\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={Concept of the Dispersion of Electric and Magnetic Inductivities and its Physical Interpretation},
 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{2014-01-15 (revised: 15 January 2014)}
\def\TheID{\makeatother }
\def\TheDate{2014-01-15}
\title{Concept of the Dispersion of Electric and Magnetic Inductivities and its Physical Interpretation}
\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]{F.F.  Mende}

             \affil[1]{  B.I. Verkin Institute}

\renewcommand\Authands{ and }

\date{\small \em Received: 12 December 2013 Accepted: 3 January 2014 Published: 15 January 2014}

\maketitle


\begin{abstract}
        


In a number of scientific publications is asserted that the permittivity and permeability of material media depends on frequency. But even Maxwell himself, who was the author of the basic equations of electrodynamics, believed that ? and ? were frequency-independent fundamental constants. The article shows that Max well was right, and the recognition of the presence of dispersion in the dielectric constant and magnetic permeability is a physical and methodological error. In it is shown that the kinetic inductance of charge has the same fundamental value as the dielectric and magnetic constant of material media. Are introduced the new concepts of the magneto electro kinetic wave and electro magneto potential waves, and also the kinetic capacitance.

\end{abstract}


\keywords{max well questions; plasma media; dielectric media; magnetic media; permittivity; permeability; kinetic inductivity; polarization vector; london equat}

\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
ow the idea of ? and µ-dispersion appeared and evolved is illustrated vividly in the monograph of well-known specialists in physics of plasma \hyperref[b0]{[1]}: while working at the equations of electrodynamics of material, media, G. Maxwell looked upon electric and magnetic inductivities as constants (that is why this approach was so lasting). Much later, at the beginning of the XX century, G. Heavisidr and R.Wull put forward their explanation for phenomena of optical dispersion (in particular rainbow) in which electric and magnetic inductivities came as functions of frequency. Quite recently, in the mid-50ies of the last century, physicists arrived at the conclusion that these parameters were dependent not only on the frequency but on the wave vector as well. That was a revolutionary breakaway from the current concepts. The importance of the problem is clearly illustrated by what happened at a seminar held by L. D. Landau in 1954, where he interrupted A. L. Akhiezer reporting on the subject: "Nonsense, the refractive index cannot be a function of the refractive index". Note, this was said by L. D. Landau, an outstanding physicist of our time.\par
What is the actual situation? Running ahead, I can admit that Maxwell was right: both ? and µ are frequency -independent constants characterizing one or another material medium. Since dispersion of electric and magnetic inductivities of material media is one of the basic problems of the present -day physics and electrodynamics, the system of views on these questions has to be radically altered again. 
\section[{II.}]{II.} 
\section[{Plasma Media}]{Plasma Media}\par
It is noted in the introduction that dispersion of electric and magnetic inductivities of material media is a commonly accepted idea \hyperref[b0]{[1]}\hyperref[b1]{[2]}\hyperref[b2]{[3]}\hyperref[b3]{[4]}\hyperref[b4]{[5]}. The idea is however not correct.\par
To explain this statement and to gain a better understanding of the physical essence of the problem, we start with a simple example showing how electric lumped-parameter circuits can be described \hyperref[b5]{[6]}. As we can see below, this example is directly concerned with the problem of our interest and will give us a better insight into the physical picture of the electro dynamic processes in material media.\par
