\documentclass[11pt,twoside]{article}\makeatletter

\IfFileExists{xcolor.sty}%
  {\RequirePackage{xcolor}}%
  {\RequirePackage{color}}
\usepackage{colortbl}
\usepackage{wrapfig}
\usepackage{ifxetex}
\ifxetex
  \usepackage{fontspec}
  \usepackage{xunicode}
  \catcode`⃥=\active \def⃥{\textbackslash}
  \catcode`❴=\active \def❴{\{}
  \catcode`❵=\active \def❵{\}}
  \def\textJapanese{\fontspec{Noto Sans CJK JP}}
  \def\textChinese{\fontspec{Noto Sans CJK SC}}
  \def\textKorean{\fontspec{Noto Sans CJK KR}}
  \setmonofont{DejaVu Sans Mono}
  
\else
  \IfFileExists{utf8x.def}%
   {\usepackage[utf8x]{inputenc}
      \PrerenderUnicode{–}
    }%
   {\usepackage[utf8]{inputenc}}
  \usepackage[english]{babel}
  \usepackage[T1]{fontenc}
  \usepackage{float}
  \usepackage[]{ucs}
  \uc@dclc{8421}{default}{\textbackslash }
  \uc@dclc{10100}{default}{\{}
  \uc@dclc{10101}{default}{\}}
  \uc@dclc{8491}{default}{\AA{}}
  \uc@dclc{8239}{default}{\,}
  \uc@dclc{20154}{default}{ }
  \uc@dclc{10148}{default}{>}
  \def\textschwa{\rotatebox{-90}{e}}
  \def\textJapanese{}
  \def\textChinese{}
  \IfFileExists{tipa.sty}{\usepackage{tipa}}{}
\fi
\def\exampleFont{\ttfamily\small}
\DeclareTextSymbol{\textpi}{OML}{25}
\usepackage{relsize}
\RequirePackage{array}
\def\@testpach{\@chclass
 \ifnum \@lastchclass=6 \@ne \@chnum \@ne \else
  \ifnum \@lastchclass=7 5 \else
   \ifnum \@lastchclass=8 \tw@ \else
    \ifnum \@lastchclass=9 \thr@@
   \else \z@
   \ifnum \@lastchclass = 10 \else
   \edef\@nextchar{\expandafter\string\@nextchar}%
   \@chnum
   \if \@nextchar c\z@ \else
    \if \@nextchar l\@ne \else
     \if \@nextchar r\tw@ \else
   \z@ \@chclass
   \if\@nextchar |\@ne \else
    \if \@nextchar !6 \else
     \if \@nextchar @7 \else
      \if \@nextchar (8 \else
       \if \@nextchar )9 \else
  10
  \@chnum
  \if \@nextchar m\thr@@\else
   \if \@nextchar p4 \else
    \if \@nextchar b5 \else
   \z@ \@chclass \z@ \@preamerr \z@ \fi \fi \fi \fi
   \fi \fi  \fi  \fi  \fi  \fi  \fi \fi \fi \fi \fi \fi}
\gdef\arraybackslash{\let\\=\@arraycr}
\def\@textsubscript#1{{\m@th\ensuremath{_{\mbox{\fontsize\sf@size\z@#1}}}}}
\def\Panel#1#2#3#4{\multicolumn{#3}{){\columncolor{#2}}#4}{#1}}
\def\abbr{}
\def\corr{}
\def\expan{}
\def\gap{}
\def\orig{}
\def\reg{}
\def\ref{}
\def\sic{}
\def\persName{}\def\name{}
\def\placeName{}
\def\orgName{}
\def\textcal#1{{\fontspec{Lucida Calligraphy}#1}}
\def\textgothic#1{{\fontspec{Lucida Blackletter}#1}}
\def\textlarge#1{{\large #1}}
\def\textoverbar#1{\ensuremath{\overline{#1}}}
\def\textquoted#1{‘#1’}
\def\textsmall#1{{\small #1}}
\def\textsubscript#1{\@textsubscript{\selectfont#1}}
\def\textxi{\ensuremath{\xi}}
\def\titlem{\itshape}
\newenvironment{biblfree}{}{\ifvmode\par\fi }
\newenvironment{bibl}{}{}
\newenvironment{byline}{\vskip6pt\itshape\fontsize{16pt}{18pt}\selectfont}{\par }
\newenvironment{citbibl}{}{\ifvmode\par\fi }
\newenvironment{docAuthor}{\ifvmode\vskip4pt\fontsize{16pt}{18pt}\selectfont\fi\itshape}{\ifvmode\par\fi }
\newenvironment{docDate}{}{\ifvmode\par\fi }
\newenvironment{docImprint}{\vskip 6pt}{\ifvmode\par\fi }
\newenvironment{docTitle}{\vskip6pt\bfseries\fontsize{22pt}{25pt}\selectfont}{\par }
\newenvironment{msHead}{\vskip 6pt}{\par}
\newenvironment{msItem}{\vskip 6pt}{\par}
\newenvironment{rubric}{}{}
\newenvironment{titlePart}{}{\par }

