연적으로 따라오는
물리적 성질이 경계를 중심으로 아래 위로 전자장의 세기가
exponential 하게 감소하는 성질입니다. 

보통 표면모드를 말할 때 표면을 중심으로 빛의 세기가 양방향으로
지수적으로 감소하여 표면에 bound 되어 있다고 말을 하고 이러한
상태에서는 metal에 의한 Ohmic loss만이 모드 dissipation의
원인이라고 말하는 경우가 많습니다. 왜냐하면 이 경우는 Kretschmann structure에서 보이는 것과 같은 phase-matching에 의한 높은 인덱스
를 갖는 외부로의 광파 커플링은 없기 때문입니다.

하지만, metal은 loss 를 가지고 있고 dielectric/metal 경계에 평행한
방향을 x방향, 수직한 방향을 z 방향이라고 하면

표면모드의 x 방향 wavevector component Kx는 복소수가 됩니다.
lossless dielectric material에서 kz=((2*pi/lambda)^2-Kx)^0.5로
마찬가지로 복소수가 됩니다.

Kz 방향이 복소수라는 것은 lossless dielectric medium에서 z 방향으로의 전자장 변화가 단순한 exponential 감소가 아닌 위상도 변하는, 즉
z 방향으로의 Poynting vector를 계산했을때 0이 아닌 그런한 변화를
한다는 것을 의미합니다.

즉 표면파라고 해도 금속미디엄이 loss를 갖고 있기 때문에 lossless한
dielectric medium으로도 반드시 일정한 정도의 radiation loss가 발생합니다. 간단한 계산을 통해 ohmic loss와 radiation loss의 값을 정확히 구해 볼 수 있습니다.
즉 표면 모드라는 말이 반드시 표면에 평행한 방향으로만 에너지를 전달
하는 모드가 아니라는 것을 알 수 있습니다.

이러한 뜻에서 표면 모드를 표면을 따라 에너지가 전달되는 파가 아닌

" 표면을 중심으로 전자장의 phase-velocity가 모두 바깥을
향하는 모드"

로 이야기하는 것은 어떨까 하는 생각을 해봅니다.




>Polariton in Wikipedia
>Plasmon in Wikipedia
>Zenneck (surface) wave in Wikipedia
>
>이런 것들에 대해서도 팀 구성원 사이에
>
>명확한 이해, 통일된 개념, 정확한 단어 사용이 특허나 돈이다.


Similarly ... term unification ... surface wave, Zenneck wave, plasmons .....

Let's think about surface mode.

More specifically, let us consider the physical definition and loss problem of the surface plasmon polariton mode that we are interested in.

Simply

lossless dielectric
--------------------------
lossy metal

The surface mode at the interface is
The physical conditions for obtaining from the Maxwell equation, namely
'Used to obtain the surface mode solution in the Maxwell equation
Mathematical conditions specified from the physical conditions of the surface mode '
In words

"The phase-velocity of the electromagnetic field around the surface is all outside
Mode "

is. If you get harm in these conditions, you will inevitably come
The physical property is the center of the boundary.
It is an exponentially decreasing property.

In normal surface mode, the intensity of the light around the surface is bi-directional
It is exponentially decreasing to say that it is bound to the surface.
In case of Ohmic loss due to metal,
Often it is said to be the cause. This is because the high index by phase-matching as shown in the Kretschmann structure
Because there is no external wave coupling.

However, metal has loss and is parallel to the dielectric / metal boundary
If the direction is x direction and the vertical direction is z direction

The x-direction wavevector component Kx of surface mode is complex.
In a lossless dielectric material, kz = ((2 * pi / lambda) ^ 2-Kx) ^ 0.5
It is also a complex number.

The complex number in the Kz direction is the fact that the electromagnetic field change from the lossless dielectric medium to the z direction changes not only in exponential reduction but also in phase
When we calculate the poynting vector in the z direction, we make such a non-zero change
It means that.

In other words, even if surface waves are metal,
Even with a dielectric medium, there is always a certain amount of radiation loss. It is possible to obtain the exact values ​​of ohmic loss and radiation loss by simple calculation.
In other words, the term surface mode only transfers energy in a direction parallel to the surface
You can see that this is not the mode you are in.