In a parallel resonance circuit including a capacitor ? and an inductance coil L, the applied voltage U and the total current I ? through the circuit are related as? + = + = ? t d U L t d U d C I I I L C 1 , where t d U d C I C = is the current through the capacitor, ? = t d U L I L 1\par
is the current through the inductance coil. For the harmonic voltage U = U 0 sin ?tt U L C I ? ? ? cos 1 0 ? ? ? ? ? ? ? ? ? = ? . (2.1)\par
The term in brackets is the total susceptance ? ? of the circuit, which consists of the capacitive ? ? and inductive ? L components From the mathematical (i.e. other than physical) standpoint, we may assume a circuit that has only a capacitor and no inductance coil. Its frequencydependent capacitance isL C L c x ? ? ? ? ? 1 ? = + = . H © 2014 Global Journals Inc. (US) 
\section[{Global Journal of Researches in Engineering}]{Global Journal of Researches in Engineering}? ? ? ? ? ? ? ? ? = ? ? ? 1 ) ( * C C . (2.2)\par
Another approach is possible, which is correct too.\par
Eq. (2.1) can be re-written ast U L I ? ? ? ? cos 1 0 2 0 2 ? ? ? ? ? ? ? ? ? ? = ? .\par
In this case the circuit is assumed to include only an inductance coil and no capacitor. Its frequencydependent inductance is ? ? ? ? ? ? ? ? ? = 1 ) ( * 2 0 2 ? ? ? L L . (\textbf{2}) ( * ? L .\par
We shall not consider here any other cases, e.g., series or more complex circuits. It is however important to note that applying the above method, any circuit consisting of the reactive components C and L can be described either through frequency -dependent inductance or frequency -dependent capacitance.\par
But this is only a mathematical description of real circuits with constant -value reactive elements.\par
It is well known that the energy stored in the capacitor and inductance coil can be found as2 2 1 U C W C = , (2.6) 2 2 1 I L W L = . (\textbf{2.7)}\par
But what can be done if we have) ( * ? C and 
\section[{) ( * ? L}]{) ( * ? L}\par
? There is no way of substituting them into Eqs.\par
(2.6) and (2.7) because they can be both positive and negative. It can be shown readily that the energy stored in the circuit analyzed is2 2 1 U d d W X ? ? ? = ? ,\textbf{(2.8)}\par
or [ ] 2 ) ( * 2 1 U d C d W ? ? ? ? = ? , (\textbf{2}) ( * 1 2 1 U d L d W ? ? ? ? ? ? ? ? ? ? ? ? = ? . (3.10)\par
Having written Eqs. (2.8), (2.9) or (2.10) in greater detail, we arrive at the same result:, 2 1 2 1 2 2 I L U C W + = ?\par
Where U is the voltage at the capacitor and I is the current through the inductance coil. Below we consider the physical meaning jog the magnitudes ?(?) and µ(?) for material media.\par
A superconductor is a perfect plasma medium in which charge carriers (electrons) can move without friction. In this case the equation of motion isE e t d V d m ? ? = , (\textbf{2.11)}\par
Where m and e are the electron mass and charge, respectively; E ? is the electric field strength, V ? is the velocity. Taking into account the current density, V e n j ? ? = (2.12)\par
we can obtain from Eq. (2.11)? = t d E m e n j L ? ? 2 .\par
(\par
In Eqs. (2.12) and (2. ? = t d E L j k L ? ? 1 . (2.14)\par
Here L k is the kinetic inductivity of the medium \hyperref[b6]{[7]}\hyperref[b7]{[8]}\hyperref[b8]{[9]}\hyperref[b9]{[10]}\hyperref[b10]{[11]}. Its existence is based on the fact that a charge carrier has a mass and hence it possesses inertia properties.\par
For harmonic fields we have is the current through the inductance coil.t E E ? sin 0 ? ? = and Eq. (2.14) becomes t E L j k L ? ? cos 1 0 ? = ? . (\textbf{2}\par
In this case the Maxwell equations take the following form , 1 ,0 0 ? + = + = ? = t d E L t E j j H rot t H E rot k L C ? ? ? ? ? ? ? ? ? ? ? ? µ (2.16)\par
Where ? 0 and µ 0 are the electric and magnetic inductivities in vacuum, = + + H L t H H rot rot k ? ? ? µ ? ? ? µ .\par
(2.17)\par
For time-independent fields, Eq. (2.17) transforms into the London equation \hyperref[b11]{[12]} 0 0 = + H L H rot rot k ? ? µ , where 0 2 µ ? k L L =\par
is the London depth of penetration.\par