\newcolumntype{L}[1]{){\raggedright\arraybackslash}p{#1}}
\newcolumntype{C}[1]{){\centering\arraybackslash}p{#1}}
\newcolumntype{R}[1]{){\raggedleft\arraybackslash}p{#1}}
\newcolumntype{P}[1]{){\arraybackslash}p{#1}}
\newcolumntype{B}[1]{){\arraybackslash}b{#1}}
\newcolumntype{M}[1]{){\arraybackslash}m{#1}}
\definecolor{label}{gray}{0.75}
\def\unusedattribute#1{\sout{\textcolor{label}{#1}}}
\DeclareRobustCommand*{\xref}{\hyper@normalise\xref@}
\def\xref@#1#2{\hyper@linkurl{#2}{#1}}
\begingroup
\catcode`\_=\active
\gdef_#1{\ensuremath{\sb{\mathrm{#1}}}}
\endgroup
\mathcode`\_=\string"8000
\catcode`\_=12\relax

\usepackage[a4paper,twoside,lmargin=1in,rmargin=1in,tmargin=1in,bmargin=1in,marginparwidth=0.75in]{geometry}
\usepackage{framed}

\definecolor{shadecolor}{gray}{0.95}
\usepackage{longtable}
\usepackage[normalem]{ulem}
\usepackage{fancyvrb}
\usepackage{fancyhdr}
\usepackage{graphicx}
\usepackage{marginnote}

\renewcommand{\@cite}[1]{#1}


\renewcommand*{\marginfont}{\itshape\footnotesize}

\def\Gin@extensions{.pdf,.png,.jpg,.mps,.tif}

  \pagestyle{fancy}

\usepackage[pdftitle={The Electric Field Driven Generator},
 pdfauthor={}]{hyperref}
\hyperbaseurl{}

	 \paperwidth210mm
	 \paperheight297mm
              
\def\@pnumwidth{1.55em}
\def\@tocrmarg {2.55em}
\def\@dotsep{4.5}
\setcounter{tocdepth}{3}
\clubpenalty=8000
\emergencystretch 3em
\hbadness=4000
\hyphenpenalty=400
\pretolerance=750
\tolerance=2000
\vbadness=4000
\widowpenalty=10000

\renewcommand\section{\@startsection {section}{1}{\z@}%
     {-1.75ex \@plus -0.5ex \@minus -.2ex}%
     {0.5ex \@plus .2ex}%
     {\reset@font\Large\bfseries}}
\renewcommand\subsection{\@startsection{subsection}{2}{\z@}%
     {-1.75ex\@plus -0.5ex \@minus- .2ex}%
     {0.5ex \@plus .2ex}%
     {\reset@font\Large}}
\renewcommand\subsubsection{\@startsection{subsubsection}{3}{\z@}%
     {-1.5ex\@plus -0.35ex \@minus -.2ex}%
     {0.5ex \@plus .2ex}%
     {\reset@font\large}}
\renewcommand\paragraph{\@startsection{paragraph}{4}{\z@}%
     {-1ex \@plus-0.35ex \@minus -0.2ex}%
     {0.5ex \@plus .2ex}%
     {\reset@font\normalsize}}
\renewcommand\subparagraph{\@startsection{subparagraph}{5}{\parindent}%
     {1.5ex \@plus1ex \@minus .2ex}%
     {-1em}%
     {\reset@font\normalsize\bfseries}}


\def\l@section#1#2{\addpenalty{\@secpenalty} \addvspace{1.0em plus 1pt}
 \@tempdima 1.5em \begingroup
 \parindent \z@ \rightskip \@pnumwidth 
 \parfillskip -\@pnumwidth 
 \bfseries \leavevmode #1\hfil \hbox to\@pnumwidth{\hss #2}\par
 \endgroup}
\def\l@subsection{\@dottedtocline{2}{1.5em}{2.3em}}
\def\l@subsubsection{\@dottedtocline{3}{3.8em}{3.2em}}
\def\l@paragraph{\@dottedtocline{4}{7.0em}{4.1em}}
\def\l@subparagraph{\@dottedtocline{5}{10em}{5em}}
\@ifundefined{c@section}{\newcounter{section}}{}
\@ifundefined{c@chapter}{\newcounter{chapter}}{}
\newif\if@mainmatter 
\@mainmattertrue
\def\chaptername{Chapter}
\def\frontmatter{%
  \pagenumbering{roman}
  \def\thechapter{\@roman\c@chapter}
  \def\theHchapter{\roman{chapter}}
  \def\thesection{\@roman\c@section}
  \def\theHsection{\roman{section}}
  \def\@chapapp{}%
}
\def\mainmatter{%
  \cleardoublepage
  \def\thechapter{\@arabic\c@chapter}
  \setcounter{chapter}{0}
  \setcounter{section}{0}
  \pagenumbering{arabic}
  \setcounter{secnumdepth}{6}
  \def\@chapapp{\chaptername}%
  \def\theHchapter{\arabic{chapter}}
  \def\thesection{\@arabic\c@section}
  \def\theHsection{\arabic{section}}
}
\def\backmatter{%
  \cleardoublepage
  \setcounter{chapter}{0}
  \setcounter{section}{0}
  \setcounter{secnumdepth}{2}
  \def\@chapapp{\appendixname}%
  \def\thechapter{\@Alph\c@chapter}
  \def\theHchapter{\Alph{chapter}}
  \appendix
}
\newenvironment{bibitemlist}[1]{%
   \list{\@biblabel{\@arabic\c@enumiv}}%
       {\settowidth\labelwidth{\@biblabel{#1}}%
        \leftmargin\labelwidth
        \advance\leftmargin\labelsep
        \@openbib@code
        \usecounter{enumiv}%
        \let\p@enumiv\@empty
        \renewcommand\theenumiv{\@arabic\c@enumiv}%
	}%
  \sloppy
  \clubpenalty4000
  \@clubpenalty \clubpenalty
  \widowpenalty4000%
  \sfcode`\.\@m}%
  {\def\@noitemerr
    {\@latex@warning{Empty `bibitemlist' environment}}%
    \endlist}

