
$W=\int_{0}^{2} F d x$
$=\int_{0}^{2} 3.0 \times 10^{-4} e^{-0.2 x} \times 10 \times 3 d x$
$=9 \times 10^{-3} \int_{0}^{2} e^{-0.2 x} d x$
$=\frac{9 \times 10^{-3}}{0.2}\left[-e^{-0.2 \times 2}+1\right] B=3.0 \times 10^{-4} e^{-0.2 x}$
(By exponential function)
$=\frac{9 \times 10^{-3}}{0.2} \times\left[1-e^{-0.4}\right]$
$=9 \times 10^{-3} \times(0.33)=2.97 \times 10^{-3}\, \mathrm{J}$
Power required to move the conductor is, $P=\frac{W}{t}$
$P=\frac{2.97 \times 10^{-3}}{(0.2) \times 5 \times 10^{-3}}=2.97 \,\mathrm{W}$

Statement $I:$ Biot-Savart's law gives us the expression for the magnetic field strength of an infinitesimal current element (IdI) of a current carrying conductor only.
Statement $II :$ Biot-Savart's law is analogous to Coulomb's inverse square law of charge $q$, with the former being related to the field produced by a scalar source, Idl while the latter being produced by a vector source, $q$. In light of above statements choose the most appropriate answer from the options given below:
$\left[{m}_{{p}}=1.67 \times 10^{-27} {kg}, {e}=1.6 \times 10^{-19} {C},\right.$ Speed of light $\left.=3 \times 10^{8} {m} / {s}\right]$
(Assume that the current is flowing in the clockwise direction.)