As Eq. (2.16) shows, the inductivities of plasma (both electric and magnetic) are frequencyindependent and equal to the corresponding parameters for vacuum. Besides, such plasma has another fundamental material characteristic -kinetic inductivity.\par
Eqs. (2.16) hold for both constant and variable fields. For harmonic fieldst E E ? sin 0 ? ? = , Eq.(2.16) gives t E L H rot k ? ? ? ? cos 1 0 0 ? ? ? ? ? ? ? ? ? ? ? = . (2.18)\par
Taking the bracketed value as the specific susceptance ? x of plasma, we can write t E H rot X ? ? cos 0 ? ? = , (\textbf{2}) ( * 1 1 2 2 0 0 ? ? ? ? ? ? ? ? ? ? ? ? = ? ? ? ? ? ? ? ? ? = ? = k X L , (2.20) and ? ? ? ? ? ? ? ? ? = ? ? ? ? ? ? 2 0 1 ) ( * , where k L 0 2 1 ? ? ? =\par
is the plasma frequency. Now Eq. (2.19) can be re-written ast E H rot ? ? ? ? ? ? cos 1 0 2 2 0 ? ? ? ? ? ? ? ? ? ? ? = , or t E H rot ? ? ? ? cos ) ( * 0 ? ? = .\par
The ?*(?) -parameter is conventionally called the frequency-dependent electric inductivity of plasma. In reality however this magnitude includes simultaneously the electric inductivity of vacuum aid the kinetic inductivity of plasma. It can be found as? ? ? ? X = ) ( * . It is evident that there is another way of writing ? ? , * 1 1 1 1 2 2 0 k k k X L L L ? ? ? ? ? ? ? ? ? = ? ? ? ? ? ? ? ? ? = ? = (2.21) where ? ? ? ? ? ? X k k L L 1 1 ) ( * 2 2 = ? ? ? ? ? ? ? ? ? = .\par
L k *(?) written this way includes both ? 0 and L k .\par
Eqs. (2.20) and (2.21) are equivalent, and it is safe to say that plasma is characterized by the frequency-dependent kinetic inductance L k *(?) rather than by the frequency-dependent electric inductivity ?*(?).\par
Eq. (2.18) can be re-written using the parameters ?*(?) and L k *(?) Thus, the parameter ?*(?) is not an electric inductivity though it has its dimensions. The same can be said about L k *(?).t E H rot ? ? ? ? cos ) ( * 0 ? ? = , (2.22) or t E L H rot k ? ? ? cos ) ( * 1 0 ? ? = . (\textbf{2}\par
We can see readily that? ? ? ? X = ) ( * , ? ? ? X k L 1 ) ( * = .\par
These relations describe the physical meaning of ?*(?) and L k *(?).\par
Of course, the parameters ?*(?) and L k *(?) are hardly usable for calculating energy by the following equations2 0 2 1 E W E ? = and 2 0 2 1 j L W k j = .\par
For this purpose the Eq. (2.9)-type fotmula was devised in \hyperref[b1]{[2]}:[ ] 2 0 ) ( * 2 1 E d d W ? ? ? ? ? = .\par
(2.24)\par
Using Eq. (2.24), we can obtain2 0 2 0 0 2 0 2 2 0 0 2 1 2 1 1 2 1 2 1 j L E E L E W k k + = ? + = ? ? ? ?\par
The same result is obtainable from We have found that ?(?) is not dielectric inductivity permittivity. Instead, it includes two frequency-independent parameters ? 0 and L k . What is the reason for the physical misunderstanding of the parameter ?(?)? This occurs first of all because for the case of plasma the2 0 ) ( * 1 2 1 E d L d W k ? ? ? ? ? ? ? ? ? ? ? ? = .? t d E L k ? 1 -type term is not explicitly present in the second Maxwell equation.\par
There is however another reason for this serious mistake in the present-day physics \hyperref[b1]{[2]} as an example. This study states that there is no difference between dielectrics and conductors at very high frequencies. On this basis the authors suggest the existence of a polarization vector in conducting media and this vector is introduced from the relationm m r e n r e P ? ? ? = ? = , (2.25)\par
Where n is the charge carrier density, m r ? is the current charge displacement. This approach is physically erroneous because only bound charges can polarize and form electric dipoles when the external field overcoming the attraction force of the bound charges accumulates extra electrostatic energy in the dipoles. In conductors the charges are not bound and their displacement would not produce any extra electrostatic energy. This is especially obvious if we employ the induction technique to induce current (i.e. to displace charges) in a ring conductor. In this case there is no restoring force to act upon the charges, hence, no electric polarization is possible. In \hyperref[b1]{[2]} the polarization vector found from Eq. (2.25) is introduced into the electric induction of conducting media E P E D p ? ? ? ? ? ? ? ? ? ? ? ? ? = + = 2 2 0 0 1 ) ( * ) ( * ? ? ? ? ? ? .\par