\def\tableofcontents{\section*{\contentsname}\@starttoc{toc}}
\parskip0pt
\parindent1em
\def\Panel#1#2#3#4{\multicolumn{#3}{){\columncolor{#2}}#4}{#1}}
\newenvironment{reflist}{%
  \begin{raggedright}\begin{list}{}
  {%
   \setlength{\topsep}{0pt}%
   \setlength{\rightmargin}{0.25in}%
   \setlength{\itemsep}{0pt}%
   \setlength{\itemindent}{0pt}%
   \setlength{\parskip}{0pt}%
   \setlength{\parsep}{2pt}%
   \def\makelabel##1{\itshape ##1}}%
  }
  {\end{list}\end{raggedright}}
\newenvironment{sansreflist}{%
  \begin{raggedright}\begin{list}{}
  {%
   \setlength{\topsep}{0pt}%
   \setlength{\rightmargin}{0.25in}%
   \setlength{\itemindent}{0pt}%
   \setlength{\parskip}{0pt}%
   \setlength{\itemsep}{0pt}%
   \setlength{\parsep}{2pt}%
   \def\makelabel##1{\upshape ##1}}%
  }
  {\end{list}\end{raggedright}}
\newenvironment{specHead}[2]%
 {\vspace{20pt}\hrule\vspace{10pt}%
  \phantomsection\label{#1}\markright{#2}%

  \pdfbookmark[2]{#2}{#1}%
  \hspace{-0.75in}{\bfseries\fontsize{16pt}{18pt}\selectfont#2}%
  }{}
      \def\TheFullDate{2019-01-15 (revised: 15 January 2019)}
\def\TheID{\makeatother }
\def\TheDate{2019-01-15}
\title{The Electric Field Driven Generator}
\author{}\makeatletter 
\makeatletter
\newcommand*{\cleartoleftpage}{%
  \clearpage
    \if@twoside
    \ifodd\c@page
      \hbox{}\newpage
      \if@twocolumn
        \hbox{}\newpage
      \fi
    \fi
  \fi
}
\makeatother
\makeatletter
\thispagestyle{empty}
\markright{\@title}\markboth{\@title}{\@author}
\renewcommand\small{\@setfontsize\small{9pt}{11pt}\abovedisplayskip 8.5\p@ plus3\p@ minus4\p@
\belowdisplayskip \abovedisplayskip
\abovedisplayshortskip \z@ plus2\p@
\belowdisplayshortskip 4\p@ plus2\p@ minus2\p@
\def\@listi{\leftmargin\leftmargini
               \topsep 2\p@ plus1\p@ minus1\p@
               \parsep 2\p@ plus\p@ minus\p@
               \itemsep 1pt}
}
\makeatother
\fvset{frame=single,numberblanklines=false,xleftmargin=5mm,xrightmargin=5mm}
\fancyhf{} 
\setlength{\headheight}{14pt}
\fancyhead[LE]{\bfseries\leftmark} 
\fancyhead[RO]{\bfseries\rightmark} 
\fancyfoot[RO]{}
\fancyfoot[CO]{\thepage}
\fancyfoot[LO]{\TheID}
\fancyfoot[LE]{}
\fancyfoot[CE]{\thepage}
\fancyfoot[RE]{\TheID}
\hypersetup{citebordercolor=0.75 0.75 0.75,linkbordercolor=0.75 0.75 0.75,urlbordercolor=0.75 0.75 0.75,bookmarksnumbered=true}
\fancypagestyle{plain}{\fancyhead{}\renewcommand{\headrulewidth}{0pt}}

\date{}
\usepackage{authblk}

\providecommand{\keywords}[1]
{
\footnotesize
  \textbf{\textit{Index terms---}} #1
}

\usepackage{graphicx,xcolor}
\definecolor{GJBlue}{HTML}{273B81}
\definecolor{GJLightBlue}{HTML}{0A9DD9}
\definecolor{GJMediumGrey}{HTML}{6D6E70}
\definecolor{GJLightGrey}{HTML}{929497} 

\renewenvironment{abstract}{%
   \setlength{\parindent}{0pt}\raggedright
   \textcolor{GJMediumGrey}{\rule{\textwidth}{2pt}}
   \vskip16pt
   \textcolor{GJBlue}{\large\bfseries\abstractname\space}
}{%   
   \vskip8pt
   \textcolor{GJMediumGrey}{\rule{\textwidth}{2pt}}
   \vskip16pt
}