In this sense the surface mode is not a wave transmitted energy along the surface

"The phase-velocity of the electromagnetic field around the surface is all outside
Mode "

I think about how to talk about it.


> Polariton in Wikipedia
> Plasmon in Wikipedia
> Zenneck (surface) wave in Wikipedia
>
> This is something that also happens between team members
>
> Clear understanding, unified concept, and precise word usage are patents or money.

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Patents by Inventor James F. Corum
https://translate.google.com/translate?hl=ko&sl=en&tl=ko&u=https%3A%2F%2Fpatents.justia.com%2Finventor%2Fjames-f-corum&anno=2


James F. Corum has filed for patents to protect the following inventions. This listing includes patent applications that are pending as well as patents that have already been granted by the United States Patent and Trademark Office (USPTO).

ADAPTATION OF POLYPHASE WAVEGUIDE PROBES
Publication number: 20190058327
Abstract: Disclosed are various embodiments for transmitting energy conveyed in the form of a guided surface-waveguide mode along a lossy conducting medium such as, eg, the surface of a terrestrial medium by exciting a polyphase waveguide probe. A probe control system can be used to adjust the polyphase waveguide probe based at least in part upon characteristics of the lossy conducting medium.
Type: Application
Filed: October 23, 2018
Publication date: February 21, 2019
Inventors: James F. Corum, Kenneth L. Corum
OBJECT IDENTIFICATION SYSTEM AND METHOD
Publication number: 20190050612
Abstract: A method of managing objects in a site (424) includes producing a guided surface wave with a guided surface waveguide probe (P), the guided surface wave having sufficient energy density to power object identification tags (402) in an entirety of the site; receiving reply signals from the object identification tags, each object identification tag associated with an object (404); and identifying geolocation of one or more the objects according to received reply signals from the object identification tags that are associated with the one or more of the objects.
Type: Application
Filed: August 26, 2016
Publication date: February 14, 2019
Inventors: JAMES D. LILLY, KENNETH L. CORUM, JAMES F. CORUM, JOSEPH F. PINZONE
REMOTE SURFACE SENSING USING GUIDED SURFACE WAVE MODES ON LOSSY MEDIA
Publication number: 20190049568
Abstract: Disclosed are various systems and methods for remote surface sensing using guided surface wave modes on lossy media. One system, among others, includes a guided surface waveguide probe configured to launch a guided surface wave along a surface of a lossy conducting medium, and a receiver configured to receive backscatter reflected by a remotely located object illuminated by the guided surface wave. One method, among others, includes launching a guided surface wave along a surface of a lossy conducting medium by exciting a charge terminal of a guided surface waveguide probe, and receiving backscatter reflected by a remotely located object illuminated by the guided surface wave.
Type: Application
Filed: October 8, 2018
Publication date: February 14, 2019
Inventors: James F. Corum, Kenneth L. Corum
Adaptation of energy consumption node for guided surface wave reception
Patent number: 10205326
Abstract: Disclosed, in one example, is an energy consumption node. The node includes a guided surface wave receive structure configured to obtain electrical energy from a guided surface wave traveling along a terrestrial medium. The node also includes a distribution system coupled to the guided surface wave receive structure and configured to distribute the obtained electrical energy to an electrical load coupleable to the distribution system.
Type: Grant
Filed: September 9, 2015
Date of Patent: February 12, 2019
Assignee: CPG Technologies, LLC
Inventors: James F. Corum, Kenneth L. Corum, James D. Lilly
GUIDED SURFACE WAVEGUIDE PROBE STRUCTURES
Publication number: 20190044209
Abstract: Disclosed a guided surface waveguide probe including a charge terminal configured to generate an electromagnetic field and a support apparatus that supports the charge terminal above a lossy conducting medium, wherein the electromagnetic field generated by the charge terminal synthesizes a wave front incident at a complex Brewster angle of incidence (?i,B) of the lossy conducting medium.
Type: Application
Filed: March 9, 2017
Publication date: February 7, 2019
Inventors: James F. Corum, Kenneth L. Corum
MEASURING AND REPORTING POWER RECEIVED FROM GUIDED SURFACE WAVES
Publication number: 20190041438
Abstract: Disclosed are various approaches for measuring and reporting the amount of electrical power consumed by an electrical load attached to a guided surface wave receive structure. A guided surface wave receive structure is configured to obtain electrical energy from a guided surface wave traveling along a terrestrial medium. An electrical load is coupled to the guided surface wave receive structure, the electrical load being experienced as a load at an excitation source coupled to a guided surface waveguide probe generating the guided surface wave. An electric power meter coupled to the electrical load and configured to measure the electrical load.
Type: Application
Filed: October 5, 2018
Publication date: February 7, 2019