Thus, the total accumulated energy is2 2 2 0 1 2 1 2 1 E L E W k ? ? ? + = ? .\par
(2.26) However, the second term in the right-hand side of Eq. (2.26) is the kinetic energy (in contrast to dielectrics for which this term is the potential energy).\par
Hence, the electric induction vector D*(?) does not correspond to the physical definition of the electric induction vector.\par
The physical meaning of the introduced vector) ( * ? P ? is clear from E L E P k L ? ? ? 2 1 ) ( * ? ? ? ? = = .\par
The interpretation of ?(?) as frequencydependent inductivity has been harmful for correct understanding of the real physical picture (especially in the educational processes). Besides, it has drawn away the researchers attention from some physical phenomena in plasma, which first of all include the transverse plasma resonance and three energy components of the magneto electro kinetic wave propagating in plasma \hyperref[b12]{[13]}\hyperref[b13]{[14]}. 
\section[{III.}]{III.} 
\section[{Dielectric Media}]{Dielectric Media}\par
Applied fields cause polarization of bound charges in dielectrics. The polarization takes some energy from the field source, and the dielectric accumulates extra electrostatic energy. The extent of displacement of the polarized charges from the equilibrium is dependent on the electric field and the coefficient of elasticity ?, characterizing the elasticity of the charge bonds. These parameters are related as ). 1 ( ) ( * 2 0 2 2 0 ? ? ? ? ? ? ? ? ? ? = p\par
It is appropriate to examine two limiting cases:?>>? 0 and?<<? 0 . If ?>>? 0 , ) 1 ( ) ( * 2 2 0 ? ? ? ? ? ? ? p ? =\par
, and the dielectric behaves just like plasma. This case has prompted the idea that at high frequencies there is no difference between dielectrics and plasma. The idea served as a basis for introducing the polarization vector in conductors \hyperref[b1]{[2]}. The difference however exists and it is of fundamental importance. In dielectrics, because of inertia, the amplitude of charge vibrations is very small at high frequencies and so is the polarization vector. The polarization vector is always zero in conductors.\par
For ?<<? 0 , IV. 
\section[{Magnetic Media}]{Magnetic Media}\par
The resonance phenomena in plasma and dielectrics are characterized by repeated electrostatickinetic and kinetic-electrostatic transformations of the charge motion energy during oscillations. This can be described as an electrokinetic process, and devices based on it (lasers, masers, filters, etc.) can be classified as electrokinetic units.\par
However, another type of resonance is also possible, namely, magnetic resonance. Within the current concepts of frequency-dependent permeability, it is easy to show that such dependence is related to magnetic resonance. For example, let us consider ferromagnetic resonance. A ferrite magnetized by applying a stationary field ? 0 parallel to the z-axis will act as an anisotropic magnet in relation to the variable external field. The complex permeability of this medium has the form of a tensor \hyperref[b14]{[15]}: Being the natural professional frequency, and? ? ? ? ? ? ? ? ? ? ? ? ? ? ? = L T T i i µ ? µ ? ? ? µ µ 0 0 0 ) ( * 0 ) ( * , where , 1 , ) ( , )\textbf{( 1 )}? 0 = µ 0 (µ?1)? 0 (4.2)\par
is the medium magnetization.\par
Taking into account Eqs.   ? ? ? ? ? ? ? ? ? ? ? ? ? = 2 2 2 0 ) 1 ( 1 . For ?>>? t H E rot y ? ? ? µ µ ? ? ? ? ? ? ? ? ? ? ? =? ? ? + = t d H t H E rot y y ? ? ? ) 1 ( 2 0 0 µ µ ? ? µ , or ? + = t d H C t H E rot y k y ? ? ? 1 0 ? ? µ . For ?<<? t H E rot y ? ? µ µ ? ? 0 = . The quantity ) 1 ( 1 2 0 ? ? = µ µ k C\par