\usepackage[absolute,overlay]{textpos}

\makeatother 
      \usepackage{lineno}
      \linenumbers
      
\begin{document}

             \author[1]{Katsuo  Sakai}

\renewcommand\Authands{ and }

\date{\small \em Received: 12 December 2018 Accepted: 31 December 2018 Published: 15 January 2019}

\maketitle


\begin{abstract}
        


Dr. Feynman predicted it to be theoretically possible to generate electric energy from an electric field. For realizing his predict, a new electrostatic generating method was proposed by the author that uses Asymmetric electrostatic force as the driving force of a charge carrier for the generator. Therefore this generator was named the electric field driven generator.After experimenting with many models using pendulum-type equipment, rotation-type equipment was tried.This experimental equipment produced electricity continuously when the applied voltage to the high voltage electrode was higher than 5.8 kV. This result was estimated by a simulation, and the measured collection currents for different high voltages almost agreed with the simulated collection current. Therefore the theory of the electric field driven generator was confirmed, and Feynman's dream has become reality.

\end{abstract}


\keywords{electrostatic generator; asymmetric electrostatic force; charge carrier; electric field driven; electric energy.}

\begin{textblock*}{18cm}(1cm,1cm) % {block width} (coords) 
\textcolor{GJBlue}{\LARGE Global Journals \LaTeX\ JournalKaleidoscope\texttrademark}
\end{textblock*}

\begin{textblock*}{18cm}(1.4cm,1.5cm) % {block width} (coords) 
\textcolor{GJBlue}{\footnotesize \\ Artificial Intelligence formulated this projection for compatibility purposes from the original article published at Global Journals. However, this technology is currently in beta. \emph{Therefore, kindly ignore odd layouts, missed formulae, text, tables, or figures.}}
\end{textblock*}


