Maxwell's equations are traditionally introduced as four independent postulates, each grounded in a distinct experimental law. Although empirically sound, this approach can obscure the logical structure that unifies them. This paper offers a pedagogical reconstruction based on local charge conservation, Helmholtz's theorem, and the experimental fact that electromagnetic disturbances propagate in vacuum with speed (c). A few natural auxiliary assumptions -- linearity, locality, and the simplest possible coupling to sources -- are stated explicitly. From the continuity equation and the physical necessity of a mediating field we argue that the electric and magnetic fields must be introduced. Helmholtz's theorem then demands that both divergences and curls of these fields be specified; coupling them to the available scalar and vector sources yields the inhomogeneous equations. Consistency with charge conservation forces the displacement current, making it a logical requirement rather than an empirical addition. The homogeneous equations follow from the same framework: (abla cdot mathbf{B} = 0) is the most parsimonious choice consistent with experiment, and requiring wave propagation at speed (c) fixes Faraday's law uniquely as (abla times mathbf{E} = -partial_t mathbf{B}). Once Maxwell's equations are established, the Lorentz force density (homathbf{E} + mathbf{J}timesmathbf{B}) emerges as the only dimensionally consistent expression compatible with the local conservation of momentum derived directly from the field equations. The argument employs only elementary vector calculus and is accessible to advanced undergraduates. We suggest that this unified narrative, which reveals the internal coherence of electromagnetism, can serve as a valuable complement to the traditional empirical presentation.