(c) Force acting between two current carrying conductors
$F = \frac{\mu_{0}}{2\pi}\frac{I_{1}I_{2}}{d}\ l\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ldots(i)$
Where, $d =$ distance between the conductors,
$\ \ l =$ length of each conductor.
Again, $F^{'} = \frac{\mu_{0}}{2\pi}\frac{\left( - 2I_{1} \right)\left( I_{2} \right)}{(3d)}\ .l$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ = - \frac{\mu_{0}}{2\pi}\frac{2I_{1}I_{2}}{3d}\ .l\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ldots(ii)$
Thus, from Eqs. (i) and (ii)
$\frac{F^{'}}{F} = - \frac{2}{3}$
$\Rightarrow \ \ F^{'} = - \frac{2}{3}\ F$