\let\tabcellsep& 	 	 		 
\section[{Introduction}]{Introduction}\par
oday there are many kinds of electric power generators. Each has some advantages and some disadvantages. The ideal electric power generator would never produce carbon dioxide and would be safe, stable, low cost, small, and last a long time.\par
The well-known physicist Richard P, Feynman estimated that, in theory, getting energy from an electric field is possible; however the shape of the electric field that would make this possible has not been discovered. \hyperref[b0]{[1]} An electrostatic power generator that can get energy from an electric field would be the ideal electric power generator.\par
Nine years ago, the author discovered Asymmetric electrostatic force \hyperref[b1]{[2]}, \hyperref[b2]{[3]}, which makes generating energy from an electric field possible. This new force acts on an asymmetrically shaped conductor in a normal electric field. Retrieving energy from an electric field becomes possible when the shape of the charged conductor-not the electric field-is changed.\par
Several experiments were performed using pendulum-type experimental equipment \hyperref[b3]{[4]}, \hyperref[b4]{[5]}; however, all those experiments failed.\par
II. Theory of the Electric Field Driven Generator a) Asymmetric electrostatic force For a long time, the main purposes of electrostatic research were electro photography and electro spray coating. Both technologies make use of charged fine powders that are moved by electrostatic force. When this electrostatic force was calculated, the charged fine powder was regarded as a point charge, and the well-known Coulomb's formula \hyperref[b0]{(1)} was used. The magnitude of this electrostatic force doesn't change when the direction of the electric field turns over as shown in Figure  {\ref 1}. \hyperref[b0]{(1)} where f: an electrostatic force that acts on a point charge, q: quantity of charge of a point charge; and E: intensity of the electric field in which a point charge is placed.\par
The application of this formula is limited to point charges and sphere-shaped charged carriers \hyperref[b5]{[6]}.\par
In contrast, a new electrostatic generator that uses a non-spherical charged carrier was presented recently \hyperref[b6]{[7,}\hyperref[b7]{8]}. This generator uses an asymmetric shaped conductor as its charge carrier. The electrostatic force that acts on this asymmetrically shaped charged carrier was both simulated \hyperref[b2]{[3]} and experimentally measured \hyperref[b1]{[2]}. As a result, the magnitude of this electrostatic force was found to change when the direction of the electric field is reversed as shown in Figure  {\ref 2}.\par
This changeable electrostatic force was named as Asymmetric electrostatic force.\par
As shown in Figure  {\ref 2}, the left side of the electric field is called the forward electric field and the right side of the electric field is the backward electric field. The magnitude of the electrostatic force becomes less than half when the direction of the electric field is reversed. 
\section[{b) The basic theory of the electric field driven generator}]{b) The basic theory of the electric field driven generator}\par
An electrostatic generator builds the electric charge to a high potential by mechanical force against the electric force that acts on this charge. The mechanical force cannot carry the charge directly, therefore, the charge is packed into a suitable body. We call this body the charge carrier. The most popular electrostatic generator is the Van de Graaff electrostatic generator \hyperref[b8]{[9]}invented by Dr. Van de Graaff in 1931.Today, it is used with a large voltage power supply and can produce ten million volts. In this machine, an insulating belt is used as a charge carrier. Figure \hyperref[fig_1]{3} shows an example of this generator. 
\section[{Global Journal of Computer Science and Technology}]{Global Journal of Computer Science and Technology}\par
Volume XIX Issue II Version I  The principle of this electrostatic generator is shown schematically in Fig. \hyperref[fig_2]{4}. In Figure \hyperref[fig_2]{4}, the bold green line represents the potential, and the blue arrows represent the forces. The small red circles represent electrons, and the sky blue plates represent the charge carriers. In the Van de Graaff electrostatic generator, the charge carrieris directly transported by a strong mechanical force, Fm, against the electrostatic force, Fe.\par
In contrast, in the electric field driven generator, the charge carrier is first moved to the forward electric field caused by the high voltage source (electret) according to the electrostatic force Fe1.In this process, the charge carrier gains kinetic energy from the electric field. Then, the charge carrieris moved into the backward electric field, expending the given energy against electrostatic force Fe2.\par
The shape of this charge carrier is asymmetric. Therefore, Asymmetric electrostatic force acts on this charge carrier. Thus, the absolute value of Fe1 is larger than that of Fe2.As a result, the charge carrier can arrive at a potential (-200V) that is higher than the initial potential (0V).\par
Abasic unit of the electric field driven generator that is driven by Asymmetric electrostatic force is concretely shown in Figure \hyperref[fig_3]{5}. The high voltage source gives a positive high voltage. The injection electrodes are grounded. The collection electrodes are kept at a negative low voltage. As a result, the high voltage source and the injection electrodes produce a forward electric field for a negative charge between them. The high voltage source and the collection electrodes produce a backward electric field for a negative charge between them. The line of electric force is depicted as red arrow dotted lines in Figure \hyperref[fig_3]{5}.\par
A gutter shape conductor is used as a charge carrier that carries negative charge (electron) from the injection electrodes to the collection electrodes through the high voltage sources.\par
Asymmetric electrostatic phenomenon produces a large electrostatic force in the forward electric field and it produces a weak electrostatic force in the backward electric field. Therefore, the charge carrier gains a large amount of kinetic energy in the forward electric field. Then, it loses some of its kinetic energy in the backward electric field. As a result, the charge carrier maintains extra kinetic energy when it arrives at the collection electrodes. The carried charge can be built to a higher potential by this extra energy. This result means that the equipment described by fig. \hyperref[fig_3]{5} can produces an electric energy. Namely this equipment is the new electrostatic generator.\par
The just above mentioned explanation is the principle of the electric field driven generator. This principle is different from that of the Van de Graaff electrostatic generator.\par
