åćęč³Ŗć§ććå°ē·ć®é·ć \(l\) ćØęé¢ē© \(S\) ć«ćć£ć¦ęµęå¤ćå¤ććć¾ććé·ćć»ć©ęµęć大ććļ¼é»åćéćč·é¢ćé·ćļ¼ć太ćć»ć©ęµęćå°ććļ¼é»åć®éćéćåŗćļ¼ć
ęč³Ŗåŗęć®ćęµęć®ćććććć蔨ćć®ćęµęē \(\rho\)ćé¢äæå¼ćÆ \(R = \rho \cdot l / S\) ć§ććåå½¢ęé¢ćŖć \(S = \pi (d/2)^2 \propto d^2\) ćŖć®ć§ćē“å¾ć® 2 ä¹ć«åęÆä¾ćć¾ćć
ē“å¾ć®ęÆćÆå¹³ę¹ę ¹ćå „ćē¹ćč¦č½ćØććććļ¼\(R \propto 1/d^2\) ćŖć®ć§ \(d \propto 1/\sqrt{R}\)ļ¼ćåä½ęē®ćÆ \(1\ \mathrm{mm} = 10^{-3}\ \mathrm{m}\)ć\(1\ \mathrm{mm^2} = 10^{-6}\ \mathrm{m^2}\)ćęµęēć®åä½ćÆ \(\Omega \cdot \mathrm{m}\)ć