  In this present investigation, we explore the elastic scattering of pions
with nuclei ($\pi$-$A$), primarily influenced by the $\Delta$(1232) resonance,
within the Eikonal-Glauber model. The medium effects are incorporated by
considering nuclear-density ($\rho_A$) dependent masses of baryons and strong
coupling constants. These dependencies are computed and parameterized up to
$\mathcal{O}(\rho_A^2)$ based on the quark-meson coupling (QMC) model. The
Wood-Saxon type density profile is utilized for the bound nucleons within
finite nuclei. The element $\pi^+$-$N$ scattering cross section for the Glauber
approach is determined using the conventional effective Lagrangian method.
Subsequently, we analyze the total cross sections for elastic scattering with
$^4$He and $^{12}$C targets. Our numerical results demonstrate a favorable
agreement with JINR data for the $^4$He target, accurately reproducing the
total cross-section. However, when considering the $^{12}$C target, deviations
of approximately $\lesssim10\%$. We also consider the multiple-scattering
effects inside the nucleus approximately, using the single-channel meson-baryon
Bethe-Salpeter equation, resulting in the effective width broadening of the
$\Delta$ resonance to reproduce the data better.