III.   The charge carrier disk is a 0.5 mm thickness PET plate with a diameter of 100 mm. ADB (Autonomous Decentralized Bearing) bearings were fixed on the center of the disk. The ADB bearing can rotate easily around the steel shaft because the kinetic friction coefficient is only 0.0015. 
\section[{Experiment Instrument}]{Experiment Instrument}\par
The six charge carrier electrodes were placed at 60-degree intervals as shown Figure  {\ref 8}. The charge carrier electrodes were made from double-sided goldplated aluminum plates with 0.1 mm thicknesses. The electrostatic force always acts on the gold surfaces perpendicularly. The charge carrier electrode was created in a gutter shape with a height of 60 mm and width and breadth of 5 mm each. The total weight was only 1.4 g.\par
The two charge injection electrodes, two high voltage electrodes, and two charge collection electrodes were placed on the main PET base plate at 60-degree intervals as shown in Figure  {\ref 8}. Each electrode was placed on a Teflon base to reducing the leak current as shown in Figure  {\ref 7}.\par
Those six electrodes had an outer electrode and inner electrode, and the distance between them was 20 mm. The injection electrodes and the high voltage electrodes ware made from aluminum plates with 0.1 mm thicknesses. The collection electrodes were made from aluminum plating with 0.1 mm thickness and PET film with 0.5 mm thickness. The electrodes consisted of three layers: aluminum plate, PET film, and aluminum plate. As a result, it became a capacitor. This small capacitor was connected to the big outer capacitor (not shown in Figure  {\ref 8}). The size of this capacitor was 20cm by 20cm as was required by the surface potential meter. The capacitance of the small capacitor became 330 pF, and the capacitance of the big capacitor became 1100pF because the relative permittivity of PET is 3.2. The total capacitance of the two capacitors was 1430pf. Hereafter those two capacitors are together called the collection capacitor or, simply, the capacitor.\par
The height of the outer electrodes was 60 mm, and the height of the inner electrodes was 50 mm. The width of the outer injection electrode, the outer high voltage electrode, and the outer collection electrode were 22 mm, 22 mm, and 44 mm, respectively. The width of the inner injection electrode, the inner high voltage electrode, and the inner collection electrode were 10 mm, 10 mm, and 20 mm, respectively. The distance between the outer injection electrode and the outer high voltage electrode and the distance between the outer high voltage electrode and the outer collection electrode were 30 mm each. The distance between the inner injection electrode and the inner high voltage electrode and the distance between the inner high voltage electrode and the inner collection electrode were 25 mm each.  
\section[{C}]{C}\par
The injection electrodes were always grounded, the high voltage electrodes were connected to a high voltage power supply, and the surface potential of the collection capacitor was measured by a surface potential meter.\par
The injection electrodes and the collection electrode had aluminum foil on the inner surface as an electric connector as shown in Figure  {\ref 8}. The width was 5mm, and the length was 10mm.The foils softly connected the charge carrier electrode to the injection and collection electrode electrically.\par
The collection electrodes were wide. As a result, the collection electrodes could perform semi-Faraday gauge. When the charge carrier electrode was connected to the collection electrode by the aluminum foil, more than90\% charge on the charge carrier electrode was transferred to the collection electrode (simulation result).\par
Grounded aluminum slices (10mm x 100mm) were located just before the collection electrode. The leak current from the high voltage electrode to the collection electrode was captured here.\par
The surface potential meter (SHISHIDO ELECTROSTATIC: STATIRON-DZ 3) was used to measure the surface potential of the collection capacitor.\par
IV. 
\section[{Simulation Result}]{Simulation Result}\par
Four kinds of forces act on the moving charge carrier that consisted of a disk and six electrodes as shown in Figure \hyperref[fig_8]{9}. The forces are the electrostatic force, the kinetic friction force, the mechanical resistance force of the aluminum foil, and the air resistance force. The electrostatic force, the mechanical resistance force, and the air resistance force act on the charge carrier electrodes and the kinetic friction force acts on the rotating charge carrier disk and the ADB bearings. At first, the electrostatic force is simulated. In Figure \hyperref[fig_8]{9}, the charge carrier electrodes A and D are accelerated by a forward electrostatic force Fe1 in the forward electrostatic field between the injection electrode and the high voltage electrode. At the same time, charge carrier electrodes B and E are decelerated by a backward electrostatic force Fe2 in the backward electrostatic field between the high voltage electrode and the collection electrode. On the contrary side, the charge carrier electrodes C and F do not suffer any electrostatic force because there is no electric field in the area from the collection electrode to the injection electrode.\par
As a result, the total electrostatic force that acts on those six charge carrier electrodes is calculated by the following equation (2).2 2 2 1 × + × = Fe Fe Fet (2)\par
where Fet: total electrostatic force, Fe1: accelerating electrostatic force, and Fe2: decelerating electrostatic force. Fe1 and Fe2 were simulated by the twodimensional finite difference method. Figure  {\ref 10} shows the simulation result of Fe1 and Fe2 when the high voltage was 6.0kV. 
\section[{Figure 10: Simulation results of Fe1 and Fe2}]{Figure 10: Simulation results of Fe1 and Fe2}\par
According to Figure  {\ref 10}, the average of the total electrostatic force Fe1*2+Fe2*2 is about 0.086 mN. Therefore the total of the air resistance force, the mechanical resistance force, and the kinetic friction force must be lower than 0.086 mN.\par
Next, the air resistance force: Fa is calculated by the following equation (3).2 / ) ( 2 v S C Fa d × × × = ? (3)\par
where Cd: air resistance coefficient, ?: air density, S: front surface area of the charge carrier electrodes, and v: velocity of the charge carrier electrode.\par
The air resistance coefficient varies with the shape of the moving body. The value for the guttershaped charge carrier electrode was decided as 1.5 because the shape looks like a square pillar that has a round edge. Air density is 1.3 kg/m3. The front surface area of the charge carrier electrode is 0.0018 m2 because the breadth is 5.0 mm and the height is 60.0 mm. The velocity of the charge carrier electrode is 0.157 m/s, because the RPM (rotation per minute) is 30 for minimum stable rotation of the charge carrier, and the radius of the charge carrier disk is 0.05 m.\par
