Comments on Skin Effect in Solitary Solid Tubular Conductor

<table>Dependence of the amplitude of phasor <svg height="15.675" id="M295" style="vertical-align:-4.28859pt" version="1.1" viewbox="0 0 10.4375 15.675" width="10.4375" xmlns="http://www.w3.org/2000/svg">
<g transform="matrix(1.25,0,0,-1.25,0,15.675)">
<g transform="translate(72,-59.46)">
<text transform="matrix(1,0,0,-1,-71.95,63.79)">
<tspan style="font-size: 12.50px; " x="0" y="0">𝐽</tspan>
</text>
<g>
<path d="m -71.95,60.75 8.25,0" style="fill:none;stroke:#000000;stroke-width:0.82499999;stroke-linecap:butt;stroke-linejoin:miter;stroke-miterlimit:10;stroke-opacity:1;stroke-dasharray:none"></path>
</g>
</g>
</g>
</svg> on <svg height="7.0124998" id="M296" style="vertical-align:-0.0pt" version="1.1" viewbox="0 0 6.5 7.0124998" width="6.5" xmlns="http://www.w3.org/2000/svg">
<g transform="matrix(1.25,0,0,-1.25,0,7.0125)">
<g transform="translate(72,-66.39)">
<text transform="matrix(1,0,0,-1,-71.95,66.44)">
<tspan style="font-size: 12.50px; " x="0" y="0">𝑟</tspan>
</text>
</g>
</g>
</svg> in cases a and b of Example <a href="https://static.hindawi.com/articles/amp/volume-2011/983678/figures/#ex4">3.4</a>; number of partial conductors <svg height="11.1" id="M297" style="vertical-align:-0.17555pt" version="1.1" viewbox="0 0 56.262501 11.1" width="56.262501" xmlns="http://www.w3.org/2000/svg">
<g transform="matrix(1.25,0,0,-1.25,0,11.1)">
<g transform="translate(72,-63.12)">
<text transform="matrix(1,0,0,-1,-71.95,63.35)">
<tspan style="font-size: 12.50px; " x="0" y="0">𝑁</tspan>
<tspan style="font-size: 12.50px; " x="14.103384" y="0">=</tspan>
<tspan style="font-size: 12.50px; " x="26.143772" y="0">2</tspan>
<tspan style="font-size: 12.50px; " x="32.395271" y="0">5</tspan>
<tspan style="font-size: 12.50px; " x="38.646774" y="0">0</tspan>
</text>
</g>
</g>
</svg>.</table>

Advances in Mathematical Physics

Comments on Skin Effect in Solitary Solid Tubular Conductor

Figure 6