  We investigate the validity of the Dirac Quantization Condition (DQC) for
magnetic monopoles in noncommutative space-time. We use an approach which is
based on an extension of the method introduced by Wu and Yang. To study the
effects of noncommutativity of space-time, we consider the gauge
transformations of $U_\star(1)$ gauge fields and use the corresponding deformed
Maxwell's equations. Using a perturbation expansion in the noncommutativity
parameter $\theta$, we show that the DQC remains unmodified up to the first
order in the expansion parameter. The result is obtained for a class of
noncommutative source terms, which reduce to the Dirac delta function in the
commutative limit.