As a result, the air resistance force becomes 0.043 mN. This value is half of the electrostatic force. Therefore if the total force of the remaining two forces is about 0.043mN, the charge carrier disk will rotate continuously when the high voltage electrode was applied +6.0kV.\par
Third, the mechanical resistance force of the aluminum foils is roughly estimated, because the exact simulation of this force is very difficult.\par
The mechanical force that accelerates a piece of aluminum foil from 0 m/s to 0.157 m/s in the distance 5.0 mm was calculated with the kinetic equations. The width of the piece is 5.0 mm, the length of the piece is 5.0 mm, and the weight of the piece is 0.0008125 g. As a result, the force becomes 2.0?N. There are four pieces in one round; therefore each charge carrier electrode accepts 8.0?N. There are six charge carrier electrodes on a charge carrier; therefore the total force that acts on the charge carrier electrodes is 0.048 mN.\par
Finally, the kinetic friction force was estimated. The kinetic friction coefficient of the ADB bearings is only 0.0015, and the weight of the charge carrier was only 7.7g.; therefore the kinetic friction force will be almost zero.\par
As a result, the total force of the air resistance force, the mechanical resistance force, and the kinetic friction force is roughly estimated as 0.091mN. This total force is about the same as with the electrostatic force: 0.086mN.\par
Therefore, the charge carrier can be expected to rotate continuously and generate electricity when the high voltage electrode is applied +6.0kV or a little higher.\par
V. 
\section[{Results}]{Results}\par
The high voltage electrode was applied from +5.6kV to +9.4kV by the interval 0.2kV, and the movement of the charge carrier rotation and the surface potential meter display was taken by the digital camera (Sony Cyber-shot DSC-HV5V).\par
When the applied voltage was +5.6kV, the charge carrier could not rotate continuously, and when the applied voltage was +9.4kV, a corona discharge occurred. When the applied voltage was +5.8kV to +9.2kV, the charge carrier could rotate continuously and the surface potential changed from 0.00kV to -0.3 \textasciitilde -0.6kV.\par
One example of those measurements are shown in Figure \hyperref[fig_10]{11}. The applied voltage was +8.0kV.\par
At first, the surface potential quickly increases in a negative direction. However, the increase rate gradually slows. After 600 seconds, the increase rate becomes almost zero. This increased rate of the surface potential is proportional to the collection (generating) current;, it is the electric power generating rate. However, these results do not mean that the electric power generation became zero after 600 seconds rotation because after 1200 seconds of rotation, the surface potential increased again rapidly to a negative direction when the upper aluminum plate of the collection capacitor was instantaneously grounded. This result means that the electric power generates anytime after the capacitor is emptied. The increasing rate of the surface potential when 8.0 kV was applied at 0 second, and the increasing rate when the capacitor was grounded at 1200 second, were almost the same, as shown in Figure \hyperref[fig_10]{11}.\par
The collection current can be calculated with this surface potential change and the capacity of the collection capacitor (1430pF).\par
Therefore, the collection currents for different high voltages were calculated by measuring the surface potential change when the capacitor was grounded. The measurements were taken three times for each high voltage, and an average collection current was calculated.\par
When 7.0kV was applied to the high voltage electrode, the charge carrier started to rotate automatically and the surface potential changed as shown in Figure \hyperref[fig_0]{12}.  
\section[{C}]{C}\par
Figure \hyperref[fig_0]{12}: The surface potential change of the collection capacitor when the capacitor was grounded When 7.0kV was applied at 0 second, the surface potential shows +0.04kV as shown in Figure \hyperref[fig_0]{12}. This +0.04kV is an induced surface potential because the upper electrode of the capacitor is electrically floating between the high voltage electrode and the grounded lower electrode of the capacitor.\par
However, when the upper electrode of the capacitor was grounded at 45 second, this induced surface potential was not recognized. This result is because the charge carrier disk was rotating rapid at this time therefore the negative collection current canceled the positive induced potential quickly.\par
The increase rate of the collection currents after grounding was fast. On the other hand, the increased rate of the collection current when 7.0kV was applied at 0 second was slow. This result is because the rotation speed of the charge carrier disk increases gradually from 0 second, and the rotation speed became constant when the upper electrode of the capacitor was grounded at after 40 second.\par
Figure \hyperref[fig_12]{13} shows the measured average collection current for different high voltages. Figure \hyperref[fig_12]{13} demonstrates that the collection current almost increases in proportion with an applied high voltage, that is, generated electricity is in proportion to an applied high voltage. However, when the high voltage is higher than 8.0kV, the collection current becomes saturated and reduced. This cause will be considered in the next section.\par
Incidentally, when the applied high voltage was lower than 6.8kV, the charge carrier disk could not start to rotate automatically because the electrostatic force is lower than Static frictional force, so an air flow assisted the disk in starting rotation at first. After starting to rotate it can rotate continuously because the electrostatic force is higher than the Kinetic friction force. 
\section[{VI.}]{VI.} 
\section[{Discussion}]{Discussion}\par
In theory the collection current increases with the applied voltages. However, the measured collection current decreased when the applied voltage was higher than 8.0kV as shown in Figure \hyperref[fig_12]{13}. This unexpected result is because of the leak current that flows from the high voltage electrodes to the collection electrodes.\par
The polarity of the leak current is positive, but the collected charge in the capacitor is negative. Therefore, the collected charge was partly canceled. The grounded guard electrodes just before the collection electrodes can cut the surface leak current. However, they cannot cut the volume leak current.  The leak currents were calculated from the surface potential increase 10 seconds after the capacitor was grounded.\par
