  In our short review, we consider the transport properties of strongly
correlated Fermi systems like heavy fermion metals and high-$T_c$
superconductors. Their transport properties are defined by strong
inter-particle interaction forming flat bands in these compounds. Indeed, in
contrast to the behavior of the transport properties of conventional metals,
the strongly correlated compounds exhibit the linear in temperature
resistivity, $\rho(T)\propto T$. We analyze the magnetoresistance and show that
it under the application of magnetic field becomes negative. It is shown that
near a quantum phase transition, when the density of electronic states
diverges, semiclassical physics remains applicable to describe the resistivity
$\rho$ of strongly correlated metals due to the presence of a transverse
zero-sound collective mode, representing the phonon mode in solids. We
demonstrate that when $T$ exceeds the extremely low Debye temperature $T_D$,
the resistivity $\rho(T)$ changes linearly with $T$, since the mechanism of
formation of the $T$-dependence $\rho(T)$ is similar electron-phonon mechanism,
which predominates at high temperatures in ordinary metals. Thus, in the region
of $T$-linear resistance, electron-phonon scattering leads to a lifetime of
$\tau$ quasiparticles practically independent of the material, which is
expressed as the ratio of the Planck constant $\hbar$ to the Boltzmann constant
constant $k_B$, $T\tau\sim \hbar/k_B$. We explain that due to the
non-Fermi-liquid behavior the real part of the frequency-dependent optical
conductivity $\sigma^R_{opt}(\omega)$ exhibits a scaling behavior, and
demonstrates the unusual power law behavior
$\sigma^R_{opt}(\omega)\propto\omega^{-1}$, rather than the well-known one
shown by conventional metals, $\sigma^R_{opt}(\omega)\propto\omega^{-2}$.