can be described as kinetic capacitance \hyperref[b15]{[16]}\hyperref[b16]{[17]}. What is its physical meaning? If the direction of the magnetic moment does not coincide with that of the external magnetic field, the vector of the moment starts precessional motion at the frequency ? about the magnetic field vector. The magnetic moment m ? has the potential energyB m U m ? ? ? ? =\par
. Like in a charged condenser, U m is the potential energy because the precessional motion is inertia less (even though it is mechanical) and it stops immediately when the magnetic field is lifted. In the magnetic field the processional motion lasts until the accumulated potential energy is exhausted and the vector of the magnetic moment becomes parallel to the vector 0 H ? . Magnetic resonance occurs at the point ?=? and µ ? *(?)???. It is seen that the resonance frequency of the macroscopic magnetic resonator is independent of the line size and equals ?.\par
Thus, the parameter? ? ? ? ? ? ? ? ? ? ? = 2 2 2 0 ) 1 ( 1 ) ( * ? µ µ ? µ H\par
is not a frequency-dependent permeability.\par
V. 
\section[{Conclusion}]{Conclusion}\par
Thus, it has been found that along with the fundamental parameters ?? 0 and µµ 0 characterizing the electric and magnetic energy accumulated and transferred in the medium, there are two more basic material parameters L k and C k . They characterize kinetic and potential energy that can be accumulated and transferred in material media. L k was sometimes used to describe certain physical phenomena, for example, in super conductors, C k has never been known to exist. These four fundamental parameters ?? 0 , µµ 0 , L k and C k clarify the physical picture of the wave and resonance processes in material media in applied electromagnetic fields. Previously, only electromagnetic waves were thought to propagate and transfer energy in material media. It is clear now that the concept was not complete. In fact, magneto electro kinetic, or electro magneto potential waves travel in material media. The resonances in these media also have specific features. Unlike closed planes with electromagnetic resonance and energy exchange between electric and magnetic fields, material media have two types of resonanceelectro kinetic and magneto potential. Under the electro kinetic resonsnce the energy of the electric field changes to kinetic energy. In the case of magneto potential resonance the potential energy accumulated The notions of permittivity and permeability dispersion thus become physically groundless though ? * (?) and µ * (?) are handy for a mathematical description of the processes in material media. We should however remember their true meaning especially where educational processes are involved.\par
It is surprising that Eq. (3.29) actually accounts for the whole of electrodynamics beause all current electrodynamics problems can be solved using this equation. What is then a magnetic field? This is merely a convenient mathematical procedure which is not necessarily gives a correct result (e.g., in the case of parallel-moving charges). Now we can state that electrocurrent, rather than electromagnetic, waves travel in space. Their electric field and displacement current vectors are in the same plane and displaced by ?/2.\par
Any theory is dead unless important practical results are obtained of its basis. The use of the previously unknown transverse plasma resonance \hyperref[b13]{[14]} is one of the most important practical results following from this study.\begin{figure}[htbp]
\noindent\textbf{}\includegraphics[]{image-2.png}
\caption{\label{fig_0}}\end{figure}
        \begin{figure}[htbp]
\noindent\textbf{} \par 
\begin{longtable}{P{0.85\textwidth}}
Year 2014\\
13\\
I\\
ume XIV Issue VIII Version\\
( ) A Vol\\
Global Journal of Researches in Engineering\end{longtable} \par
  {\small\itshape [Note: .19) © 2014 Global Journals Inc. (US)]} 
\caption{\label{tab_3}}\end{figure}
 			\footnote{© 2014 Global Journals Inc. (US)} 		 		\backmatter  			  				\begin{bibitemlist}{1}
\bibitem[Akhiezer ()]{b3}\label{b3} 	 		\textit{},  		 			A I Akhiezer 		.  	 	 		\textit{Plasma Physics Nauka}  		1974.  	 