When the applied voltage is lower than 8.0kV, the leak current is almost zero. However, it rapidly increases from 8.0kV as shown in Figure \hyperref[fig_13]{14}.  The collection current can be calculated by the following equation.m n R r q A × × × × = (4)\par
where q: injected charge quantity from the injection electrode to the charge carrier electrode, r: charge collection rate from the charge carrier electrode to the collection electrode, n: number of the collection electrode, m: number of the charge carrier electrode, and R: rotation number of the charge carrier disk per minute.\par
The injected charge quantity q from the injection electrode to the charge carrier electrode was decided by a simulation. For example, it became 1.2 nano-Coulombs when the applied voltage was +6.0 kV.\par
The simulation result of the charge collection rate "r" from the charge carrier electrode to the collection electrode was more than 0.9. However, 0.9 was used because the actual equipment was a little different from the simulated equipment.\par
The number n of the collection electrode was two, and the number m of the charge carrier electrode was six.\par
The rotation number R of the charge carrier disk per minute (RPM) was counted from the experiment movie. Figure \hyperref[fig_4]{16} shows the counted RPM. Figure  {\ref 17} shows that when the applied voltage is lower than 8kv, the calculated collection current almost agrees with the measured collection current. The small difference between the experiment and the simulation may be because of a small difference between the real value and the estimated value of the injection charge quantity and the collection rate.\par
The lowest high voltage that can rotate the charge carrier continuously was estimated by the simulation as about +6.0kV. The actual lowest high voltage was +5.8kV, and the measured collection current agreed with the calculated collection current. Those results mean that the theory of the electric field driven generator is correct and this experimental equipment produced electricity: Electric energy could be produced from an electric field. 
\section[{VII.}]{VII.} 
\section[{Conclusion}]{Conclusion}\par
This experiment confirmed that the experimental equipment of the field driven electrostatic generator that uses Asymmetric electrostatic force as a driving force of the charge carrier can generate electricity continuously. Namely Electric energy was gained from an electric field. This experimental result may be the first successful attempt at this in the world.\par
The experimental equipment produced the electric field with a high voltage electrode and an electric power supply. This system was used to confirm the new theory of the electrostatic generating method. However, this system cannot be used as a commercial machine because the electric field must be produced by an electret in place of an electrode and a power supply. As a result, the electret power generator not only does not produce CO2 but also is safe, low cost, small, lightweight, and has a long life span.\begin{figure}[htbp]
\noindent\textbf{12}\includegraphics[]{image-2.png}
\caption{\label{fig_0}Fig. 1 :Fig. 2 :}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{3}\includegraphics[]{image-3.png}
\caption{\label{fig_1}Fig. 3 :}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{4}\includegraphics[]{image-4.png}
\caption{\label{fig_2}Figure 4 :}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{5}\includegraphics[]{image-5.png}
\caption{\label{fig_3}Figure 5 :}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{6}\includegraphics[]{image-6.png}
\caption{\label{fig_4}Figure 6 :}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{}\includegraphics[]{image-7.png}
\caption{\label{fig_5}}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{78}\includegraphics[]{image-8.png}
\caption{\label{fig_6}Figure 7 :Figure 8 :}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{}\includegraphics[]{image-9.png}
\caption{\label{fig_7}The}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{9}\includegraphics[]{image-10.png}
\caption{\label{fig_8}Figure 9 :}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{11}\includegraphics[]{image-11.png}
\caption{\label{fig_10}Figure 11 :}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{}\includegraphics[]{image-12.png}
\caption{\label{fig_11}The}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{13}\includegraphics[]{image-13.png}
\caption{\label{fig_12}Figure 13 :}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{14}\includegraphics[]{image-14.png}
\caption{\label{fig_13}Figure 14}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{14}\includegraphics[]{image-15.png}
\caption{\label{fig_14}Figure 14 :}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{15}\includegraphics[]{image-16.png}
\caption{\label{fig_15}Figure 15}\end{figure}
 \begin{figure}[htbp]
\noindent\textbf{1515}\includegraphics[]{image-17.png}
\caption{\label{fig_16}Figure 15 :Figure 15}\end{figure}
      			\footnote{© 2019 Global Journals} 		 		\backmatter  			  				\begin{bibitemlist}{1}
\bibitem[Sakai ()]{b3}\label{b3} 	 		‘A first trial for the new electrostatic generator that will solve the CO2 problem’.  		 			K Sakai 		.  	 	 		\textit{Proceedings of 2014 ESA annual Conference},  				 (2014 ESA annual Conference)  		2014. p. B3.  	 
\bibitem[Sakai ()]{b4}\label{b4} 	 		‘A second trial for the new electrostatic generator that is driven by Asymmetric electrostatic force’.  		 			K Sakai 		.  	 	 		\textit{Proceedings of 2016 Electrostatics Joint Conference},  				 (2016 Electrostatics Joint Conference)  		2016. p. P4.  	 
\bibitem[Sakai]{b1}\label{b1} 	 		‘Asymmetric electrostatic force’.  		 			K Sakai 		.  	 	 		\textit{Journal of Electromagnetic Analysis and Applications 2014 on the Special Issue on Electromagnetic Field Theory},  				p. .  	 
\bibitem[Sakai ()]{b7}\label{b7} 	 		\textit{Asymmetric Electrostatic Forces and a New Electrostatic Generator},  		 			K Sakai 		.  		2010. New York: Nova Science Publish.  	 	 (first ed) 
\bibitem[Halliday et al.]{b5}\label{b5} 	 		‘Electric Charge" question 1’.  		 			David Halliday 		,  		 			Robert Resnick 		,  		 			Jearl Walker 		.  	 	 		\textit{Fundamentals of Physics},  				Wiley \& sons. Inc.  	 	 (6th edition Japanese version Chapter) 
\bibitem[Feynman et al.]{b0}\label{b0} 	 		 			Richard P Feynman 		,  		 			Robert B Leighton 		,  		 			Matthew L Sands 		.  		\textit{The Feynman LECTURES ON PHYSICS Japanese version chapter 4 Electrostatics},  				p. 44.  	 	 (IWANAMI publishing company) 
\bibitem[Handbook of electrostatic ()]{b8}\label{b8} 	 		\textit{Handbook of electrostatic},  		1998. Japan. p. 962.  	 
\bibitem[Sakai ()]{b6}\label{b6} 	 		 			K Sakai 		.  		\textit{Electrostatics: Theory and Applications},  				 (New York)  		2010. Nova Science Publish.  	 	 (first ed) 
\bibitem[Sakai ()]{b2}\label{b2} 	 		\textit{Theory of Asymmetric electrostatic force},  		 			K Sakai 		.  		2017.  	 
\end{bibitemlist}
 			 		 	 
\end{document}