Inventors: James F. Corum, Kenneth L. Corum, Joseph F. Pinzone, James D. Lilly, Michael W. Miller, Stephen W. Wilson
Excitation and use of guided surface waves
Patent number: 10193595
Abstract: Disclosed are various embodiments for transmitting and receiving energy conveyed in the form of a guided surface-waveguide mode along the surface of a lossy medium such as, eg, a terrestrial medium excited by a guided surface waveguide probe.
Type: Grant
Filed: June 2, 2015
Date of Patent: January 29, 2019
Assignee: CPG TECHNOLOGIES, LLC
Inventors: James F. Corum, Kenneth L. Corum
Magnetic coils having cores with high magnetic permeability
Patent number: 10193229
Abstract: Aspects of magnetic coils having cores with relatively high magnetic permeability are described. In some embodiments, a system includes a guided surface wave receive structure configured to obtain electrical energy from a guided surface wave traveling across a terrestrial medium. The guided surface wave receive structure includes a magnetic coil and a core disposed in the magnetic coil. The core in some embodiments has a relative magnetic permeability greater than about 10 and less than about 1,000,000. An electrical load is coupled to the guided surface wave receive structure, with the electrical load being experienced as a load at an excitation source coupled to a guided surface waveguide probe generating the guided surface wave.
Type: Grant
Filed: September 10, 2015
Date of Patent: January 29, 2019
Assignee: CPG Technologies, LLC
Inventors: James F. Corum, Kenneth L. Corum, James D. Lilly
Guided surface wave transmission of multiple frequencies in a lossy media
Patent number: 10193353
Abstract: Disclosed are various embodiments for transmitting energy at multiple frequencies via a guided surface wave along the surface of a lossy medium such as, eg, a terrestrial medium by exciting a guided surface waveguide probe.
Type: Grant
Filed: December 28, 2017
Date of Patent: January 29, 2019
Assignee: CPG TECHNOLOGIES, LLC
Inventors: James F. Corum, Kenneth L. Corum, James D. Lilly, Basil F. Pinzone, Jr., Joseph F. Pinzone
HYBRID PHASED ARRAY TRANSMISSION
Publication number: 20190027841
Abstract: Disclosed are various embodiments of an electromagnetic hybrid phased array system. One such embodiment includes a guided surface waveguide probe, and a contrawound toroidal helix antenna collocated with the guided surface waveguide probe in which the contrawound toroidal helix comprises ring elements spaced from each other and wrapped around the guided surface waveguide probe. The system further includes a signal source applied to at least the guided surface waveguide probe, such that the guided surface waveguide probe and the contrawound toroidal helix contribute individual vertical electric fields to form a radiation pattern based on the phase and amplitude characteristics of the individual vertical electric fields.
Type: Application
Filed: September 10, 2018
Publication date: January 24, 2019
Inventors: James F. Corum, Kenneth L. Corum, Basil F. Pinzone, JR.
GEOLOCATION USING GUIDED SURFACE WAVES
Publication number: 20190025060
Abstract: Disclosed are various approaches for determining positions of a navigation unit and correcting for errors. The navigation unit can receive a guided surface wave using a guided surface wave receive structure. The navigation unit can then determine a potential location of the guided surface wave receive structure. Finally, the navigation unit can determine an accuracy of the potential location based at least in part on a secondary data source.
Type: Application
Filed: September 25, 2018
Publication date: January 24, 2019
Inventors: James F. Corum, Kenneth L. Corum, James D. Lilly
LONG DISTANCE TRANSMISSION OF OFFSHORE POWER
Publication number: 20190020223
Abstract: Disclosed are systems and methods for long distance transmission of offshore generated power. A turbine is located offshore. The turbine can be mechanically coupled to a generator. A guided surface waveguide probe is electrically coupled to the generator and configured to launch a guided surface wave on a terrestrial medium.
Type: Application
Filed: September 11, 2018
Publication date: January 17, 2019
Inventors: James F. Corum, Kenneth L. Corum, John Robert Ashcroft, Stephen W. Wilson, Michael W. Miller
DETERRING THEFT IN WIRELESS POWER SYSTEMS
Publication number: 20190013697
Abstract: Various embodiments for deterring theft in wireless power systems are disclosed. In one embodiment, an electrical device, comprise a guided surface wave receive structure configured to obtain electrical energy from a guided surface wave traveling along a terrestrial medium, and an electrical load coupled to the guided surface wave receive structure, the electrical load being experienced as a load at an excitation source coupled to a guided surface waveguide probe generating the guided surface wave. Processing circuitry of the electrical device may be configured to monitor the electrical load to determine whether a power consumption of the electrical load has exceeded a predefined amount of permitted power consumption and disable the wireless power receiver or the electrical load coupled to the wireless power receive structure in response to the electrical load exceeding the predefined amount of permitted power consumption.
Type: Application
Filed: August 27, 2018
