  In the strange metal phase of the high-$T_{c}$ cuprates, it is challenging to
explain the linear temperature dependence of the in-plane resistivity and the
quadratic temperature dependence of the inverse Hall angle. In this paper, we
investigate the temperature dependence of the in-plane resistivity and inverse
Hall angle in the nonlinear electrodynamics holographic model developed in our
recent work. Maxwell electrodynamics and Born-Infeld electrodynamics are
considered. Both cases support a wide spectrum of temperature scalings in
parameter space. For Maxwell electrodynamics, the T-linear in-plane resistivity
generally dominates at low temperatures and survives into higher temperatures
in a narrow strip-like manner. Meanwhile, the T-quadratic inverse Hall angle
dominates at high temperatures and extends down to lower temperatures. The
overlap between the T-linear in-plane resistivity and the T-quadratic inverse
Hall angle, if occurs, would generally present in the intermediate temperate
regime. The Born-Infeld case with $a>0$ is quite similar to the Maxwell case.
For the Born-Infeld case with $a<0$, there can be a constraint on the charge
density and magnetic field. Moreover, the overlap can occur for strong charge
density.
