  The macroscopic limit at which the quantum-to-classical transition occurs
remains as one of the long-standing questions in the foundations of quantum
theory. There are evidences that the macroscopic limit to which the quantumness
of a system persists depends on the degree of interaction due to the
measurement processes. For instance, with a system having a considerably large
Hilbert space dimension, if the measurement is performed in such a way that the
outcome of the measurement only reveals a coarse-grained version of the
information about the individual level of the concerned system then the
disturbance due to the measurement process can be considered to be
infinitesimally small. Based on such coarse-grained measurement the dependence
of Bell inequality violation on the degree of coarsening has already been
investigated [Phys. Rev. Lett. 112, 010402 (2014)]. In this paper, we first
capture the fact that when local-realism is taken to be the defining notion of
classicality, the effect of the degree of coarsening on the downfall of
quantumness of a macroscopic entangled state can be compensated by testing a
Bell-inequality of a higher number of settings from a family of symmetric
Bell-inequalities if the number of settings is odd. However, on the contrary,
we show that such compensation can not be seen when we witness such
quantum-to-classical transition using symmetric Bell inequalities having an
even number of settings. Finally, complementing the above result, we show that
when unsteerability is taken as the classicality, for both odd and even numbers
of settings the degree of coarsening at which the quantum-to-classical
transition occurs can be consistently pushed ahead by testing a linear steering
inequality of a higher number of settings and observing its violation. We
further extend our treatment for mixed macroscopic entangled states
