I2ρIr\frac{I^{2} \rho I}{r}rI2ρI
I2ρlπr2\frac{I^{2} \rho l}{\pi r^{2}}πr2I2ρl
I2ρIπr\frac{I^{2} \rho I}{\pi r}πrI2ρI
IρI2π2r2\frac{I \rho I^{2}}{\pi^{2} r^{2}}π2r2IρI2