Publication date: January 10, 2019
Inventors: James F. Corum, Kenneth L. Corum, James D. Lilly, Basil F. Pinzone, JR.
Geolocation using guided surface waves
Patent number: 10175048
Abstract: Disclosed are various approaches for determining positions of a navigation unit and correcting for errors. The navigation unit can receive a guided surface wave using a guided surface wave receive structure. The navigation unit can then determine a potential location of the guided surface wave receive structure. Finally, the navigation unit can determine an accuracy of the potential location based at least in part on a secondary data source.
Type: Grant
Filed: August 17, 2016
Date of Patent: January 8, 2019
Assignee: CPG Technologies, LLC
Inventors: James F. Corum, Kenneth L. Corum, James D. Lilly
Simultaneous multifrequency receive circuits
Patent number: 10177571
Abstract: Disclosed are various receive circuits by which to receive a plurality of guided surface waves transmitted by a plurality of guided surface waveguide probes over a surface of a terrestrial medium according to various embodiments.
Type: Grant
Filed: December 19, 2017
Date of Patent: January 8, 2019
Assignee: CPG TECHNOLOGIES, LLC
Inventors: James F. Corum, Kenneth L. Corum, Joseph F. Pinzone, James D. Lilly
Subsurface sensing using guided surface wave modes on lossy media
Patent number: 10175203
Abstract: Disclosed are various systems and methods for remote surface sensing using guided surface wave modes on lossy media. One system, among others, comprises a guided surface waveguide probe configured to launch a guided surface wave along a surface of a lossy conducting medium, and a receiver configured to receive backscatter reflected by a remotely located subsurface object illuminated by the guided surface wave. One method, among others, includes launching a guided surface wave along a surface of a lossy conducting medium by exciting a charge terminal of a guided surface waveguide probe, and receiving backscatter reflected by a remotely located subsurface object illuminated by the guided surface wave.
Type: Grant
Filed: September 9, 2015
Date of Patent: January 8, 2019
Assignee: CPG TECHNOLOGIES, LLC
Inventors: James F. Corum, Kenneth L. Corum
SIMULTANEOUS TRANSMISSION AND RECEPTION OF GUIDED SURFACE WAVES
Publication number: 20190006854
Abstract: Disclosed are various embodiments of a guided surface wave transmitter/receiver configured to transmit a guided surface wave at a first frequency and to receive guided surface waves at a second frequency, concurrently with the transmission of guided surface waves at the first frequency. The various embodiments can be configured to retransmit received power and applied the received power to an electrical load. The various embodiments of the guided surface wave transmitter/receiver also can be configured as an amplitude modulation (AM) repeater.
Type: Application
Filed: September 7, 2018
Publication date: January 3, 2019
Inventors: James F. Corum, Kenneth L. Corum, James D. Lilly, Basil F. Pinzone, JR., Joseph F. Pinzone
GUIDED-SURFACE WAVEGUIDE PROBES
Publication number: 20180366805
Abstract: Disclosed is a guided surface waveguide probe including a charge terminal configured to generate an electromagnetic field and a support apparatus that supports the charge terminal above a lossy conducting medium, wherein the electromagnetic field generated by the charge terminal synthesizes a wave front incident at a complex Brewster angle of incidence (?i,B) of the lossy conducting medium.
Type: Application
Filed: August 24, 2018
Publication date: December 20, 2018
Inventors: James F. Corum, Kenneth L. Corum, Basil F. Pinzone, JR., Joseph F. Pinzone, Paul Kendall Carlton, JR.
SITE SPECIFICATION FOR DIRECTIONAL GUIDED SURFACE WAVE TRANSMISSION IN A LOSSY MEDIA
Publication number: 20180366808
Abstract: Various examples are provided for site specification for directional guided surface wave transmission in a lossy media. In one example, a probe site includes a propagation interface including first and second regions comprising different lossy conducting mediums. A guided surface waveguide probe positioned adjacent to the first and second regions can generate at least one electric field to launch a guided surface wave along the propagation interface in a radial direction defined by the first region and restricted by the second region. The propagation interface can also include additional regions comprising the same or different lossy conducting mediums. One or more of the regions can be prepared regions. In some cases, the regions can correspond to a terrestrial medium (eg, a shoreline) and water (eg, seawater along the shoreline).
Type: Application
Filed: March 9, 2017
Publication date: December 20, 2018
Inventors: James F. CORUM, Kenneth L. CORUM, John E. ROSS, III
MODULATED GUIDED SURFACE WAVES
Publication number: 20180366804
Abstract: Disclosed are various systems and methods directed to the launching of a Zenneck surface wave embodying a modulated signal using a guided surface waveguide probe. A modulated signal is generated and coupled to a guided surface waveguide probe. A resulting Zenneck surface wave is launched that decays exponentially as a function of distance.
Type: Application
Filed: August 8, 2018
Publication date: December 20, 2018
Inventors: James F. Corum, Kenneth L. Corum