\bibitem[Mende ()]{b15}\label{b15} 	 		\textit{},  		 			F F Mende 		.  	 	 		\textit{New approachesin contemporary classical electrodynamics. Part I, Engineering Physics}  		2013. p. 1.  	 
\bibitem[Nicolsky and Nicolskaya ()]{b14}\label{b14} 	 		\textit{Electrodynamics and propagation of radio waves},  		 			V V Nicolsky 		,  		 			T I Nicolskaya 		.  		1989. Moscow, Nauka.  	 
\bibitem[Landau and Lifshits ()]{b1}\label{b1} 	 		\textit{Electrodynamics of continuous media},  		 			L D Landau 		,  		 			E M Lifshits 		.  		1973. Moscow.  	 
\bibitem[London ()]{b11}\label{b11} 	 		 			F London 		.  		\textit{Superfluids. Microscopic theory of superconductivity},  				 (Nev York)  		1950. Dower publ. 1.  	 
\bibitem[Mende]{b12}\label{b12} 	 		 			F F Mende 		.  		 \url{arXiv.org/abs/physics/0506083}  		\textit{Conception of the scalar-vector potential in contemporary electrodynamics},  				 	 
\bibitem[Mende ()]{b16}\label{b16} 	 		 			F F Mende 		.  		\textit{New approaches in contemporary classical electrodynamics. Part II, Engineering Physics},  				2013. p. 2.  	 
\bibitem[Mende]{b5}\label{b5} 	 		\textit{On refinement of certain laws of classical electrodynamics, arXiv},  		 			F F Mende 		.  		 physics/0402084.  		 	 
\bibitem[Mende ()]{b7}\label{b7} 	 		\textit{On refinement of equations of electromagnetic induction, -Kharkov},  		 			F F Mende 		.  		1988. Dep. p. .  	 	 (deposited in VINITI) 
\bibitem[Mende ()]{b9}\label{b9} 	 		\textit{On refinement of equations of electromagnetic induction,-Kharkov},  		 			F F Mende 		.  		1988. Dep. p. .  	 	 (deposited in VINITI) 
\bibitem[Mende ()]{b8}\label{b8} 	 		\textit{Origin of the new alternative electrodynamics},  		 			F F Mende 		.  		1993. Ukraine.  		 			Research Institute forCryogenic Instrument Engineering Minor State Enterprise at Institute for Low Temperature Physics and Engineering, Acad. Sci 		 	 	 (Preprint) 
\bibitem[Aleksandrov et al. ()]{b0}\label{b0} 	 		\textit{Oscillations and waves in plasma media},  		 			A F Aleksandrov 		,  		 			L S Bogdankevich 		,  		 			A A Rukhdze 		.  		1990. Moscow University Publishers.  	 
\bibitem[Mende ()]{b10}\label{b10} 	 		\textit{Role and place of the kinetic inductance of charges in classical electrodynamics, Engineering Physics},  		 			F F Mende 		.  		2012. p. 11.  	 
\bibitem[Mende and Spitsyn ()]{b6}\label{b6} 	 		\textit{Surface impedance in superconductors},  		 			F F Mende 		,  		 			A I Spitsyn 		.  		1985. Kiev, Naukova Dumka.  	 
\bibitem[
			IE
		 ()]{b4}\label{b4} 	 		 			IE 		.  		\textit{TammFundamentals ofthe theory of electricity, M.:Science},  				1989.  	 
\bibitem[Ginzburg ()]{b2}\label{b2} 	 		‘The propagation of electro magnetic waves in a plasma’.  		 			V L Ginzburg 		.  	 	 		\textit{Science}  		1967.  	 
\bibitem[Mende]{b13}\label{b13} 	 		\textit{Transversal plasma resonance in a non magnetized plasma and possibilities of practical employment of it},  		 			F F Mende 		.  		 \url{arXiv.org/abs/-physics//0506081}  		 	 
\end{bibitemlist}
 			 		 	 
\end{document}
