  We investigate the role of symmetric quantum cloning machines (QCMs) in
quantifying the mutual incompatibility of quantum observables. Specifically, we
identify a cloning-based incompatibility measure whereby the incompatibility of
a set of observables maybe quantified in terms of how well a uniform ensemble
of their eigenstates can be cloned via a symmetric QCM. We show that this new
incompatibility measure $\mathcal{Q}_{c}$ is {\it faithful} since it vanishes
only for commuting observables. We prove an upper bound for $\mathcal{Q}_{c}$
for any set of observables in a finite-dimensional system and show that the
upper bound is attained if and only if the observables are mutually unbiased.
Finally, we use our formalism to obtain the optimal quantum cloner for a pair
of qubit observables. Our work marks an important step in formalising the
connection between two fundamental concepts in quantum information theory,
namely, the no-cloning principle and the existence of incompatible observables
in quantum theory.