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REDISCOVERING THE ZENNECK SURFACE WAVE
https://papago.naver.net/website?source=en&target=ko&url=http://www.tfcbooks.com/articles/tws4.htm

In 1916 while speaking of his system for global transmission, Tesla cited the analysis of mathematician Arnold N. Sommerfeld as verification of his explanations of observed radio phenomena.  Tesla was referring to his wireless system in which, he claimed, 90% to 95% of the electrical energy was manifested at the transmitters output as "current waves" with the remainder existing as dissipating electromagnetic radiation (see Antenna Theory).  In 1909 another investigator by the name of Johann Zenneck, while working to explain Marconi's trans-oceanic results, showed that a unique type of surface wave could travel along the interface between the ground and the air.  In the words of James Corum,

"The distinguishing feature of the Zenneck wave was that the propagating energy didn't spread like radiation, but was concentrated near the guiding surface.  Sommerfeld had shown that an electromagnetic wave could be guided along a wire of finite conductivity, and Zenneck conceived that the earth's surface would perform in a manner similar to a single conducting wire." [see "Operating Principles of the Wardenclyffe Apparatus"]

In commenting on Sommerfeld's analysis of the surface wave, James R. Wait states that "The field amplitude varies inversely as the square root of the horizontal distance from the source. . . ."  It's interesting to note that Sommerfeld made a point of distinguishing between the "electrodynamic" surface wave and its Hertzian counterpart the space wave, believing that both components could be present in varying proportion in the wave complex.  It was Tesla's assertion that the exact composition of the emissions was dependent upon the design of the transmitter launching structure.

Geometry for Zenneck wave propagation.